<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2015.63033</article-id><article-id pub-id-type="publisher-id">JMP-54287</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Prediction and Derivation of the Hubble Constant from Subatomic Data Utilizing the Harmonic Neutron Hypothesis
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>onald</surname><given-names>William Chakeres</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Richard</surname><given-names>Vento</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Radiology, The Ohio State University, Columbus, USA</addr-line></aff><aff id="aff2"><addr-line>Columbus State Community College, Columbus, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>donald.chakeres@osumc.edu(OWC)</email>;<email>rpvento@aol.com(RV)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>02</month><year>2015</year></pub-date><volume>06</volume><issue>03</issue><fpage>283</fpage><lpage>302</lpage><history><date date-type="received"><day>5</day>	<month>February</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>23</month>	<year>February</year>	</date><date date-type="accepted"><day>27</day>	<month>February</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  Purpose: To accurately derive 
  H
  <sub>0</sub> from subatomic constants in abscence of any standard astronomy data. Methods: Recent astronomical data have determined a value of Hubble’s constant to range from 76.9
  <sup>+3.9</sup>
  <sub>-3.4</sub>
  <sup>+10.0</sup>
  <sub>-</sub>
  <sub>8.0</sub>
   to 67.80 &#177; 0.77 (km/s)/Mpc. An innovative prediction of H<sub>0</sub> is obtained from harmonic properties of the frequency equivalents of neutron, n<sup>0</sup>, in conjunction with the electron, e; the Bohr radius, α<sub>0</sub>; and the Rydberg constant, R. These represent integer natural unit sets. The neutron is converted from its frequency equivalent to a dimensionless 
  constant
  ,<img src="Edit_bc94c349-e457-4382-a996-db64c9253863.bmp" width="245" height="20" alt="" />
  , where “h” = Planck’s constant, and “s” is measured in seconds. The fundamental frequency, V<sub>f</sub>
  , 
  is the first integer series set <img src="Edit_4aedcdaa-d764-4ea8-add8-884db5c6c1fd.bmp" width="75" height="18" alt="" />
  .
   All other atomic data are scaled to V<sub>f</sub> as elements in a large, but a countable point set. The present value of H<sub>0</sub> is derived and Ω<sub>M</sub> assumed to be 0. An accurate derivation of H<sub>0</sub> is made using a unified power law. The integer set of the first twelve integers N<sub>12</sub> {1,2,
  …
  ,11,12}, and their harmonic fractions <img src="Edit_1c012da1-6d31-409f-83e4-3e9da475b1b3.bmp" width="147" height="18" alt="" />
   
  exponents of V<sub>f</sub> 
  represent the 
  first generation of bosons and particles. Thepartial harmonic fraction, -
  3/4, is exponent of V<sub>f</sub> which represents H<sub>0</sub>. The partial fraction 
  3/4 is 
  associated with a component of neutron beta decay kinetic energy. Results: H<sub>0</sub>
   is 
  predicted utilizing a previously published line used to derive Planck time, t<sub>p</sub>. The power law line of the experimental H<sub>0</sub>
   and 
  t<sub>p</sub>
   
  conforms to the predicted line. Conclusions: H<sub>0</sub>
   can be predicted from subatomic data related to the neutron and hydrogen.
 
</html></p></abstract><kwd-group><kwd>Hubble Constant</kwd><kwd> Neutron</kwd><kwd> Unification Model</kwd><kwd> Planck Time</kwd><kwd> Quantum Gravity</kwd><kwd> Neutron Beta Decay</kwd><kwd> Neutrino</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><sec id="s1_1"><title>1.1. The Hubble Constant</title><p>Hubble’s law refers to the observation that objects at greater than 10 megaparsecs have a Doppler shift interpretable as a relative velocity. The Doppler shift is most commonly quoted as a velocity in (km/s)/Mpc. Galaxies appear to be moving at a rate proportional to their distance from the Earth. This is typically interpreted as evidence of the expansion of the Universe. A high precision Hubble constant H<sub>0</sub>, is an important physical constant, [<xref ref-type="bibr" rid="scirp.54287-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.54287-ref6">6</xref>] . Hubble’s Law relates a velocity to H<sub>0</sub> as a proportionality constant with units of s<sup>−1</sup> times the proper distance, D. The reciprocal of H<sub>0</sub> is the Hubble time. The reported velocities at one Mpc vary with the model and published values include: 76.9<sup>+3.9</sup><sub>−3.4</sub><sup>+10.0</sup><sub>−8.0</sub> km・s<sup>−1</sup>・Mpc<sup>−1</sup>, 69.32 &#177; 0.80 km・s<sup>−1</sup>・Mpc<sup>−1</sup>, 74.3 &#177; 2.1 km・s<sup>−1</sup>・Mpc<sup>−1</sup>, 67.3 &#177; 1.2 km・s<sup>−1</sup>・Mpc<sup>−1</sup>, <xref ref-type="table" rid="table1">Table 1</xref>, [<xref ref-type="bibr" rid="scirp.54287-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.54287-ref6">6</xref>] . The methods, probes, of measurement and derivation of the H<sub>0</sub> are different. This leads to divergent estimated values based on the methods and model. The methods include the Hubble telescope, Chandra and Sunyaev-Zeldovich Effect data from the Owens Valley Radio Observatory and the Berkeley-Illinois-Maryland Association interferometric arrays, Wilkinson Microwave Anisotropy Probe, and cosmic microwave background, CMB, temperature and lensing-potential power spectra The experimental Hubble rates range from 2.18(4) &#215; 10<sup>−18</sup> s<sup>−1</sup> to 2.49(12) &#215; 10<sup>−18</sup> s<sup>−1</sup>. The reported Hubble time, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x10.png" xlink:type="simple"/></inline-formula>, equals approximately 4.35 &#215; 10<sup>17</sup> s or 13.8 byr. The approximate Hubble length equals <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x11.png" xlink:type="simple"/></inline-formula> or 13.8 blyr. In this model the predicted H<sub>0</sub> is assumed to be present experimental value with an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x12.png" xlink:type="simple"/></inline-formula> of 0.</p></sec><sec id="s1_2"><title>1.2. The Goals</title><p>The goal of this work is to derive a high precision H<sub>0</sub>, and subsequently a Hubble length, and Hubble time from natural unit frequency equivalents as integer sets of the neutron, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x13.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x14.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x15.png" xlink:type="simple"/></inline-formula>; the hydrogen ionization energy; the Rydberg constant R,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x16.png" xlink:type="simple"/></inline-formula>; the Bohr radius<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x17.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x18.png" xlink:type="simple"/></inline-formula>; and the electron, e,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x19.png" xlink:type="simple"/></inline-formula>; and the finite integer and harmonic integer set of N<sub>12</sub> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula> the harmonic fractions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x22.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] . N<sub>12</sub> are referred to as integer fraction exponents,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x23.png" xlink:type="simple"/></inline-formula>. Another goal is to demonstrate that experimental Planck time squared, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x24.png" xlink:type="simple"/></inline-formula>and H<sub>0</sub> follow a previously predicted power law relationship used to derive<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x25.png" xlink:type="simple"/></inline-formula>. [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] The proportionality constants of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x26.png" xlink:type="simple"/></inline-formula>, and H<sub>0</sub> ratios with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x27.png" xlink:type="simple"/></inline-formula> are derived, and compared to the known experimental values.</p></sec><sec id="s1_3"><title>1.3. The Harmonic Neutron Hypothesis (HNH)</title><p>The following is a review and explanation of the harmonic neutron hypothesis. It was initially copyrighted in 2006 and published in 2009, [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] . All of the physical constants are evaluated as frequency equivalents, and secondarily as dimensionless coupling constant ratios in an exponential integer or integer fraction system. Any single physical unit could be utilized, but Hertzian frequency (Hz) was arbitrarily chosen since the whole physical</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparison of experimental, experimental line fit, and derived H<sub>0</sub>, velocities, exponents, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x28.png" xlink:type="simple"/></inline-formula> for H<sub>0</sub> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x29.png" xlink:type="simple"/></inline-formula>. <xref ref-type="table" rid="table1">Table 1</xref> lists s<sup>−1</sup>, and s<sup>2</sup> for the four experimental known, line fit known, and derived values for H<sub>0</sub>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x30.png" xlink:type="simple"/></inline-formula>. The derived and line fit known experimental data are remarkable similar</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >s<sup>2</sup> or s<sup>−1</sup></th><th align="center" valign="middle" >km・s<sup>−1</sup>・Mpc<sup>−1</sup></th><th align="center" valign="middle" >Exponent</th><th align="center" valign="middle" >δ</th></tr></thead><tr><td align="center" valign="middle" >H<sub>0k</sub></td><td align="center" valign="middle" >2.49(12) &#215; 10<sup>−18</sup> s<sup>−1</sup></td><td align="center" valign="middle" >76.9<sup>+3.9</sup><sub>−3.4</sub><sup>+10.0</sup><sub>−8.0</sub></td><td align="center" valign="middle" >−7.53(12) &#215; 10<sup>−1</sup></td><td align="center" valign="middle" >−3.70(90) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >H<sub>0k</sub></td><td align="center" valign="middle" >2.408(67)&#215;10<sup>−18</sup> s<sup>−1</sup></td><td align="center" valign="middle" >74.3 &#177; 2.1</td><td align="center" valign="middle" >−7.543(8) &#215; 10<sup>−1</sup></td><td align="center" valign="middle" >−4.33(50) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >H<sub>0k</sub></td><td align="center" valign="middle" >2.24(2) &#215; 10<sup>−18</sup> s<sup>−1</sup></td><td align="center" valign="middle" >69.32 &#177; 0.80</td><td align="center" valign="middle" >−7.556(16) &#215; 10<sup>−1</sup></td><td align="center" valign="middle" >−5.62(20) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >H<sub>0k</sub></td><td align="center" valign="middle" >2.18(4) &#215; 10<sup>−18</sup> s<sup>−1</sup></td><td align="center" valign="middle" >67.3 &#177; 1.2</td><td align="center" valign="middle" >−7.562(3) &#215; 10<sup>−1</sup></td><td align="center" valign="middle" >−6.17(32) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >H<sub>0kline fit</sub></td><td align="center" valign="middle" >2.33(11) &#215; 10<sup>−18</sup> s<sup>−1</sup></td><td align="center" valign="middle" >71.9(36)</td><td align="center" valign="middle" >−7.549(11) &#215; 10<sup>−1</sup></td><td align="center" valign="middle" >−4.99(32) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >H<sub>0</sub><sub>d</sub></td><td align="center" valign="middle" >2.29726680(12) &#215; 10<sup>−18</sup> s<sup>−1</sup></td><td align="center" valign="middle" >70.886246(4)</td><td align="center" valign="middle" >−7.55202112(1) &#215; 10<sup>−1</sup></td><td align="center" valign="middle" >−5.2021124(11) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x31.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.82611(11) &#215; 10<sup>−86</sup> s<sup>2</sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >−3.670879(12)</td><td align="center" valign="middle" >−1.37371(1) &#215; 10<sup>−2</sup></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x32.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.82611(11) &#215; 10<sup>−86</sup> s<sup>2</sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >−3.670879(12)</td><td align="center" valign="middle" >−1.37371(1) &#215; 10<sup>−2 </sup></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x33.