<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd">
<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article">
 <front>
  <journal-meta>
   <journal-id journal-id-type="publisher-id">
    jhepgc
   </journal-id>
   <journal-title-group>
    <journal-title>
     Journal of High Energy Physics, Gravitation and Cosmology
    </journal-title>
   </journal-title-group>
   <issn pub-type="epub">
    2380-4327
   </issn>
   <issn publication-format="print">
    2380-4335
   </issn>
   <publisher>
    <publisher-name>
     Scientific Research Publishing
    </publisher-name>
   </publisher>
  </journal-meta>
  <article-meta>
   <article-id pub-id-type="doi">
    10.4236/jhepgc.2025.114075
   </article-id>
   <article-id pub-id-type="publisher-id">
    jhepgc-145508
   </article-id>
   <article-categories>
    <subj-group subj-group-type="heading">
     <subject>
      Articles
     </subject>
    </subj-group>
    <subj-group subj-group-type="Discipline-v2">
     <subject>
      Physics 
     </subject>
     <subject>
       Mathematics
     </subject>
    </subj-group>
   </article-categories>
   <title-group>
    A Model of the Quantum Origin of the Universe from a Quantized-Velocity Space: A Combination of the Primordial Particle Hypothesis and Quantum Gravity
   </title-group>
   <contrib-group>
    <contrib contrib-type="author" xlink:type="simple">
     <name name-style="western">
      <surname>
       Slobodan
      </surname>
      <given-names>
       Spremo
      </given-names>
     </name>
    </contrib>
   </contrib-group> 
   <aff id="affnull">
    <addr-line>
     aMathematical Grammar School, Belgrade, Serbia
    </addr-line> 
   </aff> 
   <pub-date pub-type="epub">
    <day>
     11
    </day> 
    <month>
     09
    </month>
    <year>
     2025
    </year>
   </pub-date> 
   <volume>
    11
   </volume> 
   <issue>
    04
   </issue>
   <fpage>
    1215
   </fpage>
   <lpage>
    1223
   </lpage>
   <history>
    <date date-type="received">
     <day>
      13,
     </day>
     <month>
      June
     </month>
     <year>
      2025
     </year>
    </date>
    <date date-type="published">
     <day>
      8,
     </day>
     <month>
      June
     </month>
     <year>
      2025
     </year> 
    </date> 
    <date date-type="accepted">
     <day>
      8,
     </day>
     <month>
      September
     </month>
     <year>
      2025
     </year> 
    </date>
   </history>
   <permissions>
    <copyright-statement>
     © 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>
    We present a theoretical model that combines our hypothesis of primordial particles in a space of quantized velocities with modern approaches to quantum gravity, in particular, Loop Quantum Cosmology (LQC). In this model, the Big Bang is interpreted as the result of quantum tunneling of a primordial particle from “outer” quantized-velocity space and time into a domain of space and time bounded by the speed of light. It has been shown that such a process can leave experimentally verifiable traces in the cosmic microwave background (CMB), the spectrum of gravitational waves and high-energy astrophysical signals.
   </abstract>
   <kwd-group> 
    <kwd>
     Big Bang
    </kwd> 
    <kwd>
      Big Bounce
    </kwd> 
    <kwd>
      Cosmic Microwave Background
    </kwd> 
    <kwd>
      Flat Spacetime
    </kwd> 
    <kwd>
      Loop Quantum Cosmology
    </kwd> 
    <kwd>
      Planck Mass
    </kwd> 
    <kwd>
      Quantum Gravity
    </kwd> 
    <kwd>
      Quantum of Speed
    </kwd> 
    <kwd>
      Tunneling
    </kwd>
   </kwd-group>
  </article-meta>
 </front>
 <body>
  <sec id="s1">
   <title>1. Introduction</title>
   <p>Our hypothesis about primordial particles <xref ref-type="bibr" rid="scirp.145508-1">
     [1]
    </xref>-<xref ref-type="bibr" rid="scirp.145508-5">
     [5]
    </xref> introduces the concept of quantized-velocity space, in which there exist fundamental particles, to which, in their ground state, we can assign masses equal to the Planck mass, and which exist before the creation of our space and time (For the sake of a more concise expression, in further work, we will simply call the mass attributed to these primary particles “masses of primary particles”). The transition of one of them into the domain of velocities smaller than or equal to the speed of light is interpreted as quantum tunneling that causes the creation of our space and time through the Big Bang.</p>
   <p>On the other hand, quantum gravity (especially Loop Quantum Gravity and Loop Quantum Cosmology) <xref ref-type="bibr" rid="scirp.145508-6">
     [6]
    </xref> <xref ref-type="bibr" rid="scirp.145508-7">
     [7]
    </xref> offers a framework for quantizing space and time and removing the Big Bang singularity, replacing it with a quantum bounce (the Big Bounce).</p>
   <p>In this paper, we connect these two approaches into one coherent theoretical framework and consider the experimental consequences of such a model.</p>
  </sec><sec id="s2">
   <title>
    <xref ref-type="bibr" rid="scirp.145508-"></xref>2. Theoretical Basis</title>
   <sec id="s2_1">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>2.1. Quantized-Velocity Space</title>
    <p>We assume that in the pre-space, there exist velocities:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          v 
        </mi> 
        <mi>
          n 
        </mi> 
       </msub> 
       <mo>
         = 
       </mo> 
       <mi>
         n 
       </mi> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
       <mo>
         , 
       </mo> 
       <mtext>
           
       </mtext> 
       <mtext>
           
       </mtext> 
       <mi>
         n 
       </mi> 
       <mo>
         ∈ 
       </mo> 
       <mi>
         ℕ 
       </mi> 
       <mo>
         , 
       </mo> 
      </mrow> 
     </math>(1)</p>
    <p>where 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
      </mrow> 
     </math> is the quantum velocity, and the primordial particle of mass 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mi>
          p 
        </mi> 
       </msub> 
       <mo>
         = 
       </mo> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mrow> 
         <mtext>
           Planck 
         </mtext> 
        </mrow> 
       </msub> 
      </mrow> 
     </math> has energy:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          E 
        </mi> 
        <mi>
          n 
        </mi> 
       </msub> 
       <mo>
         = 
       </mo> 
       <mfrac> 
        <mn>
          1 
        </mn> 
        <mn>
          2 
        </mn> 
       </mfrac> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mi>
          p 
        </mi> 
       </msub> 
       <msup> 
        <mrow> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mrow> 
           <mi>
             n 
           </mi> 
           <msub> 
            <mi>
              ε 
            </mi> 
            <mi>
              v 
            </mi> 
           </msub> 
          </mrow> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
        <mn>
          2 
        </mn> 
       </msup> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math>(2)</p>
   </sec>
   <sec id="s2_2">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>2.2. Tunneling through the Velocity Barrier</title>
    <p>The barrier between the quantized-velocity space and our universe is defined as:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         V 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mi>
          v 
        </mi> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         = 
       </mo> 
       <mfrac> 
        <mn>
          1 
        </mn> 
        <mn>
          2 
        </mn> 
       </mfrac> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mi>
          p 
        </mi> 
       </msub> 
       <msup> 
        <mi>
          c 
        </mi> 
        <mn>
          2 
        </mn> 
       </msup> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math></p>
    <p>The probability of tunneling is:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi mathvariant="script">
         A 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mi>
          v 
        </mi> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         ~ 
       </mo> 
       <mtext>
         exp 
       </mtext> 
       <mrow> 
        <mo>
          [ 
        </mo> 
        <mrow> 
         <mo>
           − 
         </mo> 
         <mfrac> 
          <mn>
            1 
          </mn> 
          <mi>
            ℏ 
          </mi> 
         </mfrac> 
         <mstyle displaystyle="true"> 
          <mrow> 
           <msubsup> 
            <mo>
              ∫ 
            </mo> 
            <mrow> 
             <msub> 
              <mi>
                v 
              </mi> 
              <mi>
                f 
              </mi> 
             </msub> 
            </mrow> 
            <mrow> 
             <msub> 
              <mi>
                v 
              </mi> 
              <mi>
                i 
              </mi> 
             </msub> 
            </mrow> 
           </msubsup> 
           <mrow> 
            <msqrt> 
             <mrow> 
              <mn>
                2 
              </mn> 
              <msub> 
               <mi>
                 m 
               </mi> 
               <mi>
                 p 
               </mi> 
              </msub> 
              <mrow> 
               <mo>
                 ( 
               </mo> 
               <mrow> 
                <mi>
                  V 
                </mi> 
                <mrow> 
                 <mo>
                   ( 
                 </mo> 
                 <mi>
                   v 
                 </mi> 
                 <mo>
                   ) 
                 </mo> 
                </mrow> 
                <mo>
                  − 
                </mo> 
                <mi>
                  E 
                </mi> 
                <mrow> 
                 <mo>
                   ( 
                 </mo> 
                 <mi>
                   v 
                 </mi> 
                 <mo>
                   ) 
                 </mo> 
                </mrow> 
               </mrow> 
               <mo>
                 ) 
               </mo> 
              </mrow> 
             </mrow> 
            </msqrt> 
            <mtext>
                
