<?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.2014.518200</article-id><article-id pub-id-type="publisher-id">JMP-52373</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>
 
 
  Axiom Cosmology: A New Direction
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>onghong</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>School of Automation, Wuhan University of Technology, Wuhan, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hylinin@163.com</email></corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>12</month><year>2014</year></pub-date><volume>05</volume><issue>18</issue><fpage>2041</fpage><lpage>2048</lpage><history><date date-type="received"><day>10</day>	<month>October</month>	<year>2014</year></date><date date-type="rev-recd"><day>8</day>	<month>November</month>	<year>2014</year>	</date><date date-type="accepted"><day>2</day>	<month>December</month>	<year>2014</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>
 
 
  In this work we have to deal with the axiomatization of cosmology, but it is only recently that we have hit upon a new mathematical approach to capitalize on our new set identities for the basic laws of cosmology. So our proposal of settlement is that we will propose some new laws (e.g., formation of the black hole). We introduce the concept of axiom cosmology. This principle describes the cosmology which can get freedom from the notion of the induction. We present a large-scale structure model of the universe, and this leads to successfully explanation of problem of closed universe or open universe (because from the outset it is theorem and its succinct proof). In this paper we prove that the non-singular point theorem means that a singularity cannot be mathematically defined nor physical. It allows us to overcome the mysterious, physical singularity conundrum and explain meaningful antimatter annihilations for general configurations.
 
</p></abstract><kwd-group><kwd>Axiom Cosmology</kwd><kwd> Matter</kwd><kwd> Antimatter</kwd><kwd> Dark Matter</kwd><kwd> Black Holes</kwd><kwd> Singularity</kwd><kwd> Large-Scale Structure</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Tackling the Hillber’s 6th problem (mathematical treatment of the axioms of physics), axiomatization of quantum mechanics has been a success. The problem known as stair goes on the development of physics and mathematics. In the long view of history, Galileo was one of the first modern thinkers to clearly state that the laws of nature were mathematical. In his book The Assayer he wrote “Philosophy is written in this grand book, the universe... It is written in the language of mathematics, and its characters are triangles, circles, and other geometric figures; ...” [<xref ref-type="bibr" rid="scirp.52373-ref1">1</xref>] . Generally, the modern era in cosmology began with Albert Einstein’s 1915 formulation of general relativity [<xref ref-type="bibr" rid="scirp.52373-ref2">2</xref>] , which made it possible to quantitatively predict the origin, evolution, and conclusion of the universe as a whole; his sweeping extension of Newton’s theory of gravity, and the differential geometry is the mathematical basis of general relativity. By embedding gravity in a geometrical picture of space and time, Einstein was able to think in grand terms about the global structure of the universe [<xref ref-type="bibr" rid="scirp.52373-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.52373-ref4">4</xref>] . The positive energy theorem in general relativity demonstrated―sixty years after its discovery―that Einstein’s theory was consistent and stable [<xref ref-type="bibr" rid="scirp.52373-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.52373-ref6">6</xref>] . Most modern, accepted theories of cosmology are based on general relativity and, more specifically, the predicted Big Bang [<xref ref-type="bibr" rid="scirp.52373-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.52373-ref8">8</xref>] . In the universe, the axiom field represents a particularly attractive candidate for the dark matter [<xref ref-type="bibr" rid="scirp.52373-ref9">9</xref>] . Dark matter’s existence is inferred from gravitational effects on visible matter and gravitational lensing of background radiation [<xref ref-type="bibr" rid="scirp.52373-ref10">10</xref>] . Likewise, a significant amount of non-baryonic, cold matter is necessary to explain the large-scale structure of the universe [<xref ref-type="bibr" rid="scirp.52373-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.52373-ref12">12</xref>] . Hawking was able to come to his proof using mathematical techniques that had been developed by Roger Penrose [<xref ref-type="bibr" rid="scirp.52373-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.52373-ref14">14</xref>] . To solve the problem of the singularity, Hawking, Hertog and Reall introduced a virtual time and constructed the no-boundary universe model [<xref ref-type="bibr" rid="scirp.52373-ref15">15</xref>] . The Lambda Cold Dark Matter (abbreviated ΛCDM) model affords no explanation for dark energy and dark matter in physical cosmology. It is merely a useful parametric form of the Big Bang cosmological model [<xref ref-type="bibr" rid="scirp.52373-ref16">16</xref>] . In a manner of speaking, the matter and the antimatter have a close relationship and a mutual influence; matter plays a central role in cosmology, and black holes are a favorite testing ground for quantum gravity [<xref ref-type="bibr" rid="scirp.52373-ref17">17</xref>] . However, in this case, quantum-logic is a set of rules for reasoning about propositions which takes the principles of quantum theory into account [<xref ref-type="bibr" rid="scirp.52373-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.52373-ref19">19</xref>] . It seems that what is “logical system