<?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">IJAA</journal-id><journal-title-group><journal-title>International Journal of Astronomy and Astrophysics</journal-title></journal-title-group><issn pub-type="epub">2161-4717</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijaa.2023.133010</article-id><article-id pub-id-type="publisher-id">IJAA-127401</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A New Approach to the Dark Matter/Dark Energy Puzzle
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Michael</surname><given-names>J. Longo</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Physics, University of Michigan, Ann Arbor, MI, USA</addr-line></aff><pub-date pub-type="epub"><day>30</day><month>08</month><year>2023</year></pub-date><volume>13</volume><issue>03</issue><fpage>166</fpage><lpage>171</lpage><history><date date-type="received"><day>20,</day>	<month>July</month>	<year>2023</year></date><date date-type="rev-recd"><day>28,</day>	<month>August</month>	<year>2023</year>	</date><date date-type="accepted"><day>31,</day>	<month>August</month>	<year>2023</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The dilemmas posed by dark matter and dark energy have been with us for decades without a satisfactory resolution. We propose that both DM and DE can be explained by the existence of long-lived topological gravitational vortices that were produced in the quark-gluon epoch of cosmic inflation due to the misalignment of the gravitational and strong forces. This is analogous to the misalignment mechanism proposed for the production of axions in the early universe. The masses of these topological vortices are expected to be on the order of the nucleon mass. Possible means for their detection are discussed.
 
</p></abstract><kwd-group><kwd>Dark Matter</kwd><kwd> Dark Energy</kwd><kwd> Topological Defects</kwd><kwd> Cosmic Inflation</kwd><kwd> Quark-Gluon Plasma</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The existence of dark energy has been known for at least 20 years ( [<xref ref-type="bibr" rid="scirp.127401-ref1">1</xref>] , p: 499) and for dark matter even longer ( [<xref ref-type="bibr" rid="scirp.127401-ref1">1</xref>] , p: 483). Despite many experimental searches, no convincing explanations for the nature of DM or DE have been found [<xref ref-type="bibr" rid="scirp.127401-ref1">1</xref>] . The leading contender for the nature of DE is that it is due to the cosmological constant. However, this leads to predictions that are ~60 orders of magnitude too large [<xref ref-type="bibr" rid="scirp.127401-ref2">2</xref>] .</p><p>In view of the present dilemma, it is an appropriate time to consider other paradigms to explain (hopefully) both DM and DE. We propose that both DM and DE can be explained by the existence of long-lived topological vortices that were produced as strong interactions emerged in the quark-gluon epoch of cosmic inflation ~10<sup>−10</sup> seconds after the Big Bang. There is no theory of quantum gravity so we here consider a semi-classical approach. It is convenient to use vector terminology.</p><p>Vortex formation is familiar in fluid mechanics. Vortices are formed in water by ship propellers and in the atmosphere behind airplane wings and automobiles. Long-lived vortices in the atmosphere, such as tornadoes and the Great Red Spot on Jupiter, are well-known. Spiral galaxies are ubiquitous. In an optical vortex, light is twisted like a corkscrew around its axis of travel [<xref ref-type="bibr" rid="scirp.127401-ref3">3</xref>] . Localized optical vortices, i.e., vortex solitons, have drawn much attention as physical objects of fundamental interest and also because of their potential applications to optical information processing [<xref ref-type="bibr" rid="scirp.127401-ref4">4</xref>] .</p><p>A vortex can be generated whenever two vector fields are misaligned, for example, a pressure gradient and a density gradient. The resulting vector cross product or torque generates an angular momentum ΔL = τ Δt where τ is the torque. In the ship propeller example, the vectors are the pressure on the propeller blades and the velocity of the water going past them.</p><p>A similar scenario for generating a nonzero energy density for light scalar fields is through the misalignment mechanism proposed for axions [<xref ref-type="bibr" rid="scirp.127401-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.127401-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.127401-ref7">7</xref>] . Co et al. [<xref ref-type="bibr" rid="scirp.127401-ref8">8</xref>] propose a misalignment scenario where the axion field has a nonzero initial velocity that can be generated from the explicit breaking of the axion shift symmetry in the early universe. In the scenario proposed here, the breakdown occurs much later, in the quark-gluon epoch.