Pub Date : 2026-01-16DOI: 10.1016/j.dark.2026.102225
Yu-Xiang Huang , Sen Guo , En-Wei Liang , Kai Lin
Understanding how dark matter affects the immediate environment of black holes (BHs) is crucial for interpreting horizon-scale observations. We study rotating BHs surrounded by perfect fluid dark matter (PFDM), exploring their observable features through both analytical and numerical approaches. Using the existence criterion of the innermost stable circular orbit (ISCO), we first derive joint constraints on the PFDM intensity parameter k and the spin parameter a. Within the resulting physically allowed parameter regime, we perform high-resolution, general-relativistic ray-tracing simulations of thin accretion disks at 87 GHz and 230 GHz, capturing the detailed brightness morphology and photon ring structure shaped by PFDM. By incorporating angular diameter measurements of M87* and Sgr A* from the Event Horizon Telescope (EHT), we further narrow down the viable parameter space and directly compare synthetic images with EHT observations of M87*. We find that the inclusion of PFDM improves the agreement with the observed compact shadow and asymmetric brightness distribution, suggesting that dark matter may leave observable imprints on horizon-scale images. Our results position PFDM as a physically motivated extension to the Kerr geometry and highlight a promising astrophysical pathway for probing dark matter near BHs with current and future VLBI campaigns.
{"title":"Impact of perfect fluid dark matter on the appearance of rotating black hole","authors":"Yu-Xiang Huang , Sen Guo , En-Wei Liang , Kai Lin","doi":"10.1016/j.dark.2026.102225","DOIUrl":"10.1016/j.dark.2026.102225","url":null,"abstract":"<div><div>Understanding how dark matter affects the immediate environment of black holes (BHs) is crucial for interpreting horizon-scale observations. We study rotating BHs surrounded by perfect fluid dark matter (PFDM), exploring their observable features through both analytical and numerical approaches. Using the existence criterion of the innermost stable circular orbit (ISCO), we first derive joint constraints on the PFDM intensity parameter <em>k</em> and the spin parameter <em>a</em>. Within the resulting physically allowed parameter regime, we perform high-resolution, general-relativistic ray-tracing simulations of thin accretion disks at 87 GHz and 230 GHz, capturing the detailed brightness morphology and photon ring structure shaped by PFDM. By incorporating angular diameter measurements of M87* and Sgr A* from the Event Horizon Telescope (EHT), we further narrow down the viable parameter space and directly compare synthetic images with EHT observations of M87*. We find that the inclusion of PFDM improves the agreement with the observed compact shadow and asymmetric brightness distribution, suggesting that dark matter may leave observable imprints on horizon-scale images. Our results position PFDM as a physically motivated extension to the Kerr geometry and highlight a promising astrophysical pathway for probing dark matter near BHs with current and future VLBI campaigns.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102225"},"PeriodicalIF":6.4,"publicationDate":"2026-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022830","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 : 2026-01-16DOI: 10.1016/j.dark.2026.102224
Wei Yang , Yu-Xuan Kang , Arshad Ali , Tao-Tao Sui , Chen-Hao Wu , Ya-Peng Hu
Scalar perturbations in the inflation can be amplified when the base inflation potential Vb(ϕ) incorporates a local bump f(ϕ) such as . This modification will lead to a peak in the curvature power spectrum, increasing a significant abundance of primordial black holes (PBHs). However, since there is no underlying physical reason for the choice of f(ϕ), it is essential to investigate the effects of various bump functions on PBH generation. In this paper, we choose the well-known Starobinsky potential as the base inflation potential to compare the effects produced by different bumps, specifically focusing on the Lorentz and Gaussian bumps which are widely used. To clearly illustrate the differences between these two bumps, we keep parameters in bump functions the same. We find an interesting and novel result that the Lorentz cases manifest a stronger ability to enhance the power spectrum and produce more abundance of PBHs than Gaussian cases. Moreover, we also investigate the different effects of bump functions on the scalar-induced gravitational waves (SIGWs). The results indicate that the Lorentz bump generates SIGWs with a higher energy density, which can be potentially detected in the future. Our study gives valuable insights into the choice and constraints on the bump functions, and the different effects may distinguish the two bump cases for practical purposes in future experiments.
