Xiangdong Zhang
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
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Research Interests
Xiangdong Zhang has a total of 58 co-authors. Here are the top co-authors by number of shared publications:
Yunlong Liu
Kunming University of Science and Technology
15 shared publications- Yongge Ma
Beijing Normal University
14 shared publications - Cong Zhang
Beijing Normal University
10 shared publications - Gaoping Long
Jinan University
7 shared publications - Haida Li
South China University of Technology
6 shared publications - Moisés Bravo-Gaete
Universidad Católica del Maule
6 shared publications
Latest Publications
- Open Access
- 11 November 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (11)
Critical collapse of a self-interacting scalar field in asymptotically anti-de Sitter spacetime
We study the critical gravitational collapse of a spherically symmetric scalar field in asymptotically anti-de Sitter (AdS) spacetime. The scalar field potential adopted here is inversely proportional to the square of the AdS curvature radius $$\ell $$ , and the system admits a well-known exact static solution [1]. Working in polar coordinates, we first confirm that type II critical collapse occurs for a range of distinct initial configurations when $$\ell =8$$ , where the measured echoing period and critical exponent are in excellent agreement with Choptuik’s classic results. We then fine-tune the initial amplitude of the scalar field for a series of AdS radii $$\ell $$ , performing calculations in both polar coordinates and double null coordinates to cross-validate our results. We find that the form of the potential does not alter the critical behavior of gravitational collapse in any meaningful way: in particular, both the echoing period ( $$\Delta \approx 3.4$$ ) and critical exponent ( $$\gamma \approx 0.37$$ ) remain essentially unchanged across all tested values of $$\ell $$ . We also analyze the evolution equation near the center during critical collapse, find that the cosmological term and scalar field potential term are negligible, and conclude that the spacetime near the center is approximately conformally flat.- 11 November 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (11)
Open AccessCritical collapse of a self-interacting scalar field in asymptotically anti-de Sitter spacetime
We study the critical gravitational collapse of a spherically symmetric scalar field in asymptotically anti-de Sitter (AdS) spacetime. The scalar field potential adopted here is inversely proportional to the square of the AdS curvature radius $$\ell $$ , and the system admits a well-known exact static solution [1]. Working in polar coordinates, we first confirm that type II critical collapse occurs for a range of distinct initial configurations when $$\ell =8$$ , where the measured echoing period and critical exponent are in excellent agreement with Choptuik’s classic results. We then fine-tune the initial amplitude of the scalar field for a series of AdS radii $$\ell $$ , performing calculations in both polar coordinates and double null coordinates to cross-validate our results. We find that the form of the potential does not alter the critical behavior of gravitational collapse in any meaningful way: in particular, both the echoing period ( $$\Delta \approx 3.4$$ ) and critical exponent ( $$\gamma \approx 0.37$$ ) remain essentially unchanged across all tested values of $$\ell $$ . We also analyze the evolution equation near the center during critical collapse, find that the cosmological term and scalar field potential term are negligible, and conclude that the spacetime near the center is approximately conformally flat. - Open Access
- 5 November 2026
- Published by IOP Publishing in Classical and Quantum Gravity
Periodic orbits and gravitational waveforms of spinning particles in nonlocal Gravity
In this paper, we investigate the dynamics and gravitational-wave signatures of periodic orbits of spinning test particles moving in the equatorial plane around static, spherically symmetric black holes within the framework of Deser-Woodard nonlocal gravity. Based on the Mathisson-Papapetrou-Dixon equations, combined with the Tulczyjew spin supplementary condition, we derive the orbital dynamic equations for spinning particles moving in the equatorial plane and impose a timelike constraint to exclude unphysical superluminal trajectories. By comparing with the classical Schwarzschild black hole, we systematically analyze the effects of the nonlocal gravitational parameters ζ and b on the effective potential governing the radial motion of particles and the innermost stable circular orbit. In addition, gravitational waveforms exhibit significant phase differences: an increase in ζ induces a phase delay, whereas an increase in b results in a phase advance. A oneyear simulation of the orbital evolution of an extreme mass ratio inspiral demonstrates that when b = 2 and ζ ≈ 10 -6 , the mismatch between the gravitational waveforms predicted for the nonlocal gravity black hole and those for the Schwarzschild black hole reaches the distinguishable threshold (M = 0.0125), providing a basis for observational discrimination between general relativity and nonlocal gravity.
