<?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.2017.84029</article-id><article-id pub-id-type="publisher-id">JMP-74634</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>
 
 
  Higgs Field and Gauge Invariance in Spacetime Transformations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yougang</surname><given-names>Feng</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>College of Physics, Guizhou University, Guiyang, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>03</month><year>2017</year></pub-date><volume>08</volume><issue>04</issue><fpage>448</fpage><lpage>458</lpage><history><date date-type="received"><day>February</day>	<month>7,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>March</month>	<year>7,</year>	</date><date date-type="accepted"><day>March</day>	<month>10,</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>
 
 
  The concepts of the mass charge and the Higgs potential are proposed. The generation of the Higgs potential is a mutation, and the particles’ masses originate from the mechanism that the particles with mass charges obtain static energies under the potential, and the energies are regarded as the potential energies of the particles in the Higgs field, shared jointly by the field and the particles. The mass charge as an intrinsic property of a particle cannot change with its motion, and the potential’s change obeys the Lorentz transformation. When time warps the massless particles get masses, which are tensors. There is gauge invariance in the self-similar transformations of the spacetime, resulting in superlight and the cosmic inflation with the maximum speed more than five times light velocity, and the universe has been so far expanding at the superlight speed due to the dark energies (two thirds of the universe energies). An explicit figure for the creation of four types of Higgs fields is drawn. The orders of magnitudes of three characteristic temperatures relating to the time phase transitions are estimated. Finally, the effect of the Higgs field on the weak interaction and the spins’ chirality is discussed.
 
</p></abstract><kwd-group><kwd>Mass</kwd><kwd> Higgs</kwd><kwd> Potential</kwd><kwd> Gauge</kwd><kwd> Superlight</kwd><kwd> Inflation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>One of the most efficient methods in physics is the consideration of the symmetry of a physical system. Group theory and representation theory are the powerful tools for handling the symmetries of such a system. However, many patterns of nature are very complicated and irregular, in front of which the traditional geometry looks weak [<xref ref-type="bibr" rid="scirp.74634-ref1">1</xref>] . The degree of their irregularity and fragmentation is usually identical in all scales, which means there are fractal structures. Meanwhile those acquainted symmetry theories used in the conventional quantum theory cannot be directly applied in the analysis on fractals. Self similarities and hierarchies are required to be firstly considered. The spacetime lattice model revealed that in the evolution of the universe there had been fractal structures for the spacetime with higher dimensions than four [<xref ref-type="bibr" rid="scirp.74634-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] . The model shows us since the big bang generated the universe temperature is bound to have a decisive effect upon its growth process. The spontaneous breaking of the time local symmetry is an irreversible process and can be described by the renormalization group theory. In addition, according to the space lattice model, the vibration of the space lattices represents the fluctuation of thermal radiation energy, and the S bosons as the quanta of the radiation fluctuation should be matter particles, different from the quasiparticles such as the phonons, the quanta of the crystal lattice vibration. The time model suggests that the time field plays a main character in the standard model without which there could be no local symmetry-breaking. The time field is just the Higgs field.</p><p>The standard model has uniformly solved the Higgs mechanism and the Nambu-Goldstone mechanism by two ways on the imaginary plane [<xref ref-type="bibr" rid="scirp.74634-ref4">4</xref>] : one is on the real axis, and another is on the imaginary axis. However, the imaginary way doesn’t exist in our real world. We think the combination of the dynamic lattice model and the static model in the spacetime model is a better substitution for the ways [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] : the particles get masses through the Higgs mechanism in the static lattice model; the particles in the dynamic lattice model are still massless at the same time. The fact that the Higgs particles obtain masses in the Higgs field implies that the interaction of the Higgs particles and others may not the mechanism for getting other particles’ masses. Moreover, unlike the electric charge, the particle’s mass may not be the intrinsic property. Otherwise, it wouldn’t change in the relative motion. It seems that we should find more reasonable account for the mechanism. It is necessary to give an explicit physical pattern for the fractal structures of spacetime in order to study the connection between the normal spacetime and the fractal spacetime, especially the gauge invariance in the transformations. Talking about the transformation depends on the specific temperatures linking to the Higgs field. To ignore the temperature makes it impossible for us to understand the details of the critical behavior and the specific process for the spontaneous breaking of the local time symmetry, hindering our learning of the nature of the Higgs field and the real cause for the getting particle’s mass. Thus, the estimation of some characteristic temperatures should be done. The nature that the Higgs field is the time field contributes to our understanding about what role the field plays in the weak interaction. Up to this point, we set out to prove it.