<p>Two-dimensional conformal field theories (CFTs) defined on non-orientable Riemann surfaces obey consistency Cardy conditions analogous to those in the orientable case. We revisit those conditions for irrational theories with central charge <i>c</i> &gt; 1 in the context of two-point functions of primaries on the Real Projective plane <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27175_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi mathvariant="double-struck">RP</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {\mathbbm{RP}}^2 \)</EquationSource> </InlineEquation> and the partition function on the Klein bottle <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27175_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi mathvariant="double-struck">K</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {\mathbbm{K}}^2 \)</EquationSource> </InlineEquation>. Using the irrational versions of the Virasoro fusion and modular kernels we derive universal expressions for the non-orientable CFT data at large conformal dimension, assuming a gap in the spectrum of scalar primaries. In particular, we derive asymptotic formulas at finite central charge for the averaged Light-Light-Heavy product <i>C</i><sub><i>LLH</i></sub> × Γ<sub><i>H</i></sub> of OPE coefficients with the <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27175_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi mathvariant="double-struck">RP</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {\mathbbm{RP}}^2 \)</EquationSource> </InlineEquation> one-point function normalizations, as well as for the parity-weighted density of heavy scalar primaries (or equivalently the density of heavy <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27175_Article_IEq4.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi mathvariant="normal">Γ</mi> <mi>H</mi> <mn>2</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\Gamma}_H^2 \)</EquationSource> </InlineEquation>). We discuss the gravitational interpretation of the results.</p>

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Universal dynamics in non-orientable CFT2

  • Ioannis Tsiares

摘要

Two-dimensional conformal field theories (CFTs) defined on non-orientable Riemann surfaces obey consistency Cardy conditions analogous to those in the orientable case. We revisit those conditions for irrational theories with central charge c > 1 in the context of two-point functions of primaries on the Real Projective plane RP 2 \( {\mathbbm{RP}}^2 \) and the partition function on the Klein bottle K 2 \( {\mathbbm{K}}^2 \) . Using the irrational versions of the Virasoro fusion and modular kernels we derive universal expressions for the non-orientable CFT data at large conformal dimension, assuming a gap in the spectrum of scalar primaries. In particular, we derive asymptotic formulas at finite central charge for the averaged Light-Light-Heavy product CLLH × ΓH of OPE coefficients with the RP 2 \( {\mathbbm{RP}}^2 \) one-point function normalizations, as well as for the parity-weighted density of heavy scalar primaries (or equivalently the density of heavy Γ H 2 \( {\Gamma}_H^2 \) ). We discuss the gravitational interpretation of the results.