- 5 November 2026
- Published by IOP Publishing in Classical and Quantum Gravity
Open AccessPeriodic orbits and gravitational waveforms of spinning particles in nonlocal Gravity
In this paper, we investigate the dynamics and gravitational-wave signatures of periodic orbits of spinning test particles moving in the equatorial plane around static, spherically symmetric black holes within the framework of Deser-Woodard nonlocal gravity. Based on the Mathisson-Papapetrou-Dixon equations, combined with the Tulczyjew spin supplementary condition, we derive the orbital dynamic equations for spinning particles moving in the equatorial plane and impose a timelike constraint to exclude unphysical superluminal trajectories. By comparing with the classical Schwarzschild black hole, we systematically analyze the effects of the nonlocal gravitational parameters ζ and b on the effective potential governing the radial motion of particles and the innermost stable circular orbit. In addition, gravitational waveforms exhibit significant phase differences: an increase in ζ induces a phase delay, whereas an increase in b results in a phase advance. A oneyear simulation of the orbital evolution of an extreme mass ratio inspiral demonstrates that when b = 2 and ζ ≈ 10 -6 , the mismatch between the gravitational waveforms predicted for the nonlocal gravity black hole and those for the Schwarzschild black hole reaches the distinguishable threshold (M = 0.0125), providing a basis for observational discrimination between general relativity and nonlocal gravity.
- 4 November 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (10)
Distinguishability of magnetic massive black holes from environmental mimics with inspiral gravitational waves
- 4 November 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (10)
Distinguishability of magnetic massive black holes from environmental mimics with inspiral gravitational waves
- 18 October 2026
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 141 (10) , 1190
Scalar superradiance in the charged black-bounce spacetimes
- 18 October 2026
- Published by Springer Nature in The European Physical Journal Plus
- Vol. 141 (10) , 1190
Scalar superradiance in the charged black-bounce spacetimes
- Open Access
- 23 June 2026
- Published by Elsevier in SSRN Electronic Journal
Non-singular Inflation-Dark Energy Unification Model of Loop Quantum Cosmology
Unifying the early-universe inflationary paradigm with late-time cosmic acceleration, while resolving the initial Big Bang singularity, remains one of the most profound challenges in modern cosmology. In this paper, we propose a non-singular quintessential inflation model embedded within the effective dynamics of Loop Quantum Cosmology (LQC) based on a Generalized Regularization Scheme. The quantum geometry effects naturally replace the initial singularity with a quantum bounce, followed by a phase of superinflation that sets robust initial conditions for the subsequent slow-roll inflation. To achieve a viable late-time dark energy epoch and address the coincidence problem, we introduce a coupling between the scalar field and massive neutrinos, known as Mass-Varying Neutrinos(MaVaNs). As neutrinos become non-relativistic in the post-inflationary evolution, their backreaction effectively freezes the scalar field, triggering the late-time accelerated expansion. We numerically trace the full background dynamics from the quantum bounce to the present day. Furthermore, we tightly constrain the model parameters utilizing the observational data, including the Type Ia supernovae sample, the Dark Energy Spectroscopic Instrument (DESI) Baryon Acoustic Oscillations (BAO) and Cosmic Microwave Background (CMB) distance priors. Our results demonstrate that this unified LQC-MaVaNs quintessential framework is highly consistent with current precision cosmological observations, and importantly, offers a viable methodology to observationally constrain the Barbero-Immirzi parameter.
- 23 June 2026
- Published by Elsevier in SSRN Electronic Journal
Open AccessNon-singular Inflation-Dark Energy Unification Model of Loop Quantum Cosmology
Unifying the early-universe inflationary paradigm with late-time cosmic acceleration, while resolving the initial Big Bang singularity, remains one of the most profound challenges in modern cosmology. In this paper, we propose a non-singular quintessential inflation model embedded within the effective dynamics of Loop Quantum Cosmology (LQC) based on a Generalized Regularization Scheme. The quantum geometry effects naturally replace the initial singularity with a quantum bounce, followed by a phase of superinflation that sets robust initial conditions for the subsequent slow-roll inflation. To achieve a viable late-time dark energy epoch and address the coincidence problem, we introduce a coupling between the scalar field and massive neutrinos, known as Mass-Varying Neutrinos(MaVaNs). As neutrinos become non-relativistic in the post-inflationary evolution, their backreaction effectively freezes the scalar field, triggering the late-time accelerated expansion. We numerically trace the full background dynamics from the quantum bounce to the present day. Furthermore, we tightly constrain the model parameters utilizing the observational data, including the Type Ia supernovae sample, the Dark Energy Spectroscopic Instrument (DESI) Baryon Acoustic Oscillations (BAO) and Cosmic Microwave Background (CMB) distance priors. Our results demonstrate that this unified LQC-MaVaNs quintessential framework is highly consistent with current precision cosmological observations, and importantly, offers a viable methodology to observationally constrain the Barbero-Immirzi parameter.