</p><p>In Section 2, introducing the mass charge and the Higgs potential, we explain the mechanism for the getting of mass and give an explicit figure for the self- similar transformations, in which gauge invariance is found, leading to superlight in the fractal structures. In Section 3, we discuss four types of Higgs fields and three characteristic temperatures for the time phase transitions, and their orders of magnitudes are estimated. We find the temperature region of the cosmic inflation, and the maximum inflation speed is calculated. We conclude that the universe has been so far expanding due to the dark energies, which are two thirds of the universe energies (about 66.7%). Finally, we discuss how the Higgs field effects statistically on the weak interaction and the spins’ chirality. Section 4 is conclusion remark.</p></sec><sec id="s2"><title>2. Theory</title><sec id="s2_1"><title>2.1. Mass Charge and Higgs Potential</title><p>The so-called independent freedom degree in the principle of the partition of the independent freedom degrees refers to the independent dimension [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] , the real time is an independent one. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x2.png" xlink:type="simple"/></inline-formula> be a mass charge for a particle, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x3.png" xlink:type="simple"/></inline-formula>be the potential function of the Higgs field, the particle obtains its static energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x4.png" xlink:type="simple"/></inline-formula> under the potential</p><disp-formula id="scirp.74634-formula12"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x5.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x6.png" xlink:type="simple"/></inline-formula>is a physical parameter on the time dimension; it has vanishing components in the space as the orthogonality between them, and</p><disp-formula id="scirp.74634-formula13"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x7.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x8.png" xlink:type="simple"/></inline-formula>, is the component in the time and space, respectively. It should be emphasized that the static energy is the potential energy of the particle in the Higgs field, shared jointly by the field and the particle. The mass is given by</p><disp-formula id="scirp.74634-formula14"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x9.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x10.png" xlink:type="simple"/></inline-formula> is the light speed. As a quantum parameter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x11.png" xlink:type="simple"/></inline-formula>is proportional to the time-order intensity at absolute zero <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x12.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.74634-ref2">2</xref>] , and</p><disp-formula id="scirp.74634-formula15"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x13.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x14.png" xlink:type="simple"/></inline-formula> is a constant. Since the Higgs particles condense, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x15.png" xlink:type="simple"/></inline-formula> has a saturated value, hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x16.png" xlink:type="simple"/></inline-formula> is a constant.</p><p>We can construct a field (the space field) variable <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x17.png" xlink:type="simple"/></inline-formula> by means of the property of the S bosons [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] , and combining Equation (1), we get the Klein- Gorden field equation</p><disp-formula id="scirp.74634-formula16"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x18.png"  xlink:type="simple"/></disp-formula><p>We take <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x19.png" xlink:type="simple"/></inline-formula> unit. Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x20.png" xlink:type="simple"/></inline-formula>, so<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x21.png" xlink:type="simple"/></inline-formula>. The mass charge is the intrinsic property of the S boson, it cannot change, thus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x22.png" xlink:type="simple"/></inline-formula>. Therefore,</p><disp-formula id="scirp.74634-formula17"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x23.png"  xlink:type="simple"/></disp-formula><p>Because the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x24.png" xlink:type="simple"/></inline-formula> is independent of time [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] , i.e., the S bosons move at the light speed in the space, except the time dimension. So the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x25.png" xlink:type="simple"/></inline-formula> in Equation (5) should be the potential’s components in the space, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x26.png" xlink:type="simple"/></inline-formula>, rather than the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x27.png" xlink:type="simple"/></inline-formula>.This consequence accords with Equation (2), vice versa. Equation (6) opens to us that if a particle is independent of the time dimension, available to the dynamic lattice model, the relevant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x28.png" xlink:type="simple"/></inline-formula>; conversely, fitting to the static lattice model and the relevant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x29.png" xlink:type="simple"/></inline-formula>,, being constant.