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.8261712(1) &#215; 10<sup>−86</sup> s<sup> </sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >−3.670879366(1)</td><td align="center" valign="middle" >−1.3736509(1) &#215; 10<sup>−2 </sup></td></tr></tbody></table></table-wrap><p>system can logically be evaluated as a unified quantum spectrum. The primary natural unit is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x34.png" xlink:type="simple"/></inline-formula>. All possible physical values are defined by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x35.png" xlink:type="simple"/></inline-formula> and integer fractions. The unit system of the HNH is maximally simplified with the units for Planck’s constant, charge, and speed of light all equaling 1. Energy, mass, frequency, temperature are all equal. The distance is 1 divided by frequency. The speed of light equals <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x36.png" xlink:type="simple"/></inline-formula> times the dis-</p><p>tance<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x37.png" xlink:type="simple"/></inline-formula>, Compton radius of the neutron. The maximum Lorentz factor equals<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x38.png" xlink:type="simple"/></inline-formula>. Velocity squared is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x39.png" xlink:type="simple"/></inline-formula>.</p><p>The primary hypothesis is that the fundamental constants are inter-related by simple, ubiquitous mathematical and geometric integer patterns. The first twelve integers, N<sub>12</sub>, and their harmonic fractions, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x40.png" xlink:type="simple"/></inline-formula>, provide the basis for a coherent theory defining the first generation of bosons and particles, used in a power law computation for defining physical phenomena, <xref ref-type="table" rid="table2">Table 2</xref>. The model utilizes the dimensional analysis methods of Rayleigh’s method and the Buckingham Pi Theorem, where the exponential base is the dimensionless neutron annihilation frequency, Hz-s, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x41.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x42.png" xlink:type="simple"/></inline-formula>, and the exponents are combinations of 1 plus or minus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x43.png" xlink:type="simple"/></inline-formula>. Buckingham’s pi theorem states that physical laws are independent of the form of the physical units. Therefore, acceptable laws of physics are homogeneous in all dimensions.</p><p>The Equality Pair Transformations (EPTs) inter―relate matter, electromagnetic energy, and kinetic energy transformations. EPT are common physical phenomena that can be described by Feynman diagrams, but necessitate a definitional approach when utilized in this model. Each EPT is associated with a point transformation from one state to another, or from one force to another, such as, kinetic energy to electromagnetic energy, electromagnetic energy to matter, or vice-versa. This occurs when there is a scale equality of two different states or forces. The pair is identically scaled phenomena, but can represent two different dual (paired) physical manifestations of different forces or states. This is the essence of particle-wave duality paradox. Examples are matter-antimatter pair production or annihilation; or the transformation of electromagnetic energy to kinetic energy as in the photoelectric effect. Not only is there a conservation-equality of total energy-matter, but also a transformation of state or force. These transformations are always associated with symmetric pairs.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> First generation particles and bosons. <xref ref-type="table" rid="table2">Table 2</xref> lists the first generation physical constants related to neutron beta decay, n<sub>ie</sub>, n<sub>ife</sub>, and the partial harmonic fractions associated with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x44.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x45.png" xlink:type="simple"/></inline-formula>. There is no physical entity associated with the n<sub>ife</sub>, 9</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Constant unit</th><th align="center" valign="middle" >n<sub>ie</sub> or n<sub>ife</sub></th><th align="center" valign="middle" >1 &#177; 1/n<sub>ife</sub>, qf</th></tr></thead><tr><td align="center" valign="middle" >Elemental gravitational kinetic energy of the electron in hydrogen</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >−1</td></tr><tr><td align="center" valign="middle" >h, electromagnetic energy, boson</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0, 1 − 1/1</td></tr><tr><td align="center" valign="middle" >n<sup>0</sup>, elemental mass, strong force</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >Beta decay kinetic energy, anti-neutrino mass, cosmic background microwave, CMB, peak spectral radiance</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1/2, 1 − 1/2</td></tr><tr><td align="center" valign="middle" >Rydberg constant, R, em energy, boson</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2/3, 1 − 1/3</td></tr><tr><td align="center" valign="middle" >Beta decay kinetic energy, muon anti―neutrino</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3/4, 1 − 1/4</td></tr><tr><td align="center" valign="middle" >Bohr radius, α<sub>0</sub>, distance, or beta decay kinetic energy</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >4/5, 1 − 1/5</td></tr><tr><td align="center" valign="middle" >Beta decay kinetic energy, Tau anti―neutrino</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >5/6, 1 − 1/6</td></tr><tr><td align="center" valign="middle" >Electron, e, mass, matter</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >6/7, 1 − 1/7</td></tr><tr><td align="center" valign="middle" >Beta decay kinetic energy</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >7/8, 1 − 1/8</td></tr><tr><td align="center" valign="middle" >Up quark, u, matter</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >9/10, 1 − 1/10</td></tr><tr><td align="center" valign="middle" >Down quark, d, matter</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >10/11,1 − 1/11</td></tr><tr><td align="center" valign="middle" >α<sup>−1</sup>, reciprocal fine structure constant, coupling constant</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >1/11</td></tr><tr><td align="center" valign="middle" >Higgs boson, H<sup>0</sup>, boson</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >12/11, 1 + 1/11</td></tr><tr><td align="center" valign="middle" >W, Z, boson</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >13/12, 1 + 1/12</td></tr></tbody></table></table-wrap><p>The primary fundamental EPT scaling HNH is neutron anti-neutron pair production, and is the scaling factor used to derive further observable phenomena. The fundamental EPT ratio set is composed of a natural physical unit as a consecutive integer series representing the transformation of electromagnetic energy into frequency multiples matter associated with neutron/anti-neutron pair production. The integrally spaced dimensionless elements, v<sub>f</sub> in V<sub>f</sub>, are based on the ratio of the respective annihilation frequencies of that physical constant to that of the neutron. At the point where the photon integer frequency series has enough energy to be scaled identically with elemental neutral matter equivalent represents the fundamental EPT. The series restarts again at 1 with each integer representing the number of nucleons in elemental matter or groups of nucleons at the EPT of pair production point. Elements in the set V<sub>f</sub> scale all of the possible physical phenomena under consideration.</p></sec><sec id="s1_4"><title>1.4. The Empirical Observations Leading to the HNH</title><p>The neutron annihilation frequency, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x46.png" xlink:type="simple"/></inline-formula>, is the fundamental coupling constant, and the basis for EPTs on the set V<sub>f</sub>. We assume that there exists a gravitational binding energy of the electron to the proton in hydrogen, equally as important to the units of gravitational energy, as the ionization energy of hydrogen is to the electromagnetic force. The genesis of this hypothesis was based on the empirical observation that there are integer exponent relationships of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x47.png" xlink:type="simple"/></inline-formula> between the twice the frequency equivalent of the gravitational binding energy of the electron in hydrogen, the energy of Planck’s constant, h-Hz, and the frequency equivalent of the neutron.</p><p>Twice the frequency equivalent of the gravitational binding energy of the electron in hydrogen, 2 &#215; 2.90024(22) &#215; 10<sup>−24</sup> Hz equals 5.80048(44) &#215; 10<sup>−24</sup> Hz. We label here the gravitational binding energy of the electron in hydrogen as the elemental graviton. The frequency equivalent of Planck’s constant, h, is 1 Hz. Here,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x48.png" xlink:type="simple"/></inline-formula>Hz is 2.271859078(50) &#215; 10<sup>23</sup> Hz. The reciprocal of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x49.png" xlink:type="simple"/></inline-formula> is 4.4016815(1) &#215; 10<sup>−24</sup>, and is almost iden-</p><p>tical to twice the binding gravitational frequency of the electron in hydrogen.</p><p>The factor two in the gravitational binding energy of the electron to the proton arises from the fact that it is a kinetic energy. This “2” has the same origin as the “2” in the Schwarzschild radius equation, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x50.png" xlink:type="simple"/></inline-formula>, and both transform kinetic energy into an electromagnetic equivalent. This is also the “2” associated with an equality “pair”. All three force-state unit values are separated by a ratio of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x51.png" xlink:type="simple"/></inline-formula> Each represents unit step values for elemental gravitational kinetic, electromagnetic, and the elemental strong nuclear forces. The frequency</p><p>equivalent of the gravitational electron binding energy when multiplied by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x52.png" xlink:type="simple"/></inline-formula> equals 1.3178, and the nor-</p><p>malized value of 1 Hz for Planck’s constant h, times<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x53.png" xlink:type="simple"/></inline-formula>, equals <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x54.png" xlink:type="simple"/></inline-formula> in Hz. The coupling constant ratios are</p><p>represented by an injective mapping of the sequence: {−1, 0, 1, 2} to exponents of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x55.png" xlink:type="simple"/></inline-formula> Hz. These integer</p><p>exponents, are referred to as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x56.png" xlink:type="simple"/></inline-formula> for integer exponents. Each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x57.png" xlink:type="simple"/></inline-formula> is associated with a different force and state. Thus there is a discrete quantum relationship similar to blackbody spectra, and a power law. The distribution of energy over time is exponential for many physical systems including magnetic resonance relaxation.</p><p>Energy multiples of Planck’s constant, h, is also an integer based wavelength or frequency system. This is identical to the resonant modes of a vibrating string. Planck’s constant represents integral units of electromagnetic energy. Though h is quantum by definition, its actual physical manifestation in black body radiation appears to be continuous. When the divisions between the physical values associated with each n unit are smaller than experimental accuracy then the physical system appears to be Almost Everywhere (A.E.) continuous, but is none the less conceptually and mathematically integer-based <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>If this initial EPT observation is valid, then there logically should be a similarly scaled transformation between the unit values of the gravitational and electromagnetic forces. At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x58.png" xlink:type="simple"/></inline-formula> integral steps of gravitational units, i.e. twice the elemental graviton, this energy could represent an electromagnetic wave with a frequency of</p><p>1 Hz. At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x59.png" xlink:type="simple"/></inline-formula> integral steps of electromagnetic units, at 1 Hz, this energy could represent a neutron, at a fre-</p><p>quency of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x60.png" xlink:type="simple"/></inline-formula> Hz. At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x61.png" xlink:type="simple"/></inline-formula> integral steps of nucleon units, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x62.png" xlink:type="simple"/></inline-formula>Hz, this mass could represent the unit mass</p><p>of a black hole, at a frequency of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x63.png" xlink:type="simple"/></inline-formula> Hz, 5.16134367(12) &#215; 10<sup>46</sup> Hz. This is an extremely dense from of</p><p>matter, and must be the mass of individual unit forming a black hole analogous of neutrons forming elemental matter. This latter mass’s Compton radius is smaller than its Schwarzschild radius, and must represent the matter of a black hole.