Glueball–baryon interactions in holographic QCD

Studying the Witten–Sakai–Sugimoto model with type IIA string theory, we find the glueball–baryon interaction is predicted in this model. The glueball is identified as the 11D gravitational waves or graviton described by the M5-brane supergravity solution. Employing the relation of M-theory and type...

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Main Author: Si-Wen Li
Format: Article
Language:English
Published: Elsevier 2017-10-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269317306329
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spelling doaj-4150f2d0e4cd4cce84b2fa7ae9eb67552020-11-25T01:49:13ZengElsevierPhysics Letters B0370-26932017-10-01773142149Glueball–baryon interactions in holographic QCDSi-Wen Li0Department of Modern Physics, University of Science and Technology of China, Hefei 230026, Anhui, ChinaStudying the Witten–Sakai–Sugimoto model with type IIA string theory, we find the glueball–baryon interaction is predicted in this model. The glueball is identified as the 11D gravitational waves or graviton described by the M5-brane supergravity solution. Employing the relation of M-theory and type IIA string theory, glueball is also 10D gravitational perturbations which are the excited modes by close strings in the bulk of this model. On the other hand, baryon is identified as a D4-brane wrapped on S4 which is named as baryon vertex, so the glueball–baryon interaction is nothing but the close string/baryon vertex interaction in this model. Since the baryon vertex could be equivalently treated as the instanton configurations on the flavor brane, we identify the glueball–baryon interaction as “graviton–instanton” interaction in order to describe it quantitatively by the quantum mechanical system for the collective modes of baryons. So the effective Hamiltonian can be obtained by considering the gravitational perturbations in the flavor brane action. With this Hamiltonian, the amplitudes and the selection rules of the glueball–baryon interaction can be analytically calculated in the strong coupling limit. We show our calculations explicitly in two characteristic situations which are “scalar and tensor glueball interacting with baryons”. Although there is a long way to go, our work provides a holographic way to understand the interactions of baryons in hadronic physics and nuclear physics by the underlying string theory.http://www.sciencedirect.com/science/article/pii/S0370269317306329
collection DOAJ
language English
format Article
sources DOAJ
author Si-Wen Li
spellingShingle Si-Wen Li
Glueball–baryon interactions in holographic QCD
Physics Letters B
author_facet Si-Wen Li
author_sort Si-Wen Li
title Glueball–baryon interactions in holographic QCD
title_short Glueball–baryon interactions in holographic QCD
title_full Glueball–baryon interactions in holographic QCD
title_fullStr Glueball–baryon interactions in holographic QCD
title_full_unstemmed Glueball–baryon interactions in holographic QCD
title_sort glueball–baryon interactions in holographic qcd
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2017-10-01
description Studying the Witten–Sakai–Sugimoto model with type IIA string theory, we find the glueball–baryon interaction is predicted in this model. The glueball is identified as the 11D gravitational waves or graviton described by the M5-brane supergravity solution. Employing the relation of M-theory and type IIA string theory, glueball is also 10D gravitational perturbations which are the excited modes by close strings in the bulk of this model. On the other hand, baryon is identified as a D4-brane wrapped on S4 which is named as baryon vertex, so the glueball–baryon interaction is nothing but the close string/baryon vertex interaction in this model. Since the baryon vertex could be equivalently treated as the instanton configurations on the flavor brane, we identify the glueball–baryon interaction as “graviton–instanton” interaction in order to describe it quantitatively by the quantum mechanical system for the collective modes of baryons. So the effective Hamiltonian can be obtained by considering the gravitational perturbations in the flavor brane action. With this Hamiltonian, the amplitudes and the selection rules of the glueball–baryon interaction can be analytically calculated in the strong coupling limit. We show our calculations explicitly in two characteristic situations which are “scalar and tensor glueball interacting with baryons”. Although there is a long way to go, our work provides a holographic way to understand the interactions of baryons in hadronic physics and nuclear physics by the underlying string theory.
url http://www.sciencedirect.com/science/article/pii/S0370269317306329
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