TY - JOUR
T1 - On the spectra of scalar mesons from HQCD models
AU - Mintakevich, Oded
AU - Sonnenschein, Jacob
PY - 2008/8/1
Y1 - 2008/8/1
N2 - We determine the holographic spectra of scalar mesons from the fluctuations of the embedding of flavor D-brane probes in HQCD models. The models we consider include a generalization of the Sakai Sugimoto model at zero temperature and at the ''high-temperature intermediate phase", where the system is in a deconfining phase while admitting chiral symmetry breaking and a non-critical 6d model at zero temperature. All these models are based on backgrounds associated with near extremal N c D4 branes and a set of N f << N c flavor probe branes that admit geometrical chiral symmetry breaking. We point out that the spectra of these models include a 0 - branch which does not show up in nature. At zero temperature we found that the masses of the mesons M n depend on the ''constituent quark mass" parameter m c q and on the excitation number n as M n 2 ∼ m c q and M 2 n ∼ n 1.7 for the ten dimensional case and as M n ∼ m c q and M n ∼ n 0.75 in the non-critical case. At the high temperature intermediate phase we detect a decrease of the masses of low spin mesons as a function of the temperature similar to holographic vector mesons and to lattice calculations.
AB - We determine the holographic spectra of scalar mesons from the fluctuations of the embedding of flavor D-brane probes in HQCD models. The models we consider include a generalization of the Sakai Sugimoto model at zero temperature and at the ''high-temperature intermediate phase", where the system is in a deconfining phase while admitting chiral symmetry breaking and a non-critical 6d model at zero temperature. All these models are based on backgrounds associated with near extremal N c D4 branes and a set of N f << N c flavor probe branes that admit geometrical chiral symmetry breaking. We point out that the spectra of these models include a 0 - branch which does not show up in nature. At zero temperature we found that the masses of the mesons M n depend on the ''constituent quark mass" parameter m c q and on the excitation number n as M n 2 ∼ m c q and M 2 n ∼ n 1.7 for the ten dimensional case and as M n ∼ m c q and M n ∼ n 0.75 in the non-critical case. At the high temperature intermediate phase we detect a decrease of the masses of low spin mesons as a function of the temperature similar to holographic vector mesons and to lattice calculations.
KW - AdS-CFT correspondence
KW - Brane dynamics in gauge theories
KW - Gauge-gravity correspondence
UR - http://www.scopus.com/inward/record.url?scp=54749111779&partnerID=8YFLogxK
U2 - 10.1088/1126-6708/2008/08/082
DO - 10.1088/1126-6708/2008/08/082
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AN - SCOPUS:54749111779
SN - 1126-6708
VL - 2008
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 8
M1 - 082
ER -