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The function that does that is here |
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For LFV B meson decays I find in the 'bpll_lfv.py' file there is no specification of different flavor of quarks! Although in the file it is mentioned that for Lepton flavour violating decays
def _define_obs_B_Mll(M, ll):
_process_tex = _hadr_lfv[M]['tex']+' '+_tex_lfv[''.join(ll)]
_process_taxonomy = r'Process :: $b$ hadron decays :: FCNC decays :: $B\to P\ell^+\ell^-$ :: $' + _process_tex + r"$"
_obs_name = "BR("+M+''.join(ll)+")"
etc.
I'm not sure how is it referring to different quark flavors for decays such as B-Ke\mu which is at quark level 'b->s' transition! Is it picking up that information from the
_hadr_lfv[M]
which is defined as_hadr_lfv = { 'B0->K': {'tex': r"\bar B^0\to \bar K^0", 'B': 'B0', 'P': 'K0', }, 'B+->K': {'tex': r"B^-\to K^-", 'B': 'B+', 'P': 'K+', }, 'B0->pi': {'tex': r"\bar B^0\to \pi^0", 'B': 'B0', 'P': 'pi0', }, 'B+->pi': {'tex': r"B^-\to \pi^-", 'B': 'B+', 'P': 'pi+', }, }
?If that is the case, then how this information is translated to the Wilson coefficients with different quark flavors ?
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