</p></sec><sec id="s2"><title>2. Background</title><p>Edery [<xref ref-type="bibr" rid="scirp.127401-ref9">9</xref>] has studied vortex solutions in Einstein gravity and found numerically static solutions in which a complex scalar field φ and a gauge field A<sub>μ</sub> have a non-singular profile in an anti-deSitter (2 + 1)-dimensional space-time background. Vortices with different winding numbers n, vacuum expectation value v, and cosmological constant Λ were obtained. These vortices have positive mass and are not black holes as they have no event horizon. The works of Edery and others show that it is plausible that gravitational vortices are produced late in inflation but they give no real insight as to their masses, mass density, and lifetimes.</p><p>There is a significant literature on cosmological gravitational particle production (CGPP) in an expanding universe. A review by Ford [<xref ref-type="bibr" rid="scirp.127401-ref10">10</xref>] gives estimates for particle creation rates by gravitational fields in specific inflationary cosmology models, including some exactly soluble models. He concludes that particle creation by the gravitational field could play a significant role in cosmological evolution and that gravitational particle creation could be a promising model for the origin of the dark matter.</p><p>Recently Kolb et al. [<xref ref-type="bibr" rid="scirp.127401-ref11">11</xref>] discuss CGPP which is expected to occur during the period of inflation and the transition into a hot big bang cosmology. Particles may be produced even if they only couple directly to gravity, and so CGPP provides a natural explanation for the origin of dark matter. They study the gravitational production of massive spin-2 particles assuming two different couplings to matter and calculate the spectrum and abundance of massive spin-2 particles that result from inflation on a hilltop potential. They conclude that CGPP might provide a viable mechanism for the generation of massive spin-2 particle dark matter during inflation and identify the favorable region of parameter space in terms of the spin-2 particle’s mass and the reheating temperature.</p><p>These CGPP models generally assume the particles are produced during inflation and the exponential expansion acts as a gravitational amplifier. They are focused mainly on production and detection of thermal relics with mass typically in the range a few GeV to a hundred GeV or nonthermal WIMPs with masses in the range 10<sup>12</sup> to 10<sup>16</sup> GeV. The gyrons discussed here are produced in the quark-gluon epoch when gravitational forces are comparable to strong interaction forces, so that gyron masses would be comparable to baryon masses as discussed below.</p></sec><sec id="s3"><title>3. Formation of Long-Lived Topological Vortices in the Quark-Gluon Plasma</title><p>Vector misalignments, as discussed above, are inevitable in the quark-gluon epoch of cosmic evolution due to the local misalignment between the gravitational force vectors and the strong and electromagnetic forces between the emerging quarks and gluons. This generates spatial vortices in the evolving universe. (They might also be produced in the earlier electroweak epoch.) The vortices acquire a mass due to their coupling to the strong/electromagnetic fields. These vortices should be long-lived and may grow in size as the universe expands [<xref ref-type="bibr" rid="scirp.127401-ref9">9</xref>] . Further torques can only spin their angular momentum up or down. Unlike other topological defects, such as strings and walls [<xref ref-type="bibr" rid="scirp.127401-ref12">12</xref>] , they are produced late in inflation and so are not “inflated” out. Just as for other topological defects they carry energy and thus experience gravitational forces. Their creation is analogous to the formation of a gravitational singularity–a black hole–when two neutron stars collide. The latter happens much later in inflation on a much grander scale.