<p>The precise measurement of the width difference ∆Γ<sub><i>s</i></sub> among the mass eigenstates of the <i>B</i><sub><i>s</i></sub>-<InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <msub> <mover accent="true"> <mi>B</mi> <mo stretchy="true">¯</mo> </mover> <mi>s</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {\overline{B}}_s \)</EquationSource> </InlineEquation> system requires the calculation of the corresponding decay matrix to order <i>α</i><sub><i>s</i></sub>/<i>m</i><sub><i>b</i></sub>. QCD corrections to power-suppressed terms in the Heavy Quark Expansion involve the renormalization of dimension-7 four-quark operators for which no general methodology is available yet. In the <InlineEquation ID="IEq3"> <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> scheme one-loop corrections to matrix elements of dimension-7 operators violate the power counting, but we find the responsible terms to be infrared-finite and show that they can be absorbed into finite counterterms proportional to dimension-6 operators. We calculate all these counterterms and subsequently verify the consistency of our results with hadronic matrix elements calculated in the limit of a large number <i>N</i><sub><i>c</i></sub> of colours. The condition of correct power counting implies constraints on the possible definitions of evanescent operators.</p>

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Decay matrix of B-\( \overline{B} \) mixing: mixing of dimension-seven operators into dimension-six operators under renormalization

  • Artyom Hovhannisyan,
  • Ulrich Nierste

摘要

The precise measurement of the width difference ∆Γs among the mass eigenstates of the Bs- B ¯ s \( {\overline{B}}_s \) system requires the calculation of the corresponding decay matrix to order αs/mb. QCD corrections to power-suppressed terms in the Heavy Quark Expansion involve the renormalization of dimension-7 four-quark operators for which no general methodology is available yet. In the MS ¯ \( \overline{\textrm{MS}} \) scheme one-loop corrections to matrix elements of dimension-7 operators violate the power counting, but we find the responsible terms to be infrared-finite and show that they can be absorbed into finite counterterms proportional to dimension-6 operators. We calculate all these counterterms and subsequently verify the consistency of our results with hadronic matrix elements calculated in the limit of a large number Nc of colours. The condition of correct power counting implies constraints on the possible definitions of evanescent operators.