<p>The Kaon bag parameter <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27091_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msub> <mover accent="true"> <mi>B</mi> <mo stretchy="true">̂</mo> </mover> <mi>K</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {\hat{B}}_K \)</EquationSource> </InlineEquation> plays a critical role in constraining the parameters of the CKM matrix and in probing physics beyond the Standard Model. In this work, we improve the precision of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27091_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msub> <mover accent="true"> <mi>B</mi> <mo stretchy="true">̂</mo> </mover> <mi>K</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {\hat{B}}_K \)</EquationSource> </InlineEquation> to next-to-next-to-leading order (NNLO) and provide world averages for both 3- and 4-flavour theories. In the course of this, as our main technical development, we carry out the two-loop matching between the RI-(S)MOM and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27091_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mi>MS</mi> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overline{\textrm{MS}} \)</EquationSource> </InlineEquation> schemes. Our world averages combine all available lattice data, including conversion between the 3- and 4-flavour theories as appropriate. We obtain the result <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27091_Article_IEq5.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="141" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mover accent="true"> <mi>B</mi> <mo stretchy="true">̂</mo> </mover> <mi>K</mi> <mfenced close=")" open="("> <mrow> <mi>f</mi> <mo>=</mo> <mn>3</mn> </mrow> </mfenced> </msubsup> <mo>=</mo> <mn>0.7627</mn> <mfenced close=")" open="("> <mn>60</mn> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( {\hat{B}}_K^{\left(f=3\right)}=0.7627(60) \)</EquationSource> </InlineEquation>, which comprises the complete set of 3- and 4-flavour lattice results and can be used directly in phenomenological applications. The error is dominated by lattice uncertainties and missing higher-order corrections (residual scale dependence). Our averages include a PDG rescaling factor of 1.28 reflecting a mild tension among the lattice inputs after inclusion of NNLO corrections in the scheme conversion and matching across flavour thresholds. Our averages imply an updated value |<i>ϵ</i><sub><i>K</i></sub>| = 2<i>.</i>171(65)<sub>pert.</sub>(71)<sub>non-pert.</sub>(153)<sub>param.</sub> × 10<sup><i>−</i>3</sup>. We briefly discuss applications of our results to <i>D</i>-meson mixing.</p>

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RI-(S)MOM to \( \overline{\textrm{MS}} \) conversion for BK at two-loop order

  • Martin Gorbahn,
  • Sebastian Jäger,
  • Sandra Kvedaraitė

摘要

The Kaon bag parameter B ̂ K \( {\hat{B}}_K \) plays a critical role in constraining the parameters of the CKM matrix and in probing physics beyond the Standard Model. In this work, we improve the precision of B ̂ K \( {\hat{B}}_K \) to next-to-next-to-leading order (NNLO) and provide world averages for both 3- and 4-flavour theories. In the course of this, as our main technical development, we carry out the two-loop matching between the RI-(S)MOM and MS ¯ \( \overline{\textrm{MS}} \) schemes. Our world averages combine all available lattice data, including conversion between the 3- and 4-flavour theories as appropriate. We obtain the result B ̂ K f = 3 = 0.7627 60 \( {\hat{B}}_K^{\left(f=3\right)}=0.7627(60) \) , which comprises the complete set of 3- and 4-flavour lattice results and can be used directly in phenomenological applications. The error is dominated by lattice uncertainties and missing higher-order corrections (residual scale dependence). Our averages include a PDG rescaling factor of 1.28 reflecting a mild tension among the lattice inputs after inclusion of NNLO corrections in the scheme conversion and matching across flavour thresholds. Our averages imply an updated value |ϵK| = 2.171(65)pert.(71)non-pert.(153)param. × 103. We briefly discuss applications of our results to D-meson mixing.