<p>We consider the universal behavior of half-BPS correlators in <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25848_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N} \)</EquationSource> </InlineEquation> = 4 super-Yang-Mills in the cusp limit where two consecutive separations <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25848_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>x</mi> <mn>12</mn> <mn>2</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {x}_{12}^2 \)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25848_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>x</mi> <mn>23</mn> <mn>2</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {x}_{23}^2 \)</EquationSource> </InlineEquation> become lightlike. Through the Lagrangian insertion procedure, the Sudakov double-logarithmic divergence of the <i>n</i>-point correlator is related to the (<i>n</i> + 1)-point correlator where the inserted Lagrangian “pinches” to the soft-collinear region of the cusp. We formulate this constraint as a new <i>graphical rule</i> for the <i>f</i>-graphs of the four-point correlator, which turns out to be the most constraining rule known so far. By exploiting this single graphical rule, we bootstrap the planar integrand of the four-point correlator up to ten loops (<i>n</i> = 14) and fix all 22024902 but one coefficient at eleven loops (<i>n</i> = 15); the remaining coefficient is then fixed using the triangle rule. We verify the “Catalan conjecture” for the coefficients of the family of <i>f</i>-graphs known as “anti-prisms” where the coefficient of the twelve-loop (<i>n</i> = 16) anti-prism is found to be −42 by a local analysis of the bootstrap equations. We also comment on the implication of our graphical rule for the non-planar contributions.</p>

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The cusp limit of correlators and a new graphical bootstrap for correlators/amplitudes to eleven loops

  • Song He,
  • Canxin Shi,
  • Yichao Tang,
  • Yao-Qi Zhang

摘要

We consider the universal behavior of half-BPS correlators in N \( \mathcal{N} \) = 4 super-Yang-Mills in the cusp limit where two consecutive separations x 12 2 \( {x}_{12}^2 \) , x 23 2 \( {x}_{23}^2 \) become lightlike. Through the Lagrangian insertion procedure, the Sudakov double-logarithmic divergence of the n-point correlator is related to the (n + 1)-point correlator where the inserted Lagrangian “pinches” to the soft-collinear region of the cusp. We formulate this constraint as a new graphical rule for the f-graphs of the four-point correlator, which turns out to be the most constraining rule known so far. By exploiting this single graphical rule, we bootstrap the planar integrand of the four-point correlator up to ten loops (n = 14) and fix all 22024902 but one coefficient at eleven loops (n = 15); the remaining coefficient is then fixed using the triangle rule. We verify the “Catalan conjecture” for the coefficients of the family of f-graphs known as “anti-prisms” where the coefficient of the twelve-loop (n = 16) anti-prism is found to be −42 by a local analysis of the bootstrap equations. We also comment on the implication of our graphical rule for the non-planar contributions.