<p>The non-leptonic <i>D</i><sup>0</sup> → <i>K</i><sup>−</sup><i>K</i><sup>+</sup> and <i>D</i><sup>0</sup> → <i>π</i><sup>−</sup><i>π</i><sup>+</sup> decays are powerful probes of the Standard Model and are related to each other through the <i>U</i> -spin symmetry of the strong interaction. Using lattice QCD inputs we calculate the corresponding colour-allowed tree amplitudes in factorisation and demonstrate that non-factorisable contributions and <i>U</i> -spin-breaking effects at the level of 50% allow us to accommodate the measured branching ratios in the Standard Model. An exciting direct probe of such non-factorisable and <i>U</i> -spin breaking effects is provided by the <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>D</mi> <mn>0</mn> </msup> <mo>→</mo> <msubsup> <mi>K</mi> <mi mathvariant="normal">S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi mathvariant="normal">S</mi> <mn>0</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {D}^0\to {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \)</EquationSource> </InlineEquation> channel. This decay is governed by non-factorisable exchange topologies and essentially vanishes in the <i>U</i> -spin limit, although it is experimentally well established with a prominent branching ratio. Extrapolating our <i>D</i><sup>0</sup> → <i>K</i><sup>−</sup><i>K</i><sup>+</sup> results using the isospin symmetry, we find a consistent benchmark picture. Specifically, we can accommodate the measured <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>D</mi> <mn>0</mn> </msup> <mo>→</mo> <msubsup> <mi>K</mi> <mi mathvariant="normal">S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi mathvariant="normal">S</mi> <mn>0</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {D}^0\to {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \)</EquationSource> </InlineEquation> branching ratio with <i>U</i> -spin-breaking effects at the 50% level and exchange amplitudes at the level of 50% of the colour-allowed <i>D</i><sup>0</sup> → <i>K</i><sup>−</sup><i>K</i><sup>+</sup>, <i>D</i><sup>0</sup> → <i>π</i><sup>−</sup><i>π</i><sup>+</sup> tree contributions. Finally, we explore the resulting range for direct CP violation in <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>D</mi> <mn>0</mn> </msup> <mo>→</mo> <msubsup> <mi>K</mi> <mi mathvariant="normal">S</mi> <mn>0</mn> </msubsup> <msubsup> <mi>K</mi> <mi mathvariant="normal">S</mi> <mn>0</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {D}^0\to {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \)</EquationSource> </InlineEquation>, obtaining upper bounds in our benchmark scenarios of a few per mille, offering an exciting target for future measurements.</p>

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Standard model benchmarks for D0KK+, ππ+, \( {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \) decays

  • Robert Fleischer,
  • Maria Laura Piscopo,
  • K. Keri Vos,
  • B. Yağmur Zubaroğlu

摘要

The non-leptonic D0KK+ and D0ππ+ decays are powerful probes of the Standard Model and are related to each other through the U -spin symmetry of the strong interaction. Using lattice QCD inputs we calculate the corresponding colour-allowed tree amplitudes in factorisation and demonstrate that non-factorisable contributions and U -spin-breaking effects at the level of 50% allow us to accommodate the measured branching ratios in the Standard Model. An exciting direct probe of such non-factorisable and U -spin breaking effects is provided by the D 0 K S 0 K S 0 \( {D}^0\to {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \) channel. This decay is governed by non-factorisable exchange topologies and essentially vanishes in the U -spin limit, although it is experimentally well established with a prominent branching ratio. Extrapolating our D0KK+ results using the isospin symmetry, we find a consistent benchmark picture. Specifically, we can accommodate the measured D 0 K S 0 K S 0 \( {D}^0\to {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \) branching ratio with U -spin-breaking effects at the 50% level and exchange amplitudes at the level of 50% of the colour-allowed D0KK+, D0ππ+ tree contributions. Finally, we explore the resulting range for direct CP violation in D 0 K S 0 K S 0 \( {D}^0\to {K}_{\mathrm{S}}^0{K}_{\mathrm{S}}^0 \) , obtaining upper bounds in our benchmark scenarios of a few per mille, offering an exciting target for future measurements.