</p><p>In the relative motion, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x30.png" xlink:type="simple"/></inline-formula>changes on the Lorentz transformation,</p><disp-formula id="scirp.74634-formula18"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x31.png"  xlink:type="simple"/></disp-formula><p>It results in the change of the mass for a particle moving along the x (x’) axis at the velocity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x32.png" xlink:type="simple"/></inline-formula> with respect to the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x33.png" xlink:type="simple"/></inline-formula>, and the mass is</p><disp-formula id="scirp.74634-formula19"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x34.png"  xlink:type="simple"/></disp-formula><p>The mass charge is the proper physical property of the particle, not changing with the motion. For the particle moving at the light speed, Equation (7) makes the potential no sense, since the particle is independent of the time in the dynamic lattice model [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] . The relevant energy-momentum relation becomes</p><disp-formula id="scirp.74634-formula20"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x35.png"  xlink:type="simple"/></disp-formula><p>where E and p are respectively the energy and the momentum for the particle. We may let the unit of the mass charge be <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x36.png" xlink:type="simple"/></inline-formula> in the quantum theory, then the potential will be <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x37.png" xlink:type="simple"/></inline-formula> if the unit of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x38.png" xlink:type="simple"/></inline-formula> is taken.</p><p>Except quarks and those composite particles like the protons and neutrons containing internal structures, all of elementary matter particles have their own mass charges, even if for those massless particles such as S bosons, photons, and gravitons. Both a particle and its antiparticle have the same mass charge, and the charges of particles of different types are distinguishable from each other. Since the particles sharing the time dimension only have limited moving speed, and they always immerge in the Higgs potential, which is full of the whole time dimension, such that there is no negative mass. The uniqueness of the mass charge leads to that unlike the electric neutrality for the electric charges, there is no the mass neutrality for the mass charges. The mass conservation depends only on the static energy conservation, if the mass conservation holds, so does the mass charges.</p><p>Let’s set up a man-made reference coordinate system, its time axis is always orthogonal to the space, no matter whether or not warps the real tome, i.e., the natural time. The field of the natural time does be the Higgs field. When the natural time warps, the Higgs potential varies with the space position, it may be represented by a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x39.png" xlink:type="simple"/></inline-formula> matrix in the reference system as the following</p><disp-formula id="scirp.74634-formula21"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x40.png"  xlink:type="simple"/></disp-formula><p>The particle gets its static energy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x41.png" xlink:type="simple"/></inline-formula> under the potential<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x42.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.74634-formula22"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x43.png"  xlink:type="simple"/></disp-formula><p>where the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x44.png" xlink:type="simple"/></inline-formula> is the components of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x45.png" xlink:type="simple"/></inline-formula>. The S bosons, photons, and gravitons will become massive particles, their masses behave in a tensor form</p><disp-formula id="scirp.74634-formula23"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x46.png"  xlink:type="simple"/></disp-formula><p>where the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x47.png" xlink:type="simple"/></inline-formula> is the components of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x48.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s2_2"><title>2.2. Gauge Invariance and Superlight</title><sec id="s2_2_1"><title>2.2.1. Two Descriptions for the Transformations</title><p>An ordered block of the cubic lattice model exists really in the 3-dimensional space, however, it’s impossible to compute accurately the block’s ordered state in the space. Reference [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] tells us that it can be solved in a higher dimensional space by means of topological analysis: the block is equivalent to a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula>-dimensional simple connected space, where the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x50.png" xlink:type="simple"/></inline-formula> is the fractal dimension of its sub-block. An explicit explanation of the self-similar transformations conduces to understand the reason why there exists the gauge invariance. There are two descriptions for the transformations: direct and equivalent. The spacetime lattice model is topologically the cubic lattice system, its transformations can be directly described by the self-similar transformation theory [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] , which is called the direct description: On the zero-th hierarchy there are only infinite original