            </mtext> 
            <mtext>
              d 
            </mtext> 
            <mi>
              v 
            </mi> 
           </mrow> 
          </mrow> 
         </mstyle> 
        </mrow> 
        <mo>
          ] 
        </mo> 
       </mrow> 
       <mo>
         , 
       </mo> 
      </mrow> 
     </math>(3)</p>
    <p>and the total probability is:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         P 
       </mi> 
       <mo>
         = 
       </mo> 
       <msup> 
        <mrow> 
         <mrow> 
          <mo>
            | 
          </mo> 
          <mi mathvariant="script">
            A 
          </mi> 
          <mo>
            | 
          </mo> 
         </mrow> 
        </mrow> 
        <mn>
          2 
        </mn> 
       </msup> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math></p>
   </sec>
   <sec id="s2_3">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>2.3. Entry into Quantum Space and Time</title>
    <p>After successful tunneling, the energy of the particle is interpreted as the energy density: The quantum Friedman equation (from LQC dynamics) is:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msup> 
        <mi>
          H 
        </mi> 
        <mn>
          2 
        </mn> 
       </msup> 
       <mo>
         = 
       </mo> 
       <mfrac> 
        <mrow> 
         <mn>
           8 
         </mn> 
         <mi>
           π 
         </mi> 
         <mi>
           G 
         </mi> 
        </mrow> 
        <mn>
          3 
        </mn> 
       </mfrac> 
       <mi>
         ρ 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <mn>
           1 
         </mn> 
         <mo>
           − 
         </mo> 
         <mfrac> 
          <mi>
            ρ 
          </mi> 
          <mrow> 
           <msub> 
            <mi>
              ρ 
            </mi> 
            <mi>
              c 
            </mi> 
           </msub> 
          </mrow> 
         </mfrac> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math>(4)</p>
   </sec>
  </sec><sec id="s3">
   <title>
    <xref ref-type="bibr" rid="scirp.145508-"></xref>3. The Passage of a Primordial Particle through the Velocity Barrier and the Natural Coexistence of the Hypothesis of Primordial Particles with Quantum Gravity</title>
   <p>We define the Lagrangian for a particle moving in its own space and time with an effective quantum of velocity, assuming: 1D motion of a particle of mass 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
     </mrow> 
    </math> with a parameterized time parameter 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
       τ 
     </mi> 
    </math>:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        ℒ 
      </mi> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mn>
         2 
       </mn> 
      </mfrac> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <msup> 
       <mrow> 
        <mrow> 
         <mo>
           ( 
         </mo> 
         <mrow> 
          <mfrac> 
           <mrow> 
            <mtext>
              d 
            </mtext> 
            <mi>
              x 
            </mi> 
           </mrow> 
           <mrow> 
            <mtext>
              d 
            </mtext> 
            <mi>
              τ 
            </mi> 
           </mrow> 
          </mfrac> 
         </mrow> 
         <mo>
           ) 
         </mo> 
        </mrow> 
       </mrow> 
       <mn>
         2 
       </mn> 
      </msup> 
      <mo>
        − 
      </mo> 
      <mi>
        V 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         x 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        . 
      </mo> 
     </mrow> 
    </math>(5)</p>
   <p>To describe tunneling, we introduce the potential barrier that protects our universe from particles from an external space as:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        V 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         x 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        = 
      </mo> 
      <mrow> 
       <mo>
         { 
       </mo> 
       <mrow> 
        <mtable columnalign="left"> 
         <mtr columnalign="left"> 
          <mtd columnalign="left"> 
           <mrow> 
            <mn>
              0 
            </mn> 
            <mo>
              , 
            </mo> 
           </mrow> 
          </mtd> 
          <mtd columnalign="left"> 
           <mrow> 
            <mi>
              x 
            </mi> 
            <mo>
              &lt; 
            </mo> 
            <mn>
              0 
            </mn> 
            <mtext>
                
            </mtext> 
            <mtext>
                
            </mtext> 
            <mrow> 
             <mo>
               ( 
             </mo> 
             <mrow> 
              <mtext>
                external space 
              </mtext> 
             </mrow> 
             <mo>
               ) 
             </mo> 
            </mrow> 
           </mrow> 
          </mtd> 
         </mtr> 
         <mtr columnalign="left"> 
          <mtd columnalign="left"> 
           <mrow> 
            <msub> 
             <mi>
               V 
             </mi> 
             <mn>
               0 
             </mn> 
            </msub> 
            <mo>
              , 
            </mo> 
           </mrow> 
          </mtd> 
          <mtd columnalign="left"> 
           <mrow> 
            <mn>
              0 
            </mn> 
            <mo>
              &lt; 
            </mo> 
            <mi>
              x 
            </mi> 
            <mo>
              &lt; 
            </mo> 
            <mi>
              a 
            </mi> 
            <mtext>
                
            </mtext> 
            <mtext>
                
            </mtext> 
            <mrow> 
             <mo>
               ( 
             </mo> 
             <mrow> 
              <mtext>
                potential barrier 
              </mtext> 
             </mrow> 
             <mo>
               ) 
             </mo> 
            </mrow> 
           </mrow> 
          </mtd> 
         </mtr> 
         <mtr columnalign="left"> 
          <mtd columnalign="left"> 
           <mrow> 
            <mn>
              0 
            </mn> 
            <mo>
              , 
            </mo> 
           </mrow> 
          </mtd> 
          <mtd columnalign="left"> 
           <mrow> 
            <mi>
              x 
            </mi> 
            <mo>
              &gt; 
            </mo> 
            <mi>
              a 
            </mi> 
            <mtext>
                
            </mtext> 
            <mtext>
                
            </mtext> 
            <mrow> 
             <mo>
               ( 
             </mo> 
             <mrow> 
              <mtext>
                our universe 
              </mtext> 
             </mrow> 
             <mo>
               ) 
             </mo> 
            </mrow> 
            <mo>
              . 
            </mo> 
           </mrow> 
          </mtd> 
         </mtr> 
        </mtable> 
       </mrow> 
      </mrow> 
     </mrow> 
    </math>(6)</p>
   <p>This barrier can represent “boundary conditions” between dimensionally different spaces.</p>
   <p>In a way analogous to classical mechanics, tunneling can be described by solving the Schrödinger equation through the barrier:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        ψ 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         x 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        ~ 
      </mo> 
      <msup> 
       <mtext>
         e 
       </mtext> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mi>
          κ 
        </mi> 
        <mi>
          x 
        </mi> 
       </mrow> 
      </msup> 
      <mo>
        , 
      </mo> 
      <mtext>
          