- Open Access
Higher-Dimensional Quantum-Corrected Oppenheimer–Snyder Model with a Cosmological Constant
We extended the higher-dimensional quantum Oppenheimer–Snyder model to the case with a cosmological constant. For the AdS case, we discuss its thermodynamic properties in extended phase space formalism and make a comparison with classical black holes. For quantum-corrected small black holes in AdS spacetime, the temperature no longer diverges but tends to zero. Additionally, the heat capacity exhibits characteristic behavior indicative of an extra phase transition induced by quantum corrections, highlighting the profound impact of quantum effects on black hole thermodynamics.
Open AccessHigher-Dimensional Quantum-Corrected Oppenheimer–Snyder Model with a Cosmological Constant
We extended the higher-dimensional quantum Oppenheimer–Snyder model to the case with a cosmological constant. For the AdS case, we discuss its thermodynamic properties in extended phase space formalism and make a comparison with classical black holes. For quantum-corrected small black holes in AdS spacetime, the temperature no longer diverges but tends to zero. Additionally, the heat capacity exhibits characteristic behavior indicative of an extra phase transition induced by quantum corrections, highlighting the profound impact of quantum effects on black hole thermodynamics.
- 1 June 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (06)
Gravitational lensing effect from the revised Deser-Woodard nonlocal gravity
We investigate the gravitational lensing effects of a static spherically symmetric black hole (BH) within the framework of the revised Deser-Woodard (D-W) nonlocal gravity. By analyzing the deflection angle in both the weak and strong field limits, we derive several distinguishing features of the model. In the weak field limit, we report a leading-order correction to the deflection angle directly attributed to the non-local nature of the theory. In the strong field limit, we find that the lensing corrections are almost linearly dependent on the coupling parameter ζ while being exponentially suppressed by the exponent parameter n . Furthermore, the gravitational lensing effect in the revised D-W model at a given time shares similar scale-invariant behavior to General Relativity and conformal gravity, offering a potential pathway to distinguish it from other alternatives using astronomical observations.
- 1 June 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (06)
Gravitational lensing effect from the revised Deser-Woodard nonlocal gravity
We investigate the gravitational lensing effects of a static spherically symmetric black hole (BH) within the framework of the revised Deser-Woodard (D-W) nonlocal gravity. By analyzing the deflection angle in both the weak and strong field limits, we derive several distinguishing features of the model. In the weak field limit, we report a leading-order correction to the deflection angle directly attributed to the non-local nature of the theory. In the strong field limit, we find that the lensing corrections are almost linearly dependent on the coupling parameter ζ while being exponentially suppressed by the exponent parameter n . Furthermore, the gravitational lensing effect in the revised D-W model at a given time shares similar scale-invariant behavior to General Relativity and conformal gravity, offering a potential pathway to distinguish it from other alternatives using astronomical observations.
- 16 May 2026
- Published by Elsevier in Physics of the Dark Universe
- Vol. 52
Periodic orbits and gravitational waveforms of black holes in bumblebee gravity
- 16 May 2026
- Published by Elsevier in Physics of the Dark Universe
- Vol. 52
Periodic orbits and gravitational waveforms of black holes in bumblebee gravity
- Open Access
- 10 May 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (5)
Novel five-dimensional rotating Lifshitz black holes with electric and axionic charges
In this work, we construct a new family of exact five-dimensional charged and rotating asymptotically Lifshitz black holes. The spacetime solves Einstein equations coupled to a dilaton, two Abelian gauge fields, and axionic scalars supplemented by two generalized Chern-Simons terms. This configuration is characterized by a range of the free dynamical exponent z and possesses nontrivial thermodynamical parameters, where we verify the first law of black hole thermodynamics and derive the corresponding Smarr relation. As an application of this new gravitational background, we then investigate a holographic superconductor in the rotating Lifshitz background. We study the condensation of the scalar operator and the AC conductivity of the dual system. These results show that increasing the rotation parameter suppresses the condensate and weakens the superconducting phase, while increasing the dynamical critical exponent enhances the superconducting order. To the best of our knowledge, these solutions provide the first explicit family of five-dimensional rotating Lifshitz black holes supported simultaneously by electric and axionic charges.