of cosmology” in physics is unknown. The problem will get surprisingly little attention from the cosmology world, yet this paper is an interesting step forward in exploring cosmological logic to some extent. So, we need an accurate law, no need for a hasty approximation. Let us start out by understanding set theory of the universe that axiom holds [<xref ref-type="bibr" rid="scirp.52373-ref20">20</xref>] . First of all, it is interesting to note that the set theory, cosmology and quantum mechanics have showed blood relationship, but then we also discover that the global geometry has a deep kinship with them. The aim of the research is to provide a powerful tool, and it is tempting to use the tool to solve big problems of cosmology, such as overcoming physical singularity of space-time using set operations. In cosmology, to introduce the principle of duality and the laws of mathematics is translated into the physical laws, i.e. use quantifiers to express the quantum mechanics object and cosmology object as a logical expression. The study found some of the physics laws such as the zero-point symbiosis law. We introduce the large-scale structure model of the universe. For explanation, we discuss some basic theories on the closed universe, open universe and lattice angle. How can we make mathematics model for antimatter? For example, when matter and antimatter meet, do they annihilate in a big explosion and convert their mass to energy? Still, to conclude this section, I am pushing to bring forward the axiom cosmology.</p></sec><sec id="s2"><title>2. Cosmological Set Theory and Large-Scale Structure Models</title><p>The concept of set to appear in cosmology, only when the cosmology and set theory, which neatly unifies. In the background of the conception are the matter set and the antimatter set, and how to work with the operation and the rules. The universe axiom systems contain these set laws, that is, domination laws, identity laws, complementation laws, difference-set law and Liu’s law, etc. (see [<xref ref-type="bibr" rid="scirp.52373-ref20">20</xref>] ).</p><p>In addition, the cosmic set is a kind of application logic. This logic is said to be mathematical logic of the universe. The domination logic has a natural cosmology interpretation, and the explanation does not depend on experience, so we can use it to structure the cosmological mathematical structure. These logical inconsistencies can be avoided by building set theory starting with basic assumptions, called axioms; for instance, the identities of universe algebraic is used to model the astrophysics.</p><p>In this section, we will briefly describe some components of the cosmological sets, and go on to describe later in the article. Let us to view universe mathematically first and establish a geometry for it later. Sets can be represented graphically using curve. We draw a curved surface to indicate the universal set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x5.png" xlink:type="simple"/></inline-formula>, which is the set of the curve. We use notation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x6.png" xlink:type="simple"/></inline-formula> to denote the curve diagram of the sets, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x7.png" xlink:type="simple"/></inline-formula>is a finite set. In curved surface, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x8.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x9.png" xlink:type="simple"/></inline-formula> be a coordinate set of operation. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x10.png" xlink:type="simple"/></inline-formula> be a universe operation. The tow operations in cosmology that we will use most are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x11.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x12.png" xlink:type="simple"/></inline-formula>.</p><p>From general topology, a set 1 (one), called the space, whose elements are called points. So the following theorem will help us to compute a convex for the universe, and it will also be useful when we apply global geometry theory to depicting dark matter, dark energy and black holes.</p><sec id="s2_1"><title>2.1. Theorem (Curl of U)</title><p>In space, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x13.png" xlink:type="simple"/></inline-formula> be a topological space, so</p><disp-formula id="scirp.52373-formula999"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x14.png"  xlink:type="simple"/></disp-formula><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x15.png" xlink:type="simple"/></inline-formula>. The sector between the curve <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x16.png" xlink:type="simple"/></inline-formula> and the curve <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x17.png" xlink:type="simple"/></inline-formula> be a convex in <xref ref-type="fig" rid="fig1">Figure 1</xref>(a).</p><p>Explicit proof for the theorem: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x18.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x19.png" xlink:type="simple"/></inline-formula> be drawing out two geodesics from vertex<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula>, and minimal neighborhood of the vertex G is split into two sectors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula> be two points in sector P, and X, Y adjacent to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x25.png" xlink:type="simple"/></inline-formula> so that geodesic <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x26.png" xlink:type="simple"/></inline-formula> cannot bypass the curve <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x27.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x28.png" xlink:type="simple"/></inline-formula> in <xref ref-type="fig" rid="fig1">Figure 1</xref>(b). Let point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x29.