      </mtext> 
      <mtext>
          
      </mtext> 
      <mi>
        κ 
      </mi> 
      <mo>
        = 
      </mo> 
      <msqrt> 
       <mrow> 
        <mfrac> 
         <mrow> 
          <mn>
            2 
          </mn> 
          <msub> 
           <mi>
             m 
           </mi> 
           <mi>
             p 
           </mi> 
          </msub> 
          <mrow> 
           <mo>
             ( 
           </mo> 
           <mrow> 
            <msub> 
             <mi>
               V 
             </mi> 
             <mn>
               0 
             </mn> 
            </msub> 
            <mo>
              − 
            </mo> 
            <mi>
              E 
            </mi> 
           </mrow> 
           <mo>
             ) 
           </mo> 
          </mrow> 
         </mrow> 
         <mrow> 
          <msup> 
           <mi>
             ℏ 
           </mi> 
           <mn>
             2 
           </mn> 
          </msup> 
         </mrow> 
        </mfrac> 
       </mrow> 
      </msqrt> 
      <mo>
        , 
      </mo> 
     </mrow> 
    </math>(7)</p>
   <p>and the probability of tunneling (the transmission coefficient) is:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        T 
      </mi> 
      <mo>
        ≈ 
      </mo> 
      <msup> 
       <mtext>
         e 
       </mtext> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          2 
        </mn> 
        <mi>
          κ 
        </mi> 
        <mi>
          a 
        </mi> 
       </mrow> 
      </msup> 
      <mo>
        , 
      </mo> 
     </mrow> 
    </math></p>
   <p>where the above-mentioned values are:</p>
   <p>
    <math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
       E 
     </mi> 
    </math>: Energy of the particle in its own space and time.</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         V 
       </mi> 
       <mn>
         0 
       </mn> 
      </msub> 
     </mrow> 
    </math>: The barrier between dimensions (e.g., the gravity wall or velocity threshold).</p>
   <p>
    <math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
       a 
     </mi> 
    </math>: The width of the barrier in the corresponding coordinates (e.g., in the velocity space, if it is modelled).</p>
   <sec id="s3_1">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>3.1. Application of Primary Particle Tunneling to the Origin of Our Universe</title>
    <p>If one primary particle manages to tunnel into our space, then its energy 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          E 
        </mi> 
        <mi>
          p 
        </mi> 
       </msub> 
       <mo>
         ~ 
       </mo> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mi>
          P 
        </mi> 
       </msub> 
       <msup> 
        <mi>
          c 
        </mi> 
        <mn>
          2 
        </mn> 
       </msup> 
      </mrow> 
     </math> is released, and this leads to the initial state of our universe, the Big Bang.</p>
    <p>Given the quantum velocity 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
      </mrow> 
     </math>, this tunneling is a very rare but possible quantum fluctuation.</p>
   </sec>
   <sec id="s3_2">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>3.2. Feynman Path Integral Formulated for the Space of Quantized Velocities</title>
    <p>By formulating the path of integral formalism (the Feynman path integral) through the space of quantized velocities, we will logically continue our hypothesis. This will allow us to describe the probability of a primordial particle passing through a velocity barrier, analogous to quantum tunneling, but in the space of discrete velocities, not classical coordinates.</p>
   </sec>
   <sec id="s3_3">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>3.3. Basic Feynman Path Integral</title>
    <p>In standard quantum mechanics, the amplitude of the transition of a particle from point 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          x 
        </mi> 
        <mi>
          i 
        </mi> 
       </msub> 
      </mrow> 
     </math> to 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          x 
        </mi> 
        <mi>
          f 
        </mi> 
       </msub> 
      </mrow> 
     </math> in time 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        t 
      </mi> 
     </math> is given by:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mrow> 
        <mo>
          〈 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            x 
          </mi> 
          <mi>
            f 
          </mi> 
         </msub> 
         <mo>
           , 
         </mo> 
         <msub> 
          <mi>
            t 
          </mi> 
          <mi>
            f 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          | 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            x 
          </mi> 
          <mi>
            i 
          </mi> 
         </msub> 
         <mo>
           , 
         </mo> 
         <msub> 
          <mi>
            t 
          </mi> 
          <mi>
            i 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          〉 
        </mo> 
       </mrow> 
       <mo>
         = 
       </mo> 
       <mstyle displaystyle="true"> 
        <mrow> 
         <mo>
           ∫ 
         </mo> 
         <mi mathvariant="script">
           D 
         </mi> 
        </mrow> 
       </mstyle> 
       <mrow> 
        <mo>
          [ 
        </mo> 
        <mrow> 
         <mi>
           x 
         </mi> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mi>
            t 
          </mi> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
        <mo>
          ] 
        </mo> 
       </mrow> 
       <msup> 
        <mtext>
          e 
        </mtext> 
        <mrow> 
         <mfrac> 
          <mi>
            i 
          </mi> 
          <mi>
            ℏ 
          </mi> 
         </mfrac> 
         <mi>
           S 
         </mi> 
         <mrow> 
          <mo>
            [ 
          </mo> 
          <mrow> 
           <mi>
             x 
           </mi> 
           <mrow> 
            <mo>
              ( 
            </mo> 
            <mi>
              t 
            </mi> 
            <mo>
              ) 
            </mo> 
           </mrow> 
          </mrow> 
          <mo>
            ] 
          </mo> 
         </mrow> 
        </mrow> 
       </msup> 
       <mo>
         , 
       </mo> 
      </mrow> 
     </math></p>
    <p>where 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         S 
       </mi> 
       <mrow> 
        <mo>
          [ 
        </mo> 
        <mrow> 
         <mi>
           x 
         </mi> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mi>
            t 
          </mi> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
        <mo>
          ] 
        </mo> 
       </mrow> 
      </mrow> 
     </math> is a classical action:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         S 
       </mi> 
       <mo>
         = 
       </mo> 
       <mstyle displaystyle="true"> 
        <mrow> 
         <msubsup> 
          <mo>
            ∫ 
          </mo> 
          <mrow> 
           <msub> 
            <mi>
              t 
            </mi> 
            <mi>
              i 
            </mi> 
           </msub> 
          </mrow> 
          <mrow> 
           <msub> 
            <mi>
              t 
            </mi> 
            <mi>
              f 
            </mi> 
           </msub> 
          </mrow> 
         </msubsup> 
         <mi>
           ℒ 
         </mi> 
        </mrow> 
       </mstyle> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <mi>
           x 
         </mi> 
         <mo>
           , 
         </mo> 
         <mover accent="true"> 
          <mi>
            x 
          </mi> 
          <mo>
            ˙ 
          </mo> 
         </mover> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mtext>
         d 
       </mtext> 
       <mi>
         t 
       </mi> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math></p>
   </sec>
   <sec id="s3_4">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>3.4. Path Integral in Discrete-Velocity Space</title>
    <p>In our model, the basic dynamic variable is not the position 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        x 
      </mi> 
     </math> but the velocity 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        v 
      </mi> 
     </math>, which is quantized as (1). We will introduce a new path, so that instead of a path through space 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         x 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mi>
          t 
        </mi> 
        <mo>
          ) 
        </mo> 
       </mrow> 
      </mrow> 
     </math>, we observe a discrete sequence of velocities through “time” 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        τ 
      </mi> 
     </math>:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mrow> 
        <mo>
          { 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mn>
            0 
          </mn> 
         </msub> 
         <mo>
           , 
         </mo> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mn>
            1 
          </mn> 
         </msub> 
         <mo>
           , 
         </mo> 
         <mo>
           ⋯ 
         </mo> 
         <mo>
           , 
         </mo> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mi>
            N 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          } 
        </mo> 
       </mrow> 
       <mo>
         , 
       </mo> 
       <mtext>
           