lattices, some of them form a first-order sub-block of D-dimension on the first hierarchy, and the original lattices become the lattices in the inner space of the first-order sub-block. On the first hierarchy some the first-order sub-blocks make up a first-order block with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x51.png" xlink:type="simple"/></inline-formula>-dimension, these sub-blocks map into the lattices in the first-order block at the same time. Thus, the first time self-similar transformation succeeds on the first hierarchy, and the blocks have the same symmetry as the original lattices’. On the r-th hierarchy, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x52.png" xlink:type="simple"/></inline-formula>, there are r-order sub-blocks, each sub-block contains lattices, each of which is the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x53.png" xlink:type="simple"/></inline-formula>)-order block on the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x54.png" xlink:type="simple"/></inline-formula>)-th hierarchy. On this r-th hierarchy some r-order sub-blocks construct a r-order block, and these r-order sub-blocks become the lattices in the r-order block. Only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x55.png" xlink:type="simple"/></inline-formula>, the whole system is an ordered block, and the system turns into the ordered state, otherwise disordered.</p><p>Equivalent description: Because there is no interaction between the sub-block and the block [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] , from the point of view of the interaction the system is viewed as a reducible system including two independent irreducible subsystems: the sub-blocks subsystem and the blocks subsystem. The two subsystems exist on the same hierarchy. Each subsystem has its own self-similar transformation: 1. Some (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x56.png" xlink:type="simple"/></inline-formula>)-order sub-blocks of the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x57.png" xlink:type="simple"/></inline-formula>)-th hierarchy form a r-order sub-block on the r-th hierarchy, and these (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x58.png" xlink:type="simple"/></inline-formula>)-order sub-blocks become the lattices in the r-order sub-block. 2. Some (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x59.png" xlink:type="simple"/></inline-formula>)-order blocks of the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x60.png" xlink:type="simple"/></inline-formula>)-th hierarchy produce cooperatively a r-order block on the r-th hierarchy, these (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x61.png" xlink:type="simple"/></inline-formula>)-order blocks shrinks into the lattices in the r-order block.</p></sec><sec id="s2_2_2"><title>2.2.2. Gauge Invariance</title><p>It’s necessary to reaffirm the scaling law here, although it has been described in the reference [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] . The rule of the hierarchy is that the r-order sub-blocks (blocks) exist only on the r-th hierarchy, they should shrink into the lattices on the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x62.png" xlink:type="simple"/></inline-formula>)-th hierarchy; as a lattice the sub-block (block) has no internal structure. The scaling law concerns with the distinguishability of the internal space of a sub-block (block), relating to two cases: 1. If we describe the system by using the interaction between the r-order sub-blocks (blocks) and omit the interaction between the lattices in the sub-blocks (blocks) as the illustration of the Formula (7) in the reference [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] , the internal space of each sub-block (block) should be thought of as indistinguishable on the r-th hierarchy although the sub-blocks (blocks) are not the lattices, and their outside space is just the 4-dimensional spacetime. 2. If we consider only the similar structures of the r-order sub-blocks (blocks), the internal space of each sub-block (block) is distinguishable with a definite fractal dimension. For the first case, there are infinite sub-blocks on the r-th hierarchy, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x63.png" xlink:type="simple"/></inline-formula>,we make the symmetric center of a r-order sub-block represent it, the radius of the sphere covering the center equals<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x64.png" xlink:type="simple"/></inline-formula>, where c is the light speed, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x65.png" xlink:type="simple"/></inline-formula> is the time element of the sub-block, the orientation of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x66.png" xlink:type="simple"/></inline-formula> can be either positive or negative. The sphere equation is</p><disp-formula id="scirp.74634-formula24"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x67.png"  xlink:type="simple"/></disp-formula><p>The coordinates of a point on the sphere is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x68.png" xlink:type="simple"/></inline-formula>, the left side of Equation (13) is the square of the distance between the sphere center and the point. Since the outside space of the sub-block is the 4-dimensional spacetime, Equation (13) manifests the Lorentz gauge. In the second case mentioned above, the r-order sub-block is just the lattice in a (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x69.png" xlink:type="simple"/></inline-formula>)-order sub-block on the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x70.png" xlink:type="simple"/></inline-formula>)-th hierarchy, the radius of the sphere covering this lattice is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x71.