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Point plots of a consecutive integer series in linear, 1/n, and log<sub>e</sub>(n) formats. <xref ref-type="fig" rid="fig1">Figure 1</xref> plots three different geometric, mathematical formats of the consecutive integer sequence of n from −∞ to ∞. All three of these are seen in the model, but each in the appropriate physical and mathematical context. All are discrete series of individual points. The top row is a standard linear plot which is bound on both extremes by −∞ to ∞. The middle plot is 1/n. It is bound from −1 to +1. This is the origin of the fundamental constants where there is dense clustering the closer the mass is to the neutron, and increasingly sparse at the extremes. <xref ref-type="fig" rid="fig2">Figure 2</xref>, <xref ref-type="fig" rid="fig3">Figure 3</xref> demonstrates that a 2d unit based system is associated with these identical harmonic fraction possibilities. The lower plot is log<sub>e</sub>(n). It also extends from by −∞ to ∞. This pattern also has a pseudo-continuous appearance as n increases. For a large V<sub>f</sub> system only those n values that are small will appear to be discrete</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/10-7502135x64.png"/></fig></sec><sec id="s1_5"><title>1.5. Assignment of Fundamental Physical Constants to Principal Quantum Numbers, n<sub>ief</sub></title><p>In this method all of the physical phenomena are evaluated as exponents of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x65.png" xlink:type="simple"/></inline-formula>. Each physical constant is associated with an integer identical to all quantum systems. The known exponent, exp<sub>k</sub>, of the base <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x66.png" xlink:type="simple"/></inline-formula></p><p>for any physical constant is the natural log <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x67.png" xlink:type="simple"/></inline-formula> of the frequency equivalent of that constant divided by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x68.png" xlink:type="simple"/></inline-formula>. This is a classic exponent base transformation. The difference between the known exponent and</p><p>its associated partial fraction represents the δ factor.</p><p>Inspection of an integer-based exponent system of the forces/states, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x69.png" xlink:type="simple"/></inline-formula>Hz is a linear plot in the ex-</p><p>ponential domain Figures 1-4. The only other possible point values are the harmonic fractions, &#177;1/n<sub>ife</sub> and harmonic mixed partial fractions, 1 &#177; 1/n<sub>ife</sub>. These integer based exponents are associated with the observable fundamental constants. For this paper the only n<sub>ife</sub><sub> </sub>utilized are points in N<sub>12</sub>, since they are associated with the first generation of kinetic energies, particles, and bosons of neutron beta decay, <xref ref-type="table" rid="table2">Table 2</xref>, <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>Assignment of the n<sub>ife</sub> is dependent on that value fulfilling a power law relationship with the natural unit values of the first two natural integer sets. For the simplest situation the fundamental constant is related to the n<sub>ife</sub><sub> </sub>closest to 1 divided by 1 minus the exponent of the constant. If that value is positive then the partial harmonic fraction is 1 − 1/n<sub>ife</sub>. If the value is negative then the partial harmonic fraction is 1 + 1/n<sub>ife</sub>. This is not the greatest integer function. However, the n<sub>ife</sub> value can be driven far from the closest n<sub>ife</sub> value by the power law imperative or the fact that some of the constants are divided or multiple by 2. Utilizing these relationships it is possible to logically assign the physical phenomena of the neutron beta decay process to a specific partial harmonic fraction, <xref ref-type="table" rid="table2">Table 2</xref> [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] .</p><p>The simplest sinusoidal system that is related to a consecutive integer series is the possible wavelengths and frequencies of a vibrating string. This is associated with the harmonic sequence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x70.png" xlink:type="simple"/></inline-formula>, and the origin of “harmonic” in the model’s name. <xref ref-type="fig" rid="fig1">Figure 1</xref>. Many of the properties of the model are analogous to or identical with the mathematics and physics of music. Pure number properties are important in music, and the HNH physical model such as positive or negative, even or odd, and prime, and composite. These properties also represent imperatives that define the n<sub>ife</sub> of associated entities and the hierarchy of the physical constants.</p><p>Thus, the HNH model hypothesizes that physical constants represent a multi-layered simultaneously linear and exponential inter-locking, transformational integer series, with classic harmonic properties, in both the linear and exponential domains. These types of harmonic/repeating pattern systems are remarkably unified, where if any frequency and its associated integer value are known, then an infinite number of associated possible harmonic fractions and frequencies of the system are defined in Tables 2-4, <xref ref-type="fig" rid="fig1">Figure 1</xref> of reference [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] .</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Combined integer point and exponential plot of the fundamental unit forces separated by a ratio of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula>; multi- physical units of the X-axis. <xref ref-type="fig" rid="fig2">Figure 2</xref> is an exponential plot of the multiple X-axis unit values and their associated degenerate integer possibilities for energy, mass, frequency, distance dimension, velocity, density, gravitational, EM, elemental strong, and black hole elements. Each is a series of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula> points starting at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula> and n increasing from left to right. They start as individual points, red circles, but become pseudo-continuous to the right. Each force unit value is separated by a ratio of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula>, red dots and vertical blue lines. The upper row represents the distances, EM wavelengths, and mass Compton radii. Points to left of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula> represent possible degenerate velocity ratios <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x77.png" xlink:type="simple"/></inline-formula> values, of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x78.png" xlink:type="simple"/></inline-formula>. The points to the right of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x79.png" xlink:type="simple"/></inline-formula> represent all of the possible kinetic elemental graviton energy levels, two times the gravitational binding energy of the electron in hydrogen. Points to the right of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x80.png" xlink:type="simple"/></inline-formula><sup> </sup>are identical to Planck’s equation E equals n Hz times h, and black body radiators. The points to the right of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x81.png" xlink:type="simple"/></inline-formula><sup> </sup>represent the chemical periodic chart and continues to any combination of elemental masses. The points to the right of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x82.png" xlink:type="simple"/></inline-formula> must represent highly dense element units of matter of black holes, BH</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/10-7502135x71.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> A universal harmonic 2d plane with an exponential base of 4 demonstrating the properties of a universal ratio, exponent, 1/n calculator. <xref ref-type="fig" rid="fig3">Figure 3</xref> is a 2d plot of a system identical in character to the universal harmonic exponent plane, <xref ref-type="fig" rid="fig4">Figure 4</xref>. This is a simplified example where the V<sub>f</sub> = 4. This is both an integer and exponential series. The number, 4, is chosen to illustrate the nature of this 2d space in a comprehensible fashion. This 2d space represents a very powerful geometry that is similar to a slide rule, but with infinite flexibility. This includes all of the possibilities that cannot be displayed on a line plot. The blue points represent the only valid integer exponents of V<sub>f</sub>. In this case any absolute sum of an x and y vector that adds to 1 is a potentially valid integer exponent point. The only other possible valid points are those that fall on lines that connect between two integer points, blue dots. Any absolute x plus y orthogonal distance of 1 is identical to multiplying or dividing that number by 4 in the frequency domain. Therefore an absolute unit distance from the (0,0) point forms a diamond pattern. This is identical to the actual physical constants seen in <xref ref-type="fig" rid="fig4">Figure 4</xref> from [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] . The exponent of V<sub>f</sub> equals x + y at any point. The red lines are identity lines, all with the same exponent and frequency. The δ-values represent the exponent minus the x value, or (x + y) − x, and therefore equals y. The black solid and dashed lines all converge on (0,0), which equals a frequency of 1. In this specialized case these lines define v<sub>f</sub> of 1, 4, 16, and 64. The vertical dashed blue lines represent the fractional exponents of each v<sub>f</sub> of 1/2 and 2/3. The X-axis literally represents any exponent. In a continuous system any exponent of any V<sub>f</sub> represents the intersection of a vertical line at x, and the line connecting (0,0) to any V<sub>f</sub> value at x equals 1. The values of any point on a line in this space is defined totally from the perspective of V<sub>f</sub>. Two points can define any ratio, and simultaneously define any δ-line. Lines not passing through (0,0) also define a well-defined pattern, but are more complicated to describe</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/10-7502135x83.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Universal 2d harmonic plane plot of the known and derived subatomic entities, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula>, H<sub>0</sub>. <xref ref-type="fig" rid="fig4">Figure 4</xref> is a universal harmonic exponent plot of the relevant physical constants. The X-axis equals the qf − 1 or sum of qf<sub>d</sub> − 1. The Y-axis is the difference between the known or derived exponents and their qfs, and δs known or derived. This is a power law test of the model. The slopes and y-intercepts of the three lines are sums and differences of the three published values. The previously published points related to h, n<sup>0</sup>, e, R, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula>are plotted. These points define three lines. The electron and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula> define the wk-line with slope of awk and y-intercept, bwk (blue solid line). The EM line is defined by h and R (dashed blue line). The green dashed line is the derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula> line for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula>. The known <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula> point is plotted as a green dot. The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula> point is centered at the red circle and the derived line fit value are all superimposed. The blue points are four of the experimental values for H<sub>0</sub> with their associated<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula>. These are plotted at the x-value of −3/4-1 since the derived qf = −3/4. The line fit of the experimental <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x94.png" xlink:type="simple"/></inline-formula> point and the four H<sub>0</sub> points is plotted at the green dot. The solid green <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x95.png" xlink:type="simple"/></inline-formula>-line is the best fit of the experimental data and closely parallels the derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x96.png" xlink:type="simple"/></inline-formula>-line. The experimental solid green <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x97.png" xlink:type="simple"/></inline-formula>-line fit data for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x98.