       </mtext> 
       <mtext>
           
       </mtext> 
       <msub> 
        <mi>
          v 
        </mi> 
        <mi>
          i 
        </mi> 
       </msub> 
       <mo>
         = 
       </mo> 
       <msub> 
        <mi>
          n 
        </mi> 
        <mi>
          i 
        </mi> 
       </msub> 
       <mo>
         ⋅ 
       </mo> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math>(8)</p>
    <p>Discrete time steps: We will assume that the total “time” (perhaps imaginary, due to tunneling) is divided into 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        N 
      </mi> 
     </math> steps. Thus, the path integral now becomes the sum over all possible discrete velocity sequences:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi mathvariant="script">
         A 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mi>
            i 
          </mi> 
         </msub> 
         <mo>
           → 
         </mo> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mi>
            f 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         = 
       </mo> 
       <munder> 
        <mstyle mathsize="140%" displaystyle="true"> 
         <mo>
           ∑ 
         </mo> 
        </mstyle> 
        <mrow> 
         <mrow> 
          <mo>
            { 
          </mo> 
          <mrow> 
           <mi>
             v 
           </mi> 
           <mrow> 
            <mo>
              ( 
            </mo> 
            <mi>
              τ 
            </mi> 
            <mo>
              ) 
            </mo> 
           </mrow> 
          </mrow> 
          <mo>
            } 
          </mo> 
         </mrow> 
        </mrow> 
       </munder> 
       <mi>
         exp 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <mfrac> 
          <mi>
            i 
          </mi> 
          <mi>
            ℏ 
          </mi> 
         </mfrac> 
         <munderover> 
          <mstyle mathsize="140%" displaystyle="true"> 
           <mo>
             ∑ 
           </mo> 
          </mstyle> 
          <mrow> 
           <mi>
             j 
           </mi> 
           <mo>
             = 
           </mo> 
           <mn>
             1 
           </mn> 
          </mrow> 
          <mi>
            N 
          </mi> 
         </munderover> 
         <mtext>
             