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x72.png" xlink:type="simple"/></inline-formula> is the velocity at which the massless particles move in the inner space of the sub-block, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x73.png" xlink:type="simple"/></inline-formula>is the lattice’s time element and its orientation takes positive or negative. Like the Equation (13), its sphere equation is expressed as</p><disp-formula id="scirp.74634-formula25"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x74.png"  xlink:type="simple"/></disp-formula><p>The outside spacetime of the lattice does be the inner spacetime of the sub- block, which is (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x75.png" xlink:type="simple"/></inline-formula>)-dimensions (the space is D-dimensional). The r-order sub-block and the lattice in the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x76.png" xlink:type="simple"/></inline-formula>)-order sub-block are the same object. As the self-similar transformation the scale should be invariant, thus</p><disp-formula id="scirp.74634-formula26"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x77.png"  xlink:type="simple"/></disp-formula><p>With the same reason, for the r-order block on the r-th hierarchy its covering sphere leads to equation</p><disp-formula id="scirp.74634-formula27"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x78.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x79.png" xlink:type="simple"/></inline-formula> is the time element of the block, it can be positive or negative. The same object becomes the lattice in the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x80.png" xlink:type="simple"/></inline-formula>)-order block, the equation for its covering sphere follows</p><disp-formula id="scirp.74634-formula28"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x81.png"  xlink:type="simple"/></disp-formula><p>The outside spacetime of the lattice is the inner spacetime of the block (the space is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x82.png" xlink:type="simple"/></inline-formula>-dimensions), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x83.png" xlink:type="simple"/></inline-formula>is the velocity at which the massless particles move in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x84.png" xlink:type="simple"/></inline-formula>-dimensional spacetime. As the scaling law, all of lattices have the same time element<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x85.png" xlink:type="simple"/></inline-formula>, just like the lattice spin <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x86.png" xlink:type="simple"/></inline-formula> in the Ising model [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] . By the scaling law, Equations (16) and (17) yield</p><disp-formula id="scirp.74634-formula29"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x87.png"  xlink:type="simple"/></disp-formula><p>Equations (15) and (18) imply gauge invariance in the transformations. The gauge belongs only to the metric space, which here is the spacetime, and as the scale the length standard at each spacetime point is of locality. The so-called scale is also named after the gauge. The self-similar transformations keep the gauge constant in local range. All of these fractal structures with invariant gauge make up of a gauge system. It is just the spacetime itself. In this sense, the properties of the gauge fields exhibit the intrinsic properties of the spacetime.</p></sec><sec id="s2_2_3"><title>2.2.3. Superlight</title><p>The one-to-one relation between the time lattice model and the Ising model suggests that the sub-block’s time element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula> corresponds to the sub-block’s spin<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x89.png" xlink:type="simple"/></inline-formula>, the block’s time element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x90.png" xlink:type="simple"/></inline-formula> to the block’s spin<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x91.png" xlink:type="simple"/></inline-formula>, and the lattice’s time element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x92.png" xlink:type="simple"/></inline-formula> to the lattice’s spin s. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x93.png" xlink:type="simple"/></inline-formula>, like <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x94.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] . Using the Formula (6.1) of the reference [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] , we have</p><disp-formula id="scirp.74634-formula30"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x95.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x96.png" xlink:type="simple"/></inline-formula> is the coordinate number for the sub-block of the cubic lattice, and D is its fractal dimension, hence</p><disp-formula id="scirp.74634-formula31"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x97.png"  xlink:type="simple"/></disp-formula><p>Similarly, the block’s time element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x98.png" xlink:type="simple"/></inline-formula> is given by the Formula (6.2) for the same reference, and</p><disp-formula id="scirp.74634-formula32"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x99.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x100.