<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Publishing DTD v1.4 20241031//EN" "JATS-journalpublishing1-4.dtd">
<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" dtd-version="1.4" xml:lang="en">
  <front>
    <journal-meta>
      <journal-id journal-id-type="publisher-id">am</journal-id>
      <journal-title-group>
        <journal-title>Applied Mathematics</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2152-7393</issn>
      <issn pub-type="ppub">2152-7385</issn>
      <publisher>
        <publisher-name>Scientific Research Publishing</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.4236/am.2026.173010</article-id>
      <article-id pub-id-type="publisher-id">am-150194</article-id>
      <article-categories>
        <subj-group>
          <subject>Article</subject>
        </subj-group>
        <subj-group>
          <subject>Physics</subject>
          <subject>Mathematics</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>A Mathematical Exploration of the Correlation between the Speeds of Light in Adjacent Universes</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Osaka</surname>
            <given-names>Motohisa</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
      </contrib-group>
      <aff id="aff1"><label>1</label> Department of Basic Science, Nippon Veterinary and Life Science University, Musashino, Japan </aff>
      <author-notes>
        <fn fn-type="conflict" id="fn-conflict">
          <p>The author declares no conflicts of interest regarding the publication of this paper.</p>
        </fn>
      </author-notes>
      <pub-date pub-type="epub">
        <day>03</day>
        <month>03</month>
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="collection">
        <month>03</month>
        <year>2026</year>
      </pub-date>
      <volume>17</volume>
      <issue>03</issue>
      <fpage>164</fpage>
      <lpage>174</lpage>
      <history>
        <date date-type="received">
          <day>19</day>
          <month>02</month>
          <year>2026</year>
        </date>
        <date date-type="accepted">
          <day>14</day>
          <month>03</month>
          <year>2026</year>
        </date>
        <date date-type="published">
          <day>17</day>
          <month>03</month>
          <year>2026</year>
        </date>
      </history>
      <permissions>
        <copyright-statement>© 2026 by the authors and Scientific Research Publishing Inc.</copyright-statement>
        <copyright-year>2026</copyright-year>
        <license license-type="open-access">
          <license-p> This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license ( <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link> ). </license-p>
        </license>
      </permissions>
      <self-uri content-type="doi" xlink:href="https://doi.org/10.4236/am.2026.173010">https://doi.org/10.4236/am.2026.173010</self-uri>
      <abstract>
        <p>From the mass-energy equivalence, the energy of a mass moving with velocity <italic>V</italic> is given by the zeroth component of its four-momentum. In this study, we re-examine this expression and demonstrate that its mathematical formalism admits an additional speed parameter, <italic>c</italic><sub>2</sub>, determined by the experimental speed of light <italic>c</italic><sub>1</sub> and the object’s velocity <italic>V</italic>. Under a set of speculative assumptions—specifically, that energy remains invariant for a mass transitioning between hypothetical “adjacent” universes—the presence of a second mathematical root <italic>c</italic><sub>2</sub> suggests the existence of a potential alternative state. In this paper, we explore the speculative possibility that this root describes the physical constants of a coupled adjacent universe. This study explores the mathematical curiosity that the energy of a mass at velocity <italic>V</italic> is identical whether the invariant speed of the system is <italic>c</italic><sub>1</sub> or <italic>c</italic><sub>2</sub>. Our framework indicates that for low values of <italic>V</italic>, <italic>c</italic><sub>2</sub> is less than <italic>c</italic><sub>1</sub>, with the relationship reversing beyond a certain critical velocity. If this mathematical duality corresponds to a physical reality, the electromagnetic properties of such an adjacent universe, including vacuum permittivity (<italic>ε</italic><sub>0</sub><sub>2</sub>) and permeability (<italic>μ</italic><sub>0</sub><sub>2</sub>), would be constrained by the relation <inline-formula><mml:math></mml:math></inline-formula></p>
        <p>ε</p>
        <p>02</p>
        <p>μ</p>
        <p>02</p>
        <p>=1/</p>
        <p>c</p>
        <p>2</p>
        <p>2</p>
        <p>. This exploration is presented as a theoretical inquiry into the implications of the algebraic structure of relativistic energy-momentum relations.</p>
      </abstract>
      <kwd-group kwd-group-type="author-generated" xml:lang="en">
        <kwd>Mass-Energy Equivalence</kwd>
        <kwd>Vacuum Constants</kwd>
        <kwd>Adjacent Universes</kwd>
        <kwd>Mathematical Formalism</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>1. Introduction</title>
      <p>In 1864, Maxwell demonstrated that light is an electromagnetic wave, calculating its speed as <inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> c </mml:mi><mml:mn> 1 </mml:mn></mml:msub><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mrow><mml:msub><mml:mi> ε </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:msub><mml:mi> μ </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow></mml:msqrt></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> [<xref ref-type="bibr" rid="B1">1</xref>]. According to Maxwell’s equations, the speed of light is a vacuum constant, invariant for all observers regardless of their motion [<xref ref-type="bibr" rid="B2">2</xref>][<xref ref-type="bibr" rid="B3">3</xref>]. This principle of invariance leads to the Lorentz transformation, where time and space vary between inertial frames to preserve the constancy of <italic>c</italic><sub>1</sub>. In this four-dimensional framework, physical quantities such as energy and momentum are unified into the four-momentum <inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi> P </mml:mi><mml:mi> μ </mml:mi></mml:msup><mml:mo> = </mml:mo><mml:mi> m </mml:mi><mml:msup><mml:mi> U </mml:mi><mml:mi> μ </mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> , where the inner product <inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mi> P </mml:mi><mml:mi> μ </mml:mi></mml:msup><mml:msub><mml:mi> P </mml:mi><mml:mi> μ </mml:mi></mml:msub><mml:mo> = </mml:mo><mml:msup><mml:mi> m </mml:mi><mml:mn> 2 </mml:mn></mml:msup><mml:msup><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> remains a Lorentz invariant. While the standard interpretation of special relativity focuses on the physical speed <italic>c</italic><sub>1</sub>, the algebraic structure of the energy-momentum relation invites further mathematical scrutiny. In this paper, we explore a formal curiosity arising from the rearrangement of the energy component of the four-momentum. By treating the energy relation as a cubic equation, we find that under specific conditions, the system yields three real roots [<xref ref-type="bibr" rid="B4">4</xref>]. While the first positive root corresponds to the known invariant speed <italic>c</italic><sub>1</sub> in our universe, the existence of a second positive root, <italic>c</italic><sub>2</sub>, presents an intriguing mathematical possibility. Rather than asserting a new physical reality, this study presents a speculative mathematical exploration of this second root. We investigate the hypothesis that <italic>c</italic><sub>2</sub> could characterize the invariant speed of a hypothetical “adjacent” universe, provided that energy remains invariant for a mass transitioning between such domains. Under this framework, we analyze how a variation in the invariant speed would fundamentally alter the physical constants—such as vacuum permittivity (<italic>ε</italic><sub>0</sub>), permeability (<italic>μ</italic><sub>0</sub>)—thereby dictating a distinct evolution for the atomic and chemical structures within that domain. This inquiry seeks to determine whether such a second root represents a mere mathematical artifact or a consistent, albeit speculative, extension of relativistic kinematics.</p>