         </mtext> 
         <mtext>
           Δ 
         </mtext> 
         <mi>
           τ 
         </mi> 
         <mo> 
         </mo> 
         <mi>
           ℒ 
         </mi> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mrow> 
           <msub> 
            <mi>
              v 
            </mi> 
            <mi>
              j 
            </mi> 
           </msub> 
          </mrow> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math>(9)</p>
    <p>Here the Lagrangian is in discrete form:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         ℒ 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mi>
            j 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         = 
       </mo> 
       <mfrac> 
        <mn>
          1 
        </mn> 
        <mn>
          2 
        </mn> 
       </mfrac> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mi>
          p 
        </mi> 
       </msub> 
       <msubsup> 
        <mi>
          v 
        </mi> 
        <mi>
          j 
        </mi> 
        <mn>
          2 
        </mn> 
       </msubsup> 
       <mo>
         − 
       </mo> 
       <mi>
         V 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mi>
            j 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         , 
       </mo> 
      </mrow> 
     </math>(10)</p>
    <p>where 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         V 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <msub> 
          <mi>
            v 
          </mi> 
          <mi>
            j 
          </mi> 
         </msub> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
      </mrow> 
     </math> is a potential “velocity barrier” e.g.:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         V 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mi>
          v 
        </mi> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         = 
       </mo> 
       <mrow> 
        <mo>
          { 
        </mo> 
        <mrow> 
         <mtable columnalign="left"> 
          <mtr columnalign="left"> 
           <mtd columnalign="left"> 
            <mrow> 
             <mn>
               0 
             </mn> 
             <mo>
               , 
             </mo> 
            </mrow> 
           </mtd> 
           <mtd columnalign="left"> 
            <mrow> 
             <mi>
               v 
             </mi> 
             <mo>
               &gt; 
             </mo> 
             <msub> 
              <mi>
                v 
              </mi> 
              <mi>
                c 
              </mi> 
             </msub> 
            </mrow> 
           </mtd> 
          </mtr> 
          <mtr columnalign="left"> 
           <mtd columnalign="left"> 
            <mrow> 
             <msub> 
              <mi>
                V 
              </mi> 
              <mn>
                0 
              </mn> 
             </msub> 
             <mo>
               , 
             </mo> 
            </mrow> 
           </mtd> 
           <mtd columnalign="left"> 
            <mrow> 
             <mi>
               v 
             </mi> 
             <mo>
               ≤ 
             </mo> 
             <msub> 
              <mi>
                v 
              </mi> 
              <mi>
                c 
              </mi> 
             </msub> 
            </mrow> 
           </mtd> 
          </mtr> 
         </mtable> 
        </mrow> 
       </mrow> 
      </mrow> 
     </math>(11)</p>
    <p>where 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          v 
        </mi> 
        <mi>
          c 
        </mi> 
       </msub> 
      </mrow> 
     </math> is some critical velocity (e.g. 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        c 
      </mi> 
     </math>) below which the particle “enters” our universe.</p>
    <p>Thus, tunneling occurs if a particle manages to transition from state 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          v 
        </mi> 
        <mi>
          n 
        </mi> 
       </msub> 
       <mo>
         &gt; 
       </mo> 
       <mi>
         c 
       </mi> 
      </mrow> 
     </math> to 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          v 
        </mi> 
        <mi>
          k 
        </mi> 
       </msub> 
       <mo>
         ≤ 
       </mo> 
       <mi>
         c 
       </mi> 
      </mrow> 
     </math>, thereby passing through the forbidden region 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          V 
        </mi> 
        <mn>
          0 
        </mn> 
       </msub> 
       <mo>
         &gt; 
       </mo> 
       <mi>
         E 
       </mi> 
      </mrow> 
     </math>.</p>
    <p>Approximation in the continuous limit:</p>
    <p>For very fine discretization and 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         v 
       </mi> 
       <mo>
         → 
       </mo> 
       <mtext>
         continuous 
       </mtext> 
      </mrow> 
     </math>, we get:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi mathvariant="script">
         A 
       </mi> 
       <mo>
         = 
       </mo> 
       <mstyle displaystyle="true"> 
        <mrow> 
         <mo>
           ∫ 
         </mo> 
         <mi mathvariant="script">
           D 
         </mi> 
        </mrow> 
       </mstyle> 
       <mrow> 
        <mo>
          [ 
        </mo> 
        <mrow> 
         <mi>
           v 
         </mi> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mi>
            τ 
          </mi> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
        <mo>
          ] 
        </mo> 
       </mrow> 
       <mo> 
       </mo> 
       <mtext>
         exp 
       </mtext> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <mfrac> 
          <mi>
            i 
          </mi> 
          <mi>
            ℏ 
          </mi> 
         </mfrac> 
         <mstyle displaystyle="true"> 
          <mrow> 
           <msubsup> 
            <mo>
              ∫ 
            </mo> 
            <mrow> 
             <msub> 
              <mi>
                τ 
              </mi> 
              <mi>
                i 
              </mi> 
             </msub> 
            </mrow> 
            <mrow> 
             <msub> 
              <mi>
                τ 
              </mi> 
              <mi>
                f 
              </mi> 
             </msub> 
            </mrow> 
           </msubsup> 
           <mrow> 
            <mrow> 
             <mo>
               ( 
             </mo> 
             <mrow> 
              <mfrac> 
               <mn>
                 1 
               </mn> 
               <mn>
                 2 
               </mn> 
              </mfrac> 
              <msub> 
               <mi>
                 m 
               </mi> 
               <mi>
                 p 
               </mi> 
              </msub> 
              <msup> 
               <mi>
                 v 
               </mi> 
               <mn>
                 2 
               </mn> 
              </msup> 
              <mo>
                − 
              </mo> 
              <mi>
                V 
              </mi> 
              <mrow> 
               <mo>
                 ( 
               </mo> 
               <mi>
                 v 
               </mi> 
               <mo>
                 ) 
               </mo> 
              </mrow> 
             </mrow> 
             <mo>
               ) 
             </mo> 
            </mrow> 
            <mtext>
              d 
            </mtext> 
            <mi>
              τ 
            </mi> 
           </mrow> 
          </mrow> 
         </mstyle> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math>(12)</p>
    <p>In “tunneling” (evanescent) conditions, with Wick rotation ( 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         τ 
       </mi> 
       <mo>
         → 
       </mo> 
       <mi>
         i 
       </mi> 
       <mi>
         τ 
       </mi> 
      </mrow> 
     </math>), we get the imaginary time integral:</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi mathvariant="script">
          A 
        </mi> 
        <mi>
          E 
        </mi> 
       </msub> 
       <mo>
         ~ 
       </mo> 
       <mtext>
         exp 
       </mtext> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <mo>
           − 
         </mo> 
         <mfrac> 
          <mn>
            1 
          </mn> 
          <mi>
            ℏ 
          </mi> 
         </mfrac> 
         <mstyle displaystyle="true"> 
          <mrow> 
           <mo>
             ∫ 
           </mo> 
           <mrow> 
            <mrow> 
             <mo>
               ( 
             </mo> 
             <mrow> 
              <mi>
                V 
              </mi> 
              <mrow> 
               <mo>
                 ( 
               </mo> 
               <mi>
                 v 
               </mi> 
               <mo>
                 ) 
               </mo> 
              </mrow> 
              <mo>
                − 
              </mo> 
              <mfrac> 
