The holographic description of a baryon in non-critical string theory
Thermodynamics functions of dense matter with baryon density have been calculated using AdS/CFT duality. The confining phase of the near-extremal AdS6 background constructed from the intersecting brane configuration has been considered. The obtained results have been compared with the critical ones...
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Published in | Journal of physics. G, Nuclear and particle physics Vol. 39; no. 6; pp. 65004 - 12 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
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Bristol
IOP Publishing
01.06.2012
Institute of Physics |
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Abstract | Thermodynamics functions of dense matter with baryon density have been calculated using AdS/CFT duality. The confining phase of the near-extremal AdS6 background constructed from the intersecting brane configuration has been considered. The obtained results have been compared with the critical ones obtained using the Sakai-Sugimoto or Klebanov-Strassler models. Our results show that at large Nc and low baryon density the baryon-baryon interaction is repulsive as expected. Also a dynamical baryon has been considered in this model and its binding energy has been calculated. Results show that the baryon binding energy for our configuration is roughly 2.74 GeV. Moreover, the mass of quarks that composed the dynamical baryon has been approximated at roughly 372 MeV. |
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AbstractList | Thermodynamics functions of dense matter with baryon density have been calculated using AdS/CFT duality. The confining phase of the near-extremal AdS sub(6) background constructed from the intersecting brane configuration D4/D4/D4 has been considered. The obtained results have been compared with the critical ones obtained using the Sakai-Sugimoto or Klebanov-Strassler models. Our results show that at large Nc and low baryon density the baryon-baryon interaction is repulsive as expected. Also a dynamical baryon has been considered in this model and its binding energy has been calculated. Results show that the baryon binding energy for our configuration is roughly 2.74 GeV. Moreover, the mass of quarks that composed the dynamical baryon has been approximated at roughly 372 MeV. Thermodynamics functions of dense matter with baryon density have been calculated using AdS/CFT duality. The confining phase of the near-extremal AdS6 background constructed from the intersecting brane configuration has been considered. The obtained results have been compared with the critical ones obtained using the Sakai-Sugimoto or Klebanov-Strassler models. Our results show that at large Nc and low baryon density the baryon-baryon interaction is repulsive as expected. Also a dynamical baryon has been considered in this model and its binding energy has been calculated. Results show that the baryon binding energy for our configuration is roughly 2.74 GeV. Moreover, the mass of quarks that composed the dynamical baryon has been approximated at roughly 372 MeV. |
Author | Morad, R Sadeghi, J Pahlavani, M R |
Author_xml | – sequence: 1 givenname: M R surname: Pahlavani fullname: Pahlavani, M R email: m.pahlavani@umz.ac.ir organization: Mazandaran University Sciences Faculty, Department of Physics, PO Box 47415-416, Babolsar, Iran – sequence: 2 givenname: J surname: Sadeghi fullname: Sadeghi, J email: pouriya@ipm.ir organization: Mazandaran University Sciences Faculty, Department of Physics, PO Box 47415-416, Babolsar, Iran – sequence: 3 givenname: R surname: Morad fullname: Morad, R email: r.morad@umz.ac.ir organization: Mazandaran University Sciences Faculty, Department of Physics, PO Box 47415-416, Babolsar, Iran |
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Cites_doi | 10.1143/PTP.121.241 10.4310/ATMP.1998.v2.n2.a1 10.1103/PhysRevD.79.026005 10.1142/S0217751X99001676 10.1103/PhysRevD.75.086003 10.1143/PTP.119.461 10.1103/PhysRevC.82.025201 10.1143/PTP.117.1157 10.1016/S0370-2693(98)00377-3 10.4310/ATMP.1998.v2.n2.a2 10.1143/PTP.113.843 10.1088/0954-3899/38/5/055002 10.3938/jkps.52.1734 10.1103/PhysRevD.84.126010 10.1103/PhysRevD.76.061901 10.1103/PhysRevD.69.066007 10.1103/PhysRevLett.95.261602 10.1103/PhysRevD.79.105024 10.1103/PhysRevD.78.086006 10.1142/S0217751X04020865 10.1143/PTP.114.1083 10.1016/j.physletb.2004.10.048 10.1016/j.physletb.2007.01.030 10.1016/j.nuclphysb.2008.10.004 10.1103/PhysRevLett.80.4859 10.1007/s10773-010-0557-1 |
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Keywords | Dense matter String theory Baryon-baryon interactions Thermodynamic function Elementary particle mass Duality Baryons Brane world Binding energy Quark mass Models Mathematical physics Nuclear physics |
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References | Rozali M (21) 2008 22 23 26 Kim K-Y (44) 2008 Kim K-Y (24) 2008 28 29 Brandhuber A (7) 1998 Kuperstein S (36) 2004 Dymarskya A (34) 2011 Witten E (2) 1998; 2 Casero R (38) 2006 Bigazzi F (37) 2005 Hong D K (19) 2007 Maldacena J M (1) 1998; 2 Mazu V (41) 2008 Witten E (13) 1998 30 Seki S (18) 2009 10 32 11 33 Bergman O (20) 2007 35 14 15 16 17 Kuperstein S (39) 2004 Kruczenski M (5) 2004 Pahlavani M R (31) 2011; 38 Kim K-Y (27) 2008 3 4 6 Klebanov I R (12) 2000 8 9 Park J (25) 2008 40 42 43 |
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Snippet | Thermodynamics functions of dense matter with baryon density have been calculated using AdS/CFT duality. The confining phase of the near-extremal AdS6... Thermodynamics functions of dense matter with baryon density have been calculated using AdS/CFT duality. The confining phase of the near-extremal AdS sub(6)... |
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SubjectTerms | AdS/CFT correspondence Approximation baryon Baryons binding eneregy Binding energy Confining Density Exact sciences and technology Mathematical models noncritical string theory Nuclear physics Particle physics Physics String theory The physics of elementary particles and fields |
Title | The holographic description of a baryon in non-critical string theory |
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