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arXiv 1611.08093hep-lat
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有限密度格点量子色动力学中的符号问题

Sign problem in finite density lattice QCD

V. A. Goy, V. Bornyakov, D. Boyda, A. Molochkov, A. Nakamura, A. Nikolaev, V. Zakharov

摘要:

为解决符号问题而开发的规范方法可能会受到一种新类型的符号问题的影响。在正则方法中,大配分函数被写成逸度展开式:$Z_G(μ,T) = \sum_n Z_C(n,T) ξ^n$,其中$ξ=\exp(μ/T)$是逸度,$Z_C(n,T)$是蒙特卡罗更新$\langle z_n\rangle$的平均值。我们发现,在每个Monte Carlo步骤中,$z_n$的复相与$n$成正比。虽然$\langle z_n\rangle$取实正值,但当$n$较大时,$z_n$的值迅速波动,特别是在限制相,这给出了对$n$的限制。我们讨论这个问题的可能补救措施。

英文摘要:

The canonical approach, which was developed for solving the sign problem, may suffer from a new type of sign problem. In the canonical approach, the grand partition function is written as a fugacity expansion: $Z_G(μ,T) = \sum_n Z_C(n,T) ξ^n$, where $ξ=\exp(μ/T)$ is the fugacity, and $Z_C(n,T)$ are given as averages over a Monte Carlo update, $\langle z_n\rangle$. We show that the complex phase of $z_n$ is proportional to $n$ at each Monte Carlo step. Although $\langle z_n\rangle$ take real positive values, the values of $z_n$ fluctuate rapidly when $n$ is large, especially in the confinement phase, which gives a limit on $n$. We discuss possible remedies for this problem.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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