The Belle Collaboration has recently measured the complete set of angular coefficient functions for the exclusive decays <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mover accent="true"><a:mi>B</a:mi><a:mo stretchy="false">¯</a:mo></a:mover><a:mo stretchy="false">→</a:mo><a:msup><a:mi>D</a:mi><a:mo>*</a:mo></a:msup><a:mo stretchy="false">(</a:mo><a:mi>D</a:mi><a:mi>π</a:mi><a:mo stretchy="false">)</a:mo><a:mo>ℓ</a:mo><a:msub><a:mover accent="true"><a:mi>ν</a:mi><a:mo stretchy="false">¯</a:mo></a:mover><a:mo>ℓ</a:mo></a:msub></a:math>, with <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:mo>ℓ</j:mo><j:mo>=</j:mo><j:mi>e</j:mi></j:math>, <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"><l:mrow><l:mi>μ</l:mi></l:mrow></l:math>, in four bins of the parameter <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"><n:mi>w</n:mi><n:mo>=</n:mo><n:mfrac><n:mrow><n:msubsup><n:mi>m</n:mi><n:mi>B</n:mi><n:mn>2</n:mn></n:msubsup><n:mo stretchy="false">+</n:mo><n:msubsup><n:mi>m</n:mi><n:msup><n:mi>D</n:mi><n:mo stretchy="false">*</n:mo></n:msup><n:mn>2</n:mn></n:msubsup><n:mo stretchy="false">−</n:mo><n:msup><n:mi>q</n:mi><n:mn>2</n:mn></n:msup></n:mrow><n:mrow><n:mn>2</n:mn><n:msub><n:mi>m</n:mi><n:mi>B</n:mi></n:msub><n:msub><n:mi>m</n:mi><n:msup><n:mi>D</n:mi><n:mo stretchy="false">*</n:mo></n:msup></n:msub></n:mrow></n:mfrac></n:math>, with <t:math xmlns:t="http://www.w3.org/1998/Math/MathML" display="inline"><t:mi>q</t:mi></t:math> the lepton pair momentum [M. T. Prim (Belle Collaboration), ]. Under the assumption that physics beyond the Standard Model does not contribute to such modes, the measurements are useful to determine the hadronic form factors describing the <v:math xmlns:v="http://www.w3.org/1998/Math/MathML" display="inline"><v:mi>B</v:mi><v:mo stretchy="false">→</v:mo><v:msup><v:mi>D</v:mi><v:mo>*</v:mo></v:msup></v:math> matrix elements of the Standard Model weak current, and to improve the determination of <y:math xmlns:y="http://www.w3.org/1998/Math/MathML" display="inline"><y:mo stretchy="false">|</y:mo><y:msub><y:mi>V</y:mi><y:mrow><y:mi>c</y:mi><y:mi>b</y:mi></y:mrow></y:msub><y:mo stretchy="false">|</y:mo></y:math>. On the other hand, they can be used to assess the impact of possible new physics contributions. In a bottom-up approach, we extend the Standard Model effective Hamiltonian governing this mode with the inclusion of the full set of Lorentz invariant <cb:math xmlns:cb="http://www.w3.org/1998/Math/MathML" display="inline"><cb:mrow><cb:mi mathvariant="normal">d</cb:mi><cb:mo>=</cb:mo><cb:mn>6</cb:mn></cb:mrow></cb:math> operators compatible with the gauge symmetry of the theory. The measured angular coefficient functions can tightly constrain the couplings in the generalized Hamiltonian. We present the first results of this analysis, discussing how improvements can be achieved when more complete data on the angular coefficient functions will be available. Published by the American Physical Society 2024
No takes yet. Share an insight, caveat, or question.
Colangelo et al. (2024) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: