Pub Date : 2026-02-03DOI: 10.1016/j.dark.2026.102240
Gabriela Garcia-Arroyo , Isidro Gómez-Vargas , J. Alberto Vázquez
Galactic rotation curves are crucial for understanding the distribution of mass in galaxies. Despite advances in precision observations, there are discrepancies between the inferred mass from luminosity and the observed rotational velocities, often attributed to dark matter. While traditional parametric models provide valuable insights, they struggle with complex galactic features like prominent bulges and non-circular motions. In this study, we apply artificial neural networks to generate robust, data-driven models, tailored to each galaxy, for the rotation curves of spiral galaxies using high-quality observational data. Our approach demonstrates that neural networks can effectively capture the intricate structure of rotation curves without relying on predefined astrophysical assumptions. By comparing the data-based models with the Navarro-Frenk-White model under two different assumptions for the stellar component, we classify galaxies based on the model that best fits their rotation curves, offering insights into the limitations and strengths of both theoretical and data-based methods. This work highlights the potential of machine learning techniques in identifying galaxies whose dynamics are not well captured by standard theoretical models, pointing to the need for more refined physical descriptions.
{"title":"Data-driven modeling of rotation curves with artificial neural networks","authors":"Gabriela Garcia-Arroyo , Isidro Gómez-Vargas , J. Alberto Vázquez","doi":"10.1016/j.dark.2026.102240","DOIUrl":"10.1016/j.dark.2026.102240","url":null,"abstract":"<div><div>Galactic rotation curves are crucial for understanding the distribution of mass in galaxies. Despite advances in precision observations, there are discrepancies between the inferred mass from luminosity and the observed rotational velocities, often attributed to dark matter. While traditional parametric models provide valuable insights, they struggle with complex galactic features like prominent bulges and non-circular motions. In this study, we apply artificial neural networks to generate robust, data-driven models, tailored to each galaxy, for the rotation curves of spiral galaxies using high-quality observational data. Our approach demonstrates that neural networks can effectively capture the intricate structure of rotation curves without relying on predefined astrophysical assumptions. By comparing the data-based models with the Navarro-Frenk-White model under two different assumptions for the stellar component, we classify galaxies based on the model that best fits their rotation curves, offering insights into the limitations and strengths of both theoretical and data-based methods. This work highlights the potential of machine learning techniques in identifying galaxies whose dynamics are not well captured by standard theoretical models, pointing to the need for more refined physical descriptions.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"52 ","pages":"Article 102240"},"PeriodicalIF":6.4,"publicationDate":"2026-02-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146116671","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-02DOI: 10.1016/j.dark.2026.102241
Matias P. Gonzalez, Roberto A. Lineros
We generalize thermal WIMP (Weakly Interacting Massive Particle) freeze-out within Tsallis nonextensive statistics. Using Curado–Tsallis q-distributions fq(E; μ, T) we compute q-deformed number and energy densities, pressure, entropy density and Hubble rate, {nq, ρq, Pq, sq, Hq}. The Boltzmann equation is generalized accordingly to obtain the comoving abundance Yχ,q(x) and relic density Ωχ,qh2 for a dark-matter candidate χ in a model-independent setup. The thermally averaged cross section is expanded as up to p-wave. The freeze-out parameter xf(q) is determined from Γann,q(Tf) ≃ Hq(Tf) using a q-logarithmic inversion, with the expansion rate modified through ultra-relativistic rescalings Rρ(q) of the effective relativistic degrees of freedom g* and g*s. We show that xf increases with q and that QCD-threshold features propagate into Yχ,q(x) and Ωχ,qh2. We then perform two q-grid scans: fixing ⟨σv⟩q while varying the dark-matter mass mχ, and fixing mχ while varying the s-wave coefficient a. For an s-wave dominated scenario we construct χ2 profiles in these planes by comparing Ωχ,qh2 with the Planck benchmark . In both cases we find a clear degeneracy in the preferred nonextensive parameter qbest along valleys in parameter space. However, fixed-mass scans (varying ⟨σv⟩q) are significantly more constraining than fixed-cross-section scans, reflecting that Ωχ,qh2 is mainly controlled by ⟨σv⟩q, so that for realistic cross sections the best-fit qbest remains close to the extensive limit q → 1.
