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Charged black string immersed in a quintessence fluid and string cloud

Published 4 Jun 2026 in gr-qc | (2606.06435v1)

Abstract: We present a new static solution describing a charged black string immersed in a Kiselev-type quintessence fluid and a cloud of strings. The metric and field equations are solved for a general quintessence state parameter, with explicit results provided for the physically relevant case $w_q = -2/3$. We analyze the event-horizon structure and the Kretschmann scalar, verify energy-condition constraints, and derive thermodynamic properties including the Hawking temperature and heat capacity to identify stability regimes. Finally, we investigate the photon cylinder for null geodesics. The solution generalizes known charged black-string spacetimes by simultaneously including quintessence and a string-cloud parameter.

Summary

  • The paper introduces a novel analytic solution for a charged black string immersed in a quintessence fluid and string cloud set within an AdS background.
  • The paper identifies modified horizon structures and thermodynamic phase transitions stemming from the interplay of quintessence and string cloud parameters.
  • The paper examines null geodesics to reveal a photon cylinder whose location and characteristics are significantly affected by the combined matter fields.

Charged Black String Solutions with Quintessence Fluid and String Cloud in Anti-de Sitter Spacetime

Introduction

The study explores the most general static solution for a charged black string immersed in both a Kiselev-type quintessence fluid and a cloud of strings within an anti-de Sitter (AdS) background. The confluence of these matter fields prompts significant modifications in horizon structure, curvature singularities, and the thermodynamic landscape of the black string. The analysis is directed primarily at the physically compelling case of the Kiselev parameter wq=−2/3w_q = -2/3, corresponding to a quintessence state interpolating between cosmological constant and string cloud matter. The work encompasses analytic metric construction, energy condition analysis, thermodynamic behavior, and photon cylinder structure.

Metric Structure and Field Equations

The Einstein-Maxwell equations are addressed with explicit matter sector contributions from: (i) electromagnetic fields, (ii) the anisotropic Kiselev fluid with arbitrary wq∈[−1,−1/3]w_q \in [-1, -1/3], and (iii) a string cloud characterized by density parameter aa. The static, cylindrically symmetric black string ansatz leads to a metric function whose general solution is

f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,

where NqN_q and α\alpha encapsulate quintessence and string cloud effects, respectively.

For wq=−2/3w_q = -2/3, the metric function reduces to:

f(r)=r2ℓ2−2Mr+Q2r2+Nqr+α.f(r) = \frac{r^2}{\ell^2} - \frac{2M}{r} + \frac{Q^2}{r^2} + N_q r + \alpha. Figure 1

Figure 1: The effect of varying the string cloud parameter α\alpha on the metric function f(r)f(r), illustrating horizon transitions and the possible emergence of naked singularities.

The vertical displacement controlled by wq∈[−1,−1/3]w_q \in [-1, -1/3]0 tunes the number of event horizons, including transitions to extremal or horizonless geometries depending on the parameter regime. The explicit inclusion of both matter components generalizes previous black string solutions, recovering them as particular limits.

Energy Conditions and Physical Admissibility

By explicit computation, the energy densities and pressures for the composite stress-energy tensor reveal dependencies on the sign and values of wq∈[−1,−1/3]w_q \in [-1, -1/3]1 and wq∈[−1,−1/3]w_q \in [-1, -1/3]2. The weak energy condition (WEC) and strong energy condition (SEC) impose explicit constraints:

  • WEC establishes positivity requirements for densities and principal pressures, leading to conditions on wq∈[−1,−1/3]w_q \in [-1, -1/3]3. For wq∈[−1,−1/3]w_q \in [-1, -1/3]4, a negative wq∈[−1,−1/3]w_q \in [-1, -1/3]5 is required for positive physical energy density.
  • SEC does not lead to constraints on the string cloud, but constrains the sign and magnitude of the Kiselev term.

These energy conditions delimit the physical configurational space for the black string solution and ensure absence of unphysical matter content at the classical level.