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x99.png" xlink:type="simple"/></inline-formula> are very close to their derived values, the dashed green line, <xref ref-type="table" rid="table1">Table 1</xref>. None of the other qfs of −1/2, −5/6, or −7/8 are within orders of magnitude of the H<sub>0</sub>, and do not represent valid qfs for H<sub>0</sub>. The vertical thin red lines are associated with the hypothesized possible negative even harmonic fractions, −1/2, −3/4, −5/6, −7/8. The thick vertical red lines are the values along the wk-line used to derive the energy lost in the neutron beta decay process, qf +1/2, +3/4, +5/6, and +7/8</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/10-7502135x84.png"/></fig><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> List of natural units used in the derivations. <xref ref-type="table" rid="table3">Table 3</xref> lists the published values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x100.png" xlink:type="simple"/></inline-formula>, and the slopes and intercepts of the wk and EM lines used for the derivation of H<sub>0</sub>. These are the only natural values used for all of the derivations. See Equations (13)-(15)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Physical constant</th><th align="center" valign="middle" >Value</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x101.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.271859078(50) &#215; 10<sup>23</sup></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x102.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >53.780055612(22)</td></tr><tr><td align="center" valign="middle" >bwk: y-intercept, weak force, wk line</td><td align="center" valign="middle" >3.51638329(18) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >awk: slope, weak force, wk line</td><td align="center" valign="middle" >3.00036428(15) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >bem: y-intercept, electromagnetic, EM line</td><td align="center" valign="middle" >−3.45168347(17) &#215; 10<sup>−3</sup></td></tr><tr><td align="center" valign="middle" >aem: slope, electromagnetic, EM line</td><td align="center" valign="middle" >−3.45168347(17) &#215; 10<sup>−3</sup></td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Comparison of derived and known proportionality constants of H<sub>0</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x103.png" xlink:type="simple"/></inline-formula>, and n<sup>0</sup>. <xref ref-type="table" rid="table4">Table 4</xref> is a comparison of derived and now proportionality constants of H<sub>0</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x104.png" xlink:type="simple"/></inline-formula>, and n<sup>0</sup>. The derived values fall within the range of the known values</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Proportionality constant</th><th align="center" valign="middle" >Known</th><th align="center" valign="middle" >Derived</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x105.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.02(15) &#215; 10<sup>−41</sup></td><td align="center" valign="middle" >1.01118370(17) &#215; 10<sup>−41</sup></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x106.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >8.03(40) &#215; 10<sup>−110</sup></td><td align="center" valign="middle" >8.0382241(5) &#215; 10<sup>−110</sup></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x107.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.272(64) &#215; 10<sup>68</sup></td><td align="center" valign="middle" >1.25796898(7) &#215; 10<sup>68</sup></td></tr></tbody></table></table-wrap></sec><sec id="s1_6"><title>1.6. Previous Derivations of the HNH and the Relationship to the Derivation of the Hubble Constant</title><p>The Harmonic Neutron Hypothesis was previously used to derive the energy/matter lost in the transformation of a neutron to hydrogen, the masses of the quarks, the Higgs boson, and the Planck time [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] . Purely kinetic factors of neutron beta are related to the even-numbered denominators in the harmonic fractions, 1/2, 3/4, 5/6, and 7/8. It is logically hypothesized that the additive inverse partial harmonic fractions, which includes −1/2, −3/4, −5/6, and −7/8 should be related to the cosmic kinetic fundamental constants including, the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x108.png" xlink:type="simple"/></inline-formula>, cosmic microwave background radiation, CMB, and dark matter/dark energy.</p><p>The HNH has accurately derived Planck time, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x109.png" xlink:type="simple"/></inline-formula>, from this same sets of integers. [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] . It is also logical to hypothesize that other cosmic fundamental constants should be related to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x110.png" xlink:type="simple"/></inline-formula>. Our derivation shows that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x111.png" xlink:type="simple"/></inline-formula> is identical to the Newtonian gravitational constant, G, in the frequency domain. The product of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x112.png" xlink:type="simple"/></inline-formula> and the frequency equivalents of two masses and distance separating them equals the gravitational binding energy as a frequency equivalent of that system. The derived values associated with the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x113.png" xlink:type="simple"/></inline-formula>-line at the partial harmonic fractions −1/2, −3/4, −5/6, and −7/8 should be related to the cosmic kinetic fundamental constants including<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x114.png" xlink:type="simple"/></inline-formula>, cosmic microwave background radiation, CMB, dark matter and energy.</p></sec><sec id="s1_7"><title>1.7. Similarities of the HNH and Magnetic Resonance Imaging</title><p>None of the individual elements of the HNH are new or radically depart from standard physics or mathematical methods. The perspective taken, the nomenclature used, and methods are not standard, but are nonetheless logically and mathematically valid. To understand this method, a significant intellectual investment is essential since it is not intuitively obvious. The model is from a global perspective very similar to magnetic resonance imaging. MRI, which was assumed to be impossible at the time of its introduction based on classical physics interpretations of optical imaging criteria, yet disproven [<xref ref-type="bibr" rid="scirp.54287-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref16">16</xref>] . Both MRI and the HNH are spectral analysis methods. Both have two different domains that simultaneously define the identical object/system. One domain is in standard linear physical 3d space, and the other is in a mathematically transformed domain related to phase and frequency, the k-space for MRI. In this model it relates to an exponential universal harmonic plane, Figures 2-4. Both represent the identical physical system, but are defined in different mathematical terms.</p></sec><sec id="s1_8"><title>1.8. Why the Harmonic Neutron Hypothesis Is Based on Classical Physics and Not Numerology</title><p>The standard components of the HNH will be highlighted in italics. The HNH model is not in conflict with the Standard Model or overturns its methods or tenants. The actual physical values used are equivalent to standard unit values, but they are all transformed into frequency; harmonic fraction plus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x115.png" xlink:type="simple"/></inline-formula>; or exponential equivalents. They are evaluated as dimensionless coupling constant ratios, and proportionality constants. For example the ratio of the mass of the electron divided by the mass of the neutron equals the frequency equivalent of the electron divided by the frequency equivalent of the neutron independent of unit.</p><p>This model is independent of any specific physical unit system. Converting the standard units to this unit 1 format does not change the absolute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x116.png" xlink:type="simple"/></inline-formula> integer value, The reason for this non-intuitive mathematical imperative is that any arbitrary mass unit changes the arbitrary Avogadro’s number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x117.png" xlink:type="simple"/></inline-formula>, canceling out any effect of the initial mass unit. Transforming the arbitrary distance, time, and speed of light units to 1 are canceled out by changing the unit distance ratio with the fixed Compton radius, and changing the time unit to 1. Time and distance in the speed of light are proportional so the changes parallel each other, and cancel out any choice of those initial arbitrary values.</p><p>The combined components of the hypothesis are controversial because they are not well understood, are different from standard nomenclature, and novel. The concepts and mathematics are actually not complicated, but require a significantly different conceptual approach. All of the physical relationships are viewed solely as ex-</p><p>ponents (integer fractions plus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x118.png" xlink:type="simple"/></inline-formula>) or ratios of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x119.png" xlink:type="simple"/></inline-formula>.In the linear domain these are ratios, coupling con-</p><p>stants/proportionality constants. One example would be the ratio of the frequency equivalent of the ionization energy of hydrogen divided by the frequency equivalent of the Bohr Radius, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x120.png" xlink:type="simple"/></inline-formula>[<xref ref-type="bibr" rid="scirp.54287-ref11">11</xref>] . This is equivalent to Coulomb’s constant in the frequency domain.</p><p>All of the ratios are scaled by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x121.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x122.png" xlink:type="simple"/></inline-formula>, and therefore proportionality constants. Therefore, in this paper there should be a derivable proportionality constant that inter-relates<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x123.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x124.png" xlink:type="simple"/></inline-formula>, and H<sub>0</sub>, <xref ref-type="table" rid="table4">Table 4</xref>. Presently there is no known proportionality constant relating these three physical constants.</p><p>In this model the identical consecutive integer and harmonic fraction sequences are seen, as exponents of the fundamental frequency, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x125.png" xlink:type="simple"/></inline-formula>, of the system, Figures 1-3. The origin of this exponential pattern is not from a standing wave sinusoidal pattern, but from a consecutive integer exponential sequence defining the forces. In this type of ratio system, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x126.png" xlink:type="simple"/></inline-formula> is raised to an exponent in the sequence, the results represent the only possible observable frequencies of the derived or known physical constants. When this sequence of points is plotted on a 2d-plane, the only possible exponents are the integer, the harmonic fraction, and the partial fractional sequence of 1/n and 1 &#177; 1/n, where n equals N<sub>12</sub>, <xref ref-type="fig" rid="fig3">Figure 3</xref>, <xref ref-type="fig" rid="fig4">Figure 4</xref>. The resulting 2d-plane represents a universal 2d-exponential “slide rule”, <xref ref-type="fig" rid="fig3">Figure 3</xref> [<xref ref-type="bibr" rid="scirp.54287-ref17">17</xref>] .</p><p>The hypothesis is based on classic harmonic fractions, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x127.png" xlink:type="simple"/></inline-formula>and partial harmonic fractions, 1 &#177; 1/n for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x128.png" xlink:type="simple"/></inline-formula>. This offers a tremendously powerful, predictive attribute of the model since associating a physical constant with a specific harmonic fraction creates a series of other discrete harmonics and characterizes the whole system from an initial two-element data set. This is how H<sub>0</sub> can be derived with no direct physical measurement. An analogy is Moseley’s law on ion emission spectra.</p><p>Another important concept is resonance and products of harmonic numbers. Resonance is the tendency of a system to oscillate with greater amplitude at some frequencies rather than at others. If two systems have common frequency components there will be greater coupling and potential transfer of energy between them. For a musical example, two prime number frequencies can only resonant at the product of the two prime frequencies. This pure number property defines a higher order hierarchy of physically associated entities.