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x30.png" xlink:type="simple"/></inline-formula>. Then:</p><p>1) Point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x31.png" xlink:type="simple"/></inline-formula> on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x32.png" xlink:type="simple"/></inline-formula> in <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) and,</p><p>2) Point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x33.png" xlink:type="simple"/></inline-formula> on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x34.png" xlink:type="simple"/></inline-formula> in <xref ref-type="fig" rid="fig1">Figure 1</xref>(c).</p><p>For part 1), let geodesic <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula> on the outside of sector P, than the intersection of the G and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula>. Notice that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula> be a segment of geodesic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula>. With the same <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x40.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x41.png" xlink:type="simple"/></inline-formula>, and also on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x42.png" xlink:type="simple"/></inline-formula>, as in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x43.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x44.png" xlink:type="simple"/></inline-formula>, and also on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x45.png" xlink:type="simple"/></inline-formula>, then geodesic:</p><disp-formula id="scirp.52373-formula1000"><label>. (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x46.png"  xlink:type="simple"/></disp-formula><p>So we conclude that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x47.png" xlink:type="simple"/></inline-formula> on the outside of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x48.png" xlink:type="simple"/></inline-formula>. However, this is impossible.</p><p>For part 2), let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x50.png" xlink:type="simple"/></inline-formula>on geodesic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x51.png" xlink:type="simple"/></inline-formula>, with the same <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x52.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x53.png" xlink:type="simple"/></inline-formula>, and also on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x54.png" xlink:type="simple"/></inline-formula>, so the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x55.png" xlink:type="simple"/></inline-formula></p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> (a) The sector between the curve A and the curve U be a convex; (b) (c) The diagram showing that the sector P is convex; (b) Point F on GA; (c) Point F on GU.</title></caption><fig id ="fig1_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x56.png"/></fig><fig id ="fig1_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x57.png"/></fig><fig id ="fig1_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x58.png"/></fig></fig-group><p>of the geodesic <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x59.png" xlink:type="simple"/></inline-formula> replaced by the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x60.png" xlink:type="simple"/></inline-formula> of the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x61.png" xlink:type="simple"/></inline-formula>, as in all segment on geodesic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x62.png" xlink:type="simple"/></inline-formula>, substitute them completely, (in universal logic, the substitution principle we could use here) and though it is outside sector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x63.png" xlink:type="simple"/></inline-formula>. Prove that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x64.png" xlink:type="simple"/></inline-formula> is convex.</p><p>Interpretations for the theorem: In this proof, we often went further than that, if using a parametric equation, such as the differential equation of the geodesic, only work on differential geometry―nothing else. As far as curve goes, we know, convex closed curve and circumference are homeomorphism. The shape of the curved surface, on the other hand, is associated with the curvature. If they exist, it as a point on the convex surface can be divided into three categories as its own characteristics, namely, smoothing-point (tangent cone is a plane), diamond-point (tangent cone is a dihedral), and cone-point (tangent cone is less than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x65.png" xlink:type="simple"/></inline-formula>). Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x66.png" xlink:type="simple"/></inline-formula> be plane angle and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x67.png" xlink:type="simple"/></inline-formula> be dihedral, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x68.png" xlink:type="simple"/></inline-formula>. So, the distortion of the convex polyhedron is predictable for us, by contrast, the galaxy can distort the space-time in which it sits. Beyond that, we may see integral geometry for the convex surface in sector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x69.png" xlink:type="simple"/></inline-formula>. We will continue to discuss on this sector as a top priority. But there is much more to it than that. What does it mean to say that a sector is convex surface? The convex sector is a curved universe, physically. It’s this curving of the fabric of the universe that gravitational waves are fluctuations in the curvature of space which propagate through the universe as gravitational waves, so outward from its source, and we feel as gravity. Meanwhile, that the light travels in curve lines is certain in the large-scale universe.