Module flavio.physics.running.betafunctions
Functions for running of QCD and QED gauge couplings below the weak scale.
Functions
def beta_qcd(als, ale, mu, f)-
Expand source code
def beta_qcd(als, ale, mu, f): r"""Right-hand side of the QCD beta function written in the (unconventional) form $d \alpha_s /d\mu= \beta(\mu)$ """ #FIXME QED part only implemented for f=5 b=np.zeros((3,3), dtype=float) b[0,0] = (33 - 2*f)/3 b[1,0] = (102 - (38*f)/3.) b[2,0] = (1428.5 - (5033*f)/18. + (325*f**2)/54.) b[0,1] = -((22)/(9)) b[1,1] = -(308/27) b[0,2] = (4945/243) couplings = np.array([[ (als/4./pi)**ps*(ale/4./pi)**pe for pe in range(3)] for ps in range(3)]) return -1/2./pi/mu*als**2*(couplings*b).sum()Right-hand side of the QCD beta function written in the (unconventional) form $d \alpha_s /d\mu= \beta(\mu)$
def beta_qcd_qed(alpha, mu, nf)-
Expand source code
def beta_qcd_qed(alpha, mu, nf): r"""RHS of the QCD and QED beta function written in the (unconventional) form $$\frac{d}{d\mu} \vec\alpha = \vec\beta(\mu)$$ where $\vec\alpha^T=(\alpha_s,\alpha_e)$ """ bs = beta_qcd(alpha[0], alpha[1], mu, nf) be = beta_qed(alpha[1], alpha[0], mu, nf) return np.array([bs, be])RHS of the QCD and QED beta function written in the (unconventional) form $$\frac{d}{d\mu} \vec\alpha = \vec\beta(\mu)$$ where $\vec\alpha^T=(\alpha_s,\alpha_e)$
def beta_qed(ale, als, mu, f)-
Expand source code
def beta_qed(ale, als, mu, f): r"""RHS of the QED beta function written in the (unconventional) form $d \alpha_e /d\mu= \beta(\mu)$ """ #FIXME only implemented for f=5 b=np.zeros((2,2), dtype=float) b[0,0] = (80/9) b[1,0] = (464/27) b[0,1] = (176/9) couplings = np.array([[ (ale/4./pi)**pe*(als/4./pi)**ps for ps in range(2)] for pe in range(2)]) return 1/2./pi/mu*ale**2*(couplings*b).sum()RHS of the QED beta function written in the (unconventional) form $d \alpha_e /d\mu= \beta(\mu)$
def betafunctions_qcd_qed_nf(nf)-
Expand source code
def betafunctions_qcd_qed_nf(nf): return lambda x, mu: beta_qcd_qed(x, mu, nf)