Deconfinement Transition of AdS/QCD at ${\cal O}(α'^3)$
| dc.creator | Cai, Rong-Gen | |
| dc.creator | Ohta, Nobuyoshi | |
| dc.date | 2007-07-13 | |
| dc.date | 2007-09-24 | |
| dc.date.accessioned | 2026-07-07T10:56:43Z | |
| dc.date.available | 2026-07-07T10:56:43Z | |
| dc.description | We study the confinement/deconfinement phase transition of holographic AdS/QCD models by using Ricci flat $AdS_5$ black holes up to ${\cal O}(α'^3)$, which corresponds to the $λ$ expansion correction in the dual field theory to $λ^{-3/2}$, where $λ$ is the 't Hooft coupling constant. We consider two cases: one is the hard-wall AdS/QCD model where a small radius region of the $AdS_5$ is removed; the other is the case where one of spatial coordinates for the $AdS_5$ space is compactified, resulting in Witten's QCD model in 2+1 dimensions. We find that in the hard-wall AdS/QCD model, the deconfinement temperature decreases when the $λ$ expansion corrections are taken into account, while in Witten's QCD model, the deconfinement transition always happens when the ratio of inverse temperature $β$ to the period $β_s$ of the compactified coordinate decreases to one, $β/β_s=1$, the same as the case without the ${\cal O}(α'^3)$ correction. | |
| dc.description | Latex, 14 pages; v2: the version to appear in PRD | |
| dc.identifier | https://arxiv.org/abs/0707.2013 | |
| dc.identifier | http://arxiv.org/abs/0707.2013 | |
| dc.identifier | Phys.Rev.D76:106001,2007 | |
| dc.identifier | doi:10.1103/PhysRevD.76.106001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/186506 | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Deconfinement Transition of AdS/QCD at ${\cal O}(α'^3)$ | |
| dc.type | text |