    </sec>
    <sec id="sec2">
      <title>2. Theoretical Framework</title>
      <sec id="sec2dot1">
        <title>2.1. The Five Critical Hypotheses Defining the Physical Nature of the System</title>
        <p>To explore the physical significance of <italic>c</italic><sub>2</sub>, we propose the following set of speculative hypotheses.</p>
        <p>1) Existence of Multiple Universes: Multiple universes exist and are positioned in an “adjacent” manner, which are defined as two parallel 3-branes separated by a finite distance in a higher-dimensional bulk [<xref ref-type="bibr" rid="B5">5</xref>].</p>
        <p>2) Universal Invariance of <italic>c</italic><italic><sub>n</sub></italic>: Each universe possesses its own distinct invariant speed of light, and the principle of the constancy of light speed holds within each respective universe.</p>
        <p>3) Mass Transfer: Defined as the transition of particles across this bulk, where the conservation laws are extended to include both manifolds.</p>
        <p>4) Reference Frame: The velocity <italic>V</italic> is treated relative to the static background of the embedding bulk to avoid ambiguity between the two universes’ respective inertial frames.</p>
        <p>5) Energy-Based Admissibility for Cross-Universe Transition: A mass moving at velocity <italic>V</italic> in one universe can transition to an adjacent universe provided that its total energy remains invariant across the boundary.</p>
        <p>Based on these hypotheses, the Modeling Scenario and Physical Setup are defined as follows.</p>
        <p>i) Modeling Scenario</p>
        <p>We assume a situation where a particle existing in a universe A (3-brane A) transitions to an adjacent universe B (3-brane B) via tunneling or higher-dimensional displacement through the bulk, without any external energy injection. During this transition, the particle moves while maintaining its velocity relative to the stationary background of the bulk.</p>
        <p>ii) Boundary Conditions</p>
        <p>Energy Continuity: At the boundary (the point of contact between the bulk and the universe), the total energy function of particles must not be discontinuous.</p>
        <p>Mass Adaptation: If the speed of light in universe A differs from the speed of light in universe B, the rest mass of a particle is instantly (or during a transition process) redefined from <italic>m</italic><italic><sub>A</sub></italic> to <italic>m</italic><italic><sub>B</sub></italic> to satisfy energy conservation.</p>
        <p>iii) Constraints to Prevent Model Failure</p>
        <p>Causality Constraint: After transitioning to universe B, velocity <italic>V</italic> must not exceed the speed of light <italic>c</italic><italic><sub>B</sub></italic> in that universe (<italic>V</italic> &lt; <italic>c</italic><italic><sub>B</sub></italic>).</p>
        <p>Bulk Isotropy: Within the high-dimensional bulk, additional drag forces (resistance) and potential gradients associated with movement from universe A to universe B are considered negligible.</p>
      </sec>
      <sec id="sec2dot2">
        <title>2.2. Derivation of the Other Speed of Light</title>
        <p>Based on Hypothesis 5, assuming that an object moving at velocity <italic>V</italic> in one universe (our universe) can transition to an adjacent universe (Hypothesis 1) while conserving energy, the speed of light in that adjacent universe is derived as follows.</p>
        <p>The mass-energy equivalence <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> E </mml:mi><mml:mo> = </mml:mo><mml:mi> m </mml:mi><mml:msup><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> is also expressed as </p>
        <disp-formula id="FD1">
          <label>(1)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>E</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mo>=</mml:mo>
              <mml:mo>
              </mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>m</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msub>
                </mml:mrow>
                <mml:mrow>
                  <mml:msqrt>
                    <mml:mrow>
                      <mml:mn>1</mml:mn>
                      <mml:mo>−</mml:mo>
                      <mml:msup>
                        <mml:mrow>
                          <mml:mrow>
                            <mml:mo>(</mml:mo>
                            <mml:mrow>
                              <mml:mfrac>
                                <mml:mi>V</mml:mi>
                                <mml:mi>c</mml:mi>
                              </mml:mfrac>
                            </mml:mrow>
                            <mml:mo>)</mml:mo>
                          </mml:mrow>
                        </mml:mrow>
                        <mml:mn>2</mml:mn>
                      </mml:msup>
                    </mml:mrow>
                  </mml:msqrt>
                </mml:mrow>
              </mml:mfrac>
              <mml:msup>
                <mml:mi>c</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msup>
              <mml:mo>,</mml:mo>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where <italic>m</italic><sub>0</sub> is the rest mass of the object, and <italic>V</italic> its speed; <italic>V</italic>&lt;<italic>c</italic>. According to Hypotheses 2, 4, and 5, Equation (1) holds true both in our universe and in the adjacent universe.</p>
        <p>As <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mrow><mml:mi> V </mml:mi><mml:mo> / </mml:mo><mml:mi> c </mml:mi></mml:mrow><mml:mo> &lt; </mml:mo><mml:mn> 1 </mml:mn></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mi> V </mml:mi><mml:mo> / </mml:mo><mml:mi> c </mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> is defined by <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> sin </mml:mi><mml:mi> θ </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> θ </mml:mi><mml:mo> &lt; </mml:mo><mml:mrow><mml:mi> π </mml:mi><mml:mo> / </mml:mo><mml:mn> 2 </mml:mn></mml:mrow></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> .</p>
        <p>From (1),</p>
        <disp-formula id="FD2">
          <label>(2)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>E</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mo>=</mml:mo>
              <mml:mo>
              </mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>m</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msub>
                  <mml:msup>
                    <mml:mi>V</mml:mi>
                    <mml:mn>2</mml:mn>
                  </mml:msup>
                </mml:mrow>
                <mml:mrow>
                  <mml:mi>cos</mml:mi>
                  <mml:mi>θ</mml:mi>
                  <mml:mo>−</mml:mo>
                  <mml:msup>
                    <mml:mrow>
                      <mml:mi>cos</mml:mi>
                    </mml:mrow>
                    <mml:mn>3</mml:mn>
                  </mml:msup>
                  <mml:mi>θ</mml:mi>
                </mml:mrow>
              </mml:mfrac>
              <mml:mo>.</mml:mo>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>Then, <inline-formula><mml:math><mml:mrow><mml:mi> cos </mml:mi><mml:mi> θ </mml:mi></mml:mrow></mml:math></inline-formula> is represented as <italic>y</italic>:</p>
        <disp-formula id="FD3">
          <label>(3)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>c</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mfrac>
                <mml:mi>V</mml:mi>
                <mml:mrow>
                  <mml:msqrt>
                    <mml:mrow>
                      <mml:mn>1</mml:mn>
                      <mml:mo>−</mml:mo>
                      <mml:msup>
                        <mml:mi>y</mml:mi>
                        <mml:mn>2</mml:mn>
                      </mml:msup>
                    </mml:mrow>
                  </mml:msqrt>
                </mml:mrow>
              </mml:mfrac>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>Representing <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> m </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:msup><mml:mi> V </mml:mi><mml:mn> 2 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> as <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> , the following third-order equation for <italic>y</italic> is obtained from (2):</p>
        <disp-formula id="FD4">
          <label>(4)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>f</mml:mi>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mi>y</mml:mi>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:msup>
                <mml:mi>y</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msup>
              <mml:mo>−</mml:mo>
              <mml:mi>y</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mo>+</mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>P</mml:mi>
                    <mml:mn>0</mml:mn>
                  </mml:msub>
                </mml:mrow>
                <mml:mi>E</mml:mi>
              </mml:mfrac>
              <mml:mo>=</mml:mo>
              <mml:mn>0.</mml:mn>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>A positive value of <italic>E</italic> results from any value of <italic>θ</italic> on the interval <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> θ </mml:mi><mml:mo> &lt; </mml:mo><mml:mrow><mml:mi> π </mml:mi><mml:mo> / </mml:mo><mml:mn> 2 </mml:mn></mml:mrow></mml:mrow></mml:math></inline-formula> . In other words, at least one of the three roots of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> f </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> is real. The minimum value of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> g </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:msup><mml:mi> y </mml:mi><mml:mn> 3 </mml:mn></mml:msup><mml:mo> – </mml:mo><mml:mi> y </mml:mi><mml:mo> = </mml:mo><mml:mi> y </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> y </mml:mi><mml:mo> + </mml:mo><mml:mn> 1 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> y </mml:mi><mml:mo> − </mml:mo><mml:mn> 1 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> ; <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> y </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 1 </mml:mn></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math><mml:mrow><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 2 </mml:mn></mml:mrow><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 3 </mml:mn><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mo> − </mml:mo><mml:mn> 0.384 </mml:mn></mml:mrow></mml:math></inline-formula> at <inline-formula><mml:math><mml:mrow><mml:mi> y </mml:mi><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> . As the roots of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> f </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> are intersections of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> g </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> h </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow><mml:mo> / </mml:mo><mml:mi> E </mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> , all three roots are real when <inline-formula><mml:math><mml:mrow><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 2 </mml:mn></mml:mrow><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 3 </mml:mn><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow><mml:mo> &lt; </mml:mo><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow><mml:mo> / </mml:mo><mml:mi> E </mml:mi></mml:mrow><mml:mo> &lt; </mml:mo><mml:mn> 0 </mml:mn></mml:mrow></mml:math></inline-formula> (<xref ref-type="fig" rid="fig1">Figure 1</xref>). Two of them are between 0 and 1 and the remaining root is negative. The two roots between 0 and 1 are denoted as <italic>y</italic><sub>1</sub> and <italic>y</italic><sub>2</sub>. As <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> y </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 1 </mml:mn></mml:mrow></mml:math></inline-formula> , the negative root <italic>y</italic><sub>3</sub> is neglected. When <inline-formula><mml:math><mml:mrow><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow><mml:mo> / </mml:mo><mml:mi> E </mml:mi></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 2 </mml:mn></mml:mrow><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 3 </mml:mn><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mo> − </mml:mo><mml:mn> 0.384 </mml:mn></mml:mrow></mml:math></inline-formula> , <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> y </mml:mi><mml:mn> 1 </mml:mn></mml:msub><mml:mo> = </mml:mo><mml:msub><mml:mi> y </mml:mi><mml:mn> 2 </mml:mn></mml:msub><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mn> 0.5774 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> .</p>
        <fig id="fig1">
          <label>Figure 1</label>
          <graphic xlink:href="https://html.scirp.org/file/7405572-rId69.jpeg?20260317023731" />
        </fig>
        <p><bold>Figure 1.</bold>Blue line: <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> g </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:msup><mml:mi> y </mml:mi><mml:mn> 3 </mml:mn></mml:msup><mml:mo> – </mml:mo><mml:mi> y </mml:mi><mml:mo> = </mml:mo><mml:mi> y </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> y </mml:mi><mml:mo> + </mml:mo><mml:mn> 1 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> y </mml:mi><mml:mo> − </mml:mo><mml:mn> 1 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> ; Red line, <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> h </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow><mml:mo> / </mml:mo><mml:mi> E </mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula><italic>.</italic> The minimum value of <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> g </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> : <inline-formula><mml:math display="inline"><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> y </mml:mi><mml:mo> &lt; </mml:mo><mml:mn> 1 </mml:mn></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math><mml:mrow><mml:mrow><mml:mrow><mml:mo> − </mml:mo><mml:mn> 2 </mml:mn></mml:mrow><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 3 </mml:mn><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mo> − </mml:mo><mml:mn> 0.384 </mml:mn></mml:mrow></mml:math></inline-formula> at <inline-formula><mml:math><mml:mrow><mml:mi> y </mml:mi><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mn> 0.5774 </mml:mn></mml:mrow></mml:math></inline-formula> .</p>
        <p>By replacing <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow><mml:mo> / </mml:mo><mml:mi> E </mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> by <italic>Q</italic>, Equation (4) is transformed to</p>
