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arXiv 2501.09693math.SPmath-phmath.MPmath.PR
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基于随机游走展开的量子图热含量Faber-Krahn不等式

Faber-Krahn inequality for the heat content on quantum graphs via random walk expansion

Patrizio Bifulco, Matthias Täufer

AI总结:

该研究探究量子图热含量的Rayleigh-Faber-Krahn不等式类似结论,用谱理论和随机游走方法证明其在大小时间极端情形成立,还提出热含量的新随机游走表达式,全时段结论仍待解决。

摘要:

我们研究量子图上的热含量,并探究Rayleigh-Faber-Krahn不等式的类似结论是否成立。该结论指的是,在体积相等的图中,时刻$T$的热含量将由区间(对应经典Rayleigh-Faber-Krahn不等式中球的图类比结构)取到最大值。我们证明该结论在极端时刻(即小时间和大时间情形下)成立。为此我们采用两种互补的方法:大时间区域下,我们借助谱理论方法,运用Mercer定理;小时间区域则通过随机游走方法处理,用到Feynman-Kac公式与度量图上的布朗运动。特别地,在证明小时间情形的过程中,我们推导出热含量的一种新表达式,将其表示为(离散)随机游走的期望返回时间的正线性组合——与已有的著名方法(如Roth公式)相比,该表述似乎能带来更多洞见,且对我们的证明至关重要。度量图上热含量的Rayleigh-Faber-Krahn不等式是否在所有时刻都成立这一问题仍未解决。

英文摘要:

We study the heat content on quantum graphs and investigate whether an analogon of the Rayleigh-Faber-Krahn inequality holds. This means that heat content at time $T$ among graphs of equal volume would be maximized by intervals (the graph analogon of balls as in the classic Rayleigh-Faber-Krahn inequality). We prove that this holds at extremal times, that is at small and at large times. For this, we employ two complementary approaches: In the large time regime, we rely on a spectral-theoretic approach, using Mercer's theorem whereas the small-time regime is dealt with by a random walk approach using the Feynman-Kac formula and Brownian motions on metric graphs. In particular, in proving the latter, we develop a new expression for the heat content as a positive linear combination of expected return times of (discrete) random walks - a formulation which seems to yield additional insights compared to previously available methods such as the celebrated Roth formula and which is crucial for our proof. The question whether a Rayleigh-Faber-Krahn inequality for the heat content on metric graphs holds at all times remains open.

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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