Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:1202.2605 · Journal of High Energy Physics

Holographic studies of entanglement entropy in superconductors

Tameem Albash, Clifford V. Johnson

Published May 1, 2012• 97 citations
arXivHTMLPDF
DOI
10.1007/jhep05(2012)079

Related papers

Holographic Entanglement Entropy in Insulator/Superconductor Transition

•Jan 1, 2012•33 citations

Holographic entanglement entropy in insulator/superconductor transition

Rong-Gen Cai, Song He, Li Li +1 more

arXiv:1203.6620•Journal of High Energy Physics•Jul 1, 2012•86 citations

Entanglement entropy in holographic p-wave superconductor/insulator model

Rong-Gen Cai, Li Li, Li-Fang Li +1 more

arXiv:1303.4828•Journal of High Energy Physics•Jun 1, 2013•31 citations

Entanglement Entropy for Time Dependent Two Dimensional Holographic Superconductor

N.S. Mazhari, D. Momeni, Kairat Myrzakulov +1 more

We studied entanglement entropy for a time dependent two dimensional holographic superconductor. We showed that the conserved charge of the system plays the role of the critical parameter to have condensation.

arXiv:1602.08720•Apr 1, 2018•0 citations

Holographic Entanglement Entropy in the dS/CFT Correspondence and Entanglement Entropy in the Sp(N) Model

Yoshiki Sato

•Mar 23, 2016•0 citations

Holographic entanglement entropy of a 1 + 1 dimensional p-wave superconductor

Sumit R. Das, Mitsutoshi Fujita A, Bom Soo Kim

We examine the behavior of entanglement entropy S EE of a subsystem A in a fully backreacted holographic model of a 1 + 1 dimensional p wave superconductor across the phase transition. For a given temperature, the system goes to a superconducting phase beyond a critical value of the charge density. The entanglement entropy, considered as a function of the charge density at a given temperature, has a cusp at the critical point. In addition, we find that there are three different behaviors in the condensed phase, depending on the subsystem size. For a subsystem size l smaller than a critical size l c1, S EE continues to increase as a function of the charge density as we cross the phase transition. When l lies between l c1 and another critical size l c2 the entanglement entropy displays a non-monotonic behavior, while for l > l c2 it decreases monotonically. At large charge densities S EE appears to saturate. The non-monotonic behavior leads to a novel phase diagram for this system.

arXiv:1705.10392•Journal of High Energy Physics•Sep 1, 2017•9 citations
We examine the behavior of entanglement entropy S EE of a subsystem A in a fully backreacted holographic model of a 1 + 1 dimensional p wave superconductor across the phase transition. For a given temperature, the system goes to a superconducting phase beyond a critical value of the charge density. The entanglement entropy, considered as a function of the charge density at a given temperature, has a cusp at the critical point. In addition, we find that there are three different behaviors in the condensed phase, depending on the subsystem size. For a subsystem size l smaller than a critical size l c1, S EE continues to increase as a function of the charge density as we cross the phase transition. When l lies between l c1 and another critical size l c2 the entanglement entropy displays a non-monotonic behavior, while for l > l c2 it decreases monotonically. At large charge densities S EE appears to saturate. The non-monotonic behavior leads to a novel phase diagram for this system.