</p><p>The HNH presents itself as a natural unit system. A natural unit system incorporates known physical units rather than arbitrary units. A natural unit model with all of the other constants driven to 1 greatly simplify the mathematics. This model is based on the annihilation frequency of the neutron, as the fundamental frequency similar to Planck units. In Planck units all of the different fundamental constants are converted into a single common standard unit such as Hz, seconds, kilograms, or meters. The neutron is a logical unified fundamental physical entity that is centered between atomic, subatomic, and cosmic entities.</p></sec><sec id="s1_9"><title>1.9. Why <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x129.png" xlink:type="simple"/></inline-formula> Are Not the Exact Fundamental Constants’ Physical Values, and Why Are δ-Values Essential?</title><p>In the simplest exponential harmonic series, all of the possible frequency values could be defined and related solely to a single fundamental frequency and the harmonic fraction series, <xref ref-type="fig" rid="fig2">Figure 2</xref>, <xref ref-type="fig" rid="fig3">Figure 3</xref> [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] . The HNH and physical reality are far more complicated. This arises from a mathematical imperative. Known fixed number values of the products of 2 and pi are associated with specific exponent integer-fraction values. These arise from the product ratio relationships of R, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x130.png" xlink:type="simple"/></inline-formula>, e, and, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x131.png" xlink:type="simple"/></inline-formula>[<xref ref-type="bibr" rid="scirp.54287-ref11">11</xref>] .</p><p>There are four product ratio relationships of these entities associated with the hydrogen atom. For example the</p><p>integer fraction associated with 2 must be related to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x132.png" xlink:type="simple"/></inline-formula> raised to (10/1155). Also 2pi must be related to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x133.png" xlink:type="simple"/></inline-formula> raised to (39/1155). Additionally, 2 raised to (1/(10/1155)) is 5.8744 &#215; 10<sup>34</sup>, and (2pi) raised to</p><p>(1/(39/1155)) is 4.34916 &#215; 10<sup>23</sup>. There is no common fundamental frequency that can fulfill these conflicting mathematical imperatives. Nature’s solution is to have small δ-values added to the quantum harmonic fractions that “shim” these various values to a common fundamental frequency, in this case <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x134.png" xlink:type="simple"/></inline-formula> Hz. These δ-values represent the known or derived exponent minus the harmonic fraction. This makes the system more complicated, but fulfills the imperative of a resonant system.</p></sec><sec id="s1_10"><title>1.10. Computations Using the Universal Harmonic 2d Exponential Plane</title><p>Each physical constant is plotted as a harmonic fraction minus one on the X-axis and the Y-axis is the plot of δ (the exponent minus the harmonic fraction), <xref ref-type="fig" rid="fig3">Figure 3</xref>, <xref ref-type="fig" rid="fig4">Figure 4</xref>. This is described as the universal harmonic plane. It is universal since it can perform any ratio, product, or power calculation, and all of the physical constants are plotted on this common 2d space. [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref17">17</xref>] . It is harmonic since the X-axis is defined by sums and differences of integers and harmonic fractions only.</p><p>The physical datum of each point has the identical value as its standard exponent, and can be translated to its standard routine physical value. The difference between two points on the 2d universal plane represents a proportionally constant, a ratio in the linear domain, a power law. This harmonic plane also has all of the classic mathematical properties of lines. A line connecting any two points can define a proportionality relationship of two or more physical constants. It is possible to derive any harmonic value from the slope and y-intercept of a</p><p>δ-line and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x135.png" xlink:type="simple"/></inline-formula>, if the harmonic fraction is known or derived. Different forces can be associated with different</p><p>or common δ-lines.</p></sec><sec id="s1_11"><title>1.11. Derivation of Experimentally Unmeasured Physical Constants</title><p>In Physics, under most circumstances if one knows a natural unit within a ratio or product relationship that value can be used as a constant, but it does not have inherent predictive value to other multiple other related physical constants. In a harmonic system if the natural unit is known and its associated quantum integer value then an infinite series of other values/constants, can potentially be derived. [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] This is a classic property or quantum spectrum.</p><p>Many of these constants can be derived since the actual δ-values can be derived from the three finite point sets described above sets, provided the harmonic fraction is logically derived. [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] . The data define two lines on</p><p>the universal harmonic plane. Their slopes and y-intercepts along with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x136.png" xlink:type="simple"/></inline-formula> are all that is necessary to derive</p><p>many of the other physical constants in this model. One line is related to the weak kinetic entities, and one related to the electromagnetic entities. The only other possible valid force δ lines are related to sums and differences of the slopes and y-intercepts of those two lines, <xref ref-type="fig" rid="fig4">Figure 4</xref>. Harmonic fractions, other than the very limited set used here, opens the possibility to derive the actual δ-values since they would represent just another point on a valid line following the power law and quantum spectrum properties.</p></sec><sec id="s1_12"><title>1.12. Value of the HNH Method and New Insights into the Meaning and Origin of Hubble’s Constant</title><p>The value of the HNH method is that it can derive and predict physical constants beyond what can be experimentally measured [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] . The Standard Model today cannot unify or scale quantum and cosmic phenomena simultaneously. The HNH also demonstrates the inter-relationship of the constants. The derived values have high precision since the calculations are based on high precision atomic data to begin with, and not on experimental data related to the physical constant in question [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] . In the present paper no astronomical data is utilized in the derivation of H<sub>0</sub>.</p><p>The methodology of HNH derivation generates new insights into connections between the subatomic entities of neutron beta decay, kinetic energy, and the neutrinos, leading to frequency expressions of the neutron, t<sub>P</sub>, gravity, H<sub>0</sub>; and the apparent expansion of the universe.</p></sec></sec><sec id="s2"><title>2. Methods and Results</title><sec id="s2_1"><title>2.1. Conversion of Physical Constants to Frequency Equivalents</title><p>Floating point accuracy is based upon known experimental atomic data, of approximately 5 &#215; 10<sup>−8</sup>. All of the known fundamental constants are converted to frequency equivalents, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x137.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x138.png" xlink:type="simple"/></inline-formula>, for the four (4) physical constants used in the HNH derivation of H<sub>0</sub>. Equations (1)-(4), <xref ref-type="table" rid="table3">Table 3</xref>. The masses are converted by multiplying by c<sup>2</sup> (speed of light squared) then dividing by h (Planck’s constant). The distances are converted by dividing the wavelength into c. Energies in Joules are converted by dividing by h. The eV value for the neutron is 939.565378(21) &#215; 10<sup>6</sup>. Its frequency in Hz is converted to eV by multiplying by the constant, 4.13566750(21) &#215; 10<sup>?15</sup> eV/Hz. The eV was converted to frequency by multiplying by the constant 2.41798930(13) &#215; 10<sup>14</sup> Hz/eV. N<sub>A</sub> is Avogadro’s number, 6.02214129(27) &#215; 10<sup>23</sup> mol<sup>−1</sup>. Converting the standard units to where they are all 1’s does not change<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x139.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.54287-formula35"><graphic  xlink:href="http://html.scirp.org/file/10-7502135x140.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula36"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x141.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula37"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x142.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula38"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x143.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula39"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x144.png"  xlink:type="simple"/></disp-formula><p>All of the data for the fundamental constants were obtained from the websites (http://physics.nist.gov/cuu/Constants/ and www.wikipedia.org. The NIST site http://physics.nist.gov/cuu/Constants/energy.html has an online physical unit converter that can be used for these types of conversions.</p></sec><sec id="s2_2"><title>2.2. The Frequency Equivalent and Exponential Domains; Calculation of Known Exponents, exp<sub>k</sub>, n<sub>ifek</sub>, qf<sub>k</sub>, and Known δ<sub>k</sub> Values from Frequency Equivalents</title><p>This model has two parallel domains both describing the identical physical values. One domain is the frequency</p><p>equivalent of any physical value. The other domain is the exponent of the base<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x145.png" xlink:type="simple"/></inline-formula>,which when raised to</p><p>that exponent equals the frequency equivalent of that specific value. Equation (5). The known exponent, exp<sub>k</sub>, of</p><p>a fundamental constant is the ratio of the log<sub>e</sub> of the frequency equivalent, n<sub>k</sub>s, divided by the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x146.png" xlink:type="simple"/></inline-formula>, Equation (5). Here,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x147.png" xlink:type="simple"/></inline-formula>. Subscript k denotes a known experimental value and</p><p>subscript d represents a derived value.</p><disp-formula id="scirp.54287-formula40"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x148.png"  xlink:type="simple"/></disp-formula><p>Every value in the physical domain is defined completely in terms of its ratio and exponent relationship with</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x149.png" xlink:type="simple"/></inline-formula>. All other constants are 1. Each domain describes the identical physical value, but one does so in the</p><p>standard physics linear/frequency domain, and the other in the exponential domain which is unique to the HNH model. The value of viewing the fundamental constants in the exponential domain is that their harmonic integer inter-relationships are clearly defined. The other is that any physical relationship can be displayed and calculated across all of the forces, and at any scale in this virtual 2d space. Despite the fact the HNH model utilizes virtual space, that space accurately defines true physical phenomena.</p><p>In the Standard Model, only a subset of physical values are quantum by definition or computational in character. In the HNH model every aspect of physical systems is quantized by integral steps. There are regions where the system appears to be experimentally continuous in the Standard Model, but this is not true in the HNH model, <xref ref-type="fig" rid="fig1">Figure 1</xref>. In the Standard Model there are physical values that equal 0, such as a velocity, but in the HNH this is not the case. In regions that are A.E. continuous the true quantum values can be evaluated in the HNH model.</p><p>The known exp<sub>k</sub> minus the harmonic/quantum fraction, qf, equals the known δ<sub>k</sub>, Equation (6). The known</p><p>frequency equivalent of a constant, v<sub>k</sub>, is calculated by raising <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x150.png" xlink:type="simple"/></inline-formula> to the exp<sub>k</sub> in Equations (6). Equation (7) shows that many of the fundamental constants do not have n<sub>f</sub> equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x151.png" xlink:type="simple"/></inline-formula>, but<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x152.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.54287-formula41"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x153.