{"title":"WIMP freeze-out dynamics under Tsallis statistics","authors":"Matias P. Gonzalez, Roberto A. Lineros","doi":"10.1016/j.dark.2026.102241","DOIUrl":"10.1016/j.dark.2026.102241","url":null,"abstract":"<div><div>We generalize thermal WIMP (Weakly Interacting Massive Particle) freeze-out within Tsallis nonextensive statistics. Using Curado–Tsallis <em>q</em>-distributions <em>f<sub>q</sub></em>(<em>E</em>; <em>μ, T</em>) we compute <em>q</em>-deformed number and energy densities, pressure, entropy density and Hubble rate, {<em>n<sub>q</sub>, ρ<sub>q</sub>, P<sub>q</sub>, s<sub>q</sub>, H<sub>q</sub></em>}. The Boltzmann equation is generalized accordingly to obtain the comoving abundance <em>Y</em><sub><em>χ,q</em></sub>(<em>x</em>) and relic density Ω<sub><em>χ,q</em></sub><em>h</em><sup>2</sup> for a dark-matter candidate <em>χ</em> in a model-independent setup. The thermally averaged cross section is expanded as <span><math><mrow><msub><mrow><mo>〈</mo><mi>σ</mi><mi>v</mi><mo>〉</mo></mrow><mi>q</mi></msub><mo>≈</mo><mi>a</mi><mo>+</mo><mi>b</mi><mspace></mspace><msub><mrow><mo>〈</mo><msubsup><mi>v</mi><mrow><mrow><mi>r</mi></mrow><mi>e</mi><mi>l</mi></mrow><mn>2</mn></msubsup><mo>〉</mo></mrow><mi>q</mi></msub></mrow></math></span> up to <em>p</em>-wave. The freeze-out parameter <em>x<sub>f</sub></em>(<em>q</em>) is determined from Γ<sub>ann,<em>q</em></sub>(<em>T<sub>f</sub></em>) ≃ <em>H<sub>q</sub></em>(<em>T<sub>f</sub></em>) using a <em>q</em>-logarithmic inversion, with the expansion rate modified through ultra-relativistic rescalings <em>R<sub>ρ</sub></em>(<em>q</em>) of the effective relativistic degrees of freedom <em>g</em><sub>*</sub> and <em>g</em><sub>*<em>s</em></sub>. We show that <em>x<sub>f</sub></em> increases with <em>q</em> and that QCD-threshold features propagate into <em>Y</em><sub><em>χ,q</em></sub>(<em>x</em>) and Ω<sub><em>χ,q</em></sub><em>h</em><sup>2</sup>. We then perform two <em>q</em>-grid scans: fixing ⟨<em>σv</em>⟩<sub><em>q</em></sub> while varying the dark-matter mass <em>m<sub>χ</sub></em>, and fixing <em>m<sub>χ</sub></em> while varying the <em>s</em>-wave coefficient <em>a</em>. For an <em>s</em>-wave dominated scenario we construct <em>χ</em><sup>2</sup> profiles in these planes by comparing Ω<sub><em>χ,q</em></sub><em>h</em><sup>2</sup> with the Planck benchmark <span><math><mrow><msub><mstyle><mi>Ω</mi></mstyle><mi>c</mi></msub><msup><mi>h</mi><mn>2</mn></msup><mo>=</mo><mn>0.120</mn><mo>±</mo><mn>0.001</mn></mrow></math></span>. In both cases we find a clear degeneracy in the preferred nonextensive parameter <em>q</em><sub>best</sub> along valleys in parameter space. However, fixed-mass scans (varying ⟨<em>σv</em>⟩<sub><em>q</em></sub>) are significantly more constraining than fixed-cross-section scans, reflecting that Ω<sub><em>χ,q</em></sub><em>h</em><sup>2</sup> is mainly controlled by ⟨<em>σv</em>⟩<sub><em>q</em></sub>, so that for realistic cross sections the best-fit <em>q</em><sub>best</sub> remains close to the extensive limit <em>q</em> → 1.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"52 ","pages":"Article 102241"},"PeriodicalIF":6.4,"publicationDate":"2026-02-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146116716","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-01DOI: 10.1016/j.dark.2026.102218
Aurindam Mondal , Rathul Nath Raveendran
We investigate the quantum nature of primordial perturbations by studying the violation of Bell inequality when the initial state is taken to be a coherent state rather than the usual Bunch-Davies vacuum. As inflation progresses, the coherent state evolves into a squeezed coherent state, and we derive an analytical expression for the expectation value of the Bell operator constructed from pseudo-spin operators. Our analysis shows that although the expectation value of the Bell operator initially deviates from the vacuum case, it asymptotically saturates to the same value. Notably, this saturation occurs more rapidly for non-zero coherent state parameters, indicating that a larger one-point correlation function accelerates the approach to maximal Bell inequality violation.