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x101.png" xlink:type="simple"/></inline-formula>are the block’s coordinate number and the number of sub-blocks in a block. Thus,</p><disp-formula id="scirp.74634-formula33"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x102.png"  xlink:type="simple"/></disp-formula><p>Combining Equations (15) and (18), we get</p><disp-formula id="scirp.74634-formula34"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x103.png"  xlink:type="simple"/></disp-formula><p>Obviously, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x105.png" xlink:type="simple"/></inline-formula>, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x106.png" xlink:type="simple"/></inline-formula> (see the Formula (5) of the same reference). The consequence signifies that there are superlight phenomena in the fractal structures. Since the fractal dimension D is constant at a fixed temperature, the similarity between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x107.png" xlink:type="simple"/></inline-formula> and c, or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x108.png" xlink:type="simple"/></inline-formula> and c (the linear relationship between them) indicates the superlight is a necessary condition for the maintaining of the gauge in different dimensional spacetime. The c, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x109.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x110.png" xlink:type="simple"/></inline-formula> are actually the constant quantities for the same gauge, their values depend on the dimensions of the relevant spacetime.</p></sec></sec></sec><sec id="s3"><title>3. Discussion</title><sec id="s3_1"><title>3.1. Four Types of Higgs Fields</title><p>Consider the direct description said in the subsection 2.2.1. On the first hierarchy the original lattices form a sub-block in an ordered time state, these lattices make up the first type of Higgs field. Infinite sub-blocks construct the second type of Higgs field, and cooperate to retain the field in the disordered time state. The lattices in a block correlate to each other to build up the third type of Higgs field, and the block is in an ordered time state. The fourth type of the field is set up by infinite blocks, and the time is in disordered state for the field. After infinitely hierarchical transformations the system’s time is ordered, meanwhile the temperature is in the region of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x111.png" xlink:type="simple"/></inline-formula>. The three types of Higgs fields disappear at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x112.png" xlink:type="simple"/></inline-formula>, except the first type, which becomes the Higgs field to give the particles masses. The Higgs field is a mutant, too, the occurrence of Higgs particles. That the Higgs particles have masses is an evidence for the field’s self-energy.</p></sec><sec id="s3_2"><title>3.2. Three Characteristic Temperatures</title><p>Weinberg pointed out that the radiation would have continued to predominate over matter until the temperature dropped to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.74634-ref6">6</xref>] . If his mention is true, the estimated critical temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula> of the Bose-Einstein condensation phase transition of the time may be in the order of magnitude of about<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula>. Making use of the gauge theories, D.A. Kirzhnits and A.D. Lind got the transition temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x116.png" xlink:type="simple"/></inline-formula> of about <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x117.png" xlink:type="simple"/></inline-formula> for the electro-weak phase transition [<xref ref-type="bibr" rid="scirp.74634-ref7">7</xref>] . In the following we try to estimate the critical temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x118.png" xlink:type="simple"/></inline-formula> for the time order-disorder phase transition. According to the reference [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] , the equivalent description get the critical point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x119.png" xlink:type="simple"/></inline-formula> of the system, which is the sum of the critical point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x120.png" xlink:type="simple"/></inline-formula> of the sub-blocks subsystem and the critical point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x121.png" xlink:type="simple"/></inline-formula> of the blocks subsystem:</p><disp-formula id="scirp.74634-formula35"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x122.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.74634-formula36"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x123.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula> are the coupling constants for the sub-blocks and the blocks, respectively, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula>is Boltzmann constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula>is the minimum fractal dimension for the cubic [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] . The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula> corresponds to a fractal side<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula>, which doesn’t accords with the transformation since only the integer sides can keep the original symmetry. We use the mean value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula> of the fractal dimensions relating to the integer sides <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula> instead of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula>. We notice that rather than the Higgs field, the strong interaction is mainly responsible for the quarks’ static energies; on the other hand the coupling constant is the exchange integral associated with the interaction. The critical temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula> should guarantee the creation of the quarks, this requires that the constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x135.png" xlink:type="simple"/></inline-formula> should at least be the order of magnitude of the largest static energy among the quarks’, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x136.png" xlink:type="simple"/></inline-formula>(<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x137.png" xlink:type="simple"/></inline-formula>), the top quark’s static energy. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x138.png" xlink:type="simple"/></inline-formula>, and the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x139.png" xlink:type="simple"/></inline-formula> instead of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x140.png" xlink:type="simple"/></inline-formula>, we obtain by Equation (25)</p><disp-formula id="scirp.74634-formula37"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x141.png"  xlink:type="simple"/></disp-formula><p>The value of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x142.png" xlink:type="simple"/></inline-formula> calculated by the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x143.png" xlink:type="simple"/></inline-formula> is too small to be adopted.</p></sec><sec id="s3_3"><title>3.3. The Temperature Region of Cosmic Inflation</title><p>By the reference [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] , we know that the dark particles are also involved in the superlight particles. In the temperature region <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x144.png" xlink:type="simple"/></inline-formula> all particles travel at the superlight speed in the fractal structures. The more closely to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x145.png" xlink:type="simple"/></inline-formula> the temperature reaches, the bigger the sizes of the sub-blocks and the blocks turn into, the higher the fractal dimensions will be, and the faster than the light speed the particles’ velocities will become (see Equation (23)), and the more room will be full of the particles. The particles’ behavior results directly in the cosmic inflation [<xref ref-type="bibr" rid="scirp.74634-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.74634-ref9">9</xref>] , the huger inflation will take place in the vicinity of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x146.png" xlink:type="simple"/></inline-formula>. The maximum fractal dimension <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x147.png" xlink:type="simple"/></inline-formula> is given by the Equation (5) of the reference [<xref ref-type="bibr" rid="scirp.74634-ref5">5</xref>] when the block’s side n tends to infinity,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x148.png" xlink:type="simple"/></inline-formula>. We then get the fastest limiting speed <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x149.png" xlink:type="simple"/></inline-formula> of the inflation through Equation (23),</p><disp-formula id="scirp.74634-formula38"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x150.png"  xlink:type="simple"/></disp-formula><p>More than five times the light speed! We see that the superlight phenomena exist on all hierarchies, so the inflation is uniform in the sense of both locality and globality.</p></sec><sec id="s3_4"><title>3.4. Dark Energies</title><p>Since the fractal structures exist in the thermal equilibrium state, the cosmic energies distribute evenly in the three spacetimes. The sub-blocks and the blocks lie on the same hierarchy and share the same 4-dimansional spacetime occupied by one third of the energies (about 33.3%), the relevant particles get masses under the Higgs field when the temperature decreases, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x151.png" xlink:type="simple"/></inline-formula>, and the energies are measurable. The (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x152.png" xlink:type="simple"/></inline-formula>)-dimensional spacetime and the (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x153.png" xlink:type="simple"/></inline-formula>)-dimen- sional spacetime are full of two thirds of the energies (about 66.7%), corresponding to the accelerating expansion of the universe, they are dark energies [<xref ref-type="bibr" rid="scirp.74634-ref10">10</xref>] . Because the superlight particles keep their original high speeds after the electro-weak phase transition and the particles of the 4-dimensional spacetime, which speeds are no more than the light velocity, catch up impossibly with them, therefore, the energies cannot be measured.</p></sec><sec id="s3_5"><title>3.5. Effect of Higgs Field on Weak Interaction and Spins’ Chirality</title><p>The first effect is that the Higgs particles can transfer into<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x154.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x155.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x156.png" xlink:type="simple"/></inline-formula> particles. The second, the field as a background maintains the breaking of the time local inverse symmetry. According to the statistical mechanism the uniform space embodies that the trajectory of a representative point passes, in the time course, through any neighborhood of any point of the relevant region of the phase space. The mean value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x157.png" xlink:type="simple"/></inline-formula> of a physical parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x158.png" xlink:type="simple"/></inline-formula> is defined as</p><disp-formula id="scirp.74634-formula39"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x159.png"  xlink:type="simple"/></disp-formula><p>for the time inverse symmetry, corresponding to the detailed balance principle: a tendency of a physical system to transfer one state to another must be counterbalanced by an identical