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula42"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x154.png"  xlink:type="simple"/></disp-formula><p>The n<sub>ife</sub> (integer-fractional exponents, “ife”) and the associated quantum fractions, qf, the harmonic fractions, and the partial harmonic fractions must fulfill a power law relationship with a natural unit constant. The closest n<sub>ife</sub> to the experimental value is derived from the exp<sub>k</sub>, Equations (8), but that value may not be the actual n<sub>ife</sub> since it may not fulfill a power law relationship [<xref ref-type="bibr" rid="scirp.54287-ref10">10</xref>] . The first n<sub>ife</sub> assignments from 1 to 12 are listed in <xref ref-type="table" rid="table2">Table 2</xref>. The higher principal quantum number values are harder to assign unless the constant is known with a high precision. There have been errors in assignment in the past, for example, the strange quark was initially assigned to the qf 29/30, but later corrected to 27/28, [<xref ref-type="bibr" rid="scirp.54287-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] .</p><disp-formula id="scirp.54287-formula43"><graphic  xlink:href="http://html.scirp.org/file/10-7502135x155.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula44"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x156.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_3"><title>2.3. Association of Individual Physical Constants to Harmonic Fractions and Their Degenerate Frequency Equivalents</title><p>As <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x157.png" xlink:type="simple"/></inline-formula> is raised to exponents of a consecutive harmonic quantum fraction <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x158.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x159.png" xlink:type="simple"/></inline-formula> for</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x160.png" xlink:type="simple"/></inline-formula>it represents many of the degenerate exponent values of the fundamental constants, Equations (9)-(11). The degenerate ratios of the constant’s frequency when divided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x161.png" xlink:type="simple"/></inline-formula> represent <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x162.png" xlink:type="simple"/></inline-formula> raised to the quantum fractions qf, where the harmonic quantum fraction exponents equal 1/&#177;n where the natural number,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x163.png" xlink:type="simple"/></inline-formula>. These represent the degenerate proportionality constants relating <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x164.png" xlink:type="simple"/></inline-formula> to the degenerate n value.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x165.png" xlink:type="simple"/></inline-formula>for principal quantum number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x166.png" xlink:type="simple"/></inline-formula> to ∞ (9)</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x167.png" xlink:type="simple"/></inline-formula>for principal quantum number (10)</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x168.png" xlink:type="simple"/></inline-formula>for principal quantum number (11)</p><p>Equation (12) calculates the X-axis value for a specific quantum fraction, partial fraction, and n<sub>ife</sub>.</p><disp-formula id="scirp.54287-formula45"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x169.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_4"><title>2.4. Calculation of Known Exponents, exp<sub>k</sub> and δ<sub>k</sub> Values for n<sup>0</sup>, e, α<sub>0</sub>, R, α<sup>−1</sup>, h</title><p>By definition the exp<sub>k</sub> of the n<sup>0</sup> is 1, and the exp<sub>k</sub> of h is 0. Both have a δ<sub>k</sub> of 0. All of the electromagnetic spectrum, quantized n-Hz, have an effective <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula> (i.e. degenerate). All photons are actually not degenerate, but split with a Lorentz factor of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula> for energy and Lorentz factor of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula> for time dilation. The other quantized numbers used for e, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula>, R, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula>are related to the first four odd prime numbers. The frequency equivalent of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula>, is 5.66525639(28) &#215; 10<sup>18</sup> Hz; where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula> is 0.80291631(05). The qf is 4/5, on the X-axis location of −1/5, with principal quantum number 5, and its <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula> equals 2.91631043(14) &#215; 10<sup>−3</sup>. The exponent <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula> of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x180.png" xlink:type="simple"/></inline-formula> is 1 + 3.6453880(02) &#215; 10<sup>−3</sup>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x181.png" xlink:type="simple"/></inline-formula>3.6453880(02) &#215; 10<sup>−3</sup>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x182.png" xlink:type="simple"/></inline-formula> of 2.76391359(14) &#215; 10<sup>23</sup> Hz. The y-intercept of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x183.png" xlink:type="simple"/></inline-formula> line is referred to as the b entity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x184.png" xlink:type="simple"/></inline-formula> value, in this case<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x185.png" xlink:type="simple"/></inline-formula>.</p><p>The frequency equivalent of the electron n<sub>e</sub>, is 1.23558996(05) &#215; 10<sup>20</sup> Hz; exp<sub>e</sub> is 8.6023061(06). The qf is 6/7, X-axis location of −1/7, principal quantum number, 7, and its <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x186.png" xlink:type="simple"/></inline-formula> is 3.08775982(21) &#215; 10<sup>?3</sup>. The exponent <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x187.png" xlink:type="simple"/></inline-formula> of e is 1 + 3.60238646(18) &#215; 10<sup>?3</sup>, be 3.60238646(18) &#215; 10<sup>?3</sup><sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x188.png" xlink:type="simple"/></inline-formula></sub>of 2.7575290(01) &#215; 10<sup>23</sup> Hz.</p><p>The frequency equivalent of hydrogen ionization energy<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x189.png" xlink:type="simple"/></inline-formula>, is 3.28984196(17) &#215; 10<sup>15</sup> Hz; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x190.png" xlink:type="simple"/></inline-formula>is 6.64365544(33). The qf is 2/3, X-axis location of −1/3, principal quantum number 3, and its <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x191.png" xlink:type="simple"/></inline-formula> is −2.30112231(11) &#215; 10<sup>−3</sup>. The exponent <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x192.png" xlink:type="simple"/></inline-formula> of R is 1 −3.45168347(17) &#215; 10<sup>−3</sup>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x193.png" xlink:type="simple"/></inline-formula>−3.45168347(17) &#215; 10<sup>−3</sup>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x194.png" xlink:type="simple"/></inline-formula>of 1.88695938(09) &#215; 10<sup>23</sup> Hz.</p><p>The frequency equivalent of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x195.png" xlink:type="simple"/></inline-formula> is 1.370359991(69) &#215; 10<sup>2</sup>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x196.png" xlink:type="simple"/></inline-formula>is 9.14882590(46) &#215; 10<sup>−2</sup>. The qf is 1/11, X-axis location of −10/11, principal quantum number 11, and its <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x197.png" xlink:type="simple"/></inline-formula> is 5.7916811(03) &#215; 10<sup>−4</sup>.</p></sec><sec id="s2_5"><title>2.5. Plotting, Transformation, of Known Exponents and δ<sub>k</sub> Values on to the 2d Universal Harmonic Exponential Plane for n<sup>0</sup>, h, e, α<sub>0</sub>, and R</title><p>The known and derived exponents of physical constants are plotted/ transformed to the 2d universal harmonic plane. The X-axis is a multi-dimensional physical descriptor, Figures 2-4. The point (0, 0) represents the neutron since that is the exponent of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x198.png" xlink:type="simple"/></inline-formula> Hz divided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x199.png" xlink:type="simple"/></inline-formula><sub> </sub>Hz. The Y-axis is the related to the difference of the known exponent minus its associated qf, Equation (6). The Y-axis is not continuous in terms of the inter-relationships of the fundamental constants either. The slopes and y intercepts of the wk and EM <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x200.png" xlink:type="simple"/></inline-formula> lines also represent three “quantum” unit values though not integers. The only possible δ-values are a function of qf-1, and are discrete.</p><p>The points for the e, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x201.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x202.png" xlink:type="simple"/></inline-formula> fall above the X-axis since their <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x203.png" xlink:type="simple"/></inline-formula> are positive. Their respective X-axis values are −1/7 = (6/7 − 1), −1/5 = (4/5 − 1), −10/11 = (1/11 − 1). The point for R falls below that X-axis at x equals −1/3 = (2/3 − 1) since the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x204.png" xlink:type="simple"/></inline-formula> is negative. The differences between these points on the universal harmonic exponent plane represent the classic ratios of these same values in the frequency domain [<xref ref-type="bibr" rid="scirp.54287-ref12">12</xref>] .</p></sec><sec id="s2_6"><title>2.6. Calculation of Derived Exponents, exp<sub>d</sub>, Derived δ<sub>d</sub> Values; and Calculation of Derived δ<sub>d</sub> Slopes and Intercepts at x = −1 and x = 0</title><p>The only possible derived exponents are discrete since the only possible qf and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula> values are discrete. The lines described below transpose the natural unit sets to the harmonic 2d plane. The line connecting the e, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x207.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x208.png" xlink:type="simple"/></inline-formula>, points is logically related to the weak kinetic force, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x209.png" xlink:type="simple"/></inline-formula>-line. Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x210.png" xlink:type="simple"/></inline-formula>is a distance and related to a length dimension and velocity, therefore kinetic properties. The electron is a mass related to the weak force. The other 1/&#177;n points on the wk line represent the other possible derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x211.png" xlink:type="simple"/></inline-formula>s that are logically related to the weak force. These possibilities graphically represent the intersection points of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x212.png" xlink:type="simple"/></inline-formula> line with x values of &#177;1/n. The slope is awk, 3.000364286(15) &#215; 10<sup>−3</sup> and the y-intercept is bwk, 3.51638329(18) &#215; 10<sup>−3</sup>, Equations (13), (14).</p><disp-formula id="scirp.54287-formula46"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x213.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula47"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x214.png"  xlink:type="simple"/></disp-formula><p>These derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x215.png" xlink:type="simple"/></inline-formula> values when proposed had no known physical significance. [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] It was assumed that these other “possible valid” harmonic fraction points along a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x216.png" xlink:type="simple"/></inline-formula> line are identical in concept and physical reality to other possible “spectral lines” in a standard quantum spectrum where each spectral line is associated with a different quantum integer. In the interval these hypothesized <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x217.png" xlink:type="simple"/></inline-formula> points have been shown to be associated with many known physical entities. [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>]</p><p>The EM, line is defined by the points for the Planck constant, (−1, 0) and Rydberg R<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x218.png" xlink:type="simple"/></inline-formula>, <xref ref-type="fig" rid="fig4">Figure 4</xref>, Equation (15). This is the second line that was previously published, [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] . This is logical since h is the unit for electromagnetic energy, and R is the unit for the atomic ionization energy. It is referred to as the electromagnetic, EM <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x219.png" xlink:type="simple"/></inline-formula>-line. Its slope and y-intercept, bem, are identical and equal to −3.45168347(17) &#215; 10<sup>−3</sup>, Equation (15). This line is related to the principal quantum number 3, qf, 2/3. The other potential qf values have also been shown to be related to the quarks and mesons, [<xref ref-type="bibr" rid="scirp.54287-ref10">10</xref>] .