<?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">JHEPGC</journal-id><journal-title-group><journal-title>Journal of High Energy Physics, Gravitation and Cosmology</journal-title></journal-title-group><issn pub-type="epub">2380-4327</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jhepgc.2017.32027</article-id><article-id pub-id-type="publisher-id">JHEPGC-75556</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>
 
 
  Constraints, in Pre-Planckian Space-Time via Padmabhan’s &amp;Lambda;&lt;sub&gt;initial&lt;/sub&gt;&amp;middot;&lt;i&gt;H&lt;/i&gt;&lt;sup style=&quot;margin-left:4px;&quot;&gt;-2&lt;/sup&gt;&lt;sub style=&quot;margin-left:-17px;&quot;&gt;initial&lt;/sub&gt;&amp;asymp;&lt;i&gt;o&lt;/i&gt;(1) Approximation Leading to Initial Inflaton Constraints and Its Relation to Early Universe Graviton Production
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Andrew</surname><given-names>Walcott Beckwith</given-names></name><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><author-notes><corresp id="cor1">* E-mail:<email>Rwill9955b@gmail.com,abeckwith@uh.edu</email>;<email>Physics Department, College of Physics, Chongqing University Huxi Campus, Chongqing, China</email>;</corresp></author-notes><pub-date pub-type="epub"><day>08</day><month>02</month><year>2017</year></pub-date><volume>03</volume><issue>02</issue><fpage>322</fpage><lpage>327</lpage><history><date date-type="received"><day>January</day>	<month>11,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>April</month>	<year>18,</year>	</date><date date-type="accepted"><day>April</day>	<month>21,</month>	<year>2017</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>
 
  We are looking at what if the initial cosmological constant is 
  <img src="Edit_0508e420-6515-4f61-a026-c552e44cadbe.bmp" alt="" /> due to 
  <img src="Edit_361f0b37-5fd1-464a-8a1e-15dad36f4d16.bmp" alt="" /> if we furthermore use 
  <img src="Edit_f853841e-8d45-453c-93c8-fc5fad85fc17.bmp" alt="" /> as the variation of the time component of the metric tensor 
  <img src="Edit_3eeac5cb-ceff-4d55-91dc-8935e06769ec.bmp" alt="" /> in Pre-Planckian Space-time up to the Planckian space-time initial values. This assumes 
  <img src="Edit_25d938eb-d606-4893-af62-9e55eac73d2e.bmp" alt="" /> as an initial inflaton value, as well as employing Non-Linear Electrodynamics to the scale factor in 
  <img src="Edit_70655c7f-297d-41b5-8271-9e292bac1de8.bmp" alt="" /> , and the upshot is an expression for 
  <img src="Edit_532e80f7-60f5-4eae-9979-9121ba5207a6.bmp" alt="" /> as an initial inflaton value/squared which supports Corda’s assumptions in the Gravity’s breath Electronic Journal of theoretical physics article. We close with an idea to be worked in further detail as to density matrices and how it may relate to gravitons traversing from a Pre-Planckian to Planckian space-time regime. We will write up an idea in far greater detail in a future publication.
