<p>We consider spread-out models of lattice trees and lattice animals on <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_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>, for <i>d</i> above the upper critical dimension <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(d_{\textrm{c}}=8\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>d</mi> <mtext>c</mtext> </msub> <mo>=</mo> <mn>8</mn> </mrow> </math></EquationSource> </InlineEquation>. We define a correlation length and prove that it diverges as <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\((p_c-p)^{-1/4}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>p</mi> <mi>c</mi> </msub> <mo>-</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>4</mn> </mrow> </msup> </math></EquationSource> </InlineEquation> at the critical point <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(p_c\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mi>c</mi> </msub> </math></EquationSource> </InlineEquation>. Using this, we prove that the near-critical two-point function is bounded above by <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq5.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="223" /> </InlineMediaObject> <EquationSource Format="TEX">\(C|x|^{-(d-2)}\exp [-c(p_c-p)^{1/4}|x|]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi>C</mi> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mo stretchy="false">(</mo> <mi>d</mi> <mo>-</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </msup> <mrow> <mo>exp</mo> <mo stretchy="false">[</mo> <mo>-</mo> <mi>c</mi> </mrow> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>p</mi> <mi>c</mi> </msub> <mo>-</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>4</mn> </mrow> </msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We apply the near-critical bound to study lattice trees and lattice animals on a discrete <i>d</i>-dimensional torus (with <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(d &gt; d_{\textrm{c}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>&gt;</mo> <msub> <mi>d</mi> <mtext>c</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation>) of volume <i>V</i>. For <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq7.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(p_c-p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>p</mi> <mi>c</mi> </msub> <mo>-</mo> <mi>p</mi> </mrow> </math></EquationSource> </InlineEquation> of order <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq8.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(V^{-1/2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>V</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, we prove that the torus susceptibility is of order <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq9.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(V^{1/4}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>V</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>4</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, and that the torus two-point function behaves as <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq10.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="122" /> </InlineMediaObject> <EquationSource Format="TEX">\(|x|^{-(d-2)} + V^{-3/4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mo stretchy="false">(</mo> <mi>d</mi> <mo>-</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </msup> <mo>+</mo> <msup> <mi>V</mi> <mrow> <mo>-</mo> <mn>3</mn> <mo stretchy="false">/</mo> <mn>4</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> and thus has a plateau of size <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10955_2025_3414_Article_IEq11.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(V^{-3/4}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>V</mi> <mrow> <mo>-</mo> <mn>3</mn> <mo stretchy="false">/</mo> <mn>4</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>. The proofs require significant extensions of previous results obtained using the lace expansion.</p>

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Near-Critical and Finite-Size Scaling for High-Dimensional Lattice Trees and Animals

  • Yucheng Liu,
  • Gordon Slade

摘要

We consider spread-out models of lattice trees and lattice animals on \({\mathbb {Z}}^d\) Z d , for d above the upper critical dimension \(d_{\textrm{c}}=8\) d c = 8 . We define a correlation length and prove that it diverges as \((p_c-p)^{-1/4}\) ( p c - p ) - 1 / 4 at the critical point \(p_c\) p c . Using this, we prove that the near-critical two-point function is bounded above by \(C|x|^{-(d-2)}\exp [-c(p_c-p)^{1/4}|x|]\) C | x | - ( d - 2 ) exp [ - c ( p c - p ) 1 / 4 | x | ] . We apply the near-critical bound to study lattice trees and lattice animals on a discrete d-dimensional torus (with \(d > d_{\textrm{c}}\) d > d c ) of volume V. For \(p_c-p\) p c - p of order \(V^{-1/2}\) V - 1 / 2 , we prove that the torus susceptibility is of order \(V^{1/4}\) V 1 / 4 , and that the torus two-point function behaves as \(|x|^{-(d-2)} + V^{-3/4}\) | x | - ( d - 2 ) + V - 3 / 4 and thus has a plateau of size \(V^{-3/4}\) V - 3 / 4 . The proofs require significant extensions of previous results obtained using the lace expansion.