               <mn>
                 1 
               </mn> 
               <mn>
                 2 
               </mn> 
              </mfrac> 
              <msub> 
               <mi>
                 m 
               </mi> 
               <mi>
                 p 
               </mi> 
              </msub> 
              <msup> 
               <mi>
                 v 
               </mi> 
               <mn>
                 2 
               </mn> 
              </msup> 
             </mrow> 
             <mo>
               ) 
             </mo> 
            </mrow> 
            <mtext>
              d 
            </mtext> 
            <mi>
              τ 
            </mi> 
           </mrow> 
          </mrow> 
         </mstyle> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         , 
       </mo> 
      </mrow> 
     </math>(13)</p>
    <p>and this is an analogue of quantum tunneling through velocity space (3).</p>
   </sec>
  </sec><sec id="s4">
   <title>
    <xref ref-type="bibr" rid="scirp.145508-"></xref>4. Numerical Estimate of the Amplitude of Primary Particle Tunneling into Our Universe</title>
   <p>We will use the space of quantized velocities (1) and (8) according to our model, and a simple quasi-classical (WKB) approximation, setting some realistic parameter values.</p>
   <p>The quantum amplitude for tunneling (in the WKB approximation) through the velocity barrier is:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi mathvariant="script">
        A 
      </mi> 
      <mo>
        ~ 
      </mo> 
      <msup> 
       <mtext>
         e 
       </mtext> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          2 
        </mn> 
        <mstyle displaystyle="true"> 
         <mrow> 
          <msubsup> 
           <mo>
             ∫ 
           </mo> 
           <mrow> 
            <msub> 
             <mi>
               v 
             </mi> 
             <mi>
               f 
             </mi> 
            </msub> 
           </mrow> 
           <mrow> 
            <msub> 
             <mi>
               v 
             </mi> 
             <mi>
               i 
             </mi> 
            </msub> 
           </mrow> 
          </msubsup> 
          <mrow> 
           <mi>
             κ 
           </mi> 
           <mrow> 
            <mo>
              ( 
            </mo> 
            <mi>
              v 
            </mi> 
            <mo>
              ) 
            </mo> 
           </mrow> 
           <mtext>
             d 
           </mtext> 
           <mi>
             v 
           </mi> 
          </mrow> 
         </mrow> 
        </mstyle> 
       </mrow> 
      </msup> 
      <mo>
        , 
      </mo> 
     </mrow> 
    </math>(14)</p>
   <p>where is:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        κ 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         v 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mi>
         ℏ 
       </mi> 
      </mfrac> 
      <msqrt> 
       <mrow> 
        <mn>
          2 
        </mn> 
        <msub> 
         <mi>
           m 
         </mi> 
         <mi>
           p 
         </mi> 
        </msub> 
        <mrow> 
         <mo>
           [ 
         </mo> 
         <mrow> 
          <mi>
            V 
          </mi> 
          <mrow> 
           <mo>
             ( 
           </mo> 
           <mi>
             v 
           </mi> 
           <mo>
             ) 
           </mo> 
          </mrow> 
          <mo>
            − 
          </mo> 
          <mi>
            E 
          </mi> 
          <mrow> 
           <mo>
             ( 
           </mo> 
           <mi>
             v 
           </mi> 
           <mo>
             ) 
           </mo> 
          </mrow> 
         </mrow> 
         <mo>
           ] 
         </mo> 
        </mrow> 
       </mrow> 
      </msqrt> 
      <mo>
        . 
      </mo> 
     </mrow> 
    </math>(15)</p>
   <p>We shall assume that: - The velocity ranges from 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         i 
       </mi> 
      </msub> 
      <mo>
        &gt; 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math> to 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         f 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math> (the boundary of our universe), - 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        E 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         v 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mn>
         2 
       </mn> 
      </mfrac> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <msup> 
       <mi>
         v 
       </mi> 
       <mn>
         2 
       </mn> 
      </msup> 
     </mrow> 
    </math>, - 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        V 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         v 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        = 
      </mo> 
      <msub> 
       <mi>
         V 
       </mi> 
       <mn>
         0 
       </mn> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mtext>
        constant 
      </mtext> 
     </mrow> 
    </math> in the barrier (for 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        v 
      </mi> 
      <mo>
        ≤ 
      </mo> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         i 
       </mi> 
      </msub> 
     </mrow> 
    </math>).</p>
   <p>Tunneling occurs in the region 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        v 
      </mi> 
      <mo>
        ∈ 
      </mo> 
      <mrow> 
       <mo>
         [ 
       </mo> 
       <mrow> 
        <mi>
          c 
        </mi> 
        <mo>
          , 
        </mo> 
        <msub> 
         <mi>
           v 
         </mi> 
         <mi>
           i 
         </mi> 
        </msub> 
       </mrow> 
       <mo>
         ] 
       </mo> 
      </mrow> 
     </mrow> 
    </math>, where 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        E 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         v 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        &lt; 
      </mo> 
      <msub> 
       <mi>
         V 
       </mi> 
       <mn>
         0 
       </mn> 
      </msub> 
     </mrow> 
    </math>.</p>
   <p>We will assume the following values as numerical settings:</p>
   <p>- The Planck mass, i.e. the mass of the primordial particle: 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mrow> 
        <mtext>
          Planck 
        </mtext> 
       </mrow> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mn>
        2.18 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          8 
        </mn> 
       </mrow> 
      </msup> 
      <mtext>
          
      </mtext> 
      <mtext>
        kg 
      </mtext> 
     </mrow> 
    </math>.</p>
   <p>- Planck’s constant: 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        ℏ 
      </mi> 
      <mo>
        = 
      </mo> 
      <mn>
        1.055 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          34 
        </mn> 
       </mrow> 
      </msup> 
      <mtext>
          
      </mtext> 
      <mtext>
        J 
      </mtext> 
      <mo>
        ⋅ 
      </mo> 
      <mtext>
        s 
      </mtext> 
     </mrow> 
    </math>.</p>
   <p>- The critical velocity (the boundary velocity for our universe): 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        c 
      </mi> 
      <mo>
        = 
      </mo> 
      <mn>
        3 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         8 
       </mn> 
      </msup> 
      <mrow> 
       <mtext>
         m 
       </mtext> 
       <mo>
         / 
       </mo> 
       <mtext>
         s 
       </mtext> 
      </mrow> 
     </mrow> 
    </math>.</p>
   <p>- The initial velocity of the primordial particle: 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         i 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mn>
        5 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         8 
       </mn> 
      </msup> 
      <mrow> 
       <mtext>
         m 
       </mtext> 
       <mo>
         / 
       </mo> 
       <mtext>
         s 
       </mtext> 
      </mrow> 
     </mrow> 
    </math>.</p>
   <p>- The quantum velocity: 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         ε 
       </mi> 
       <mi>
         v 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         7 
       </mn> 
      </msup> 
      <mrow> 
       <mtext>
         m 
       </mtext> 
       <mo>
         / 
       </mo> 
       <mtext>
         s 
       </mtext> 
      </mrow> 
     </mrow> 
    </math>.</p>
   <p>- The height of the barrier: Let:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         V 
       </mi> 
       <mn>
         0 
       </mn> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mn>
         2 
       </mn> 
      </mfrac> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <msubsup> 
       <mi>
         v 
       </mi> 
       <mi>
         b 
       </mi> 
       <mn>
         2 
       </mn> 
      </msubsup> 
      <mo>
        , 
      </mo> 
      <mtext>
          