{"title":"Violation of Bell inequality from a squeezed coherent state of inflationary perturbations","authors":"Aurindam Mondal , Rathul Nath Raveendran","doi":"10.1016/j.dark.2026.102218","DOIUrl":"10.1016/j.dark.2026.102218","url":null,"abstract":"<div><div>We investigate the quantum nature of primordial perturbations by studying the violation of Bell inequality when the initial state is taken to be a coherent state rather than the usual Bunch-Davies vacuum. As inflation progresses, the coherent state evolves into a squeezed coherent state, and we derive an analytical expression for the expectation value of the Bell operator constructed from pseudo-spin operators. Our analysis shows that although the expectation value of the Bell operator initially deviates from the vacuum case, it asymptotically saturates to the same value. Notably, this saturation occurs more rapidly for non-zero coherent state parameters, indicating that a larger one-point correlation function accelerates the approach to maximal Bell inequality violation.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102218"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077975","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-01DOI: 10.1016/j.dark.2026.102233
Ghulam Fatima , Abdelmalek Bouzenada , Orhan Donmez , Allah Ditta , G. Mustafa , Farruh Atamurotov
In this study, we examine the accretion of perfect and polytropic fluids onto Barrow’s nonlinear charged black hole models, described by a static spherically symmetric spacetime with a metric function X(r) explicitly dependent on the Yang-Mills coupling parameter α, magnetic charge Q, and black hole mass M. We employ two equations of state: (i) , which incorporates a reference density ρ0 to account for a nonzero rest energy baseline, and (ii) , representing a conventional linear equations of state. Applying the steady-state approximation, we derive the conservation equations for mass, momentum, and energy, which allow analytical determination of the critical (sonic) points and the mass accretion rate. In this case, the analysis reveals that increasing either α or Q reduces the fluid inflow velocity and local sound speed while simultaneously enhancing the accretion rate near the event horizon. Also, both equations of state models exhibit smooth, continuous transitions through the sonic points, and numerical evaluations demonstrate pronounced effects of α and Q on the horizon geometry, location of critical points, fluid density, and sound speed, quantitatively illustrating the influence of nonlinear electrodynamics and Barrow deformation on relativistic accretion dynamics.
{"title":"Exact and numerical analysis of accretion dynamics with perfect and polytropic fluids around nonlinear charged black holes","authors":"Ghulam Fatima , Abdelmalek Bouzenada , Orhan Donmez , Allah Ditta , G. Mustafa , Farruh Atamurotov","doi":"10.1016/j.dark.2026.102233","DOIUrl":"10.1016/j.dark.2026.102233","url":null,"abstract":"<div><div>In this study, we examine the accretion of perfect and polytropic fluids onto Barrow’s nonlinear charged black hole models, described by a static spherically symmetric spacetime with a metric function <em>X</em>(<em>r</em>) explicitly dependent on the Yang-Mills coupling parameter <em>α</em>, magnetic charge <em>Q</em>, and black hole mass <em>M</em>. We employ two equations of state: <strong>(i)</strong> <span><math><mrow><mi>p</mi><mo>=</mo><mi>ω</mi><mo>(</mo><mi>ρ</mi><mo>−</mo><msub><mi>ρ</mi><mn>0</mn></msub><mo>)</mo></mrow></math></span>, which incorporates a reference density <em>ρ</em><sub>0</sub> to account for a nonzero rest energy baseline, and <strong>(ii)</strong> <span><math><mrow><mi>p</mi><mo>=</mo><mi>κ</mi><mi>ρ</mi></mrow></math></span>, representing a conventional linear equations of state. Applying the steady-state approximation, we derive the conservation equations for mass, momentum, and energy, which allow analytical determination of the critical (sonic) points and the mass accretion rate. In this case, the analysis reveals that increasing either <em>α</em> or <em>Q</em> reduces the fluid inflow velocity and local sound speed while simultaneously enhancing the accretion rate near the event horizon. Also, both equations of state models exhibit smooth, continuous transitions through the sonic points, and numerical evaluations demonstrate pronounced effects of <em>α</em> and <em>Q</em> on the horizon geometry, location of critical points, fluid density, and sound speed, quantitatively illustrating the influence of nonlinear electrodynamics and Barrow deformation on relativistic accretion dynamics.