{"title":"Different effects of the Lorentz and Gaussian bump functions on the formation of primordial black holes and secondary gravitational waves","authors":"Wei Yang , Yu-Xuan Kang , Arshad Ali , Tao-Tao Sui , Chen-Hao Wu , Ya-Peng Hu","doi":"10.1016/j.dark.2026.102224","DOIUrl":"10.1016/j.dark.2026.102224","url":null,"abstract":"<div><div>Scalar perturbations in the inflation can be amplified when the base inflation potential <em>V<sub>b</sub></em>(<em>ϕ</em>) incorporates a local bump <em>f</em>(<em>ϕ</em>) such as <span><math><mrow><mi>V</mi><mrow><mo>(</mo><mi>ϕ</mi><mo>)</mo></mrow><mo>=</mo><msub><mi>V</mi><mi>b</mi></msub><mrow><mo>(</mo><mi>ϕ</mi><mo>)</mo></mrow><mrow><mo>(</mo><mn>1</mn><mo>+</mo><mi>f</mi><mrow><mo>(</mo><mi>ϕ</mi><mo>)</mo></mrow><mo>)</mo></mrow></mrow></math></span>. This modification will lead to a peak in the curvature power spectrum, increasing a significant abundance of primordial black holes (PBHs). However, since there is no underlying physical reason for the choice of <em>f</em>(<em>ϕ</em>), it is essential to investigate the effects of various bump functions on PBH generation. In this paper, we choose the well-known Starobinsky potential as the base inflation potential to compare the effects produced by different bumps, specifically focusing on the Lorentz and Gaussian bumps which are widely used. To clearly illustrate the differences between these two bumps, we keep parameters in bump functions the same. We find an interesting and novel result that the Lorentz cases manifest a stronger ability to enhance the power spectrum and produce more abundance of PBHs than Gaussian cases. Moreover, we also investigate the different effects of bump functions on the scalar-induced gravitational waves (SIGWs). The results indicate that the Lorentz bump generates SIGWs with a higher energy density, which can be potentially detected in the future. Our study gives valuable insights into the choice and constraints on the bump functions, and the different effects may distinguish the two bump cases for practical purposes in future experiments.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102224"},"PeriodicalIF":6.4,"publicationDate":"2026-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022831","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 : 2026-01-16DOI: 10.1016/j.dark.2026.102223
Vishnu S Namboothiri , Krishna P․B․ , Adithya P․S․ , Titus K Mathew
Taking account of the thermal nature of the Hubble horizon of the expanding universe, we analysed the evolution of relative fluctuations of horizon energy. For this analysis, we used two approaches: (i) by treating the Hubble horizon as a system in canonical ensemble, and (ii) by considering the microscopic degrees of freedom on the horizon. In both approaches, we obtained the relative fluctuations by using two different definitions of the horizon temperature; first, the Gibbons-Hawking temperature, and second, the Kodama-Hayward temperature. For a given temperature, both approaches yield the same general evolution for the fluctuations. In the asymptotic limit, the relative energy fluctuations corresponding to the Gibbons-Hawking temperature, is [ℏG/2π]H2, and 2/Nsur for the first and second approaches respectively. Similarly, using the Kodama-Hayward temperature, the asymptotic fluctuations are [5ℏG/2π]H2, and 10/Nsur. This implies that, the magnitude of the relative fluctuations of the horizon energy is higher in the case of Kodama-Hayward temperature. The inverse dependence of the fluctuation on Nsur, the number of degrees of freedom on the horizon, reflects a familiar behaviour in ordinary thermal systems: fluctuations decrease as the number of degrees of freedom increases. Notably, we also found that the relative energy fluctuations establish a connection between the Planck length scale Lp, characteristic length scale of the very early epoch of the universe, and the length scale associated with the late-time accelerated phase. This relationship can offer valuable insights that could help in addressing the cosmological constant problem.