 
</html></p></abstract><kwd-group><kwd>Inflaton Physics</kwd><kwd> Density Matrix Equation</kwd><kwd> Gravitons</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Basic Idea, the Padmabhan Approximation of <img src="http://html.scirp.org/file/12-2180186x10.png" /></title><p>To do this, we look at [<xref ref-type="bibr" rid="scirp.75556-ref1">1</xref>] which is of the form</p><disp-formula id="scirp.75556-formula2"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x11.png"  xlink:type="simple"/></disp-formula><p>Our objective is to use Equation (1) with [<xref ref-type="bibr" rid="scirp.75556-ref2">2</xref>]</p><disp-formula id="scirp.75556-formula3"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x12.png"  xlink:type="simple"/></disp-formula><p>and [<xref ref-type="bibr" rid="scirp.75556-ref2">2</xref>]</p><disp-formula id="scirp.75556-formula4"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x13.png"  xlink:type="simple"/></disp-formula><p>and [<xref ref-type="bibr" rid="scirp.75556-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.75556-ref3">3</xref>]</p><disp-formula id="scirp.75556-formula5"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x14.png"  xlink:type="simple"/></disp-formula><p>and [<xref ref-type="bibr" rid="scirp.75556-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.75556-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75556-ref5">5</xref>]</p><disp-formula id="scirp.75556-formula6"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x15.png"  xlink:type="simple"/></disp-formula><p>and [<xref ref-type="bibr" rid="scirp.75556-ref4">4</xref>]</p><disp-formula id="scirp.75556-formula7"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x16.png"  xlink:type="simple"/></disp-formula><p>The next step will be to utilize [<xref ref-type="bibr" rid="scirp.75556-ref6">6</xref>]</p><disp-formula id="scirp.75556-formula8"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x17.png"  xlink:type="simple"/></disp-formula><p>where [<xref ref-type="bibr" rid="scirp.75556-ref6">6</xref>]</p><disp-formula id="scirp.75556-formula9"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x18.png"  xlink:type="simple"/></disp-formula><p>as well as use the Non-Linear Electrodynamic minimum value of the scale factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x19.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.75556-ref7">7</xref>] which is in the spirit of [<xref ref-type="bibr" rid="scirp.75556-ref8">8</xref>] and which is avoiding using [<xref ref-type="bibr" rid="scirp.75556-ref9">9</xref>] .</p></sec><sec id="s2"><title>2. Using the Section 1 Material to Isolate a Minimum Value of the Inflaton, beyond Equation (4)</title><p>From [<xref ref-type="bibr" rid="scirp.75556-ref4">4</xref>] we make the following approximation, i.e. simply put a relationship of the Lagrangian multiplier giving us the following: if</p><disp-formula id="scirp.75556-formula10"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x20.png"  xlink:type="simple"/></disp-formula><p>If the following is true, i.e. in a Pre-Plankian to Planckian regime of space- time</p><disp-formula id="scirp.75556-formula11"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x21.png"  xlink:type="simple"/></disp-formula><p>Here, −g is a constant, as assumed in [<xref ref-type="bibr" rid="scirp.75556-ref4">4</xref>] which means in the Pre-Planckian to Plackian regime we would have Equation (5) as a constant, so then we are looking at, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x22.png" xlink:type="simple"/></inline-formula>, an energy density as given by Zeldovich, as talked about with [<xref ref-type="bibr" rid="scirp.75556-ref10">10</xref>] setting a minimum energy density given by</p><disp-formula id="scirp.75556-formula12"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x23.png"  xlink:type="simple"/></disp-formula><p>And with the following substitution of</p><disp-formula id="scirp.75556-formula13"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x24.png"  xlink:type="simple"/></disp-formula><p>Then to first order we would be looking at Equation (11) re written as leading to</p><disp-formula id="scirp.75556-formula14"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x25.png"  xlink:type="simple"/></disp-formula><p>And if Equation (1) holds, we would have by [<xref ref-type="bibr" rid="scirp.75556-ref1">1</xref>]</p><disp-formula id="scirp.75556-formula15"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x26.png"  xlink:type="simple"/></disp-formula><p>So</p><disp-formula id="scirp.75556-formula16"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x27.png"  xlink:type="simple"/></disp-formula><p>And if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x28.png" xlink:type="simple"/></inline-formula> is the square of Planck’s length, after some algebra, and assuming <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x29.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.75556-formula17"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x30.png"  xlink:type="simple"/></disp-formula><p>We will examine the consequences of these assumptions as to what this says about the NLED approximation for the initial scale factor, as given in [<xref ref-type="bibr" rid="scirp.75556-ref7">7</xref>] .</p></sec><sec id="s3"><title>3. Conclusions: Examining the Contribution of the Inflaton</title><p>In [<xref ref-type="bibr" rid="scirp.75556-ref11">11</xref>] Corda gives a very lucid introduction as to the physics of the inflaton. We urge the readers to look at it as it refers to Equation (17), second line. In particular, it gives the template for the possible range of values for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x31.png" xlink:type="simple"/></inline-formula> in Equation (16).