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102233"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077914","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This work studies the construction of anisotropic self-gravitating star models influenced by a surrounding quintessence field described by a parameter ωq with , under the theoretical requirement of a vanishing gravitational complexity factor. The complexity-free constraint, originally proposed as a measure of the structural inhomogeneity and pressure anisotropy of relativistic stellar fluids, is employed to obtain astrophysically relevant solutions of general relativistic field equations. By considering a suitable metric potential, we derive exact expressions for the matter density, principal stresses, and anisotropy factor. The influence of the quintessence field on stellar structure is analyzed in detail, highlighting its role in tuning the pressure anisotropy and energy distribution within the stellar distribution. To ensure realistic stellar modeling, we examine central regularity, positivity of density and principal stresses, energy conditions, causality, and stability requirements. Furthermore, matching conditions with the exterior spacetime are imposed to determine the unknown constants. The resulting stellar configurations are shown to be consistent with observational data of compact stars, thereby demonstrating that the combined effects of the quintessence field and the vanishing complexity condition provide an elegant framework for modeling anisotropic relativistic configuration.
{"title":"Anisotropic compact stars under quintessence field with vanishing gravitational complexity factor","authors":"S. Khan , Javlon Rayimbaev , Sarvar Iskandarov , Aybek Seytov , Inomjon Ibragimov , Sokhibjan Muminov","doi":"10.1016/j.dark.2026.102220","DOIUrl":"10.1016/j.dark.2026.102220","url":null,"abstract":"<div><div>This work studies the construction of anisotropic self-gravitating star models influenced by a surrounding quintessence field described by a parameter <em>ω<sub>q</sub></em> with <span><math><mrow><mo>−</mo><mn>1</mn><mo><</mo><msub><mi>ω</mi><mi>q</mi></msub><mo><</mo><mo>−</mo><mfrac><mn>1</mn><mn>3</mn></mfrac></mrow></math></span>, under the theoretical requirement of a vanishing gravitational complexity factor. The complexity-free constraint, originally proposed as a measure of the structural inhomogeneity and pressure anisotropy of relativistic stellar fluids, is employed to obtain astrophysically relevant solutions of general relativistic field equations. By considering a suitable metric potential, we derive exact expressions for the matter density, principal stresses, and anisotropy factor. The influence of the quintessence field on stellar structure is analyzed in detail, highlighting its role in tuning the pressure anisotropy and energy distribution within the stellar distribution. To ensure realistic stellar modeling, we examine central regularity, positivity of density and principal stresses, energy conditions, causality, and stability requirements. Furthermore, matching conditions with the exterior spacetime are imposed to determine the unknown constants. The resulting stellar configurations are shown to be consistent with observational data of compact stars, thereby demonstrating that the combined effects of the quintessence field and the vanishing complexity condition provide an elegant framework for modeling anisotropic relativistic configuration.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102220"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077979","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This study examines the behavior of compact astrophysical objects within a matter-geometry coupled f(R) gravity model. The modified field equations are expressed for a static interior spacetime with an anisotropic matter distribution. Applying two well-defined radial components of the metric ansatz and anisotropic pressures allows for analytical solutions to these equations. In both theoretical models, integrating the differential equations introduces constants, which are fixed using boundary conditions. Furthermore, the condition of null radial pressure at the boundary is used to determine these constants. Additionally, we visually assess certain important features that ensure the physical acceptability of the proposed model and support our analysis with observational data from LMC X-4. Our theoretical research shows that both models meet the physical viability and stability requirements. Further, our investigation also contributes to the knowledge of how the modified gravity model influences the interior structure of compact stars, paving the way for future studies.