</p><p>The convex two sectors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x70.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x71.png" xlink:type="simple"/></inline-formula> (<xref ref-type="fig" rid="fig1">Figure 1</xref>(b))―the malleable fabric whose geometry can be changed by the gravity of stars, planets and matter―was born.</p><p>For the large-scale universe, we need to have a stable large-scale structure and critical cosmological angle because, candidly, the critical cosmological angle is possible in physics. Our standard from for the critical cosmological angle<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x72.png" xlink:type="simple"/></inline-formula>, is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x73.png" xlink:type="simple"/></inline-formula></p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) show the matter and dark matter for the cosmic angles<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x74.png" xlink:type="simple"/></inline-formula>. This curved space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x75.png" xlink:type="simple"/></inline-formula> is characterized by two properties:</p><p>3) If cosmic angles is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x76.png" xlink:type="simple"/></inline-formula>(or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x77.png" xlink:type="simple"/></inline-formula>), then the universe is a closed universe in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b).</p><p>4) If cosmic angles is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x78.png" xlink:type="simple"/></inline-formula>, then the universe is a open universe in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c).</p><p>Now we remark that for convex multiple sector, in general, we have the following laws.</p></sec><sec id="s2_2"><title>2.2. All Angle Law</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x79.png" xlink:type="simple"/></inline-formula> be a lattice angle (i.e. all angle), and let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x80.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.52373-formula1001"><label>. (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x81.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_3"><title>2.3. Impossibility Law</title><p>If a lattice angle <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x82.png" xlink:type="simple"/></inline-formula> and around a point in convex sector, then for any a shortest distance (i.e. geodesic) shalt not go through the point (i.e. not sucked into the singularity).</p></sec></sec><sec id="s3"><title>3. The Cosmic Laws</title><p>We could prove the existence of antimatter by cosmological argument, such as empty law:</p><disp-formula id="scirp.52373-formula1002"><label>. (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x83.png"  xlink:type="simple"/></disp-formula><p>It is a spirit in the pointer type, but we will arrive at meaning empty set, and we will give the set identities of the physical meaning. The following physical laws illustrate the relationship of matter and antimatter.</p><sec id="s3_1"><title>3.1. Black Hole Law</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x84.png" xlink:type="simple"/></inline-formula> be a black hole, and let A represent the matter sets, B represent the antimatter sets. If that is so, then</p><disp-formula id="scirp.52373-formula1003"><label>. (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x85.png"  xlink:type="simple"/></disp-formula><p>We’ve gotten to this point now: Our <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x86.png" xlink:type="simple"/></inline-formula> model for physics and explain observed phenomenon. It’s rare to find antimatter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x87.png" xlink:type="simple"/></inline-formula> in the large-scale universe<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x88.png" xlink:type="simple"/></inline-formula>, since it annihilates almost instantly when antimatter comes into contact with matter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x89.png" xlink:type="simple"/></inline-formula>. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x90.png" xlink:type="simple"/></inline-formula> only occasionally appears in high-energy collisions. Antimatter comes</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The diagram showing that the shapes of space for the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x94.png" xlink:type="simple"/></inline-formula>-critical angle, the dark matter is gray-shadowed. (a) (b) If cosmic angle<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x95.png" xlink:type="simple"/></inline-formula>, then the universe is a closed; (c) If cosmic angle<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x96.png" xlink:type="simple"/></inline-formula>, then the universe is a open.</title></caption><fig id ="fig2_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x91.png"/></fig><fig id ="fig2_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x92.png"/></fig><fig id ="fig2_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x93.png"/></fig></fig-group><p>into contact with regular matter, the two annihilate, disappearing in a high-energy flash of light. But remember to follow the black hole law so you don’t inadvertently get yourself in trouble, and do some careful calculations (or operations).</p><p>Similarly, we can also illustrate the physical significance of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x97.png" xlink:type="simple"/></inline-formula>, we have the following physical law.