Ask a Question

Prefer a chat interface with context about you and your work?

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>c</mml:mi><mml:mo>→</mml:mo><mml:mi>u</mml:mi><mml:mi>γ</mml:mi></mml:math>in Cabibbo suppressed<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>D</mml:mi></mml:math>meson radiative weak decays

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>c</mml:mi><mml:mo>→</mml:mo><mml:mi>u</mml:mi><mml:mi>γ</mml:mi></mml:math>in Cabibbo suppressed<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>D</mml:mi></mml:math>meson radiative weak decays

We investigate Cabibbo suppressed ${D}^{0}$, ${D}^{+}$, and ${D}_{s}^{+}$ radiative weak decays in order to find the best mode to test $c\ensuremath{\rightarrow}u\ensuremath{\gamma}$ decay. Combining heavy quark effective theory and the chiral Lagrangian approach we determine the decay widths. We calculate $\frac{\ensuremath{\Gamma}({D}^{0}\ensuremath{\rightarrow}\frac{{\ensuremath{\rho}}^{0}}{\ensuremath{\omega}\ensuremath{\gamma}})}{\ensuremath{\Gamma}({D}^{0}\ensuremath{\rightarrow}{\overline{K}}^{*0}\ensuremath{\gamma})}$, previously proposed to search for possible new physics. However, we …