{"title":"Dual impact of matter coupling on LMC X-4 pulsar observations and stability","authors":"Asifa Ashraf , Tayyab Naseer , Hammad Afzal , Chengxun Yuan , Ozodbek Rahimov , Ahmadjon Abdujabbarov","doi":"10.1016/j.dark.2026.102230","DOIUrl":"10.1016/j.dark.2026.102230","url":null,"abstract":"<div><div>This study examines the behavior of compact astrophysical objects within a matter-geometry coupled <em>f</em>(<em>R</em>) gravity model. The modified field equations are expressed for a static interior spacetime with an anisotropic matter distribution. Applying two well-defined radial components of the metric ansatz and anisotropic pressures allows for analytical solutions to these equations. In both theoretical models, integrating the differential equations introduces constants, which are fixed using boundary conditions. Furthermore, the condition of null radial pressure at the boundary is used to determine these constants. Additionally, we visually assess certain important features that ensure the physical acceptability of the proposed model and support our analysis with observational data from LMC X-4. Our theoretical research shows that both models meet the physical viability and stability requirements. Further, our investigation also contributes to the knowledge of how the modified gravity model influences the interior structure of compact stars, paving the way for future studies.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102230"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077972","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-01DOI: 10.1016/j.dark.2026.102231
Aylin Çalışkan
<div><div>We study the late-time cosmological implications of Weyl-type <em>f</em>(<em>Q, T</em>) modified gravity in a spatially flat FLRW background. Working in Weyl geometry, where non-metricity is sourced by a gauge field <em>w<sub>μ</sub></em>, we enforce the vanishing Weyl scalar condition <span><math><mrow><mover><mi>R</mi><mo>¯</mo></mover><mo>=</mo><mn>0</mn></mrow></math></span> through a Lagrange multiplier, which yields modified field equations containing both a Proca-like vector contribution and a matter-geometry coupling via <em>f</em>(<em>Q, T</em>). By adopting the linear ansatz <span><math><mrow><mi>f</mi><mrow><mo>(</mo><mi>Q</mi><mo>,</mo><mi>T</mi><mo>)</mo></mrow><mo>=</mo><mi>α</mi><mi>Q</mi><mo>+</mo><mfrac><mi>β</mi><mrow><mn>6</mn><msup><mi>κ</mi><mn>2</mn></msup></mrow></mfrac><mi>T</mi><mo>+</mo><mi>γ</mi></mrow></math></span> and a homogeneous Weyl vector <span><math><mrow><msub><mi>w</mi><mi>μ</mi></msub><mo>=</mo><mrow><mo>(</mo><mi>ψ</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>,</mo><mn>0</mn><mo>,</mo><mn>0</mn><mo>,</mo><mn>0</mn><mo>)</mo></mrow></mrow></math></span> (so that <span><math><mrow><mi>Q</mi><mo>=</mo><mn>6</mn><msup><mi>ψ</mi><mn>2</mn></msup></mrow></math></span>), we derive the generalized Friedmann equations and close the system under the approximation <em>λ</em> ≃ <em>κ</em><sup>2</sup>. The Weyl constraint admits the branch <span><math><mrow><mi>ψ</mi><mo>=</mo><mi>H</mi></mrow></math></span>, and consistency with the generalized Proca equation selects the massless effective mode <span><math><mrow><msubsup><mi>m</mi><mrow><mrow><mi>e</mi></mrow><mi>f</mi><mi>f</mi></mrow><mn>2</mn></msubsup><mo>=</mo><mn>0</mn></mrow></math></span>, fixing <em>α</em> and leaving (<em>β, γ</em>) as the relevant phenomenological parameters. For a dust sector (<span><math><mrow><mi>p</mi><mo>=</mo><mn>0</mn></mrow></math></span>), the dynamics reduces to a Riccati-type equation that can be integrated analytically, leading to a closed-form expression for the Hubble function <em>H</em>(<em>z</em>) and well-defined viability conditions (notably <span><math><mrow><mi>β</mi><mo>≠</mo><mo>−</mo><mn>2</mn></mrow></math></span> and <em>H</em><sup>2</sup>(<em>z</em>) ≥ 0). We then confront the model with current late-time data using an affine-invariant MCMC analysis with cosmic chronometer <em>H</em>(<em>z</em>) measurements, Pantheon+ SNe Ia, and DESI BAO. The combined dataset yields <span><math><mrow><msub><mi>H</mi><mn>0</mn></msub><mo>=</mo><mn>67.86</mn><mo>±</mo><mn>0.37</mn></mrow></math></span>, <span><math><mrow><mi>β</mi><mo>=</mo><mn>0</mn><mo>.