</p><p>I shall refer to the gravitational solitons as gyrons. Without a rigorous quantum gravity treatment, it is not possible to predict the characteristics of gyrons, in particular their masses and mass density. However, it is possible to make plausible arguments for their general properties. Like neutrinos, they decouple and move through space freely. They carry angular momentum and mass energy. The unification of the electroweak force and the strong force with the gravitational force in the so-called “Theory of Everything” requires an energy level which is generally assumed to be close to the Planck scale of 10<sup>19</sup> GeV. The unification of the electroweak force and the strong force with the gravitational force is, in turn, related to the Planck mass as G N = ℏ c / M p 2 where G<sub>N</sub> is the gravitational constant and the Planck mass M<sub>p</sub> = 1.22 &#215; 10<sup>19</sup> GeV/c<sup>2</sup>. The final symmetry breaking, that of chiral symmetry in the quark sector, occurs ~10<sup>−10</sup> seconds after the Big Bang. Gravitational forces are then comparable to strong interaction forces as quarks and baryons emerge. In this epoch, the effective coupling was on the order of the strong coupling constant α<sub>s</sub> ~0.11 [<xref ref-type="bibr" rid="scirp.127401-ref13">13</xref>] . Therefore, the effective gravitational constant at this epoch is G g ~ ℏ c / M n 2 where M<sub>n</sub> is the nucleon mass. Thus, the mass scale for gyron production is on the order of baryon masses so that the expected gyron mass is ~1 GeV/c<sup>2</sup>.</p><p>Since they are fundamentally quantum objects, it is reasonable to assume that their angular momentum is quantized in half-integer multiples of ℏ , as for other elementary particles. They could carry electric and/or magnetic charges. Their total mass density could be greater than the mass density of baryons in the universe.</p></sec><sec id="s4"><title>4. Discussion</title><p>Gyrons would interact with each other and interact gravitationally with baryonic matter. Winding number is conserved so they are long-lived, though gyrons with opposite winding numbers could annihilate each other. Dark matter causes an attractive gravitational force while dark energy appears as a repulsive force or negative energy. To explain both dark matter and dark energy would require two varieties of gyrons. Vortex solitons will repel or attract depending on their topological charge [<xref ref-type="bibr" rid="scirp.127401-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.127401-ref15">15</xref>] . The observed baryon, cold dark matter, and dark energy densities normalized to the critical density ρ<sub>critical</sub> = 9.47 &#215; 10<sup>−27</sup> kg·m<sup>−3</sup> are respectively, Ω<sub>b</sub> = 0.0223h<sup>−2</sup>, Ω<sub>c</sub> = 0.105h<sup>−2</sup>, and Ω<sub>L</sub> = 0.73h<sup>−2</sup> ( [<xref ref-type="bibr" rid="scirp.127401-ref1">1</xref>] , p: 134). Without a theory there is no way to predict the gyron mass density. A density about 5 times the baryon density for the attractive component would explain the dark matter. A density for the repulsive component about 7 times that of the attractive component would account for the dark energy. Edery [<xref ref-type="bibr" rid="scirp.127401-ref9">9</xref>] found that the cases with n = 2 and v = 2 differed from their n = 1 and v = 1 counterparts in that they had significantly higher masses, reflecting the approximate dependence of the integral mass formula on n<sup>2</sup>v<sup>2</sup>, so that a repulsive component that is 7 times the attractive component is plausible.</p><p>In this picture the “attractive” vortices are the dark matter and along with the ordinary matter cause structure formation. The repulsive component accounts for the repulsive force that is the only known attribute of dark energy which causes the acceleration of the expansion that is observed in the present universe. This picture is similar to that of quintessence [<xref ref-type="bibr" rid="scirp.127401-ref16">16</xref>] . However, quintessence is driven by an evolving scalar field which is present from the beginning of inflation, while the topological vortices posited here are elementary objects that are produced much later in the quark-gluon phase. Gyron masses ~1 GeV/c<sup>2</sup>, as discussed in Section 2, would explain the observed clustering. Gyrons could also have appeared earlier in the weak interaction dominated universe and would likely cause a CP violation that led to an excess of right- or left-handed gyrons. This would propagate the CP violation into the later universe.