      </mtext> 
      <mtext>
          
      </mtext> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         b 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mn>
        5.5 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         8 
       </mn> 
      </msup> 
      <mrow> 
       <mtext>
         m 
       </mtext> 
       <mo>
         / 
       </mo> 
       <mtext>
         s 
       </mtext> 
      </mrow> 
     </mrow> 
    </math></p>
   <p>Thus, the barrier is slightly higher than the energy of the particle, and this creates the conditions for tunneling. Tunneling between 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         f 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mi>
        c 
      </mi> 
      <mo>
        = 
      </mo> 
      <mn>
        3 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         8 
       </mn> 
      </msup> 
     </mrow> 
    </math> and 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         i 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mn>
        5 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         8 
       </mn> 
      </msup> 
     </mrow> 
    </math>, in steps of 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         ε 
       </mi> 
       <mi>
         v 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         7 
       </mn> 
      </msup> 
     </mrow> 
    </math>:</p>
   <p>That is, a total of 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        N 
      </mi> 
      <mo>
        = 
      </mo> 
      <mn>
        20 
      </mn> 
     </mrow> 
    </math> steps.</p>
   <p>At each step, we approximate:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         κ 
       </mi> 
       <mi>
         n 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mi>
         ℏ 
       </mi> 
      </mfrac> 
      <msqrt> 
       <mrow> 
        <mn>
          2 
        </mn> 
        <msub> 
         <mi>
           m 
         </mi> 
         <mi>
           p 
         </mi> 
        </msub> 
        <mrow> 
         <mo>
           ( 
         </mo> 
         <mrow> 
          <msub> 
           <mi>
             V 
           </mi> 
           <mn>
             0 
           </mn> 
          </msub> 
          <mo>
            − 
          </mo> 
          <mfrac> 
           <mn>
             1 
           </mn> 
           <mn>
             2 
           </mn> 
          </mfrac> 
          <msub> 
           <mi>
             m 
           </mi> 
           <mi>
             p 
           </mi> 
          </msub> 
          <msubsup> 
           <mi>
             v 
           </mi> 
           <mi>
             n 
           </mi> 
           <mn>
             2 
           </mn> 
          </msubsup> 
         </mrow> 
         <mo>
           ) 
         </mo> 
        </mrow> 
       </mrow> 
      </msqrt> 
     </mrow> 
    </math></p>
   <p>Then:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        S 
      </mi> 
      <mo>
        ≈ 
      </mo> 
      <mn>
        2 
      </mn> 
      <munderover> 
       <mstyle mathsize="140%" displaystyle="true"> 
        <mo>
          ∑ 
        </mo> 
       </mstyle> 
       <mrow> 
        <mi>
          n 
        </mi> 
        <mo>
          = 
        </mo> 
        <mn>
          1 
        </mn> 
       </mrow> 
       <mi>
         N 
       </mi> 
      </munderover> 
      <mtext>
          
      </mtext> 
      <msub> 
       <mi>
         κ 
       </mi> 
       <mi>
         n 
       </mi> 
      </msub> 
      <mo>
        ⋅ 
      </mo> 
      <msub> 
       <mi>
         ε 
       </mi> 
       <mi>
         v 
       </mi> 
      </msub> 
      <mo>
        ⇒ 
      </mo> 
      <mi mathvariant="script">
        A 
      </mi> 
      <mo>
        ~ 
      </mo> 
      <msup> 
       <mtext>
         e 
       </mtext> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mi>
          S 
        </mi> 
       </mrow> 
      </msup> 
     </mrow> 
    </math></p>
   <p>Result (calculated):</p>
   <p>Using these values:</p>
   <p>- 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mn>
        2.18 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          8 
        </mn> 
       </mrow> 
      </msup> 
      <mtext>
          
      </mtext> 
      <mtext>
        kg 
      </mtext> 
     </mrow> 
    </math> - 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         ε 
       </mi> 
       <mi>
         v 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         7 
       </mn> 
      </msup> 
      <mrow> 
       <mtext>
         m 
       </mtext> 
       <mo>
         / 
       </mo> 
       <mtext>
         s 
       </mtext> 
      </mrow> 
     </mrow> 
    </math> - 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        ℏ 
      </mi> 
      <mo>
        = 
      </mo> 
      <mn>
        1.055 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          34 
        </mn> 
       </mrow> 
      </msup> 
      <mtext>
          
      </mtext> 
      <mtext>
        J 
      </mtext> 
      <mo>
        ⋅ 
      </mo> 
      <mtext>
        s 
      </mtext> 
     </mrow> 
    </math> - velocity: 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         n 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mi>
        c 
      </mi> 
      <mo>
        + 
      </mo> 
      <mi>
        n 
      </mi> 
      <mo>
        ⋅ 
      </mo> 
      <msub> 
       <mi>
         ε 
       </mi> 
       <mi>
         v 
       </mi> 
      </msub> 
     </mrow> 
    </math>, 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        n 
      </mi> 
      <mo>
        = 
      </mo> 
      <mn>
        1 
      </mn> 
      <mo>
        , 
      </mo> 
      <mo>
        ⋯ 
      </mo> 
      <mo>
        , 
      </mo> 
      <mn>
        20 
      </mn> 
     </mrow> 
    </math></p>
   <p>We calculate:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        S 
      </mi> 
      <mo>
        ≈ 
      </mo> 
      <munderover> 
       <mstyle mathsize="140%" displaystyle="true"> 
        <mo>
          ∑ 
        </mo> 
       </mstyle> 
       <mrow> 
        <mi>
          n 
        </mi> 
        <mo>
          = 
        </mo> 
        <mn>
          1 
        </mn> 
       </mrow> 
       <mrow> 
        <mn>
          20 
        </mn> 
       </mrow> 
      </munderover> 
      <mfrac> 
       <mrow> 
        <mn>
          2 
        </mn> 
        <mo>
          × 
        </mo> 
        <msup> 
         <mrow> 
          <mn>
            10 
          </mn> 
         </mrow> 
         <mn>
           7 
         </mn> 
        </msup> 
       </mrow> 
       <mrow> 
        <mn>
          1.055 
        </mn> 
        <mo>
          × 
        </mo> 
        <msup> 
         <mrow> 
          <mn>
            10 
          </mn> 
         </mrow> 
         <mrow> 
          <mo>
            − 
          </mo> 
          <mn>
            34 
          </mn> 
         </mrow> 
        </msup> 
       </mrow> 
      </mfrac> 
      <mo>
        ⋅ 
      </mo> 
      <msqrt> 
       <mrow> 
        <mn>
          2 
        </mn> 
        <mo>
          ⋅ 
        </mo> 
        <mn>
          2.18 
        </mn> 
        <mo>
          × 
        </mo> 
        <msup> 
         <mrow> 
          <mn>
            10 
          </mn> 
         </mrow> 
         <mrow> 
          <mo>
            − 
          </mo> 
          <mn>
            8 
          </mn> 
         </mrow> 
        </msup> 
        <mo>
          ⋅ 
        </mo> 
        <mrow> 
         <mo>
           ( 
         </mo> 
         <mrow> 
          <msub> 
           <mi>
             V 
           </mi> 
           <mn>
             0 
           </mn> 
          </msub> 
          <mo>
            − 
          </mo> 
          <mfrac> 
           <mn>
             1 
           </mn> 
           <mn>
             2 
           </mn> 
          </mfrac> 
          <msub> 
           <mi>
             m 
           </mi> 
           <mi>
             p 
           </mi> 
          </msub> 
          <msubsup> 
           <mi>
             v 
           </mi> 
           <mi>
             n 
           </mi> 
           <mn>
             2 
           </mn> 
          </msubsup> 
         </mrow> 
         <mo>
           ) 
         </mo> 
        </mrow> 
       </mrow> 
      </msqrt> 
     </mrow> 
    </math></p>
   <p>We include 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         V 
       </mi> 
       <mn>
         0 
       </mn> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mn>
         2 
       </mn> 
      </mfrac> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <msup> 
       <mrow> 
        <mrow> 
         <mo>
           ( 
         </mo> 
         <mrow> 
          <mn>
            5.5 
          </mn> 
          <mo>
            × 
          </mo> 
          <msup> 
           <mrow> 
            <mn>
              10 
            </mn> 
           </mrow> 
           <mn>
             8 
           </mn> 
          </msup> 
         </mrow> 
         <mo>
           ) 
         </mo> 
        </mrow> 
       </mrow> 
       <mn>
         2 
       </mn> 
      </msup> 
     </mrow> 
    </math>.</p>
   <p>We get:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        S 
      </mi> 
      <mo>
        ≈ 
      </mo> 
      <mn>
        1.4 
      </mn> 
      <mo>
        × 
      </mo> 
      <msup> 
       <mrow> 
        <mn>
          10 
        </mn> 
       </mrow> 
       <mn>
         5 
       </mn> 
      </msup> 
      <mtext>
          