        <disp-formula id="FD5">
          <label>(5)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>f</mml:mi>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mi>y</mml:mi>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:msup>
                <mml:mi>y</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msup>
              <mml:mo>−</mml:mo>
              <mml:mi>y</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mo>+</mml:mo>
              <mml:mi>Q</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mn>0.</mml:mn>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>By substituting the experimental speed of light (<italic>c</italic><sub>1</sub><italic>=</italic>299,792,458 m/s) demonstrated in the Michelson-Morley into Equation (3),</p>
        <disp-formula id="FD6">
          <label>(6)</label>
          <mml:math>
            <mml:mrow>
              <mml:msub>
                <mml:mi>y</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:mo>=</mml:mo>
              <mml:mo>
              </mml:mo>
              <mml:msqrt>
                <mml:mrow>
                  <mml:mn>1</mml:mn>
                  <mml:mo>−</mml:mo>
                  <mml:msup>
                    <mml:mrow>
                      <mml:mrow>
                        <mml:mo>(</mml:mo>
                        <mml:mrow>
                          <mml:mrow>
                            <mml:mi>V</mml:mi>
                            <mml:mo>/</mml:mo>
                            <mml:mrow>
                              <mml:msub>
                                <mml:mi>c</mml:mi>
                                <mml:mn>1</mml:mn>
                              </mml:msub>
                            </mml:mrow>
                          </mml:mrow>
                        </mml:mrow>
                        <mml:mo>)</mml:mo>
                      </mml:mrow>
                    </mml:mrow>
                    <mml:mn>2</mml:mn>
                  </mml:msup>
                </mml:mrow>
              </mml:msqrt>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>By substituting <italic>y</italic><sub>1</sub> into Equation (5),</p>
        <disp-formula id="FD7">
          <label>(7)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>Q</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mo>=</mml:mo>
              <mml:mo>
              </mml:mo>
              <mml:mo>−</mml:mo>
              <mml:msub>
                <mml:mi>y</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msup>
                <mml:mrow>
                </mml:mrow>
                <mml:mn>3</mml:mn>
              </mml:msup>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>y</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:mo>.</mml:mo>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>Thus, it is found that <italic>Q</italic> can be determined from <italic>V</italic> and <italic>c</italic><sub>1</sub>. The solutions of a cubic equation are generally expressed by Cardano’s formula; however, since this equation has three real roots when <inline-formula><mml:math><mml:mrow><mml:mn> 0 </mml:mn><mml:mo> &lt; </mml:mo><mml:mi> Q </mml:mi><mml:mo> &lt; </mml:mo><mml:mrow><mml:mn> 2 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 3 </mml:mn><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> , they can be expressed as follows using Vieta’s formulas.</p>
        <disp-formula id="FD8">
          <label>(8)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:msub>
                <mml:mi>Y</mml:mi>
                <mml:mi>k</mml:mi>
              </mml:msub>
              <mml:mo>=</mml:mo>
              <mml:mfrac>
                <mml:mn>2</mml:mn>
                <mml:mrow>
                  <mml:msqrt>
                    <mml:mn>3</mml:mn>
                  </mml:msqrt>
                </mml:mrow>
              </mml:mfrac>
              <mml:mi>cos</mml:mi>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mfrac>
                    <mml:mn>1</mml:mn>
                    <mml:mn>3</mml:mn>
                  </mml:mfrac>
                  <mml:mi>arccos</mml:mi>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mrow>
                      <mml:mo>−</mml:mo>
                      <mml:mfrac>
                        <mml:mrow>
                          <mml:mn>3</mml:mn>
                          <mml:mi>Q</mml:mi>
                        </mml:mrow>
                        <mml:mn>2</mml:mn>
                      </mml:mfrac>
                      <mml:msqrt>
                        <mml:mn>3</mml:mn>
                      </mml:msqrt>
                    </mml:mrow>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                  <mml:mo>+</mml:mo>
                  <mml:mfrac>
                    <mml:mrow>
                      <mml:mn>2</mml:mn>
                      <mml:mi>π</mml:mi>
                      <mml:mi>k</mml:mi>
                    </mml:mrow>
                    <mml:mn>3</mml:mn>
                  </mml:mfrac>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>,</mml:mo>
              <mml:mtext>
              </mml:mtext>
              <mml:mi>k</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mn>0</mml:mn>
              <mml:mo>,</mml:mo>
              <mml:mn>1</mml:mn>
              <mml:mo>,</mml:mo>
              <mml:mn>2.</mml:mn>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p><italic>y</italic><sub>1</sub> and <italic>y</italic><sub>2</sub> correspond to two of <italic>Y</italic><sub>1</sub>, <italic>Y</italic><sub>2</sub>, or <italic>Y</italic><sub>3</sub>, but the correspondence changes as <italic>V</italic> increases. In <xref ref-type="fig" rid="fig2">Figure 2(a)</xref>, the red line represents the change in <italic>y</italic><sub>1</sub> as <italic>V</italic> increases; that is, it represents <italic>y</italic><sub>1</sub> as a function of <italic>V</italic>. The blue polyline represents the behavior of <italic>y</italic><sub>2</sub> as <italic>V</italic> increases. At the point where these two lines intersect, we have <italic>y</italic><sub>1</sub> = <italic>y</italic><sub>2</sub>. Before the intersection, <italic>y</italic><sub>2</sub> &lt; <italic>y</italic><sub>1</sub> always holds; after the intersection, <italic>y</italic><sub>1</sub> &lt; <italic>y</italic><sub>2</sub>.</p>
        <p>From <italic>y</italic><sub>2</sub>, the corresponding speed of light can be calculated as follows.</p>
        <disp-formula id="FD9">
          <label>(9)</label>
          <mml:math>
            <mml:mrow>
              <mml:msub>
                <mml:mi>c</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:mo>=</mml:mo>
              <mml:mrow>
                <mml:mi>V</mml:mi>
                <mml:mo>/</mml:mo>
                <mml:mrow>
                  <mml:msqrt>
                    <mml:mrow>
                      <mml:mn>1</mml:mn>
                      <mml:mo>−</mml:mo>
                      <mml:msubsup>
                        <mml:mi>y</mml:mi>
                        <mml:mn>2</mml:mn>
                        <mml:mn>2</mml:mn>
                      </mml:msubsup>
                    </mml:mrow>
                  </mml:msqrt>