</p><disp-formula id="scirp.54287-formula48"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x220.png"  xlink:type="simple"/></disp-formula><p>The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x221.png" xlink:type="simple"/></inline-formula> values are a linear function of the qf-1, and the slope and y intercepts of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x222.png" xlink:type="simple"/></inline-formula>-lines. An alternate definitions of slope and y intercept are the y values at x equals 0, and −1, Equations (16). These are interchangeably equivalent, and both are used in this method, <xref ref-type="fig" rid="fig4">Figure 4</xref>. It is possible to predict the exact exponents of unmeasured fundamental constants from these <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x223.png" xlink:type="simple"/></inline-formula> lines just like it is possible to derive lines of quantum spectrum without a physical measure if its natural unit and principal quantum number are known, Equation (17), (18).</p><disp-formula id="scirp.54287-formula49"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x224.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula50"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x225.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula51"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x226.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_7"><title>2.7. Calculation and Plotting of Compound Derived Exponents, qf<sub>d</sub>, exp<sub>d</sub>, and Derived δ<sub>d</sub> Values</title><p>Many of the fundamental constants are compound product/ratios of other fundamental constants. Therefore <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x227.png" xlink:type="simple"/></inline-formula> is a compound of four other entities. All of the possible valid force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x228.png" xlink:type="simple"/></inline-formula> lines of these composite forces can be derived since they must represent sums and differences of the slopes and y intercepts of the wk and EM lines, bwk, awk, and bem, as in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x229.png" xlink:type="simple"/></inline-formula>-line, Equations (19), (20). [<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] These are the only possible valid values in a unified harmonic system, <xref ref-type="fig" rid="fig3">Figure 3</xref>, <xref ref-type="fig" rid="fig4">Figure 4</xref>. All of the compound values are derived.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x230.png" xlink:type="simple"/></inline-formula>for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x231.png" xlink:type="simple"/></inline-formula> to 12 and products (19)</p><disp-formula id="scirp.54287-formula52"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x232.png"  xlink:type="simple"/></disp-formula><p>The compound values are plotted at their qf<sub>d</sub> − 1 X-axis values and their <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x233.png" xlink:type="simple"/></inline-formula> Y-axis values identical to the other single physical value constants, <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p></sec><sec id="s2_8"><title>2.8. Calculation of Known and Derived Proportionality Constants</title><p>Equation (21) is the proportionality constant, known or derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x234.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x235.png" xlink:type="simple"/></inline-formula>, multiplied with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x236.png" xlink:type="simple"/></inline-formula> that is associated with another fundamental constant. Equation (22) is the basic form of this relationship used in the proportionality constant derivations.</p><disp-formula id="scirp.54287-formula53"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x237.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula54"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x238.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_9"><title>2.9. Calculation and Plotting of the Known Frequency Equivalent<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x239.png" xlink:type="simple"/></inline-formula>, exp<sub>k</sub>, δ<sub>k</sub>, and 2d Point</title><p>The known experimental h-bar <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x240.png" xlink:type="simple"/></inline-formula> is 5.39106(32) &#215; 10<sup>−44</sup> s, relative error 6 &#215; 10<sup>−5</sup>. The known experimental non h-bar <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x241.png" xlink:type="simple"/></inline-formula> is 1.35134(81) &#215; 10<sup>−43</sup> s, <xref ref-type="table" rid="table1">Table 1</xref>. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x242.png" xlink:type="simple"/></inline-formula> s<sup>2</sup> non h-bar is 1.82611(11) &#215; 10<sup>−86</sup> s<sup>2</sup>. The known mean experimental non h-bar exp<sub>k</sub> is −3.670879(12). The known experimental non h-bar <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x243.png" xlink:type="simple"/></inline-formula> is −1.37371(1) &#215; 10<sup>−2</sup>. The qf of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x244.png" xlink:type="simple"/></inline-formula> is the sum of −1, −1, −6/7, −4/5 or −128/35 or −3.657142857142. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x245.png" xlink:type="simple"/></inline-formula> point is plotted at x = −128/35 −1, which equals −163/35.</p></sec><sec id="s2_10"><title>2.10. Calculation and Plotting of the Derived Frequency Equivalent<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x246.png" xlink:type="simple"/></inline-formula>, exp<sub>d</sub>, δ<sub>d</sub> Point, δ<sub>d</sub> Line</title><p>The harmonic neutron hypothesis has derived a high accuracy Planck time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x247.png" xlink:type="simple"/></inline-formula>. [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] The qf for these four entities defining <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x248.png" xlink:type="simple"/></inline-formula><sup> </sup>are −1, the gravitation binding energy of the electron −1, negative qf proton, −6/7, negative qf electron; −4/5; negative qf Bohr radius. The sum equals −128/35. This is plotted at the x-value of −163/35, −128/35-1.</p><p>The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula> compound <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x250.png" xlink:type="simple"/></inline-formula> line has a slope of awk ? bwk ? bem, and a y intercept of ?bwk ? bem at x equals 0, and y intercept of ?awk at x equals −1, Equations (23)-(25), <xref ref-type="fig" rid="fig4">Figure 4</xref>. [<xref ref-type="bibr" rid="scirp.54287-ref9">9</xref>] The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x251.png" xlink:type="simple"/></inline-formula> is −3.670879366(1), the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x252.png" xlink:type="simple"/></inline-formula> is −1.3736509(1) &#215; 10<sup>−2</sup> and the derive <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x252.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x253.png" xlink:type="simple"/></inline-formula> is 1.82617126(91) &#215; 10<sup>−86</sup> s<sup>2</sup> relative errors of 5 &#215; 10<sup>−8</sup>. The derived no h-bar <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x252.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x254.png" xlink:type="simple"/></inline-formula> equals 1.35135904(68) &#215; 10<sup>43</sup>. The equivalent <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x252.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x255.png" xlink:type="simple"/></inline-formula> h-bar value is 5.39114257(27) &#215; 10<sup>−44</sup> s. All these values are within the known experimental values.</p><disp-formula id="scirp.54287-formula55"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x256.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula56"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x257.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula57"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x258.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_11"><title>2.11. The Known Experimental Velocities, H<sub>0</sub> s<sup>−1</sup>, exp<sub>k</sub>, and δ<sub>k</sub> Ranges</title><p>The known experimental velocities at Mpc<sup>−1</sup> are 76.9<sup>+3.9</sup><sub>−3.4</sub><sup>+10.0</sup><sub>−8.0</sub> km・s<sup>−1</sup>・Mpc<sup>−1</sup>, 74.3 &#177; 2.1 km・s<sup>−1</sup>・Mpc<sup>−1</sup>, 69.32 &#177; 0.80 km・s<sup>−1</sup>・Mpc<sup>−1</sup>, 67.3 &#177; 1.2 km・s<sup>−1</sup>・Mpc<sup>−1</sup>, <xref ref-type="table" rid="table1">Table 1</xref>. These are converted to standard s<sup>−1</sup> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x259.png" xlink:type="simple"/></inline-formula> values by dividing the velocity by one Mpc, 3.085677580 &#215; 10<sup>22</sup> meters. These value are 2.49(12) &#215; 10<sup>−18</sup> s<sup>−1</sup>, 2.408(67) &#215; 10<sup>−18</sup> s<sup>−1</sup>, 2.24(2) &#215; 10<sup>−18</sup> s<sup>−1</sup>, and 2.18(4) &#215; 10<sup>−18</sup> s<sup>−1</sup>. Their respective exp<sub>k</sub> are −7.53(12) &#215; 10<sup>−1</sup>, −7.543(8) &#215; 10<sup>−1</sup>, −7.556(16) &#215; 10<sup>−1</sup>, and −7.562(3) &#215; 10<sup>−1</sup>. The respective <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x260.png" xlink:type="simple"/></inline-formula> are: −3.70(90) &#215; 10<sup>−3</sup>, −4.33(50) &#215; 10<sup>−3</sup>, −5.62(20) &#215; 10<sup>−3</sup>, and lastly, −6.17(32) &#215; 10<sup>−3</sup>.</p></sec><sec id="s2_12"><title>2.12. The Known Experimental Line Fit Values for H<sub>0k</sub> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x261.png" xlink:type="simple"/></inline-formula>, exp<sub>k</sub>, δ<sub>k</sub>, Slope and y<sub>k</sub>-Intercept at x = 0</title><p>A line fit of the known <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x263.png" xlink:type="simple"/></inline-formula> data points was completed. The line fit <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x264.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x265.png" xlink:type="simple"/></inline-formula> values are respectively 1.82611(11) &#215; 10<sup>−86</sup> s<sup>2</sup> and 2.33(11) &#215; 10<sup>−18</sup> s<sup>−1</sup>. The slope is 3.021 &#215; 10<sup>−3</sup>, and the y-intercept at x = 0 is 3.315 &#215; 10<sup>−4</sup>. The line fit <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x266.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x267.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x267.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x268.png" xlink:type="simple"/></inline-formula> are −3.670879(12), and −1.37371(1) &#215; 10<sup>−2</sup>. This is compared to the derived values in <xref ref-type="table" rid="table1">Table 1</xref>, <xref ref-type="fig" rid="fig4">Figure 4</xref>. The derived and known values correlate well.</p></sec><sec id="s2_13"><title>2.13. Derivation of the exp<sub>d</sub>, δ<sub>d</sub> for qf Values of −1/2, −3/4, −5/6, and −6/7 on the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x269.png" xlink:type="simple"/></inline-formula> δ<sub>d</sub> Line</title><p>The generalized <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x270.png" xlink:type="simple"/></inline-formula> line for any qf value is Equations (26)-(28). This equation is used to derive the possible hypothesized negative value harmonic fractions of beta neutron decay, −1/2, −3/4, −5/6, −7/8. One of these is hypothesized be related to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x270.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x271.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.54287-formula58"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x272.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula59"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x273.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula60"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x274.png"  xlink:type="simple"/></disp-formula><p>The derived<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x275.png" xlink:type="simple"/></inline-formula>, exponents, and s<sup>−1</sup> calculated values from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x276.png" xlink:type="simple"/></inline-formula> line for the possible qfs of −1/2, −3/4, −5/6, −7/8 are respectively for −1/2: −4.4681966(3) &#215; 10<sup>−3</sup>, −5.0446820(13) &#215; 10<sup>−1</sup>, 1.6498650(1) &#215; 10<sup>−12</sup> s<sup>−1</sup>, for −3/4: −5.20211263(26) &#215; 10<sup>−3</sup>, −7.5520211(04) &#215; 10<sup>−1</sup>, 2.2972668(2) &#215; 10<sup>−18</sup> s<sup>−1</sup>, for −5/6: −5.4467515(3) &#215; 10<sup>−3</sup>, −8.3878008(4) &#215; 10<sup>−1</sup>, 2.5652661(7) &#215; 10<sup>−20</sup> s<sup>−1</sup>, for −7/8: −5.5690708(3) &#215; 10<sup>−3</sup>, −8.8056907(5) &#215; 10<sup>−1</sup>, 2.7107717(3) &#215; 10<sup>−21</sup> s<sup>−1</sup>, <xref ref-type="fig" rid="fig4">Figure 4</xref>. The qf of −3/4 is most the associated qf of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x276.