{"title":"Evolution of fluctuations in horizon energy and its dependence on the degrees of freedom","authors":"Vishnu S Namboothiri , Krishna P․B․ , Adithya P․S․ , Titus K Mathew","doi":"10.1016/j.dark.2026.102223","DOIUrl":"10.1016/j.dark.2026.102223","url":null,"abstract":"<div><div>Taking account of the thermal nature of the Hubble horizon of the expanding universe, we analysed the evolution of relative fluctuations of horizon energy. For this analysis, we used two approaches: (i) by treating the Hubble horizon as a system in canonical ensemble, and (ii) by considering the microscopic degrees of freedom on the horizon. In both approaches, we obtained the relative fluctuations by using two different definitions of the horizon temperature; first, the Gibbons-Hawking temperature, and second, the Kodama-Hayward temperature. For a given temperature, both approaches yield the same general evolution for the fluctuations. In the asymptotic limit, the relative energy fluctuations corresponding to the Gibbons-Hawking temperature, is [ℏ<em>G</em>/2<em>π</em>]<em>H</em><sup>2</sup>, and 2/<em>N<sub>sur</sub></em> for the first and second approaches respectively. Similarly, using the Kodama-Hayward temperature, the asymptotic fluctuations are [5ℏ<em>G</em>/2<em>π</em>]<em>H</em><sup>2</sup>, and 10/<em>N<sub>sur</sub></em>. This implies that, the magnitude of the relative fluctuations of the horizon energy is higher in the case of Kodama-Hayward temperature. The inverse dependence of the fluctuation on <em>N<sub>sur</sub></em>, the number of degrees of freedom on the horizon, reflects a familiar behaviour in ordinary thermal systems: fluctuations decrease as the number of degrees of freedom increases. Notably, we also found that the relative energy fluctuations establish a connection between the Planck length scale <em>L<sub>p</sub></em>, characteristic length scale of the very early epoch of the universe, and <span><math><mrow><msqrt><mrow><mn>3</mn><mo>/</mo><mstyle><mi>Λ</mi></mstyle></mrow></msqrt><mo>,</mo></mrow></math></span> the length scale associated with the late-time accelerated phase. This relationship can offer valuable insights that could help in addressing the cosmological constant problem.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102223"},"PeriodicalIF":6.4,"publicationDate":"2026-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022825","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 : 2026-01-16DOI: 10.1016/j.dark.2026.102226
Agripino Sousa-Neto , Maria Aldinêz Dantas , Javier E. González , Joel C. Carvalho , Jailson Alcaniz
The Universe consists of a variety of objects that formed at different epochs, leading to variations in the formation time which represents the time elapsed from the onset of structure formation until the formation of a particular object. In this work, we present two approaches to reconstruct and constrain the galaxy formation time tf(z) using non-parametric reconstruction methods, such as Gaussian Processes (GP) and High-performance Symbolic Regression (SR). Our analysis uses age estimates of 32 old passive galaxies and the Pantheon+ type Ia supernova sample, and considers two different values of the Hubble constant H0 from the SH0ES and Planck Collaborations. When adopting the ΛCDM model and the GP reconstructions, A direct comparison of the reconstructions shows that the GP-based implementations are mutually consistent across the redshift range considered. The SR reconstructions also show good agreement with the GP results and exhibit a compatible redshift evolution of tf(z), with full agreement at intermediate and high redshifts and only a mild deviation at very low redshifts. The results also show significant differences in the formation time from SH0ES and Planck values, highlighting the impact of the H0 tension on the cosmological estimates of tf(z). Overall, this study suggests that galaxies have different evolutionary timescales and that tf is not constant, with noticeable variations at lower redshifts (z ≲ 0.5).
