slophep.Predictions.Math.BToVMathTools

slophep.Predictions.Math.BToVMathTools.angularPDF(ctx: float, ctl: float, chi: float, j: dict[float]) float[source]
slophep.Predictions.Math.BToVMathTools.angularPDF_binned(ctx_min: float, ctx_max: float, ctl_min: float, ctl_max: float, chi_min: float, chi_max: float, j: dict[float]) float[source]
slophep.Predictions.Math.BToVMathTools.angular_integrals(ctx_min: float, ctx_max: float, ctl_min: float, ctl_max: float, chi_min: float, chi_max: float) dict[float][source]
slophep.Predictions.Math.BToVMathTools.calc_norm_j(j: dict[float]) dict[float][source]
slophep.Predictions.Math.BToVMathTools.calc_unaing_obs(j: dict[float]) float[source]
slophep.Predictions.Math.BToVMathTools.h_to_A(mB, mV, h, q2)[source]

Convert HQET form factors to the basis used by flavio.

See e.g. arXiv:1309.0301, eqs. (38), (39) but notice that we use the convention of arXiv:1703.05330 for h_T3, which differs by a factor -2 from the one in arXiv:1309.0301 (see Eq. (11e) in arXiv:1703.05330 and Eq. (46b) in arXiv:1309.0301).

slophep.Predictions.Math.BToVMathTools.uniang_chi(chi: float, J: dict)[source]
slophep.Predictions.Math.BToVMathTools.uniang_ctl(ctl: float, J: dict)[source]
slophep.Predictions.Math.BToVMathTools.uniang_ctv(ctv: float, J: dict)[source]