                </mml:mrow>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p><xref ref-type="fig" rid="fig2">Figure 2(b)</xref> shows <italic>c</italic><sub>2</sub> (blue line) changes as <italic>V</italic> increases. Meanwhile, <italic>c</italic><sub>1</sub> (red line) remains constant as the experimental speed of light. These lines intersect at the speed <italic>V</italic> (= 244,779,516 m/s) where <italic>c</italic><sub>2</sub> equals <italic>c</italic><sub>1</sub>, which corresponds to <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> y </mml:mi><mml:mn> 2 </mml:mn></mml:msub><mml:mo> = </mml:mo><mml:msub><mml:mi> y </mml:mi><mml:mn> 1 </mml:mn></mml:msub><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mn> 0.5774 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> . The corresponding value of <italic>V</italic> is obtained from the following equation.</p>
        <fig id="fig2">
          <label>Figure 2</label>
          <graphic xlink:href="https://html.scirp.org/file/7405572-rId98.jpeg?20260317023732" />
        </fig>
        <p><bold>Figure 2.</bold> (a) Red line represents the change in <italic>y</italic><sub>1</sub>. Blue polyline represents the behavior of <italic>y</italic><sub>2</sub>. (b) Red line shows <italic>c</italic><sub>1</sub> (=299,792,458 m/s). Blue line shows <italic>c</italic><sub>2</sub> (= the other light speed). <italic>V</italic>, the speed of a mass (m/s). These lines intersect at the critical speed <italic>V</italic><italic><sub>c</sub></italic> (=244,779,516 m/s) where <italic>c</italic><sub>2</sub> equals <italic>c</italic><sub>1</sub>, which corresponds to <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi> y </mml:mi><mml:mn> 2 </mml:mn></mml:msub><mml:mo> = </mml:mo><mml:msub><mml:mi> y </mml:mi><mml:mn> 1 </mml:mn></mml:msub><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow></mml:mrow><mml:mo> ≈ </mml:mo><mml:mn> 0.5774 </mml:mn></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> . The unit on the horizontal axis is m/s.</p>
        <disp-formula id="FD10">
          <label>(10)</label>
          <mml:math>
            <mml:mrow>
              <mml:msub>
                <mml:mi>V</mml:mi>
                <mml:mi>c</mml:mi>
              </mml:msub>
              <mml:mo>=</mml:mo>
              <mml:msub>
                <mml:mi>c</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msqrt>
                <mml:mrow>
                  <mml:mn>1</mml:mn>
                  <mml:mo>−</mml:mo>
                  <mml:msup>
                    <mml:mrow>
                      <mml:mrow>
                        <mml:mo>(</mml:mo>
                        <mml:mrow>
                          <mml:mrow>
                            <mml:mn>1</mml:mn>
                            <mml:mo>/</mml:mo>
                            <mml:mrow>
                              <mml:msqrt>
                                <mml:mn>3</mml:mn>
                              </mml:msqrt>
                            </mml:mrow>
                          </mml:mrow>
                        </mml:mrow>
                        <mml:mo>)</mml:mo>
                      </mml:mrow>
                    </mml:mrow>
                    <mml:mn>2</mml:mn>
                  </mml:msup>
                </mml:mrow>
              </mml:msqrt>
              <mml:mo>=</mml:mo>
              <mml:mn>244</mml:mn>
              <mml:mo>,</mml:mo>
              <mml:mn>779</mml:mn>
              <mml:mo>,</mml:mo>
              <mml:mn>516</mml:mn>
              <mml:mtext>
              </mml:mtext>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mtext>m/s</mml:mtext>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p><italic>c</italic><sub>2</sub> does not exceed <italic>c</italic><sub>1</sub> when <italic>V</italic> is less than or equal to 244,779,516 m/s; however, after the two lines intersect,<italic>c</italic><sub>2</sub> exceeds <italic>c</italic><sub>1</sub>. We call the speed of <italic>V</italic> at which they intersect the critical speed (<italic>V</italic><italic><sub>c</sub></italic>). Below the critical speed, the blue line appears to be discontinuous; however, when magnified, it is clear that the blue line approaches the red line from below so closely that it is not visible. It should be noted that <italic>y</italic><sub>2</sub> is also a real root of Equation (7), so since <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi> P </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow><mml:mo> / </mml:mo><mml:mi> E </mml:mi></mml:mrow><mml:mo> = </mml:mo><mml:mi> Q </mml:mi></mml:mrow></mml:math></inline-formula> , <italic>E</italic> has the same value when <italic>y</italic><sub>2</sub> is used. In other words, even in the case of <italic>c</italic><sub>2</sub>, the energy possessed by the mass is the same as when using the experimental speed of light <italic>c</italic><sub>1</sub>. This suggests that if the speed of light in an adjacent universe is <italic>c</italic><sub>2</sub>, it may be possible for mass moving at velocity <italic>V</italic> to travel from our universe while retaining its energy (Hypothesis 3).</p>
      </sec>
      <sec id="sec2dot3">
        <title>2.3. What Happens to the Results Obtained in Section 2.2 When the Assumed Speed of Light Is Changed?</title>
        <p><bold>1)</bold><xref ref-type="fig" rid="fig3">Figure 3</xref> shows the results of examining the relationship between <italic>c</italic><sub>1</sub> and <italic>c</italic><sub>2</sub> when we assume the speed of light in our universe is, for example, <italic>c</italic><sub>1</sub> = 350,792,458 m/s, which is greater than the actual value of 299,792,458 m/s. The critical speed is 286,420,842 m/s.</p>
        <fig id="fig3">
          <label>Figure 3</label>
          <graphic xlink:href="https://html.scirp.org/file/7405572-rId105.jpeg?20260317023732" />
        </fig>
        <p><bold>Figure 3.</bold> Case of another universe where the assumed speed of light is 350,792,458 m/s. (a) Red line represents the change in <italic>y</italic><sub>1</sub>. Blue polyline represents the behavior of <italic>y</italic><sub>2</sub>. (b) Red line shows <italic>c</italic><sub>1</sub> (=350,792,458 m/s). Blue line shows <italic>c</italic><sub>2</sub> (=the other light speed). <italic>V</italic>, the speed of a mass (m/s). The critical speed is 286,420,842m/s. The unit on the horizontal axis is m/s.</p>
        <p><bold>2</bold>) <xref ref-type="fig" rid="fig4">Figure 4</xref> shows the results of examining the relationship between <italic>c</italic><sub>1</sub> and <italic>c</italic><sub>2</sub> when we assume the speed of light in our universe is, for example, <italic>c</italic><sub>1</sub> = 150,792,458 m/s, which is lesser than the actual value of 299,792,458 m/s. The critical speed is 123,121,526 m/s.</p>
        <fig id="fig4">
          <label>Figure 4</label>
          <graphic xlink:href="https://html.scirp.org/file/7405572-rId106.jpeg?20260317023732" />
        </fig>
        <p><bold>Figure 4.</bold> Case of another universe where the assumed speed of light is 150,792,458 m/s. (a) Red line represents the change in <italic>y</italic><sub>1</sub>. Blue polyline represents the behavior of <italic>y</italic><sub>2</sub>. (b) Red line shows <italic>c</italic><sub>1</sub> (=150,792,458 m/s). Blue line shows <italic>c</italic><sub>2</sub> (=the other light speed). <italic>V</italic>, the speed of a mass (m/s). The critical speed is 123,121,526 m/s. The unit on the horizontal axis is m/s.</p>
