Pando Zayas Leopoldo A, Vaman Diana
Michigan Center for Theoretical Physics, University of Michigan, Ann Arbor, Michigan 48109-1120A, USA.
Phys Rev Lett. 2003 Sep 12;91(11):111602. doi: 10.1103/PhysRevLett.91.111602.
We present an exact calculation of the finite temperature partition function for the hadronic states corresponding to a Penrose-Güven limit of the Maldacena-Nùñez embedding of the N=1 super Yang-Mills (SYM) into string theory. It is established that the theory exhibits a Hagedorn density of states. We propose a semiclassical string approximation to the finite temperature partition function for confining gauge theories admitting a supergravity dual, by performing an expansion around classical solutions characterized by temporal windings. This semiclassical approximation reveals a hadronic energy density of states of a Hagedorn type, with the coefficient determined by the gauge theory string tension as expected for confining theories. We argue that our proposal captures primarily information about states of pure N=1 SYM theory, given that this semiclassical approximation does not entail a projection onto states of large U(1) charge.
我们给出了对应于将(N = 1)超杨-米尔斯(SYM)理论嵌入弦理论的马尔达西那-努涅斯嵌入的彭罗斯-居文极限的强子态有限温度配分函数的精确计算。结果表明该理论呈现出哈格多恩态密度。对于允许超引力对偶的禁闭规范理论的有限温度配分函数,我们通过围绕以时间缠绕为特征的经典解进行展开,提出了一种半经典弦近似。这种半经典近似揭示了哈格多恩型的强子能量态密度,其系数由规范理论弦张力确定,这与禁闭理论的预期一致。我们认为,鉴于这种半经典近似并不需要投影到具有大(U(1))电荷的态上,我们的提议主要捕捉到了纯(N = 1) SYM理论态的信息。