Entanglement entropy for T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed holographic CFT

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Entanglement entropy for T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed holographic CFT ; volume:2021 ; number:2 ; day:11 ; month:2 ; year:2021 ; pages:1-30 ; date:2.2021
Journal of high energy physics ; 2021, Heft 2 (11.2.2021), 1-30, 2.2021

Creator: Chakraborty, Soumangsu
Hashimoto, Akikazu

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2021)096

URN: urn:nbn:de:101:1-2021051614270694792503

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:45 AM CEST

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Chakraborty, Soumangsu
Hashimoto, Akikazu
SpringerLink (Online service)

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$Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT$

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$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST$

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$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories$

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Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

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$The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation$

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$Perturbative renormalization of the T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed free massive Dirac fermion$

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$Expectation value of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ operator in curved spacetimes$

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Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

$Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT$

Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT

$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger$

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST$

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories$

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ + Λ2 deformed CFT on the stretched dS3 horizon$

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ + Λ2 deformed CFT on the stretched dS3 horizon

$TsT, T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and black strings$

TsT, T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and black strings

Probing the top-quark width through ratios of resonance contributions of e + e − → W + W − b b ¯ $$ \mathrm{e}}^{+}{\mathrm{e}}^{-}\to \mathrm{W}}^{+}{\mathrm{W}}^{-}\mathrm{b}\overline{\mathrm{b}} $$

$The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation$

The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation

$Perturbative renormalization of the T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed free massive Dirac fermion$

Perturbative renormalization of the T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed free massive Dirac fermion

$Expectation value of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ operator in curved spacetimes$

Expectation value of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ operator in curved spacetimes

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Entanglement entropy for T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed holographic CFT

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Other Objects (12)

Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ + Λ2 deformed CFT on the stretched dS3 horizon

TsT, T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and black strings

Probing the top-quark width through ratios of resonance contributions of e + e − → W + W − b b ¯ $$ \mathrm{e}}^{+}{\mathrm{e}}^{-}\to \mathrm{W}}^{+}{\mathrm{W}}^{-}\mathrm{b}\overline{\mathrm{b}} $$

The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation

Perturbative renormalization of the T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed free massive Dirac fermion

Expectation value of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ operator in curved spacetimes

Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ + Λ2 deformed CFT on the stretched dS3 horizon

TsT, T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and black strings

Probing the top-quark width through ratios of resonance contributions of e + e − → W + W − b b ¯ $$ \mathrm{e}}^{+}{\mathrm{e}}^{-}\to \mathrm{W}}^{+}{\mathrm{W}}^{-}\mathrm{b}\overline{\mathrm{b}} $$

The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation

Perturbative renormalization of the T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed free massive Dirac fermion

Expectation value of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ operator in curved spacetimes

Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ + Λ2 deformed CFT on the stretched dS3 horizon

TsT, T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and black strings

Probing the top-quark width through ratios of resonance contributions of e + e − → W + W − b b ¯ $$ \mathrm{e}}^{+}{\mathrm{e}}^{-}\to \mathrm{W}}^{+}{\mathrm{W}}^{-}\mathrm{b}\overline{\mathrm{b}} $$

The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation

Perturbative renormalization of the T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed free massive Dirac fermion

Expectation value of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ operator in curved spacetimes

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