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x277.png" xlink:type="simple"/></inline-formula>. The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x276.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x277.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x278.png" xlink:type="simple"/></inline-formula> from this method is the intercept of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x276.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x277.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x278.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x279.png" xlink:type="simple"/></inline-formula> line at an x value of −3/4-1. This is the harmonic fraction x location of −3/4-1, −7/4. The specific derivation of these factors for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x276.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x277.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x278.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x280.png" xlink:type="simple"/></inline-formula> are shown in Equations (29)-(31).</p><disp-formula id="scirp.54287-formula61"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x281.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula62"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x282.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54287-formula63"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x283.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_14"><title>2.14. Derived Hubble Time, Hubble Length</title><p>The derived Hubble time is the inverse of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x284.png" xlink:type="simple"/></inline-formula>, 4.3529990(17) &#215; 10<sup>17</sup> seconds. There are 3.1556926 &#215; 10<sup>7</sup> seconds per year. The derived Hubble time equals 13.7941161(13) &#215; 10<sup>9</sup> years. The derived Hubble length is 13.7941161(13) &#215; 10<sup>9</sup> light years. The reported experimental value is approximately 13.8 &#215; 10<sup>9</sup> light years.</p></sec><sec id="s2_15"><title>2.15. Comparison of Known and Derived Proportionality Constants of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x285.png" xlink:type="simple"/></inline-formula>, H<sub>0</sub> and the Neutron</title><p>The known proportionally constant of the ratio of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x286.png" xlink:type="simple"/></inline-formula> line fit <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x286.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x287.png" xlink:type="simple"/></inline-formula> divided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x286.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x287.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x288.png" xlink:type="simple"/></inline-formula> is 1.02(15) &#215; 10<sup>−41</sup>. The derived value is 1.01118370(16) &#215; 10<sup>−41</sup>, Equation (32), <xref ref-type="table" rid="table4">Table 4</xref>.</p><disp-formula id="scirp.54287-formula64"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x289.png"  xlink:type="simple"/></disp-formula><p>The known proportionally constant of the ratio from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x290.png" xlink:type="simple"/></inline-formula> line fit <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x290.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x291.png" xlink:type="simple"/></inline-formula> divided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x290.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x291.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x292.png" xlink:type="simple"/></inline-formula> is 8.03(40) &#215; 10<sup>−110</sup>. The derived value is 8.0382241(5) &#215; 10<sup>−110</sup>, Equation (33).</p><disp-formula id="scirp.54287-formula65"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x293.png"  xlink:type="simple"/></disp-formula><p>The known proportionally constant of the ratio from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x294.png" xlink:type="simple"/></inline-formula> line fit <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x295.png" xlink:type="simple"/></inline-formula> divided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x295.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x296.png" xlink:type="simple"/></inline-formula> is 1.272(64) &#215; 10<sup>68</sup>. The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x295.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x296.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x297.png" xlink:type="simple"/></inline-formula> value is 1.25796898(7) &#215; 10<sup>68</sup>, Equation (34).</p><disp-formula id="scirp.54287-formula66"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7502135x298.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. Discussion</title><p>A robust physics model that explains many of the mysteries of today remains elusive [<xref ref-type="bibr" rid="scirp.54287-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.54287-ref19">19</xref>] . A dominant unsolved problem is how to scale sub-atomic quantum, classical physics, and cosmologic phenomena simultaneously in a coherent mathematical and physical model. The HNH answers some of these questions, and actually derives accurate values of the physical cosmological and high energy constants that cannot be accurately experimentally measured [<xref ref-type="bibr" rid="scirp.54287-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.54287-ref14">14</xref>] .</p><p>Many critics of the HNH suspect that these findings are simply coincidence or numerology. The HNH is however a classic dimensionless physical system of the Buckingham Pi theorem type. The speed of light is finite, and constant within any setting. It is logical that the whole system should be based on a finite constant as well. The harmonic neutron hypothesis is highly restricted. Only three starting finite number sets are used. The derivations are not made directly from the original subatomic data, but from the unified scaling of the whole universal harmonic 2d plane, <xref ref-type="fig" rid="fig3">Figure 3</xref>, <xref ref-type="fig" rid="fig4">Figure 4</xref>. Therefore it is incorrect to interpret that H<sub>0</sub> was derived from a product ratio relationship of the four subatomic constants that would be utilized in a classic physics’ method. It is impossible to manipulate the results since all of the components are fixed previously published natural units, and harmonic integer fractions. It is not possible to derive any value by manipulating the n<sub>ife</sub> value. An argument by analogy is that it is not possible to derive any wavelength from the Rydberg series by changing the n<sub>1</sub> and n<sub>2</sub> values since R is a natural unit</p><p>The hypothesis logically states that related physical constants will naturally all fall on a single <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x299.png" xlink:type="simple"/></inline-formula> line since they are all scaled by the same proportionality constant. The derivation of H<sub>0</sub> from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x299.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x300.png" xlink:type="simple"/></inline-formula>-line is support of the hypothesis that these two are related to the same proportionality constant, Equations (32)-(34). The proportionality constants of the neutron, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x299.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x300.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x301.png" xlink:type="simple"/></inline-formula>, and H<sub>0</sub> are accurately derived. This is viewed as impossible utilizing standard methods.</p><p>The typical interpretation of the H<sub>0</sub> is that it is not felt to be a true constant, but changes with other variables defining the nature of the cosmos. It has been described as the Hubble parameter. It is experimentally impossible to prove that the H<sub>0</sub> is actually changing from the present value. In the HNH H<sub>0</sub> is felt to constant, and is analogous to the free space constants of permeability, and permittivity. Interpretation of quantum systems using classical physics concepts is inaccurate and inappropriate. In the HNH the same is true for cosmology phenomena.</p><p>It is logical that the H<sub>0</sub> should be closely related to the gravitational force, and therefore<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x302.png" xlink:type="simple"/></inline-formula>. H<sub>0</sub> is related to an expansive kinetic phenomenon, and so is the neutron beta decay process. H<sub>0</sub> and the beta decay qfs have inverse signs, 3/4 and −3/4, but identical harmonic fractions. The harmonic neutron hypothesis has shown multiple examples of this type of harmonic fraction sign symmetry with inverse sign relationships. The top quark is 1+1/10 and the up quark is 1 − 1/10. The Higgs boson is 1 + 1/11, and the down quark is 1 − 1/11. This is a non-coincidental relationship as seen with the Rydberg series and with Moseley’s law, which in the exponential domain represent inverse exponents.</p><p>Perhaps the other qfs −1/2, −5/6, or −7/8 represent the properties of dark matter and energy. It is possible to accurately derive CMB peak spectral radiance from the same <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x303.png" xlink:type="simple"/></inline-formula> line using the partial fractions 1/2 and 2 &#215; −3/4, −3/2. It is likely that dark matter and dark energy are related to the partial fraction −1/2. The properties of black holes can also be interrogated with the HNH without limitations of singularities since the Schwarzschild radius relationship can be evaluated using <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x304.png" xlink:type="simple"/></inline-formula> s<sup>2</sup>. The derived <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x304.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x305.png" xlink:type="simple"/></inline-formula> can be used to derive the masses and dimensions of black holes. Also the HNH has no singularities since the number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x304.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x305.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x306.png" xlink:type="simple"/></inline-formula> is finite, and also represents the maximum Lorentz factor.</p><p>The HNH also explains the precise logical origin of H<sub>0</sub> and unification with other fundamental constants including the neutron, hydrogen, neutrinos, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x307.png" xlink:type="simple"/></inline-formula>, G, and the kinetic energy lost in the beta decay process. The +3/4 qf is associated with kinetic energy lost during neutron beta decay. It is also associated with the muon antineutrino, as yet unpublished data. The expectation values of the neutrinos all fall on the wk line. The expectation value of the muon neutrino is related to the qf sum of 3/4 and 1/10 for the up quark on the wk line. The expectation value of the electron neutrino is related to the qf sum of 1/2 and 1/7 for the electron on the wk line. The expectation value of the Tau neutrino is related to the qf sum of 5/6 and 1/10, and for the up quark on the wk line.</p></sec><sec id="s4"><title>4. Conclusion</title><p>H<sub>0</sub> can be derived from four finite integer natural units and N<sub>12</sub>. H<sub>0</sub> is logically related by harmonic fractions to the beta decay kinetic energy based on a common harmonic fraction, 3/4, but with opposite sign. The experimental Planck time and H<sub>0</sub> data power law data is closely linked to the predicted data. The derived H<sub>0</sub> can be evaluated in the future to see if this is an accurate prediction. Derivation of accurate coupling constants of the neutron with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7502135x308.png" xlink:type="simple"/></inline-formula> and H<sub>0</sub> has never been achieved before so this is a significant result.</p></sec><sec id="s5"><title>Acknowledgements</title><p>I would like to thank Tom Budinger Ph.D. for his sage advice, and help. I would also like to thank Richard White MD for his support of this work.</p></sec><sec id="s6"><title>Cite this paper</title><p>Donald WilliamChakeres,RichardVento, (2015) Prediction and Derivation of the Hubble Constant from Subatomic Data Utilizing the Harmonic Neutron Hypothesis. 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