</p></sec><sec id="s3_2"><title>3.2. Universe Law</title><p>If the universe <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x98.png" xlink:type="simple"/></inline-formula> is compose of matter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x99.png" xlink:type="simple"/></inline-formula> and antimatter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x100.png" xlink:type="simple"/></inline-formula>, then</p><disp-formula id="scirp.52373-formula1004"><label>. (6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x101.png"  xlink:type="simple"/></disp-formula><p>Interpretations for the universe law: The antimatter area is used to existing in universe. Actually, this black hole law and universe law mean matter and antimatter is independent existence, but they have relevance.</p></sec><sec id="s3_3"><title>3.3. Natural Law (Mirror Image of U)</title><p>Antimatter is a mirror image of matter that is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x102.png" xlink:type="simple"/></inline-formula> in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). Similarly, the universe is a mirror image of black hole (empty set) that is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x103.png" xlink:type="simple"/></inline-formula> in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b).</p><p>Interpretations for the mirror image of U: In essence, understanding and controlling mirror images has led to the creation of many important matters. For every matter particle (say an electron, for example), a matching</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Matter A and black hole <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x106.png" xlink:type="simple"/></inline-formula> in mirror image. (a)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x107.png" xlink:type="simple"/></inline-formula>; (b)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x108.png" xlink:type="simple"/></inline-formula>. Although we did not quite capture how geometry; there is still much cherished value of the symbolic implication in the “empty space”.</title></caption><fig id ="fig3_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x104.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7502036x105.png"/></fig></fig-group><p>antimatter particle is thought to exist (in this case, a positron) with the same mass, but an opposite charge. This is the physical evidence of illustrated matter and antimatter. From a molecular perspective, the atoms in certain molecules can often take up two different configurations that are mirror images (chirality) of each other. From the particle physics perspective, particles and anti-particles to abide by the black hole law (upon collision), the conversion of a PARTICLE and its corresponding antiparticle into pure electromagnetic ENERGY (called annihilation radiation). The mesons to abide by the Universe law (each containing a quark and an antiquark). Of course, a particle can be out of the event horizon to infinitely far away and to abide by the universe law.</p></sec><sec id="s3_4"><title>3.4. Particle Law</title><p>If the black hole engulf the antiparticle<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x109.png" xlink:type="simple"/></inline-formula>, then</p><disp-formula id="scirp.52373-formula1005"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x110.png"  xlink:type="simple"/></disp-formula><p>where, the particle <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x111.png" xlink:type="simple"/></inline-formula> must become outgoing Hawking radiation [<xref ref-type="bibr" rid="scirp.52373-ref6">6</xref>] .</p><p>Interpretations for the particle law: So the matter-antimatter relationship is annihilation, yes, but it’s also a form of symbiosis.</p></sec><sec id="s3_5"><title>3.5. Zero-Point Symbiosis Law</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x112.png" xlink:type="simple"/></inline-formula> be matter, and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x113.png" xlink:type="simple"/></inline-formula> be antimatter. If antimatter exist in symbiosis with matter, then</p><disp-formula id="scirp.52373-formula1006"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x114.png"  xlink:type="simple"/></disp-formula><p>Interpretations for the zero-point symbiosis law: From this point of view, the relationship between matter and antimatter is more symbiotic, we call the process “zero-point symbiosis”.</p></sec><sec id="s3_6"><title>3.6. Ideal Law (Minimal with Constraints i.e. End of Quantum Theory)</title><p>In principle, we exclaim the existence of the minimal matter (or minimal antimatter) in the universe, i.e. denoted</p><p>by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x115.png" xlink:type="simple"/></inline-formula>, and partially ordered structure denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x116.png" xlink:type="simple"/></inline-formula>.</p><p>Interpretations for the ideal law: We show, in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x117.png" xlink:type="simple"/></inline-formula> case, without superpartners (or supersymmetry) quantum cosmology theory (or particle physics) does not exist, and this could be another major discovery in the sense that we would have to completely review completely our vision of universe.</p></sec><sec id="s3_7"><title>3.7. Main Theorem (Non-Singular Point of U)</title><p>Let any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7502036x118.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.52373-formula1007"><label>. (9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x119.png"  xlink:type="simple"/></disp-formula><p>Proof: By black hole law and particle law, we have</p><disp-formula id="scirp.52373-formula1008"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7502036x120.png"  xlink:type="simple"/></disp-formula><p>The proof is complete.