</p><p>Theoretical considerations aside, there are some possibilities for detecting gyrons. Gyrons with electric charge would behave like cosmic ray electrons or muons depending on their mass (but, unlike muons, they would not decay). They would undergo the same acceleration mechanisms as other cosmic rays, so their energy spectrum would be similar to that of other cosmic rays. Cosmic muons, because of their short lifetimes, must be produced locally in the Earth or atmosphere by decays of hadrons that are produced by cosmic rays or by cosmic neutrino interactions. The IceCube detector at the South Pole has detected hundreds of muon-like events produced by cosmic neutrinos [<xref ref-type="bibr" rid="scirp.127401-ref17">17</xref>] . Some of these could be due to gyrons whose electromagnetic interactions would closely resemble those of muons. A careful study of the ionization profiles in the detector, which would be different from that of muons because of their different mass, could establish whether two components were in the data. Cosmic gyrons could also masquerade as cosmic electrons. Data from the Alpha Magnetic Spectrometer on the International Space Station exhibit a significant excess of electrons starting above ~42 GeV and an excess of positrons above ~25 GeV [<xref ref-type="bibr" rid="scirp.127401-ref18">18</xref>] . These excesses have not been explained. They could reflect a previously unrecognized component in the data that mimics electrons. This could be revealed by a study of the ionization profiles in the detector.</p><p>Gyrons without electric or magnetic charge would only interact gravitationally with matter. In passing through a torsion balance or near a gravitational wave detector such as LIGO, they would leave a characteristic signal unlike the compression/expansion caused by a gravitational wave [<xref ref-type="bibr" rid="scirp.127401-ref19">19</xref>] . Another possibility is that they would contribute to the stochastic noise in pulsar timing arrays [<xref ref-type="bibr" rid="scirp.127401-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.127401-ref21">21</xref>] . The technique used by Dixit et al. [<xref ref-type="bibr" rid="scirp.127401-ref22">22</xref>] using a superconducting qubit to make repeated quantum nondemolition measurements of cavity photons could also be applied in searching for the passage of topological vortices.</p><p>The possibility that new fundamental particles are produced in the quark-gluon era is intriguing. The ingredients for their production—the final symmetry breaking in the quark sector together with the misalignment of the gravitational and strong and electromagnetic forces in the quark-gluon plasma–were there. We won’t find them if we don’t look for them.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Longo, M.J. (2023) A New Approach to the Dark Matter/Dark Energy Puzzle. International Journal of Astronomy and Astrophysics, 13, 166-171. https://doi.org/10.4236/ijaa.2023.133010</p></sec></body><back><ref-list><title>References</title><ref id="scirp.127401-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Workman, R.L. et al. (Particle Data Group) (2022) Review of Particle Physics. Progress of Theoretical and Experimental Physics, 2022, 083C01. (For Recent Reviews, See Articles on “Dark Matter” and “Dark Energy”)https://doi.org/10.1093/ptep/ptac097</mixed-citation></ref><ref id="scirp.127401-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Frieman, J.A., Turner, M.S. and Huterer, D. (2008) Dark Energy and the Accelerating Universe. Annual Review of Astronomy and Astrophysics, 46, 385-432. https://doi.org/10.1146/annurev.astro.46.060407.145243</mixed-citation></ref><ref id="scirp.127401-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Wikipedia (2013) Optical Vortex.</mixed-citation></ref><ref id="scirp.127401-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Shen, Y., Wang, X., et al. (2019) Optical Vortices 30 Years on: OAM Manipulation from Topological Charge to Multiple Singularities. Light: Science &amp; Applications, 8, Article No. 90. https://doi.org/10.1038/s41377-019-0194-2</mixed-citation></ref><ref id="scirp.127401-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Preskill, J., Wise, M. and Wilczek, F. (1983) Cosmology of the Invisible Axion. Physics Letters B, 120, 127-132. https://doi.org/10.1016/0370-2693(83)90637-8</mixed-citation></ref><ref id="scirp.127401-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Dine, M. and Fischler, W. (1983) The Not-So-Harmless Axion. Physics Letters B, 120, 137-141. https://doi.org/10.1016/0370-2693(83)90639-1</mixed-citation></ref><ref