- 10 May 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (5)
Open AccessNovel five-dimensional rotating Lifshitz black holes with electric and axionic charges
In this work, we construct a new family of exact five-dimensional charged and rotating asymptotically Lifshitz black holes. The spacetime solves Einstein equations coupled to a dilaton, two Abelian gauge fields, and axionic scalars supplemented by two generalized Chern-Simons terms. This configuration is characterized by a range of the free dynamical exponent z and possesses nontrivial thermodynamical parameters, where we verify the first law of black hole thermodynamics and derive the corresponding Smarr relation. As an application of this new gravitational background, we then investigate a holographic superconductor in the rotating Lifshitz background. We study the condensation of the scalar operator and the AC conductivity of the dual system. These results show that increasing the rotation parameter suppresses the condensate and weakens the superconducting phase, while increasing the dynamical critical exponent enhances the superconducting order. To the best of our knowledge, these solutions provide the first explicit family of five-dimensional rotating Lifshitz black holes supported simultaneously by electric and axionic charges.
- Open Access
- 1 May 2026
- Published by American Physical Society (APS) in APS Open Science
- Vol. 1, 000012
Bosonic and fermionic Love numbers of a static acoustic black hole
We compute static ($\ensuremath{\omega}\ensuremath{\rightarrow}0$) tidal Love numbers for scalar ($s=0$) and Dirac ($s=1/2$) perturbations of static acoustic black holes (ABHs) in $(3+1)$ and $(2+1)$ dimensions, respectively. By imposing horizon regularity condition and matching to the large-radius expansion, we extract the ratio between decaying and growing modes. It turns out that in $(3+1)$ dimensions the scalar Love number is generically nonzero for ABHs, while the Fermionic Love numbers follow a universal power-law form ${F}_{\ensuremath{\ell}m}^{\ifmmode\pm\else\textpm\fi{}1/2}=\ifmmode\pm\else\textpm\fi{}{4}^{\ensuremath{-}(\ensuremath{\ell}+1/2)}$. In $(2+1)$ dimensions, the scalar field exhibits a strange logarithmic structure, causing the Bosonic Love number to vanish for even $m$ but remain nontrivial for odd $m$. In contrast, the Fermionic Love number in this case retains a simple power-law form ${F}_{m}={4}^{\ensuremath{-}m}$ and is generically nonzero. These results provide insights into tidal response in analog-gravity systems and highlight qualitative differences between integer- and half-integer-spin fields.- 1 May 2026
- Published by American Physical Society (APS) in APS Open Science
- Vol. 1, 000012
Open AccessBosonic and fermionic Love numbers of a static acoustic black hole
We compute static ($\ensuremath{\omega}\ensuremath{\rightarrow}0$) tidal Love numbers for scalar ($s=0$) and Dirac ($s=1/2$) perturbations of static acoustic black holes (ABHs) in $(3+1)$ and $(2+1)$ dimensions, respectively. By imposing horizon regularity condition and matching to the large-radius expansion, we extract the ratio between decaying and growing modes. It turns out that in $(3+1)$ dimensions the scalar Love number is generically nonzero for ABHs, while the Fermionic Love numbers follow a universal power-law form ${F}_{\ensuremath{\ell}m}^{\ifmmode\pm\else\textpm\fi{}1/2}=\ifmmode\pm\else\textpm\fi{}{4}^{\ensuremath{-}(\ensuremath{\ell}+1/2)}$. In $(2+1)$ dimensions, the scalar field exhibits a strange logarithmic structure, causing the Bosonic Love number to vanish for even $m$ but remain nontrivial for odd $m$. In contrast, the Fermionic Love number in this case retains a simple power-law form ${F}_{m}={4}^{\ensuremath{-}m}$ and is generically nonzero. These results provide insights into tidal response in analog-gravity systems and highlight qualitative differences between integer- and half-integer-spin fields.