</p><p>In fact, we have got it all settled through the matter and the antimatter obey the same laws of physics, which is that the universe must be completely satisfying. So, the universe seems to be dominated by matter and not antimatter.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>・ In attempting to explain the matter and antimatter, we have put forward the concept of axiom cosmology. Our “axiom” method is very simple, when in terms of some set operations we can write the theory in a very brief space, without a lot of complication, and the conclusions could be invaluable for the presence of dark matter and dark energy.</p><p>・ It is crucial for us to have a good understanding of the nature and results for the expansion of the universe. We raise a model touching the large-scale structure of the universe, so we begin to use it to explain cosmological mysteries of closed universe or open universe. As such, the axiom cosmology is one path to the final theory.</p><p>・ What matters is that cosmological set operations we have seen have played as a tool for cosmic research. In particular, we propose to solve the problem of physical singularity in space-time, which is full of infinite axiom cosmology charms and vitality.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The author is grateful to the anonymous referees for useful comments and suggestions.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.52373-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Alpher, R.A., Bethe, H. and Gamow, G. (1948) Physical Review. Letters to the Editor, 73, 803-804.</mixed-citation></ref><ref id="scirp.52373-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Einstein, A. (1955) The Meaning of Relativity. ElecBook, London. http://www.combat-diaries.co.uk/diary29/Link%2014%20Einstein.PDF http://www.docin.com/p-535070827.html</mixed-citation></ref><ref id="scirp.52373-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Longair, M. (2006) The Cosmic Century. Cambridge University Press, Cambridge.</mixed-citation></ref><ref id="scirp.52373-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">PHYSICS 2013) About PHYSICS. http://physics.nist.gov/cgi-bin/cuu/Value?plkt</mixed-citation></ref><ref id="scirp.52373-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Schoen, R. and Shing-Tung, Y. (1979) Communications in Mathematical Physics, 65, 45-76.http://dx.doi.org/10.1007/BF01940959</mixed-citation></ref><ref id="scirp.52373-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Schoen, R. and Shing-Tung, Y. (1981) Communications in Mathematical Physics, 79, 231-260.http://dx.doi.org/10.1007/BF01942062</mixed-citation></ref><ref id="scirp.52373-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Gamow, G. (1946) Physical Review, 70, 572-573. http://dx.doi.org/10.1103/PhysRev.70.572.2</mixed-citation></ref><ref id="scirp.52373-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Drake, S. (1957) Discoveries and Opinions of Galileo. Doubleday &amp; Company, New York, 237-238.</mixed-citation></ref><ref id="scirp.52373-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Copi, C.J., Schramm, D.N. and Turner, M.S. (1995) Science, 267, 192-199. http://dx.doi.org/10.1126/science.7809624</mixed-citation></ref><ref id="scirp.52373-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Wagoner, R.V., Fowler, W.A. and Hoyle, F. (1967) The Astrophysical Journal, 148, 3-49.http://dx.doi.org/10.1086/149126</mixed-citation></ref><ref id="scirp.52373-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Vittorio, N. and Silk, J. (1984) The Astrophysical Journal, Part 2—Letters to the Editor, 285, L39-L43. http://dx.doi.org/10.1086/184361</mixed-citation></ref><ref id="scirp.52373-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Efstathiou, G. and Bond, J.R. (1986) Monthly Notices of the Royal Astronomical Society, 218, 103-121.</mixed-citation></ref><ref id="scirp.52373-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Hawking, S.W. (1976) Physical Review D, 13, 191-197. http://dieumsnh.qfb.umich.mx/archivoshistoricosmq/ModernaHist/Hawking.pdfhttp://dx.doi.org/10.1103/PhysRevD.13.191</mixed-citation></ref><ref id="scirp.52373-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Hawking, S.W. (1977) Scientific American, 36, 34-40. http://planck.phys.uwosh.edu/~rioux/thermo/pdf/Black%20Holes%20--%20Hawking.pdfhttp://dx.doi.org/10.1038/scientificamerican0177-34</mixed-citation></ref><ref id="scirp.52373-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Hawking, S.W., Hertog, T. and Reall, H.S. (2000) Physical Review D, 62, Article ID: 043501. http://arxiv.org/pdf/hep-th/0003052.pdfhttp://dx.doi.org/10.1103/PhysRevD.62.043501</mixed-citation></ref><ref id="scirp.52373-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Cooper, A.P., D’Souza, R., Kauffmann, G., Wang, J., Boylan-Kolchin, M., Guo, Q., et al. (2013) Monthly Notices of the Royal Astronomical Society, 434, 3348-3367. http://dx.doi.org/10.1093/mnras/stt1245</mixed-citation></ref><ref id="scirp.52373-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Nesvizhevsky, V.V., Borner, H.G., Petukhov, A.K., Abele, H., Baeβler, S., Rueβ, F.J., et al. (2002) Nature, Letters to Nature, 415, 297-299.</mixed-citation></ref><ref id="scirp.52373-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Birkhoff, G. and Von Neumann, J. (1936) Annals of Mathematics, 37, 823-843. http://dx.doi.org/10.2307/1968621</mixed-citation></ref><ref id="scirp.52373-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Harding, J. (2009) International Journal of Theoretical Physics, 48, 769-802. http://dx.doi.org/10.1007/s10773-008-9853-4</mixed-citation></ref><ref id="scirp.52373-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Liu, Y.H. (2014) Applied Mathematics, 5, 677-684. http://dx.doi.org/10.4236/am.2014.54065</mixed-citation></ref></ref-list></back></article>