我们考虑吉布斯采样器，或热浴动力学与对数压缩测量有关${\mathbb{<trans\; data-src="R">R（右）</trans>}}^{\mathit{<trans\; data-src="N">N个</trans>}}$描述$<trans\; data-src="\nabla ">\nabla </trans>\mathit{<trans\; data-src="\phi ">\phi </trans>}$具有凸势的界面。在对势的最小假设下，我们发现过程的谱间隙总是由${\mathrm{<trans\; data-src="gap">缺口</trans>}}_{\mathit{<trans\; data-src="N">N个</trans>}}<trans\; data-src="=">=</trans>\mathrm{<trans\; data-src="1">1</trans>}<trans\; data-src="-">负极</trans><trans\; data-src="cos">余弦</trans><trans\; data-src="(">(</trans>\mathit{<trans\; data-src="\pi ">\pi </trans>}<trans\; data-src="/">/</trans>\mathit{<trans\; data-src="N">N个</trans>}<trans\; data-src=")">)</trans>$以及所有这些$\mathit{<trans\; data-src="ϵ">ϵ</trans>}<trans\; data-src="\in ">\in </trans><trans\; data-src="(">(</trans>\mathrm{<trans\; data-src="0">0</trans>}<trans\; data-src=",">,</trans>\mathrm{<trans\; data-src="1">1</trans>}<trans\; data-src=")">)</trans>$，其ϵ-混合时间满足${\mathit{<trans\; data-src="T">T型</trans>}}_{\mathit{<trans\; data-src="N">N个</trans>}}<trans\; data-src="(">(</trans>\mathit{<trans\; data-src="ϵ">ϵ</trans>}<trans\; data-src=")">)</trans><trans\; data-src="\sim ">\sim </trans>\frac{<trans\; data-src="log">日志</trans>\mathit{<trans\; data-src="N">N个</trans>}}{\mathrm{<trans\; data-src="2">2</trans>}{\mathrm{<trans\; data-src="gap">缺口</trans>}}_{\mathit{<trans\; data-src="N">N个</trans>}}}$作为$\mathit{<trans\; data-src="N">N个</trans>}<trans\; data-src="\to ">\to </trans>\mathrm{<trans\; data-src="\infty ">\infty </trans>}$从而确立了截止现象。结果揭示了一种普遍的行为，即它们不依赖于势的选择。

Nous considérons l’ecantillonneur de Gibbs，aussi appelédynamic“热浴”，南部计量协会${\mathbb{<trans\; data-src="R">R（右）</trans>}}^{\mathit{<trans\; data-src="N">N个</trans>}}$et décrivant des接口$<trans\; data-src="\nabla ">\nabla </trans>\mathit{<trans\; data-src="\phi ">\phi </trans>}$avec电位凸。潜在的最低限度的低保制度，努斯蒙特龙que le trou spectrum du processus est toujours donnépar${\mathrm{<trans\; data-src="gap">缺口</trans>}}_{\mathit{<trans\; data-src="N">N个</trans>}}<trans\; data-src="=">=</trans>\mathrm{<trans\; data-src="1">1</trans>}<trans\; data-src="-">负极</trans><trans\; data-src="cos">余弦</trans><trans\; data-src="(">(</trans>\mathit{<trans\; data-src="\pi ">\pi </trans>}<trans\; data-src="/">/</trans>\mathit{<trans\; data-src="N">N个</trans>}<trans\; data-src=")">)</trans>$，等等$\mathit{<trans\; data-src="ϵ">ϵ</trans>}<trans\; data-src="\in ">\in </trans><trans\; data-src="(">(</trans>\mathrm{<trans\; data-src="0">0</trans>}<trans\; data-src=",">,</trans>\mathrm{<trans\; data-src="1">1</trans>}<trans\; data-src=")">)</trans>$法国巴黎圣母院ϵ满意${\mathit{<trans\; data-src="T">T型</trans>}}_{\mathit{<trans\; data-src="N">N个</trans>}}<trans\; data-src="(">(</trans>\mathit{<trans\; data-src="ϵ">ϵ</trans>}<trans\; data-src=")">)</trans><trans\; data-src="\sim ">\sim </trans>\frac{<trans\; data-src="log">日志</trans>\mathit{<trans\; data-src="N">N个</trans>}}{\mathrm{<trans\; data-src="2">2</trans>}{\mathrm{<trans\; data-src="gap">缺口</trans>}}_{\mathit{<trans\; data-src="N">N个</trans>}}}$量子力学$\mathit{<trans\; data-src="N">N个</trans>}<trans\; data-src="\to ">\to </trans>\mathrm{<trans\; data-src="\infty ">\infty </trans>}$在截止日期前，必须提交一份表格。这些结果令人振奋的是，非成分的普遍性，其重要性取决于潜在的选择。