</mo><msubsup><mn>27</mn><mrow><mo>−</mo><mn>0.13</mn></mrow><mrow><mo>+</mo><mn>0.11</mn></mrow></msubsup></mrow></math></span>, and <span><math><mrow><mi>γ</mi><mo>=</mo><mo>−</mo><mn>1.8</mn><mo>×</mo><msup><mn>10</mn><mn>4</mn></msup><mo>±</mo><mn>1.0</mn></mrow></math></span>, with a goodness of fit comparable to ΛCDM (<span><math><mrow><msubsup><mi>χ</mi><mrow
{"title":"Late-time cosmology in Weyl-type f(Q, T) modified gravity: Analytic background solutions and observational constraints from H(z), Pantheon+, and DESI","authors":"Aylin Çalışkan","doi":"10.1016/j.dark.2026.102231","DOIUrl":"10.1016/j.dark.2026.102231","url":null,"abstract":"<div><div>We study the late-time cosmological implications of Weyl-type <em>f</em>(<em>Q, T</em>) modified gravity in a spatially flat FLRW background. Working in Weyl geometry, where non-metricity is sourced by a gauge field <em>w<sub>μ</sub></em>, we enforce the vanishing Weyl scalar condition <span><math><mrow><mover><mi>R</mi><mo>¯</mo></mover><mo>=</mo><mn>0</mn></mrow></math></span> through a Lagrange multiplier, which yields modified field equations containing both a Proca-like vector contribution and a matter-geometry coupling via <em>f</em>(<em>Q, T</em>). By adopting the linear ansatz <span><math><mrow><mi>f</mi><mrow><mo>(</mo><mi>Q</mi><mo>,</mo><mi>T</mi><mo>)</mo></mrow><mo>=</mo><mi>α</mi><mi>Q</mi><mo>+</mo><mfrac><mi>β</mi><mrow><mn>6</mn><msup><mi>κ</mi><mn>2</mn></msup></mrow></mfrac><mi>T</mi><mo>+</mo><mi>γ</mi></mrow></math></span> and a homogeneous Weyl vector <span><math><mrow><msub><mi>w</mi><mi>μ</mi></msub><mo>=</mo><mrow><mo>(</mo><mi>ψ</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>,</mo><mn>0</mn><mo>,</mo><mn>0</mn><mo>,</mo><mn>0</mn><mo>)</mo></mrow></mrow></math></span> (so that <span><math><mrow><mi>Q</mi><mo>=</mo><mn>6</mn><msup><mi>ψ</mi><mn>2</mn></msup></mrow></math></span>), we derive the generalized Friedmann equations and close the system under the approximation <em>λ</em> ≃ <em>κ</em><sup>2</sup>. The Weyl constraint admits the branch <span><math><mrow><mi>ψ</mi><mo>=</mo><mi>H</mi></mrow></math></span>, and consistency with the generalized Proca equation selects the massless effective mode <span><math><mrow><msubsup><mi>m</mi><mrow><mrow><mi>e</mi></mrow><mi>f</mi><mi>f</mi></mrow><mn>2</mn></msubsup><mo>=</mo><mn>0</mn></mrow></math></span>, fixing <em>α</em> and leaving (<em>β, γ</em>) as the relevant phenomenological parameters. For a dust sector (<span><math><mrow><mi>p</mi><mo>=</mo><mn>0</mn></mrow></math></span>), the dynamics reduces to a Riccati-type equation that can be integrated analytically, leading to a closed-form expression for the Hubble function <em>H</em>(<em>z</em>) and well-defined viability conditions (notably <span><math><mrow><mi>β</mi><mo>≠</mo><mo>−</mo><mn>2</mn></mrow></math></span> and <em>H</em><sup>2</sup>(<em>z</em>) ≥ 0). We then confront the model with current late-time data using an affine-invariant MCMC analysis with cosmic chronometer <em>H</em>(<em>z</em>) measurements, Pantheon+ SNe Ia, and DESI BAO. The combined dataset yields <span><math><mrow><msub><mi>H</mi><mn>0</mn></msub><mo>=</mo><mn>67.86</mn><mo>±</mo><mn>0.37</mn></mrow></math></span>, <span><math><mrow><mi>β</mi><mo>=</mo><mn>0</mn><mo>.