The $$Q_{1,2}$$ – $$Q_7$$ interference contributions to $$b \rightarrow s \gamma $$ at $${\mathcal O}(\alpha _{\mathrm s}^2)$$ for the physical value of $$m_c$$
Tóm tắt
The
$$\bar{B}\rightarrow X_s\gamma $$
branching ratio is currently measured with around
$$5\%$$
accuracy. Further improvement is expected from Belle II. To match such a precision on the theoretical side, evaluation of
$${\mathcal O}(\alpha _{\mathrm s}^2)$$
corrections to the partonic decay
$$b \rightarrow X_s^\textrm{part}\gamma $$
are necessary, which includes the
$$b \rightarrow s \gamma $$
,
$$b \rightarrow s g\gamma $$
,
$$b \rightarrow s gg\gamma $$
,
$$b \rightarrow sq\bar{q}\gamma $$
decay channels. Here, we evaluate the unrenormalized contribution to
$$b \rightarrow s \gamma $$
that stems from the interference of the photonic dipole operator
$$Q_7$$
and the current–current operators
$$Q_1$$
and
$$Q_2$$
. Our results, obtained in the cut propagator approach at the 4-loop level, agree with those found in parallel by Fael et al. who have applied the amplitude approach at the 3-loop level. Partial results for the same quantities recently determined by Greub et al. agree with our findings, too.
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