<p>We consider the Kardar-Parisi-Zhang equation on the interval [0,&#xa0;<i>L</i>] with Neumann type boundary conditions and boundary parameters <i>u</i>,&#xa0;<i>v</i>. We show that the <i>k</i>-th order cumulant of the height behaves as <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3496_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="TEX">\(c_k(L,u,v)\, t\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>c</mi> <mi>k</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>L</mi> <mo>,</mo> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="0.166667em" /> <mi>t</mi> </mrow> </math></EquationSource> </InlineEquation> in the large time limit <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3496_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(t \rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, and we compute the coefficients <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3496_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="73" /> </InlineMediaObject> <EquationSource Format="TEX">\(c_k(L,u,v)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>c</mi> <mi>k</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>L</mi> <mo>,</mo> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We obtain an expression for the upper tail large deviation function of the height. We also consider the limit of large <i>L</i>, with <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3496_Article_IEq4.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="80" /> </InlineMediaObject> <EquationSource Format="TEX">\(u=\tilde{u}/\sqrt{L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <mover accent="true"> <mi>u</mi> <mo stretchy="false">~</mo> </mover> <mo stretchy="false">/</mo> <msqrt> <mi>L</mi> </msqrt> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3496_Article_IEq5.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="79" /> </InlineMediaObject> <EquationSource Format="TEX">\(u={\tilde{v}}/\sqrt{L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <mover accent="true"> <mi>v</mi> <mo stretchy="false">~</mo> </mover> <mo stretchy="false">/</mo> <msqrt> <mi>L</mi> </msqrt> </mrow> </math></EquationSource> </InlineEquation>, which should give the same quantities for the two parameter family <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3496_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(({\tilde{u}}, {\tilde{v}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mover accent="true"> <mi>u</mi> <mo stretchy="false">~</mo> </mover> <mo>,</mo> <mover accent="true"> <mi>v</mi> <mo stretchy="false">~</mo> </mover> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> KPZ fixed point on the interval. We employ two complementary methods. On the one hand we adapt to the interval the replica Bethe ansatz method pioneered by Brunet and Derrida for the periodic case. On the other hand, we perform a scaling limit using previous results available for the open ASEP. The latter method allows to express the cumulants of the KPZ equation in terms a functional equation involving an integral operator.</p>

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Large Time Cumulants of the KPZ Equation on an Interval

  • Guillaume Barraquand,
  • Pierre Le Doussal

摘要

We consider the Kardar-Parisi-Zhang equation on the interval [0, L] with Neumann type boundary conditions and boundary parameters uv. We show that the k-th order cumulant of the height behaves as \(c_k(L,u,v)\, t\) c k ( L , u , v ) t in the large time limit \(t \rightarrow +\infty \) t + , and we compute the coefficients \(c_k(L,u,v)\) c k ( L , u , v ) . We obtain an expression for the upper tail large deviation function of the height. We also consider the limit of large L, with \(u=\tilde{u}/\sqrt{L}\) u = u ~ / L , \(u={\tilde{v}}/\sqrt{L}\) u = v ~ / L , which should give the same quantities for the two parameter family \(({\tilde{u}}, {\tilde{v}})\) ( u ~ , v ~ ) KPZ fixed point on the interval. We employ two complementary methods. On the one hand we adapt to the interval the replica Bethe ansatz method pioneered by Brunet and Derrida for the periodic case. On the other hand, we perform a scaling limit using previous results available for the open ASEP. The latter method allows to express the cumulants of the KPZ equation in terms a functional equation involving an integral operator.