      </mtext> 
      <mtext>
          
      </mtext> 
      <mo>
        ⇒ 
      </mo> 
      <mtext>
          
      </mtext> 
      <mtext>
          
      </mtext> 
      <mi mathvariant="script">
        A 
      </mi> 
      <mo>
        ~ 
      </mo> 
      <msup> 
       <mtext>
         e 
       </mtext> 
       <mrow> 
        <mo>
          − 
        </mo> 
        <mn>
          1.4 
        </mn> 
        <mo>
          × 
        </mo> 
        <msup> 
         <mrow> 
          <mn>
            10 
          </mn> 
         </mrow> 
         <mn>
           5 
         </mn> 
        </msup> 
       </mrow> 
      </msup> 
      <mo>
        ≈ 
      </mo> 
      <mn>
        0. 
      </mn> 
     </mrow> 
    </math></p>
   <p>Interpretation:</p>
   <p>- The probability of tunneling is extremely small, but not zero, which is very important, because from this we can draw the following two conclusions: - If there is an infinite number or quasi-continuum of primary particles in the external quantized-velocity space, at least one can tunnel, and that event would trigger the Big Bang. - This low probability supports the idea of a spontaneous and rare origin of the universe as an extremely rare but inevitable fluctuation in the quantized-velocity space.</p>
   <p>Physical meaning:</p>
   <p>- If 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi mathvariant="script">
         A 
       </mi> 
       <mi>
         E 
       </mi> 
      </msub> 
     </mrow> 
    </math> is not zero, there is a non-zero probability that the particle passes from the world with 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        v 
      </mi> 
      <mo>
        &gt; 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math> to our world with 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        v 
      </mi> 
      <mo>
        ≤ 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math>. - This enables spontaneous quantum “breaking” of the velocity barrier and entering the space where classical relativity rules, i.e. our universe.</p>
   <p>This is also confirmed by the total probability with given parameter values (Planck mass, barrier height, quantum velocity, etc.), which is:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <menclose notation="box"> 
       <mrow> 
        <msub> 
         <mi>
           P 
         </mi> 
         <mrow> 
          <mtext>
            total 
          </mtext> 
         </mrow> 
        </msub> 
        <mo>
          ≈ 
        </mo> 
        <mn>
          0 
        </mn> 
       </mrow> 
      </menclose> 
     </mrow> 
    </math></p>
  </sec><sec id="s5">
   <title>
    <xref ref-type="bibr" rid="scirp.145508-"></xref>5. Formulation of an Extended Quantum-Gravity Model Incorporating Our Hypothesis of Primordial Particles as an Initial Condition of Quantum Cosmology</title>
   <p>The goal of this model is to create a combination: primordial particle hypothesis: primordial particles in quantized-velocity space  tunneling  creation of the universe; and on the other hand quantum gravity: quantization of space and time (e.g., Loop Quantum Cosmology, LQC)  dynamic metrics  Big Bounce or quantum Big Bang.</p>
   <p>Assumption: The velocity-quantized space of primordial particles</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         E 
       </mi> 
       <mi>
         n 
       </mi> 
      </msub> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mn>
         2 
       </mn> 
      </mfrac> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <msubsup> 
       <mi>
         v 
       </mi> 
       <mi>
         n 
       </mi> 
       <mn>
         2 
       </mn> 
      </msubsup> 
     </mrow> 
    </math></p>
   <p>- Certain velocities 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         n 
       </mi> 
      </msub> 
      <mo>
        &gt; 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math> are allowed in that space.</p>
   <p>Tunneling is the passage through an effective barrier:</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        V 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mi>
         v 
       </mi> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mn>
         1 
       </mn> 
       <mn>
         2 
       </mn> 
      </mfrac> 
      <msub> 
       <mi>
         m 
       </mi> 
       <mi>
         p 
       </mi> 
      </msub> 
      <msubsup> 
       <mi>
         v 
       </mi> 
       <mi>
         b 
       </mi> 
       <mn>
         2 
       </mn> 
      </msubsup> 
     </mrow> 
    </math></p>
   <p>where 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         v 
       </mi> 
       <mi>
         b 
       </mi> 
      </msub> 
      <mo>
        &gt; 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math>, and the barrier acts as a quantum threshold for entry into our universe.</p>
   <p>The tunneling leads into space and time where: - Velocity limit 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        v 
      </mi> 
      <mo>
        ≤ 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math>, - Beginning of spatial and temporal geometry.</p>
   <p>When the particle “passes” the barrier: - It is no longer just a particle, but becomes a source of curvature of space and time, - Quantum gravity is engaged: space and time are quantum generated around it.</p>
   <p>In Loop Quantum Cosmology (LQC), quantum cosmological dynamics is described by a modified Friedman equation (4):</p>
   <p>
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msup> 
       <mi>
         H 
       </mi> 
       <mn>
         2 
       </mn> 
      </msup> 
      <mo>
        = 
      </mo> 
      <mfrac> 
       <mrow> 
        <mn>
          8 
        </mn> 
        <mi>
          π 
        </mi> 
        <mi>
          G 
        </mi> 
       </mrow> 
       <mn>
         3 
       </mn> 
      </mfrac> 
      <mi>
        ρ 
      </mi> 
      <mrow> 
       <mo>
         ( 
       </mo> 
       <mrow> 
        <mn>
          1 
        </mn> 
        <mo>
          − 
        </mo> 
        <mfrac> 
         <mi>
           ρ 
         </mi> 
         <mrow> 
          <msub> 
           <mi>
             ρ 
           </mi> 
           <mi>
             c 
           </mi> 
          </msub> 
         </mrow> 
        </mfrac> 
       </mrow> 
       <mo>
         ) 
       </mo> 
      </mrow> 
      <mo>
        , 
      </mo> 
     </mrow> 
    </math></p>
   <p>where: 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
       ρ 
     </mi> 
    </math> is the energy density of the primordial particle, 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         ρ 
       </mi> 
       <mi>
         c 
       </mi> 
      </msub> 
      <mo>
        ~ 
      </mo> 
      <msub> 
       <mi>
         ρ 
       </mi> 
       <mrow> 
        <mtext>
          Planck 
        </mtext> 
       </mrow> 
      </msub> 
     </mrow> 
    </math> is the critical density from quantum gravity.</p>
   <p>This equation predicts the Big Bounce, not the singularity.</p>
  </sec><sec id="s6">
   <title>
    <xref ref-type="bibr" rid="scirp.145508-"></xref>6. Result and Discussion</title>
   <p>We hypothesized that primordial particles exist in their own flat space and time while moving at velocities much faster than that of light. This “outer space” is a quantized-velocity space. In this space, “collisions” of these particles are possible, and with some of them there exists the possibility that one primordial particle slows to a velocity slightly higher than that of light, i.e. for quantum velocity 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <msub> 
       <mi>
         ε 
       </mi> 
       <mi>
         v 
       </mi> 
      </msub> 
     </mrow> 
    </math> higher than 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
       c 
     </mi> 
    </math>. At the same time, its energy increases rapidly and it tunnels through the quantum barrier (exponentially suppressed probability).</p>
   <p>Upon entering the domain where 
    <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
      <mi>
        v 
      </mi> 
      <mo>
        ≤ 
      </mo> 
      <mi>
        c 
      </mi> 
     </mrow> 
    </math>, it becomes a source of quantum curvature. A quantum-generated space and time is initiated via the LQC formalism, so that our universe emerges with Planck conditions as a boundary.</p>
   <p>Our hypothesis provides a natural mechanism for initial entropy and time.</p>
   <p>It is possible for many other universes to arise in a similar way (each “Big Bounce” is a consequence of the tunneling of some new primordial particle).</p>
   <p>We expect that experimental confirmation of our hypothesis is possible through a quantum spectral signature in the cosmic microwave background (CMB).</p>
  </sec><sec id="s7">
   <title>
    <xref ref-type="bibr" rid="scirp.145508-"></xref>7. We Propose a Potential Experimentally Verifiable Predictive Model</title>
   <p>We combine:</p>
   <sec id="s7_1">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>7.1. Experimental Predicted Consequences</title>
    <p>1) Spectral deviations in the CMB (cosmic microwave background)</p>
    <p>Prediction: - Tunneling from the quantized space leads to a discrete structure of the initial fluctuation. - Anomalies are expected in low multipoles ( 
     <math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         ℓ 
       </mi> 
       <mo>
         &lt; 
       </mo> 
       <mn>
         30 
       </mn> 
      </mrow> 
     </math>), e.g., quadrupole depression. Observations: - Planck, WMAP: already noted certain deviations in low 
     <math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"> <mi>
        ℓ 
      </mi> 
     </math>. - Suggestion: look for discrete-frequency artifacts corresponding to 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
      </mrow> 
     </math>.</p>
    <p>2) Limits on quantum velocity 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
      </mrow> 
     </math></p>
    <p>Prediction: - If 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          ε 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
      </mrow> 
     </math> is not extremely small, it could leave a trace in the gravitational wave forest.</p>
    <p>Experimentally: - LISA, Pulsar Timing Arrays → traces of discrete structure in primordial gravitational waves.</p>
    <p>3) Imbalance between inflationary potential and initial kinetics</p>
    <p>Prediction: - The initial kinetic energy of the particle can cause asymmetry in the development of inflation.</p>
    <p>Test: - Compare predicted asymmetric models with Planck’s CMB maps of hemispheric asymmetry.</p>
    <p>4) Temporal quantization and dispersion of high-energy photons</p>
    <p>If time is also quantized (as we propose in our works):</p>
    <p>- We may expect energy-dependent delays of high-energy photons from distant sources (e.g. GRB “gamma-ray burst”).</p>
    <p>Test: - Observation of GRBs (e.g. by Fermi LAT) → look for delays dependent on 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msup> 
        <mi>
          E 
        </mi> 
        <mn>
          2 
        </mn> 
       </msup> 
      </mrow> 
     </math> ili 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msup> 
        <mi>
          E 
        </mi> 
        <mn>
          3 
        </mn> 
       </msup> 
      </mrow> 
     </math>.</p>
   </sec>
   <sec id="s7_2">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>7.2. Predictive Model</title>
    <p>We can formally write a simple model:</p>
    <p>1) Spectral index of initial fluctuations</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <mi>
         P 
       </mi> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mi>
          k 
        </mi> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         ~ 
       </mo> 
       <msup> 
        <mi>
          k 
        </mi> 
        <mrow> 
         <msub> 
          <mi>
            n 
          </mi> 
          <mi>
            s 
          </mi> 
         </msub> 
         <mo>
           − 
         </mo> 
         <mn>
           1 
         </mn> 
        </mrow> 
       </msup> 
       <mo>
         ⋅ 
       </mo> 
       <mrow> 
        <mo>
          ( 
        </mo> 
        <mrow> 
         <mn>
           1 
         </mn> 
         <mo>
           + 
         </mo> 
         <mi>
           δ 
         </mi> 
         <mo>
           ⋅ 
         </mo> 
         <mtext>
           sin 
         </mtext> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mrow> 
           <mfrac> 
            <mrow> 
             <mn>
               2 
             </mn> 
             <mi>
               π 
             </mi> 
             <mi>
               k 
             </mi> 
            </mrow> 
            <mrow> 
             <msub> 
              <mi>
                k 
              </mi> 
              <mi>
                v 
              </mi> 
             </msub> 
            </mrow> 
           </mfrac> 
          </mrow> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
        <mo>
          ) 
        </mo> 
       </mrow> 
       <mo>
         , 
       </mo> 
      </mrow> 
     </math></p>
    <p>where 
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          k 
        </mi> 
        <mi>
          v 
        </mi> 
       </msub> 
       <mo>
         ~ 
       </mo> 
       <mfrac> 
        <mrow> 
         <mn>
           2 
         </mn> 
         <mi>
           π 
         </mi> 
        </mrow> 
        <mrow> 
         <msub> 
          <mi>
            ε 
          </mi> 
          <mi>
            v 
          </mi> 
         </msub> 
        </mrow> 
       </mfrac> 
      </mrow> 
     </math> is the wave number associated with the velocity quantum.</p>
    <p>2) Effective density</p>
    <p>
     <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> 
       <msub> 
        <mi>
          ρ 
        </mi> 
        <mrow> 
         <mtext>
           eff 
         </mtext> 
        </mrow> 
       </msub> 
       <mo>
         = 
       </mo> 
       <mfrac> 
        <mn>
          1 
        </mn> 
        <mn>
          2 
        </mn> 
       </mfrac> 
       <msub> 
        <mi>
          m 
        </mi> 
        <mi>
          p 
        </mi> 
       </msub> 
       <msup> 
        <mi>
          v 
        </mi> 
        <mn>
          2 
        </mn> 
       </msup> 
       <mo>
         ⋅ 
       </mo> 
       <msup> 
        <mtext>
          e 
        </mtext> 
        <mrow> 
         <mo>
           − 
         </mo> 
         <mn>
           2 
         </mn> 
         <mi>
           S 
         </mi> 
         <mrow> 
          <mo>
            ( 
          </mo> 
          <mi>
            v 
          </mi> 
          <mo>
            ) 
          </mo> 
         </mrow> 
        </mrow> 
       </msup> 
       <mo>
         . 
       </mo> 
      </mrow> 
     </math></p>
   </sec>
   <sec id="s7_3">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>7.3. Testability</title>
    <p>| Observation | Expected traces | Experiment | CMB spectra | Low-frequency anomalies, discrete oscillatory patterns | Planck, Simons Observatory | Gravitational waves | Discrete structure in the primordial background signal | LISA, NANOGrav | Gamma-ray bursts (GRBs) | Delay of high-energy photons | Fermi LAT, CTA | Inflationary asymmetry | Hemispheric irregularity in temperature maps | Planck, CMB-S4 |.</p>
   </sec>
   <sec id="s7_4">
    <title>
     <xref ref-type="bibr" rid="scirp.145508-"></xref>7.4. Conclusions</title>
    <p>We have formulated an experimentally verifiable quantum-cosmological model according to which:</p>
    <p>A primordial particle tunnels out of a quantized-velocity space;</p>
    <p>Space and time with quantum properties are born;</p>
    <p>Traces remain in the CMB, gravitational waves, and high-energy signals.</p>
   </sec>
  </sec>
 </body><back>
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