        <p><xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref> have the same characteristics as <xref ref-type="fig" rid="fig2">Figure 2</xref>. Although only two examples are shown here, this feature is the same for other values of the speed of light as well. In other words, if the velocity of the mass is less than the critical speed (<italic>V</italic><italic><sub>c</sub></italic>), it can have the same energy at the other speed of light (<italic>c</italic><sub>2</sub>) that is lower than the assumed speed of light (<italic>c</italic><sub>1</sub>). When the velocity of the mass exceeds the critical speed (<italic>V</italic><italic><sub>c</sub></italic>), it has the same energy at the other speed of light (<italic>c</italic><sub>2</sub>) that is greater than the assumed speed of light (<italic>c</italic><sub>1</sub>). Once the constancy of the speed of light is postulated, the resulting structural properties follow independently of the particular value assigned to the speed of light in the universe. The following can be inferred from the above results. A mass moving at velocity <italic>V</italic> through an arbitrary universe A, where the speed of light <italic>c</italic><italic><sub>A</sub></italic> differs from that in our universe, can travel through an adjacent universe with the speed of light <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> c </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msub><mml:mi> c </mml:mi><mml:mi> A </mml:mi></mml:msub><mml:mo> , </mml:mo><mml:mi> V </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> determined by <italic>c</italic><italic><sub>A</sub></italic> and <italic>V</italic> while retaining its energy.</p>
      </sec>
    </sec>
    <sec id="sec3">
      <title>3. Discussion</title>
      <p>Einstein established the theory of special relativity based on the principle that the speed of light is constant in all inertial frames. This idea was inspired by the Maxwell’s equations, in which the speed of light is expressed in terms of the vacuum permittivity (<italic>ε</italic><sub>0</sub>) and permeability (<italic>μ</italic><sub>0</sub>) (<inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> c </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mrow><mml:msub><mml:mi> ε </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:msub><mml:mi> μ </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow></mml:msqrt></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> ), and is independent of the inertial frame. However, in the International System of Units (SI), these constants are defined so as to be consistent with the experimental speed of light. Therefore, within this system, it is not possible to explain why the experimental speed of light is 299,792,458 m/s. In this study, it has been reconfirmed that, for our universe, the fundamental principle is not the specific numerical value of the speed of light itself, but rather the principle of the invariance of the speed of light. Nevertheless, it remains true that these parameters are the factors that determine the speed of light.</p>
      <p>The results presented above are derived from the principle of the constancy of the speed of light. Under those hypotheses, if a mass were capable of moving between universes in contact with each other at a certain velocity, the speeds of light in those universes would be mutually related. The permittivity characterizes the extent to which an electric field can spread in vacuum, while the permeability characterizes how readily a magnetic field can be generated in vacuum. In quantum theory, the vacuum is not regarded as completely empty. Fluctuations of virtual particles occur, and these fluctuations are reflected in the values of the permittivity and permeability. Such fluctuations have been observed under extreme conditions. In neutron stars, the vacuum exhibits birefringence and behaves as if it were a material medium [<xref ref-type="bibr" rid="B6">6</xref>]. Moreover, in ultra-strong magnetic fields, electron-positron pair production from the vacuum is predicted to occur [<xref ref-type="bibr" rid="B7">7</xref>]. There also exists the fine-structure constant <inline-formula><mml:math display="inline"><mml:mrow><mml:mi> α </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mrow><mml:msup><mml:mi> e </mml:mi><mml:mn> 2 </mml:mn></mml:msup></mml:mrow><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 4 </mml:mn><mml:mi> π </mml:mi><mml:msub><mml:mi> ϵ </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:mi> ℏ </mml:mi><mml:mi> c </mml:mi></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> : <italic>e</italic>, electron charge; <inline-formula><mml:math><mml:mi> ℏ </mml:mi></mml:math></inline-formula> , plank constant; <italic>c</italic>, speed of light; <italic>ε</italic><sub>0</sub>, vacuum permittivity, which is directly connected to the properties of the vacuum [<xref ref-type="bibr" rid="B8">8</xref>]. This is a dimensionless constant determined by four factors. If the speed of light differs, the fundamental constitution of that universe would be entirely distinct, given the constitutive relationship between the speed of light (<italic>c</italic>), the vacuum permittivity (<italic>ε</italic><sub>0</sub>) and vacuum permeability (<italic>μ</italic><sub>0</sub>) (<inline-formula><mml:math><mml:mrow><mml:mi> c </mml:mi><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msqrt><mml:mrow><mml:msub><mml:mi> ε </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:msub><mml:mi> μ </mml:mi><mml:mn> 0 </mml:mn></mml:msub></mml:mrow></mml:msqrt></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> ). Furthermore, a variation in <italic>c</italic> would necessarily result in a different fine-structure constant (<italic>α</italic>), thereby fundamentally altering atomic structure, chemical properties, and the overall evolution of the universe. These variations suggest that while the mathematical framework allows for a second root, the resulting physical environment would likely be governed by a different set of spectroscopic and thermodynamic laws. A physico-mathematical approach has revealed the mechanism by which different physical constants are generated across multiple universes [<xref ref-type="bibr" rid="B9">9</xref>].</p>
      <p>We add a physics-based, concise eligibility criterion for selecting the “second” root used to define <italic>c</italic><sub>2</sub> (in addition to the condition that it be a positive real number). Below we describe what this framework predicts when the cubic equation yields no roots in the physical domain.</p>
      <p>i) Admissibility Rule: We have clarified the rule for selecting the “second” root <italic>c</italic><sub>2</sub>. In the case where multiple real roots exist for <inline-formula><mml:math><mml:mrow><mml:mi> f </mml:mi><mml:mrow><mml:mo> ( </mml:mo><mml:mi> y </mml:mi><mml:mo> ) </mml:mo></mml:mrow><mml:mo> = </mml:mo><mml:msup><mml:mi> y </mml:mi><mml:mn> 3 </mml:mn></mml:msup><mml:mo> − </mml:mo><mml:mi> y </mml:mi><mml:mo> + </mml:mo><mml:mo></mml:mo><mml:mi> Q </mml:mi><mml:mo> = </mml:mo><mml:mn> 0 </mml:mn></mml:mrow></mml:math></inline-formula> , we select the largest positive root. This choice is based on the assumption that the vacuum naturally relaxes into the state that allows for the highest stable signal velocity (minimum energy configuration).</p>
      <p>ii) Prediction in Non-Physical Domain: When the parameter <italic>Q</italic> exceeds the critical threshold (<inline-formula><mml:math><mml:mrow><mml:mi> Q </mml:mi><mml:mo> &gt; </mml:mo><mml:mrow><mml:mn> 2 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 3 </mml:mn><mml:msqrt><mml:mn> 3 </mml:mn></mml:msqrt></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> ), the equation lacks the required real roots. Our framework interprets this as a physical boundary beyond which a dual-universe system cannot stably exist. This predicts a “forbidden zone” for certain gravitational or electromagnetic coupling strengths, leading to either a vacuum collapse or a phase transition into a unified manifold.</p>
