Realization of Holographic Entanglement Temperature for a Nearly-AdS boundary
Computing the holographic entanglement entropy proposed by Ryu-Takayanagi shows that thermal energy near boundary region in \(AdS_3\) gain maximum of the temperature. The absolute maxima of temperature is \(T^{Max}_{E}= \frac{4G_3 \epsilon_{\infty}}{l}\). By simple physical investigations it has bec...
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| Abstract | Computing the holographic entanglement entropy proposed by Ryu-Takayanagi shows that thermal energy near boundary region in \(AdS_3\) gain maximum of the temperature. The absolute maxima of temperature is \(T^{Max}_{E}= \frac{4G_3 \epsilon_{\infty}}{l}\). By simple physical investigations it has become possible to predict a phase transition of first order at critical temperature \(T_c\leq T_{E}\). As they predict a tail or root towards which the AdS space ultimately tend, the boundary is considered thermalized. The Phase transitions of this form have received striking theoretical and experimental verifications so far. |
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| AbstractList | Int J Theor Phys (2016) 55: 4751 Computing the holographic entanglement entropy proposed by Ryu-Takayanagi
shows that thermal energy near boundary region in $AdS_3$ gain maximum of the
temperature. The absolute maxima of temperature is $T^{Max}_{E}= \frac{4G_3
\epsilon_{\infty}}{l}$. By simple physical investigations it has become
possible to predict a phase transition of first order at critical temperature
$T_c\leq T_{E}$. As they predict a tail or root towards which the AdS space
ultimately tend, the boundary is considered thermalized. The Phase transitions
of this form have received striking theoretical and experimental verifications
so far. Computing the holographic entanglement entropy proposed by Ryu-Takayanagi shows that thermal energy near boundary region in \(AdS_3\) gain maximum of the temperature. The absolute maxima of temperature is \(T^{Max}_{E}= \frac{4G_3 \epsilon_{\infty}}{l}\). By simple physical investigations it has become possible to predict a phase transition of first order at critical temperature \(T_c\leq T_{E}\). As they predict a tail or root towards which the AdS space ultimately tend, the boundary is considered thermalized. The Phase transitions of this form have received striking theoretical and experimental verifications so far. |
| Author | Myrzakulov, R Raza, M Momeni, D Gholizade, H |
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| BackLink | https://doi.org/10.1007/s10773-016-3098-4$$DView published paper (Access to full text may be restricted) https://doi.org/10.48550/arXiv.1505.00215$$DView paper in arXiv |
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| DOI | 10.48550/arxiv.1505.00215 |
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| Snippet | Computing the holographic entanglement entropy proposed by Ryu-Takayanagi shows that thermal energy near boundary region in \(AdS_3\) gain maximum of the... Int J Theor Phys (2016) 55: 4751 Computing the holographic entanglement entropy proposed by Ryu-Takayanagi shows that thermal energy near boundary region in... |
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| Title | Realization of Holographic Entanglement Temperature for a Nearly-AdS boundary |
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