<p>We investigate the upper tail distribution of the partition function of the directed polymer in a random environment on <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5246_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathbb {Z}}} ^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">Z</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> in the weak disorder phase. We show that the distribution of the infinite volume partition function <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5246_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(W^{\beta }_{\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>W</mi> <mi>∞</mi> <mi>β</mi> </msubsup> </math></EquationSource> </InlineEquation> displays a power-law decay, with an exponent <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5246_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="133" /> </InlineMediaObject> <EquationSource Format="TEX">\(p^*(\beta )\in [1+\frac{2}{d},\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>p</mi> <mo>∗</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>β</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <mrow> <mo stretchy="false">[</mo> <mn>1</mn> <mo>+</mo> <mfrac> <mn>2</mn> <mi>d</mi> </mfrac> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We also prove that the distribution of the suprema of the point-to-point and point-to-line partition functions display the same behavior. On the way to these results, we prove a technical estimate of independent interest: the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5246_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-norm of the partition function at the time when it overshoots a high value <i>A</i> is comparable to <i>A</i>. We use this estimate to extend the validity of many recent results that were proved under the assumption that the environment is upper bounded.</p>

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The Tail Distribution of the Partition Function for Directed Polymers in the Weak Disorder Phase

  • Stefan Junk,
  • Hubert Lacoin

摘要

We investigate the upper tail distribution of the partition function of the directed polymer in a random environment on \({{\mathbb {Z}}} ^d\) Z d in the weak disorder phase. We show that the distribution of the infinite volume partition function \(W^{\beta }_{\infty }\) W β displays a power-law decay, with an exponent \(p^*(\beta )\in [1+\frac{2}{d},\infty )\) p ( β ) [ 1 + 2 d , ) . We also prove that the distribution of the suprema of the point-to-point and point-to-line partition functions display the same behavior. On the way to these results, we prove a technical estimate of independent interest: the \(L^p\) L p -norm of the partition function at the time when it overshoots a high value A is comparable to A. We use this estimate to extend the validity of many recent results that were proved under the assumption that the environment is upper bounded.