Module flavio.physics.kdecays.klnu
Functions for $K\to\ell\nu$ and $\pi\to\ell\nu$ decays.
Functions
def F(z)-
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def F(z): return ( 3/2.*log(z) + (13-19*z)/(8*(1-z)) - (8-5*z)/(4*(1-z)**2)*z*log(z) - ((1+z)/(1-z)*log(z)+2)*log(1-z) -2*(1+z)/(1-z)*li2(1-z) ) def br_plnu(wc_obj, par, P, lep)-
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def br_plnu(wc_obj, par, P, lep): r"""Branching ratio of $P^+\to\ell^+\nu_\ell$.""" return sum([ _br_plnu(wc_obj, par, P, lep, nu) for nu in ['e','mu','tau']])Branching ratio of $P^+\to\ell^+\nu_\ell$.
def br_plnu_fct(P, lep)-
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def br_plnu_fct(P, lep): def f(wc_obj, par): return br_plnu(wc_obj, par, P, lep) return f def delta_Plnu(par, P, lep)-
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def delta_Plnu(par, P, lep): mrho = par['m_rho0'] mP = par['m_'+P] ml = par['m_'+lep] alpha_e = 1/137.035999139 # this is alpha_e(0), a constant for our purposes c1 = par['c1_'+P+'lnu'] # e.g. c1_K+lnu c2 = par['c2_'+P+'lnu'] c3 = par['c3_'+P+'lnu'] if lep=='mu': c4 = par['c4_'+P+'munu'] elif lep=='e': c4 = 0 # c_4 tends to zero with vanishing lepton mass c2t = par['c2t_'+P+'lnu'] return alpha_e/pi * (F(ml**2/mP**2) - 3/2.*log(mrho/mP) - c1 - ml**2/mrho**2 * (c2 * log(mrho**2/ml**2) + c3 + c4) + mP**2/mrho**2 * c2t * log(mrho**2/ml**2) ) def gamma_plnu(wc_obj, par, P, l)-
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def gamma_plnu(wc_obj, par, P, l): return br_plnu(wc_obj, par, P, l) / par['tau_' + P] def gamma_plnu_fct(P, l)-
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def gamma_plnu_fct(P, l): def f(wc_obj, par): return gamma_plnu(wc_obj, par, P, l) return f def r_plnu(wc_obj, par, P)-
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def r_plnu(wc_obj, par, P): # resumming logs according to (111) of 0707.4464 # (this is negligibly small for the individual rates) flavio.citations.register("Cirigliano:2007ga") rg_corr = 1.00055 return rg_corr*br_plnu(wc_obj, par, P, 'e')/br_plnu(wc_obj, par, P, 'mu') def r_plnu_fct_l(l)-
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def r_plnu_fct_l(l): def f(wc_obj, par): return gamma_plnu(wc_obj, par, 'K+', l) / gamma_plnu(wc_obj, par, 'pi+', l) return f def r_plnu_fct_p(P)-
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def r_plnu_fct_p(P): def f(wc_obj, par): return r_plnu(wc_obj, par, P) return f