arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 1707.06259math-phmath.COmath.MPmath.PRnlin.SI
收藏

量子加权Hurwitz数的零温极限

Zero-temperature limit of quantum weighted Hurwitz numbers

J. Harnad, Janosch Ortmann

摘要:

量子加权双Hurwitz数的配分函数可以用逸度为零的量子玻色气体的能量分布来解释。我们计算了零温极限下的配分函数的首项和量子加权Hurwitz数$T \rightarrow 0$,以及次阶修正。的领导项重现的情况下,均匀加权Hurwitz数的Belyi曲线。特别地,KP或Toda $τ$ -函数作为量子Hurwitz数的生成函数被示出在极限中以给出Belyi曲线的生成函数,并且在适当的缩放下,对于Hurwitz数的配分函数、权重和期望也是如此。

英文摘要:

The partition function for quantum weighted double Hurwitz numbers can be interpreted in terms of the energy distribution of a quantum Bose gas with vanishing fugacity. We compute the leading term of the partition function and the quantum weighted Hurwitz numbers in the zero temperature limit $T \rightarrow 0$, as well as the next order corrections. The leading term is shown to reproduce the case of uniformly weighted Hurwitz numbers of Belyi curves. In particular, the KP or Toda $τ$-function serving as generating function for the quantum Hurwitz numbers is shown in the limit to give the one for Belyi curves and, with suitable scaling, the same holds true for the partition function, the weights and the expectations of Hurwitz numbers.

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。

↑