{"title":"Exploring cosmological constraints on galaxy formation time","authors":"Agripino Sousa-Neto , Maria Aldinêz Dantas , Javier E. González , Joel C. Carvalho , Jailson Alcaniz","doi":"10.1016/j.dark.2026.102226","DOIUrl":"10.1016/j.dark.2026.102226","url":null,"abstract":"<div><div>The Universe consists of a variety of objects that formed at different epochs, leading to variations in the formation time which represents the time elapsed from the onset of structure formation until the formation of a particular object. In this work, we present two approaches to reconstruct and constrain the galaxy formation time <em>t<sub>f</sub></em>(<em>z</em>) using non-parametric reconstruction methods, such as Gaussian Processes (GP) and High-performance Symbolic Regression (SR). Our analysis uses age estimates of 32 old passive galaxies and the Pantheon+ type Ia supernova sample, and considers two different values of the Hubble constant <em>H</em><sub>0</sub> from the SH0ES and Planck Collaborations. When adopting the ΛCDM model and the GP reconstructions, A direct comparison of the reconstructions shows that the GP-based implementations are mutually consistent across the redshift range considered. The SR reconstructions also show good agreement with the GP results and exhibit a compatible redshift evolution of <em>t<sub>f</sub></em>(<em>z</em>), with full agreement at intermediate and high redshifts and only a mild deviation at very low redshifts. The results also show significant differences in the formation time from SH0ES and Planck values, highlighting the impact of the <em>H</em><sub>0</sub> tension on the cosmological estimates of <em>t<sub>f</sub></em>(<em>z</em>). Overall, this study suggests that galaxies have different evolutionary timescales and that <em>t<sub>f</sub></em> is not constant, with noticeable variations at lower redshifts (<em>z</em> ≲ 0.5).</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102226"},"PeriodicalIF":6.4,"publicationDate":"2026-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022826","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 : 2026-01-14DOI: 10.1016/j.dark.2026.102217
Heng-Sen Jiao , Hong-Bo Jin , Yun-Long Zhang
We investigate a framework for extracting parameters of stochastic gravitational wave background (SGWB) with peak-like templates in the millihertz frequency band, and we analyze transient contamination effects on parameter reconstruction. We present the spectrum and spectrogram under different conditions and provide the results of parameter reconstruction. Using templates from the early universe, we demonstrate that the peak-like templates outperform the broken power law (BPL) templates in power-law exponents recovery and peak frequency localization. The reconstruction results obtained using data from Fast Fourier Transform (FFT) are better than those obtained using data from Short-Time Fourier Transform (STFT) which is based on the spectrogram. For the single-peak(SP) template, the estimation accuracy of the exponent and peak frequency surpasses that of the BPL template by an order of magnitude, but it demonstrates less precision in amplitude estimation compared to the BPL template. Regarding the double-peak template, parameter estimation results derived from the FFT methodology consistently outperform those obtained using STFT. Nevertheless, transient signals exhibit a detrimental impact on parameter estimation precision, causing errors to increase by an order of magnitude, particularly in multi-peak scenarios. This framework provides an example of using templates to analyze data from space-based gravitational wave detectors.
{"title":"Parameter extraction of the stochastic gravitational wave background with peak-like templates in millihertz","authors":"Heng-Sen Jiao , Hong-Bo Jin , Yun-Long Zhang","doi":"10.1016/j.dark.2026.102217","DOIUrl":"10.1016/j.dark.2026.102217","url":null,"abstract":"<div><div>We investigate a framework for extracting parameters of stochastic gravitational wave background (SGWB) with peak-like templates in the millihertz frequency band, and we analyze transient contamination effects on parameter reconstruction. We present the spectrum and spectrogram under different conditions and provide the results of parameter reconstruction. Using templates from the early universe, we demonstrate that the peak-like templates outperform the broken power law (BPL) templates in power-law exponents recovery and peak frequency localization. The reconstruction results obtained using data from Fast Fourier Transform (FFT) are better than those obtained using data from Short-Time Fourier Transform (STFT) which is based on the spectrogram. For the single-peak(SP) template, the estimation accuracy of the exponent and peak frequency surpasses that of the BPL template by an order of magnitude, but it demonstrates less precision in amplitude estimation compared to the BPL template. Regarding the double-peak template, parameter estimation results derived from the FFT methodology consistently outperform those obtained using STFT. Nevertheless, transient signals exhibit a detrimental impact on parameter estimation precision, causing errors to increase by an order of magnitude, particularly in multi-peak scenarios. This framework provides an example of using templates to analyze data from space-based gravitational wave detectors.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102217"},"PeriodicalIF":6.4,"publicationDate":"2026-01-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022827","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 : 2026-01-14DOI: 10.1016/j.dark.2026.102214
K. El Bourakadi , M. Yu Khlopov , M. Krasnov , H. Chakir , M. Bennai
We explore how inflationary features shape the early stages of cosmic structure formation. Using the transfer function formalism, we trace the evolution of primordial perturbations, showing how causal physics and oscillatory signatures from inflation influence the matter power spectrum. The variance of smoothed density fields is then applied to model the collapse of overdense regions and predict dark matter halo abundances through the Press–Schechter framework. Extending to the baryonic sector, we analyze primordial gas collapse in minihalos, emphasizing molecular hydrogen cooling and the thermochemical pathways leading to Population III star formation. Finally, we examine primordial black holes as potential seeds for early galaxies, connecting their accretion-driven growth to the stellar masses and disk properties of high-redshift systems. Our results indicate that oscillatory features from inflation can leave measurable imprints on halo abundances and early galaxy properties, providing a testable link between high-energy physics and astrophysical observations with JWST.