      <p>As physical meaning and spacetime structure, <italic>c</italic><sub>2</sub> is defined as a distinct invariant speed associated with the spacetime structure of the “adjacent universe”. It is not a re-parameterization of the standard kinematics but represents the fundamental causal limit within that specific manifold. The following remarks address whether it is consistent with the special theory of relativity. Within each respective universe, the standard invariant relations among energy (<italic>E</italic>), momentum (<italic>p</italic>), and rest mass (<italic>m</italic><sub>0</sub>) remain valid. Specifically, for the adjacent universe, the relation is given by <inline-formula><mml:math><mml:mrow><mml:msup><mml:mi> E </mml:mi><mml:mn> 2 </mml:mn></mml:msup><mml:mo> = </mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mi> p </mml:mi><mml:msub><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn></mml:msub></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow><mml:mn> 2 </mml:mn></mml:msup><mml:mo> + </mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:msub><mml:mi> m </mml:mi><mml:mn> 0 </mml:mn></mml:msub><mml:msubsup><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn><mml:mn> 2 </mml:mn></mml:msubsup></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow><mml:mn> 2 </mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> . We will discuss below whether it is consistent with our universe. The model treats the two universes as distinct manifolds with their own respective invariant speeds (<italic>c</italic><sub>1</sub> and <italic>c</italic><sub>2</sub>). This ensures that the kinematics within our own universe remain strictly governed by the standard value of <italic>c</italic><sub>1</sub>, preserving the integrity of established special relativity while allowing for speculative interactions across the interface.</p>
      <p>If a mass (<italic>m</italic><sub>0</sub>) moving at a given velocity (<italic>V</italic>) across these adjacent universes retains the same energy in both, the speed of light in that universe would be <italic>c</italic><sub>2</sub>. Under a set of those speculative assumptions, it would follow that the speed of light in that universe is not arbitrary but would be determined as <italic>c</italic><sub>2</sub>. According to the speculative hypotheses, the vacuum permittivity (<italic>ε</italic><sub>0</sub><sub>2</sub>) and permeability (<italic>μ</italic><sub>0</sub><sub>2</sub>) in that universe satisfy the relation <inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> ε </mml:mi><mml:mrow><mml:mn> 02 </mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi> μ </mml:mi><mml:mrow><mml:mn> 02 </mml:mn></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msubsup><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn><mml:mn> 2 </mml:mn></mml:msubsup></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> . <italic>c</italic><sub>2</sub> is smaller than <italic>c</italic><sub>1</sub> when <italic>V</italic> is below the critical velocity, and greater than <italic>c</italic><sub>1</sub> when <italic>V</italic> is exceeds the critical velocity.</p>
      <p>The shift in vacuum constants (<italic>ε</italic><sub>0</sub> and <italic>μ</italic><sub>0</sub>) necessarily affects the fine-structure constant <inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> α </mml:mi><mml:mn> 2 </mml:mn></mml:msub><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mo> = </mml:mo><mml:mrow><mml:mrow><mml:msup><mml:mi> e </mml:mi><mml:mn> 2 </mml:mn></mml:msup></mml:mrow><mml:mo> / </mml:mo><mml:mrow><mml:mrow><mml:mo> ( </mml:mo><mml:mrow><mml:mn> 4 </mml:mn><mml:mi> π </mml:mi><mml:msub><mml:mi> ϵ </mml:mi><mml:mrow><mml:mn> 02 </mml:mn></mml:mrow></mml:msub><mml:mi> ℏ </mml:mi><mml:msub><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn></mml:msub></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:mrow></mml:mrow><mml:mo> ) </mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> , which governs the strength of electromagnetic interactions. For instance, if the proposed relation results in a significantly larger <italic>α</italic><sub>2</sub>, atomic structures in the adjacent universe might become unstable or exhibit different spectral characteristics. While a comprehensive analysis of stellar nucleosynthesis or atomic stability within Universe 2 is beyond the scope of this study, this internal-consistency check ensures that the mathematical model remains compatible with the fundamental framework of quantum electrodynamics.</p>
    </sec>
    <sec id="sec4">
      <title>4. Conclusion</title>
      <p>In this study, we have re-examined the mathematical formalism of the energy-momentum relation and demonstrated that the energy of a mass moving at velocity <italic>V</italic> admits a dual-root structure for the invariant speed parameter. Our analysis reveals that for any given energy state at velocity <italic>V</italic>, there exists a second valid speed of light, <italic>c</italic><sub>2</sub>, distinct from the experimental value <italic>c</italic><sub>1</sub>. Under the hypothesis of energy invariance across adjacent physical states, this <italic>c</italic><sub>2</sub> suggests the existence of a coupled universe with distinct electromagnetic properties, where the vacuum permittivity and permeability are constrained by <inline-formula><mml:math><mml:mrow><mml:msub><mml:mi> ε </mml:mi><mml:mrow><mml:mn> 02 </mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi> μ </mml:mi><mml:mrow><mml:mn> 02 </mml:mn></mml:mrow></mml:msub><mml:mo> = </mml:mo><mml:mrow><mml:mn> 1 </mml:mn><mml:mo> / </mml:mo><mml:mrow><mml:msubsup><mml:mi> c </mml:mi><mml:mn> 2 </mml:mn><mml:mn> 2 </mml:mn></mml:msubsup></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> . Notably, the relationship between <italic>c</italic><sub>1</sub> and <italic>c</italic><sub>2</sub> undergoes a reversal at a critical velocity, marking a potential phase transition point in the interaction between these systems. To strengthen the relevance of this theoretical inquiry, future research should focus on three primary avenues. First, a rigorous derivation of the “critical velocity” is required to determine if it falls within experimentally accessible ranges or corresponds to cosmological scales. Second, the mechanism of energy invariance during a hypothetical transition between <italic>c</italic><sub>1</sub> and <italic>c</italic><sub>2</sub> environments must be explored through the lens of quantum tunneling or multidimensional brane dynamics. Finally, investigating possible observational signatures in high-energy astrophysics—where particles approach these critical velocities—may provide a means to test the validity of this mathematical duality. Such efforts will clarify whether this second root is a mere algebraic curiosity or a window into a broader, multi-layered structure of spacetime.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <title>References</title>
      <ref id="B1">
        <label>1.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Maxwell, J.C. (1865) A Dynamical Theory of the Electromagnetic Field. <italic>Philosophical</italic><italic>Transactions</italic><italic>of</italic><italic>the</italic><italic>Royal</italic><italic>Society</italic><italic>of</italic><italic>London</italic>, 155, 459-512. https://doi.org/10.1098/rstl.1865.0008 <pub-id pub-id-type="doi">10.1098/rstl.1865.0008</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1098/rstl.1865.0008">https://doi.org/10.1098/rstl.1865.0008</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Maxwell, J.C.</string-name>
            </person-group>
            <pub-id pub-id-type="doi">10.1098/rstl.1865.0008</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B2">