Horizon Structure and Singularities

The event horizon radii wq∈[−1,−1/3]w_q \in [-1, -1/3]6 are the roots of a polynomial, quartic in wq∈[−1,−1/3]w_q \in [-1, -1/3]7 for wq∈[−1,−1/3]w_q \in [-1, -1/3]8, incorporating coupled contributions from wq∈[−1,−1/3]w_q \in [-1, -1/3]9, aa0, aa1, and aa2. The Kretschmann scalar aa3 is computed explicitly, revealing its divergence at aa4 (central singularity) and complex functional dependence on all matter parameters. The presence of nonzero aa5 and aa6 introduces cross-terms with aa7 and aa8, enabling finer control of curvature divergence rates at intermediate and asymptotic regimes. The qualitative structure of singularities is substantially affected by the admixture of string cloud and quintessence components.

Thermodynamics and Stability

The Hawking temperature, derived from the surface gravity, and the heat capacity aa9 (via f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,0 at f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,1) were calculated. The temperature exhibits standard black hole behavior, modulated by the linear and constant contributions of quintessence and string cloud parameters.

The heat capacity admits critical points where it diverges, associated with phase transitions between locally stable and unstable thermodynamic regimes. For f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,2, the critical horizon radii are given by a biquadratic equation:

f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,3

with reality conditions f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,4 demarcating the region of parameter space admitting second-order phase transitions. Figure 2

Figure 2: Heat capacity f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,5 vs. f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,6 for various f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,7 below the critical threshold; f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,8 is continuous and strictly positive, indicating global thermodynamic stability.

Figure 3

Figure 3: Heat capacity f(r)=r2ℓ2−2Mr+Q2r2+Nqr3wq+1+α,f(r)=\frac{r^2}{\ell^2}-\frac{2M}{r}+\frac{Q^2}{r^2}+\frac{N_q}{r^{3w_q+1}}+\alpha ,9 vs. NqN_q0 for NqN_q1 above the critical threshold; divergences correspond to phase transition points separating stable and unstable domains.

For sufficiently large NqN_q2, the model predicts a thermodynamic phase transition, with the stable region (NqN_q3) corresponding to large black strings and instability (NqN_q4) emerging in the small-radius regime.

Photon Cylinder and Null Geodesics

The study of null geodesics confirms the existence of a photon cylinder—circular null orbits at a critical radius NqN_q5. For NqN_q6, the condition for NqN_q7 is a cubic equation:

NqN_q8

demonstrating the strong influence of the quintessence and string cloud parameters in shifting the photon sphere relative to standard black string cases. In limiting parameter regimes, analytic expressions for NqN_q9 display straightforward dependencies on α\alpha0, α\alpha1, α\alpha2, and α\alpha3. The position and energy of this photon barrier directly determine strong-lensing phenomena and the behavior of high-frequency field modes. Figure 4

Figure 4: Normalized effective potential α\alpha4 for varying α\alpha5, highlighting the shift in the photon barrier and displacement of α\alpha6 by the string cloud.

Implications and Future Outlook

This work fills the gap in the characterization of noncompact black objects in AdS with a generalized matter sector, verifying that the simultaneous presence of Kiselev quintessence and a string cloud yields black string solutions with richer horizon, singularity, and thermodynamic structures. The results are relevant for the study of gravitational collapse, dynamical and thermodynamical stability of extended objects, and modifications to gravitational lensing by non-spherically symmetric horizons.

Practically, the stability criteria and photon barrier modifications could be employed in models of extended astrophysical objects or in constructing boundary scenarios for holographic studies within AdS/CFT correspondence. Theoretically, further extensions could include rotation, higher-curvature corrections (e.g., α\alpha7 modifications as in (Santos et al., 24 Feb 2026)), or dedicated analysis of dynamical/stationary instabilities, especially the Gregory-Laflamme channel, in presence of complicated matter distributions.

Conclusion

The constructed family of charged black string solutions demonstrates that the interplay of Kiselev quintessence and string clouds induces substantial modifications to both local and global geometric and thermodynamic properties. The parameter space exhibits phase transition structure, explicit energy condition signatures, and nontrivial photon cylinder features. The analysis offers a reference point for further examinations of stability, semiclassical effects, and observable phenomena in generalized cylindrical spacetimes (2606.06435).

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