{"title":"Tracing inflationary imprints through the dark ages: Implications for early stars and galaxies formation","authors":"K. El Bourakadi , M. Yu Khlopov , M. Krasnov , H. Chakir , M. Bennai","doi":"10.1016/j.dark.2026.102214","DOIUrl":"10.1016/j.dark.2026.102214","url":null,"abstract":"<div><div>We explore how inflationary features shape the early stages of cosmic structure formation. Using the transfer function formalism, we trace the evolution of primordial perturbations, showing how causal physics and oscillatory signatures from inflation influence the matter power spectrum. The variance of smoothed density fields is then applied to model the collapse of overdense regions and predict dark matter halo abundances through the Press–Schechter framework. Extending to the baryonic sector, we analyze primordial gas collapse in minihalos, emphasizing molecular hydrogen cooling and the thermochemical pathways leading to Population III star formation. Finally, we examine primordial black holes as potential seeds for early galaxies, connecting their accretion-driven growth to the stellar masses and disk properties of high-redshift systems. Our results indicate that oscillatory features from inflation can leave measurable imprints on halo abundances and early galaxy properties, providing a testable link between high-energy physics and astrophysical observations with JWST.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102214"},"PeriodicalIF":6.4,"publicationDate":"2026-01-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022822","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 : 2026-01-12DOI: 10.1016/j.dark.2026.102219
Mohammad Alshammari , M. Rizwan , Othman Abdullah Almatroud , M.Z. Bhatti , Saleh Alshammari , Z. Yousaf
In this paper, we construct and examine a new type of static, spherically symmetric wormhole geometries within the context of the minimal geometric deformation (MGD) formalism of gravitational decoupling. The seed solution is warped through an auxiliary source, with its temporal component described by holographic dark energy, thus including a phenomenologically driven dark sector. We study the resulting spacetime using several diagnostic tools: the embedding diagram is used to plot the wormhole throat and flare–out structure; the mass function is calculated to examine gravitational energy distribution; the volume integral quantifier is evaluated to determine the total amount of exotic matter needed; and the exoticity parameter is examined to describe the violation of energy conditions. Additionally, the singularity structure is analyzed to validate the regularity of spacetime, while the anisotropy factor is investigated to analyze pressure distributions between tangential and radial directions. Total effective energy–momentum tensor conservation equation is considered with emphasis on the interaction between the seed geometry and the θ-sector. Last, we analyze complexity factors to determine matter–energy content structural organization. We find that the addition of holographic dark energy in the time component of the θ-sector permits traversable, asymptotically flat wormhole solutions with regulated exotic matter and smooth geometric structures.