id="scirp.127401-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Abbott, L.F. and Sikivie, P. (1983) A Cosmological Bound on the Invisible Axion. Physics Letters B, 120, 133-136. https://doi.org/10.1016/0370-2693(83)90638-X</mixed-citation></ref><ref id="scirp.127401-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Co, R.T., Hall, L.J. and Harigaya, K. (2020) Axion Kinetic Misalignment Mechanism. Physical Review Letters, 124, Article ID: 251802. https://doi.org/10.1103/PhysRevLett.124.251802</mixed-citation></ref><ref id="scirp.127401-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Edery, A. (2021) Non-Singular Vortices with Positive Mass in 2 + 1-Dimensional Einstein Gravity with AdS&lt;sub&gt;3&lt;/sub&gt; and Minkowski Background. Journal of High Energy Physics, 1, Article No. 166. https://doi.org/10.1007/JHEP01(2021)166</mixed-citation></ref><ref id="scirp.127401-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Ford, L.H. (2021) Cosmological Particle Production: A Review. Reports on Progress in Physics, 84, Article ID: 11690. https://doi.org/10.1088/1361-6633/ac1b23</mixed-citation></ref><ref id="scirp.127401-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Kolb, E.W., Ling, S., Long, A.J. and Rosen, R.A. (2023) Cosmological Gravitational Particle Production of Massive Spin-2 Particles. arXiv: 2302.04390v1. https://doi.org/10.1007/JHEP05(2023)181</mixed-citation></ref><ref id="scirp.127401-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Nitta, M. (2022) Relations among Topological Solitons. Physical Review D, 105, Article No. 105006. https://doi.org/10.1103/PhysRevD.105.105006</mixed-citation></ref><ref id="scirp.127401-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Tanabashi, M., et al. (Particle Data Group) (2018) Review of Particle Physics. Physical Review D, 98, Article ID: 030001. https://doi.org/10.1103/PhysRevD.98.030001</mixed-citation></ref><ref id="scirp.127401-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Arthur, K. (1995) Interaction Energy of Chern-Simons Vortices. Physics Letters B, 356, 509-515. https://doi.org/10.1016/0370-2693(95)00830-E</mixed-citation></ref><ref id="scirp.127401-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Jacobs, L. and Rebbi, C. (1979) Interaction Energy of Superconducting Vortices. Physical Review B, 19, 4486-4494. https://doi.org/10.1103/PhysRevB.19.4486</mixed-citation></ref><ref id="scirp.127401-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Caldwell, R., Dave, R. and Steinhardt, P. (1998) Cosmological Imprint of an Energy Component with General Equation of State. Physical Review Letters, 80, 1582-1585. https://doi.org/10.1103/PhysRevLett.80.1582</mixed-citation></ref><ref id="scirp.127401-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Aartsen, M., et al. (2020) Characteristics of the Diffuse Astrophysical Electron and Tau Neutrino Flux with Six Years of IceCube High Energy Cascade Data. Physical Review Letters, 125, Article ID: 121104.</mixed-citation></ref><ref id="scirp.127401-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Aguilar, M., et al. (2019) Towards Understanding the Origin of Cosmic-Ray Electrons. Physical Review Letters, 122, Article ID: 101101.</mixed-citation></ref><ref id="scirp.127401-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Brito, R., Chakrabartiet, S., et al. (2021) Probing Dark Matter with Small-Scale Astrophysical Observations. Proceeding of the US Community Study on the Future of Particle Physics Snowmass 2021, Snowmass, 14 July 2022. arXiv: 2203.15954v2.</mixed-citation></ref><ref id="scirp.127401-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Xue, X. and Xia, Z.Q. (2022) High-Precision Search for Dark Photon Dark Matter with the Parkes Pulsar Timing Array. Physical Review Research, 4, L012022. https://doi.org/10.1103/PhysRevResearch.4.L012022</mixed-citation></ref><ref id="scirp.127401-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Antypas, D., Banerjee, A., et al. (2021) New Horizons: Scalar and Vector Ultralight Dark Matter. Proceeding of the US Community Study on the Future of Particle Physics Snowmass 2021, Snowmass, 14 July 2022. arXiv: 2203.14915v1.</mixed-citation></ref><ref id="scirp.127401-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Dixit, A.V., Chakram, S., He, K., Agrawal, A., Naik, R., Schuster, D. and Chou, A. (2019) Searching for Dark Matter with a Superconducting Qubit. Physical Review Letters, 126, Article ID: 141302. https://doi.org/10.1103/PhysRevLett.126.141302</mixed-citation></ref></ref-list></back></article>