</mo><msubsup><mn>27</mn><mrow><mo>−</mo><mn>0.13</mn></mrow><mrow><mo>+</mo><mn>0.11</mn></mrow></msubsup></mrow></math></span>, and <span><math><mrow><mi>γ</mi><mo>=</mo><mo>−</mo><mn>1.8</mn><mo>×</mo><msup><mn>10</mn><mn>4</mn></msup><mo>±</mo><mn>1.0</mn></mrow></math></span>, with a goodness of fit comparable to ΛCDM (<span><math><mrow><msubsup><mi>χ</mi><mrow","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102231"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077976","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-01DOI: 10.1016/j.dark.2026.102234
Fathima Shifa M․ , Shantanu Desai
We implement a search for spatial coincidence between high energy neutrinos detected by the IceCube neutrino detector (using the publicly available 10-year muon track data) and 37 magnetars, including six extragalactic sources. We use the unbinned maximum likelihood method for our analysis. We do not find any such spatial association between any of the known magnetars and IceCube-detected neutrinos. Therefore, we conclude that none of the known galactic or extragalactic magnetars contribute to the diffuse neutrino flux observed in IceCube. A stacked analysis also does not show a statistically significant excess.
{"title":"Search for spatial coincidence between magnetars and IceCube detected neutrinos","authors":"Fathima Shifa M․ , Shantanu Desai","doi":"10.1016/j.dark.2026.102234","DOIUrl":"10.1016/j.dark.2026.102234","url":null,"abstract":"<div><div>We implement a search for spatial coincidence between high energy neutrinos detected by the IceCube neutrino detector (using the publicly available 10-year muon track data) and 37 magnetars, including six extragalactic sources. We use the unbinned maximum likelihood method for our analysis. We do not find any such spatial association between any of the known magnetars and IceCube-detected neutrinos. Therefore, we conclude that none of the known galactic or extragalactic magnetars contribute to the diffuse neutrino flux observed in IceCube. A stacked analysis also does not show a statistically significant excess.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102234"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077973","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this work, we investigate a predictive class of neutrino mass matrices characterized by one texture zero and one vanishing sub-trace within the framework of the scotogenic model, wherein neutrino masses, dark matter, and neutrinoless double beta decay are intrinsically correlated. We analyze twelve viable texture structures—namely B1,4,5, , D4,5, and F5,6—and examine their implications for the effective Majorana mass (|Mee|) governing neutrinoless double beta decay (0νββ). Remarkably, all non-zero entries of the neutrino mass matrix can be parametrized in terms of this effective Majorana mass, establishing a direct theoretical link between low-energy observables and high-scale parameters of the model. Among the twelve textures, eleven predict dark matter masses of order TeV and yield correlated bounds on |Mee|—making them testable in current and forthcoming 0νββ experiments—while the textures D4 and F5,6 exhibit comparatively weaker correlations. In contrast, the texture C5 is excluded due to its requirement of unrealistically large Yukawa couplings and its inability to realize dark matter in the TeV regime. Our analysis thus identifies a subset of predictive neutrino mass textures that consistently relate dark matter phenomenology and neutrinoless double beta decay observables within the scotogenic paradigm.