{"title":"Imprints of holographic dark energy and minimally deformed wormholes in general relativity","authors":"Mohammad Alshammari , M. Rizwan , Othman Abdullah Almatroud , M.Z. Bhatti , Saleh Alshammari , Z. Yousaf","doi":"10.1016/j.dark.2026.102219","DOIUrl":"10.1016/j.dark.2026.102219","url":null,"abstract":"<div><div>In this paper, we construct and examine a new type of static, spherically symmetric wormhole geometries within the context of the minimal geometric deformation (MGD) formalism of gravitational decoupling. The seed solution is warped through an auxiliary source, <span><math><msub><mover><mi>T</mi><mi>θ</mi></mover><mrow><mi>κ</mi><mi>μ</mi></mrow></msub></math></span> with its temporal component described by holographic dark energy, thus including a phenomenologically driven dark sector. We study the resulting spacetime using several diagnostic tools: the embedding diagram is used to plot the wormhole throat and flare–out structure; the mass function is calculated to examine gravitational energy distribution; the volume integral quantifier is evaluated to determine the total amount of exotic matter needed; and the exoticity parameter is examined to describe the violation of energy conditions. Additionally, the singularity structure is analyzed to validate the regularity of spacetime, while the anisotropy factor is investigated to analyze pressure distributions between tangential and radial directions. Total effective energy–momentum tensor conservation equation is considered with emphasis on the interaction between the seed geometry and the <em>θ</em>-sector. Last, we analyze complexity factors to determine matter–energy content structural organization. We find that the addition of holographic dark energy in the time component of the <em>θ</em>-sector permits traversable, asymptotically flat wormhole solutions with regulated exotic matter and smooth geometric structures.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102219"},"PeriodicalIF":6.4,"publicationDate":"2026-01-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145977316","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 study, we test the dynamics of test particles around static and spherically symmetric BHs arising in the Einstein SU(N) non-linear sigma model. By showing the influence of general relativity and the metric function topologically in the SU(N) group, the spacetime is illustrated as dependent on the internal symmetry parameter α, significantly modifying the BH geometry. In addition, we derive analytical expressions for the energy and angular momentum of circular equatorial orbits and investigate the behavior of the effective potential to determine the orbital stability. The innermost stable circular orbits (ISCOs) are computed and their sensitivity to variations in α and the cosmological constant Λ is analyzed. In addition, we calculate the effective radial force acting on the particles and show how the parameters SU(N) influence its attractive or repulsive nature. By perturbing the stable circular orbits, we derive the radial, vertical, and orbital epicyclic frequencies for both local and distant observers. In this case, our results show that the internal gauge structure inherent in the SU(N) model has a pronounced effect on the orbital dynamics and oscillatory behavior of test particles, offering potential observational signatures in strong-field astrophysics.
{"title":"Particle motion and epicyclic frequencies in the einstein special unitary matrices sigma model of black holes","authors":"Abdelmalek Bouzenada , Imtiaz Khan , Asifa Ashraf , Emre Demir , Ertan Gudekli , Ikhtiyor Saidov , Farruh Atamurotov","doi":"10.1016/j.dark.2026.102216","DOIUrl":"10.1016/j.dark.2026.102216","url":null,"abstract":"<div><div>In this study, we test the dynamics of test particles around static and spherically symmetric BHs arising in the Einstein <em>SU</em>(<em>N</em>) non-linear sigma model. By showing the influence of general relativity and the metric function topologically in the <em>SU</em>(<em>N</em>) group, the spacetime is illustrated as dependent on the internal symmetry parameter <em>α</em>, significantly modifying the BH geometry. In addition, we derive analytical expressions for the energy and angular momentum of circular equatorial orbits and investigate the behavior of the effective potential to determine the orbital stability. The innermost stable circular orbits (ISCOs) are computed and their sensitivity to variations in <em>α</em> and the cosmological constant Λ is analyzed. In addition, we calculate the effective radial force acting on the particles and show how the parameters <em>SU</em>(<em>N</em>) influence its attractive or repulsive nature. By perturbing the stable circular orbits, we derive the radial, vertical, and orbital epicyclic frequencies for both local and distant observers. In this case, our results show that the internal gauge structure inherent in the <em>SU</em>(<em>N</em>) model has a pronounced effect on the orbital dynamics and oscillatory behavior of test particles, offering potential observational signatures in strong-field astrophysics.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102216"},"PeriodicalIF":6.4,"publicationDate":"2026-01-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022824","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 : 2026-01-09DOI: 10.1016/j.dark.2026.102211
Abdul Malik Sultan , Abdul Jawad , Hamood Ur Rehman , N. Myrzakulov , Sanjar Shaymatov
In this article, we investigate the gravitational baryogenesis mechanism in the framework of Extended Proca-Nuevo gravity, a theory where a massive vector field is non-minimally coupled to the curvature. This analysis is carried out for an early universe, encompassing three separate cosmological scenarios defined by power-law, exponential, and modified exponential scale factors. By deriving the modified field equations from the EPN action, we obtain precise solutions for each scale factor, including the influence of the vector field. We compute the baryon-to-entropy ratio using the gravitational baryogenesis formalism, where the baryon asymmetry arises from a dynamical coupling of the baryon current with the derivative of the Ricci scalar. Moreover, we discuss the stability of the assumed cosmological model in two different ways, the dynamical system analysis and squared speed of sound parameter. Our findings demonstrate that the baryon-to-entropy ratio is consistent with observational constraints in all scenarios, highlighting the potential of EPN gravity as a viable theory to explain the matter-antimatter asymmetry in the early universe. Moreover, stability analysis through dynamical system leads to a deSitter stability which is a trivial case while squared speed of sound gives that system is stable for all three scale factor models. The study further stresses the contribution of anisotropy and vector field dynamics to the cosmological evolution within modified gravity models.