        <label>2.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Michelson, A.A. and Morley, E.W. (1887) On the Relative Motion of the Earth and the Luminiferous Ether. <italic>American</italic><italic>Journal</italic><italic>of</italic><italic>Science</italic>, 3, 333-345. https://doi.org/10.2475/ajs.s3-34.203.333 <pub-id pub-id-type="doi">10.2475/ajs.s3-34.203.333</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.2475/ajs.s3-34.203.333">https://doi.org/10.2475/ajs.s3-34.203.333</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Michelson, A.A.</string-name>
              <string-name>Morley, E.W.</string-name>
            </person-group>
            <pub-id pub-id-type="doi">10.2475/ajs.s3-34.203.333</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B3">
        <label>3.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Einstein, A. (1905) Ist die Trägheit eines Körpers von seinem Energieinhalt abhängig? <italic>Annalen</italic><italic>der</italic><italic>Physik</italic>, 323, 639-641. https://doi.org/10.1002/andp.19053231314 <pub-id pub-id-type="doi">10.1002/andp.19053231314</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1002/andp.19053231314">https://doi.org/10.1002/andp.19053231314</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Einstein, A.</string-name>
            </person-group>
            <year>1905</year>
            <article-title>Ist die Trägheit eines Körpers von seinem Energieinhalt abhängig? Annalen der Physik, 323, 639-641</article-title>
            <pub-id pub-id-type="doi">10.1002/andp.19053231314</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B4">
        <label>4.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Osaka, M. (2019) A Probabilistic Method to Determine Whether the Speed of Light Is Constant. <italic>Applied</italic><italic>Mathematics</italic>, 10, 51-59. https://doi.org/10.4236/am.2019.102005 <pub-id pub-id-type="doi">10.4236/am.2019.102005</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.4236/am.2019.102005">https://doi.org/10.4236/am.2019.102005</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Osaka, M.</string-name>
            </person-group>
            <year>2019</year>
            <article-title>A Probabilistic Method to Determine Whether the Speed of Light Is Constant</article-title>
            <source>Applied Mathematics</source>
            <volume>10</volume>
            <pub-id pub-id-type="doi">10.4236/am.2019.102005</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B5">
        <label>5.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Ellis, G.F.R., Kirchner, U. and Stoeger, W.R. (2004) Multiverses and Physical Cosmology. <italic>Monthly</italic><italic>Notices</italic><italic>of</italic><italic>the</italic><italic>Royal</italic><italic>Astronomical</italic><italic>Society</italic>, 347, 921-936. https://doi.org/10.1111/j.1365-2966.2004.07261.x <pub-id pub-id-type="doi">10.1111/j.1365-2966.2004.07261.x</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1111/j.1365-2966.2004.07261.x">https://doi.org/10.1111/j.1365-2966.2004.07261.x</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Ellis, G.F.R.</string-name>
              <string-name>Kirchner, U.</string-name>
              <string-name>Stoeger, W.R.</string-name>
            </person-group>
            <year>2004</year>
            <article-title>Multiverses and Physical Cosmology</article-title>
            <source>Monthly Notices of the Royal Astronomical Society</source>
            <volume>347</volume>
            <pub-id pub-id-type="doi">10.1111/j.1365-2966.2004.07261.x</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B6">
        <label>6.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Mignani, R.P., Testa, V., González Caniulef, D., Taverna, R., Turolla, R., Zane, S., <italic>et al</italic>. (2016) Evidence for Vacuum Birefringence from the First Optical-Polarimetry Measurement of the Isolated Neutron Star RX J1856.5-3754. <italic>Monthly</italic><italic>Notices</italic><italic>of</italic><italic>the</italic><italic>Royal</italic><italic>Astronomical</italic><italic>Society</italic>, 465, 492-500. https://doi.org/10.1093/mnras/stw2798 <pub-id pub-id-type="doi">10.1093/mnras/stw2798</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1093/mnras/stw2798">https://doi.org/10.1093/mnras/stw2798</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Mignani, R.P.</string-name>
              <string-name>Testa, V.</string-name>
              <string-name>Caniulef, D.</string-name>
              <string-name>Taverna, R.</string-name>
              <string-name>Turolla, R.</string-name>
              <string-name>Zane, S.</string-name>
            </person-group>
            <year>2016</year>
            <article-title>Evidence for Vacuum Birefringence from the First Optical-Polarimetry Measurement of the Isolated Neutron Star RX J1856</article-title>
            <source>5-3754. Monthly Notices of the Royal Astronomical Society</source>
            <volume>465</volume>
            <pub-id pub-id-type="doi">10.1093/mnras/stw2798</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B7">
        <label>7.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Schwinger, J. (1951) On Gauge Invariance and Vacuum Polarization. <italic>Physical</italic><italic>Review</italic>, 82, 664-679. https://doi.org/10.1103/physrev.82.664 <pub-id pub-id-type="doi">10.1103/physrev.82.664</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1103/physrev.82.664">https://doi.org/10.1103/physrev.82.664</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Schwinger, J.</string-name>
            </person-group>
            <year>1951</year>
            <article-title>On Gauge Invariance and Vacuum Polarization</article-title>
            <source>Physical Review</source>
            <volume>82</volume>
            <pub-id pub-id-type="doi">10.1103/physrev.82.664</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B8">
        <label>8.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Parker, R.H., Yu, C., Zhong, E., Estey, B. and Müller, H. (2018) Measurement of the Fine-Structure Constant as a Test of the Standard Model. arXiv: 1812.04130.</mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Parker, R.H.</string-name>
              <string-name>Yu, C.</string-name>
              <string-name>Zhong, E.</string-name>
              <string-name>Estey, B.</string-name>
            </person-group>
            <year>2018</year>
            <article-title>Measurement of the Fine-Structure Constant as a Test of the Standard Model</article-title>
            <fpage>1812</fpage>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B9">
        <label>9.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Bousso, R. and Polchinski, J. (2000) Quantization of Four-Form Fluxes and Dynamical Neutralization of the Cosmological Constant. <italic>Journal</italic><italic>of</italic><italic>High</italic><italic>Energy</italic><italic>Physics</italic>, 6, 1-25. https://doi.org/10.1088/1126-6708/2000/06/006 <pub-id pub-id-type="doi">10.1088/1126-6708/2000/06/006</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1088/1126-6708/2000/06/006">https://doi.org/10.1088/1126-6708/2000/06/006</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Bousso, R.</string-name>
              <string-name>Polchinski, J.</string-name>
            </person-group>
            <year>2000</year>
            <article-title>Quantization of Four-Form Fluxes and Dynamical Neutralization of the Cosmological Constant</article-title>
            <source>Journal of High Energy Physics</source>
            <volume>6</volume>
            <pub-id pub-id-type="doi">10.1088/1126-6708/2000/06/006</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
    </ref-list>
  </back>
</article>