{"title":"Predictive one-zero with vanishing sub-trace texture in neutrino mass matrix in light of dark matter and neutrinoless double beta decay","authors":"Ankush Choudhary , Sangeeta Dey , Rishu Verma , Manoj Kumar , B.C. Chauhan , Mahadev Patgiri","doi":"10.1016/j.dark.2026.102228","DOIUrl":"10.1016/j.dark.2026.102228","url":null,"abstract":"<div><div>In this work, we investigate a predictive class of neutrino mass matrices characterized by one texture zero and one vanishing sub-trace within the framework of the scotogenic model, wherein neutrino masses, dark matter, and neutrinoless double beta decay are intrinsically correlated. We analyze twelve viable texture structures—namely <em>B</em><sub>1,4,5</sub>, <span><math><msub><mi>C</mi><mrow><mn>1</mn><mo>,</mo><mn>2</mn><mo>,</mo><mo>…</mo><mo>,</mo><mn>5</mn></mrow></msub></math></span>, <em>D</em><sub>4,5</sub>, and <em>F</em><sub>5,6</sub>—and examine their implications for the effective Majorana mass (|<em>M<sub>ee</sub></em>|) governing neutrinoless double beta decay (0<em>νββ</em>). Remarkably, all non-zero entries of the neutrino mass matrix can be parametrized in terms of this effective Majorana mass, establishing a direct theoretical link between low-energy observables and high-scale parameters of the model. Among the twelve textures, eleven predict dark matter masses of order TeV and yield correlated bounds on |<em>M<sub>ee</sub></em>|—making them testable in current and forthcoming 0<em>νββ</em> experiments—while the textures <em>D</em><sub>4</sub> and <em>F</em><sub>5,6</sub> exhibit comparatively weaker correlations. In contrast, the texture <em>C</em><sub>5</sub> is excluded due to its requirement of unrealistically large Yukawa couplings and its inability to realize dark matter in the TeV regime. Our analysis thus identifies a subset of predictive neutrino mass textures that consistently relate dark matter phenomenology and neutrinoless double beta decay observables within the scotogenic paradigm.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102228"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077977","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-02-01DOI: 10.1016/j.dark.2026.102236
S.D. Odintsov , V.K. Oikonomou
It is known that if the standard slow-roll inflation is followed by a power-law inflationary regime, then the trans-Planckian modes may be safely be contained in the Hubble horizon and never exit it during inflation. In this work we investigate how to realize a smooth transition between a slow-roll and a power-law inflationary regime in the context of single scalar field inflation. As we show it is possible to realize such a smooth transition by generalizing the kinetic energy of single scalar field in the form , where β(ϕ) is some appropriate function of the scalar field. Using two distinct approaches we show that it is possible to realize a smooth transition from a slow-roll to a power-law inflationary regime, and the two approaches produce identical results regarding the slow-roll regime. Also we show that the slow-roll regime is quite short, about N ∼ 30 e-foldings, with the flatness and horizon problems being solved with the synergistic effect of the two inflationary patches. The slow-roll era is found to be compatible with the Atacama Cosmology Telescope data.
{"title":"A remedy of the trans-Planckian censorship problem with smooth slow-roll to power-law inflation transitions in scalar field theory","authors":"S.D. Odintsov , V.K. Oikonomou","doi":"10.1016/j.dark.2026.102236","DOIUrl":"10.1016/j.dark.2026.102236","url":null,"abstract":"<div><div>It is known that if the standard slow-roll inflation is followed by a power-law inflationary regime, then the trans-Planckian modes may be safely be contained in the Hubble horizon and never exit it during inflation. In this work we investigate how to realize a smooth transition between a slow-roll and a power-law inflationary regime in the context of single scalar field inflation. As we show it is possible to realize such a smooth transition by generalizing the kinetic energy of single scalar field in the form <span><math><mrow><msup><mover><mi>ϕ</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>=</mo><mi>β</mi><mrow><mo>(</mo><mi>ϕ</mi><mo>)</mo></mrow><mi>V</mi><mrow><mo>(</mo><mi>ϕ</mi><mo>)</mo></mrow></mrow></math></span>, where <em>β</em>(<em>ϕ</em>) is some appropriate function of the scalar field. Using two distinct approaches we show that it is possible to realize a smooth transition from a slow-roll to a power-law inflationary regime, and the two approaches produce identical results regarding the slow-roll regime. Also we show that the slow-roll regime is quite short, about <em>N</em> ∼ 30 <em>e</em>-foldings, with the flatness and horizon problems being solved with the synergistic effect of the two inflationary patches. The slow-roll era is found to be compatible with the Atacama Cosmology Telescope data.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102236"},"PeriodicalIF":6.4,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077974","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}