tendency to switch between the tendency states in the reverse direction. The duality between the time and the energy is an intrinsic property of the nature [<xref ref-type="bibr" rid="scirp.74634-ref11">11</xref>] , not only for their values, but also for their polarity. An antiparticle posses the energy reversing to the particle’s, corresponding to the time inverse transformation. This idea is formulated as a rule of the Feynman diagrams: for instance, for two incident particles, electron and positron, the time direction referring to the latter is drawn by a reverse arrow against the electron’s. For the weak interaction system the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula> is assigned as the particle’s spin or its energy. As the spin, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula>means the spin-up state; and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula>, the spin-down state. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x163.png" xlink:type="simple"/></inline-formula>can be rewritten as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x164.png" xlink:type="simple"/></inline-formula>, corresponding to the time inverse, which means if the time is inverse symmetry, so<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x165.png" xlink:type="simple"/></inline-formula>, the two spin states have the same probability. As the energy, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x166.png" xlink:type="simple"/></inline-formula>refers to the particle’s energy, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x167.png" xlink:type="simple"/></inline-formula>to its antiparticle’s. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x168.png" xlink:type="simple"/></inline-formula>, the two types have the same total number since the time inverse symmetry. When Higgs field is established not all of lattices have the positive time direction unless at the absolute zero. The breaking of the time inverse symmetry holds locally, Equation (28) should be revised by</p><disp-formula id="scirp.74634-formula40"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x169.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x170.png" xlink:type="simple"/></inline-formula>. For weak interaction the force range is too small to have an infinite equilibrium period. The real equilibrium period should be finite, denoted as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x171.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x172.png" xlink:type="simple"/></inline-formula>. Therefore, Equation (29) changes into</p><disp-formula id="scirp.74634-formula41"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7503083x173.png"  xlink:type="simple"/></disp-formula><p>where the integral region is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7503083x174.png" xlink:type="simple"/></inline-formula>. Equation (30) states that the symmetries of the spins and the particles’ energies are statistically broken [<xref ref-type="bibr" rid="scirp.74634-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.74634-ref13">13</xref>] . The space lattice model indicates the particles such as S bosons are independent of the time [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] , Equation (30) is not available to them, which may be the primary reason why these particles are just their antiparticles.</p><p>The space field has both right-handed system and left-handed system, each system includes its own gradient field and curl field, shown as Equations (8), (9), (10), and (11) of the reference [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] . According our theory [<xref ref-type="bibr" rid="scirp.74634-ref14">14</xref>] , electric charge stimulates the right-handed system, requiring sufficiently and necessarily the right-handed spins, and mass only another system the left-handed spins are applicable to, vice versa. Therefore, electrons’ spins are chiral symmetric, and neutrinos’ spins are only left-handed rotation [<xref ref-type="bibr" rid="scirp.74634-ref15">15</xref>] . Instead of t, the negative time -t makes the left-handed system change into the right-handed system, relating to the antineutrinos’ spins. Since the S bosons are the quanta of the space field, their spins are of chiral symmetry, and the photons and the gravitons as the excitation states of the S bosons maintain the characteristics [<xref ref-type="bibr" rid="scirp.74634-ref3">3</xref>] .</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>In the evolution of the universe the time underwent three phase transitions with three characteristic temperatures. The fractal structures of the spacetime possess super symmetries and hierarchies under the gauge invariance, in which we have found the cosmic inflation and dark energies. The concepts of the mass charge and the Higgs potential make us understand the meaning of the mass. Further, the concept of mass tensor is suggested if the time warps. The particles’ helicities are determined by the space field.</p></sec><sec id="s5"><title>Cite this paper</title><p>Feng, Y.G. (2017) Higgs Field and Gauge Invariance in Spacetime Transformations. Journal of Modern Physics, 8, 448-458. https://doi.org/10.4236/jmp.2017.84029</p></sec></body><back><ref-list><title>References</title><ref id="scirp.74634-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mandelbrot, B.B. (1983) The Fractal Geometry of Nature. W.H. Freeman and Company, New York.</mixed-citation></ref><ref id="scirp.74634-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Feng, Y. (2016) Journal of Modern Physics, 7, 536-542. https://doi.org/10.4236/jmp.2016.76056</mixed-citation></ref><ref id="scirp.74634-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Feng, Y. 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