</p><p>The take away is that we are assuming a relatively large initial entropy (based upon a count of massive gravitons) being recycled from one universe to the next, which would influence the behavior of the first line of Equation (16) and tie into the behavior of the 2<sup>nd</sup> line of the inflaton Equation (16) given above. The exact particulars of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x32.png" xlink:type="simple"/></inline-formula> are being investigated.</p><p>Keep in mind the importance of the result from reference [<xref ref-type="bibr" rid="scirp.75556-ref12">12</xref>] below which forms the core of Equation (17) below</p><disp-formula id="scirp.75556-formula18"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x33.png"  xlink:type="simple"/></disp-formula><p>We have to adhere to this e fold business, and this will influence our choices as to how to model the inflaton.</p><p>Furthermore the constraints given in [<xref ref-type="bibr" rid="scirp.75556-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.75556-ref14">14</xref>] and [<xref ref-type="bibr" rid="scirp.75556-ref15">15</xref>] as to the influence of LIGO on our gravity models have to be looked into and not contravened.</p><p>This is a way of also showing if general relativity is the final theory of gravitation. i.e., if massive gravity is confirmed, as given in [<xref ref-type="bibr" rid="scirp.75556-ref16">16</xref>] , then GR is perhaps to be replaced by a scalar-tensor theory, as has been shown by Corda.</p><p>Finally is a re-do of what was brought up in [<xref ref-type="bibr" rid="scirp.75556-ref17">17</xref>] by Tang. In a density equation of stated with a relaxation procedure, between different physical states, Tank writes if m, and n are different quantum level states, then, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x34.png" xlink:type="simple"/></inline-formula> is the “Atomic coherence time”</p><disp-formula id="scirp.75556-formula19"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/12-2180186x35.png"  xlink:type="simple"/></disp-formula><p>We will here, in our work assign <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x36.png" xlink:type="simple"/></inline-formula> the same sort of physical state which would in place have if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x37.png" xlink:type="simple"/></inline-formula> in which then the solution to this problem would be given by Equation (11). The idea would be as follows. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x38.png" xlink:type="simple"/></inline-formula> model the density of states as having the flavor of gravitons preserving the essential quantum “state”<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x39.png" xlink:type="simple"/></inline-formula>, and not changing if we go from the Pre-Planckian to Planckian state.</p><p>There would be then the matter of identifying<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x41.png" xlink:type="simple"/></inline-formula>and the time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x42.png" xlink:type="simple"/></inline-formula>, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x43.png" xlink:type="simple"/></inline-formula>. In our review we would put <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x44.png" xlink:type="simple"/></inline-formula> likely as the Pre-Planck- ian to Planckian transition time.</p><p>Note that in the m = n time if our “density of states” was referring to gravitons, keeping the same states as if m = n is picked, that the second part of Equation (17) is in referral to quantum states of a graviton having a non-planar character which would not have a planar wave character.</p><p>In the case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x45.png" xlink:type="simple"/></inline-formula> we are then referring to changes in the states of presumed gravitons as information carriers, and the density equation, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x46.png" xlink:type="simple"/></inline-formula>has in Eq. (17) as a wave with explicit damped by time evolution wave component times a planar wave component.</p><p>We presume here that the frequency term, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x47.png" xlink:type="simple"/></inline-formula>would be in the high gigahertz range.</p><p>In any case, the details of this sketchy idea should be from the Pre-Planckian to Planckian regime of space-time given far more structure in a future document.</p><p>We should note that the removal of initial singularities is due to Non-Linear Electrodynamics, as seen in [<xref ref-type="bibr" rid="scirp.75556-ref7">7</xref>] , by Camara et al., which is also in tandem with [<xref ref-type="bibr" rid="scirp.75556-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.75556-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.75556-ref20">20</xref>] which give also frequency specifications, which could also affect<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/12-2180186x48.png" xlink:type="simple"/></inline-formula>, i.e. a tie in, with Gravitons, and Nonlinear Electrodynamics, which should be developed further.</p></sec><sec id="s4"><title>Acknowledgements</title><p>This work is supported in part by National Nature Science Foundation of China grant No. 11375279.</p></sec><sec id="s5"><title>Cite this paper</title><p>Beckwith, A.W. 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