Journal of High Energy Physics | |
Flavored anisotropic black holes | |
Regular Article - Theoretical Physics | |
Ana Garbayo1  Alfonso V. Ramallo1  José Manuel Penín2  Niko Jokela2  Carlos Hoyos3  | |
[1] Departamento de Física de Partículas, Universidade de Santiago de Compostela, E-15782, Santiago de Compostela, Spain;Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, E-15782, Santiago de Compostela, Spain;Department of Physics and Helsinki Institute of Physics, P.O.Box 64, FIN-00014 University of Helsinki, Helsinki, Finland;Helsinki Institute of Physics, P.O.Box 64, FIN-00014 University of Helsinki, Helsinki, Finland;Department of Physics, Universidad de Oviedo, E-33007/33004, Oviedo, Spain;Instituto de Ciencias y Tecnologías espaciales de Asturias (ICTEA), Universidad de Oviedo, E-33007/33004, Oviedo, Spain; | |
关键词: AdS-CFT Correspondence; D-Branes; Gauge-Gravity Correspondence; | |
DOI : 10.1007/JHEP10(2022)061 | |
received in 2022-08-17, accepted in 2022-09-19, 发布年份 2022 | |
来源: Springer | |
【 摘 要 】
We construct a black hole geometry dual to a (2+1)-dimensional defect in an ambient (3+1)-dimensional gauge theory at non-zero temperature and quark density. The geometry is a solution to the equations of motion of type IIB supergravity with brane sources, a low energy limit of an intersection of stacks of color D3-branes and flavor D5-branes. We consider the case in which the number of D5-branes is large and they can be homogeneously distributed along the directions orthogonal to the defect, creating in this way a multilayer structure. The quark density is generated by exciting a gauge field in the worldvolume of the dynamic brane sources. We study the thermodynamics of the anisotropic black hole and compute the energy density of the dual theory, as well as the pressures and speeds of sound along the directions parallel and orthogonal to the defect. We also calculate transport coefficients in the shear channel, quark-antiquark potentials, and the entanglement entropies for slab subregions. These analyses give us a good overview on how the degrees of freedom are spread, entangled, and behave in this unquenched system in the deconfining phase at strong coupling.
【 授权许可】
Unknown
© The Author(s) 2022
【 预 览 】
Files | Size | Format | View |
---|---|---|---|
RO202305113858606ZK.pdf | 1130KB | download |
【 参考文献 】
- [1]
- [2]
- [3]
- [4]
- [5]
- [6]
- [7]
- [8]
- [9]
- [10]
- [11]
- [12]
- [13]
- [14]
- [15]
- [16]
- [17]
- [18]
- [19]
- [20]
- [21]
- [22]
- [23]
- [24]
- [25]
- [26]
- [27]
- [28]
- [29]
- [30]
- [31]
- [32]
- [33]
- [34]
- [35]
- [36]
- [37]
- [38]
- [39]
- [40]
- [41]
- [42]
- [43]
- [44]
- [45]
- [46]
- [47]
- [48]
- [49]
- [50]
- [51]
- [52]
- [53]
- [54]
- [55]
- [56]
- [57]
- [58]
- [59]
- [60]
- [61]
- [62]
- [63]
- [64]
- [65]
- [66]
- [67]
- [68]
- [69]
- [70]
- [71]
- [72]
- [73]
- [74]
- [75]
- [76]
- [77]
- [78]
- [79]
- [80]
- [81]
- [82]
- [83]
- [84]
- [85]
- [86]
- [87]
- [88]
- [89]
- [90]