{"title":"Feasible regions of GB phenomenon in extended Proca-Nuevo gravity","authors":"Abdul Malik Sultan , Abdul Jawad , Hamood Ur Rehman , N. Myrzakulov , Sanjar Shaymatov","doi":"10.1016/j.dark.2026.102211","DOIUrl":"10.1016/j.dark.2026.102211","url":null,"abstract":"<div><div>In this article, we investigate the gravitational baryogenesis mechanism in the framework of Extended Proca-Nuevo gravity, a theory where a massive vector field is non-minimally coupled to the curvature. This analysis is carried out for an early universe, encompassing three separate cosmological scenarios defined by power-law, exponential, and modified exponential scale factors. By deriving the modified field equations from the EPN action, we obtain precise solutions for each scale factor, including the influence of the vector field. We compute the baryon-to-entropy ratio using the gravitational baryogenesis formalism, where the baryon asymmetry arises from a dynamical coupling of the baryon current with the derivative of the Ricci scalar. Moreover, we discuss the stability of the assumed cosmological model in two different ways, the dynamical system analysis and squared speed of sound parameter. Our findings demonstrate that the baryon-to-entropy ratio is consistent with observational constraints in all scenarios, highlighting the potential of EPN gravity as a viable theory to explain the matter-antimatter asymmetry in the early universe. Moreover, stability analysis through dynamical system leads to a deSitter stability which is a trivial case while squared speed of sound gives that system is stable for all three scale factor models. The study further stresses the contribution of anisotropy and vector field dynamics to the cosmological evolution within modified gravity models.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102211"},"PeriodicalIF":6.4,"publicationDate":"2026-01-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146022828","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 : 2026-01-08DOI: 10.1016/j.dark.2026.102213
Taishi Katsuragawa , Shin’ichi Nojiri , Sergei D. Odintsov
We study wormhole geometries embedded in an expanding universe within a four-scalar non-linear σ model, where the target-space metric is identified with the spacetime Ricci tensor. In this framework, wormholes can remain stable even when conventional energy conditions are violated. However, once cosmological expansion is included, the effective energy density and pressure are modified by the cosmological fluid, enabling the energy conditions to be satisfied. We further present intriguing geometries in which a finite future singularity appears in our universe but not in another universe connected by the wormhole. Near the throat, the hypersurface becomes timelike, allowing trajectories to traverse to the other universe before the singularity and return afterwards. We also construct wormhole solutions motivated by galactic dark-matter halo profiles, where the required non-vanishing pressure arises naturally from the four-scalar non-linear σ model.
{"title":"Wormhole spacetimes in an expanding universe: Energy conditions and future singularities","authors":"Taishi Katsuragawa , Shin’ichi Nojiri , Sergei D. Odintsov","doi":"10.1016/j.dark.2026.102213","DOIUrl":"10.1016/j.dark.2026.102213","url":null,"abstract":"<div><div>We study wormhole geometries embedded in an expanding universe within a four-scalar non-linear <em>σ</em> model, where the target-space metric is identified with the spacetime Ricci tensor. In this framework, wormholes can remain stable even when conventional energy conditions are violated. However, once cosmological expansion is included, the effective energy density and pressure are modified by the cosmological fluid, enabling the energy conditions to be satisfied. We further present intriguing geometries in which a finite future singularity appears in our universe but not in another universe connected by the wormhole. Near the throat, the hypersurface becomes timelike, allowing trajectories to traverse to the other universe before the singularity and return afterwards. We also construct wormhole solutions motivated by galactic dark-matter halo profiles, where the required non-vanishing pressure arises naturally from the four-scalar non-linear <em>σ</em> model.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"51 ","pages":"Article 102213"},"PeriodicalIF":6.4,"publicationDate":"2026-01-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145977318","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}