Module flavio.physics.bdecays.test_bll
Classes
class TestBll (methodName='runTest')-
Expand source code
class TestBll(unittest.TestCase): def test_bsll(self): # just some trivial tests to see if calling the functions raises an error self.assertGreater(br_lifetime_corr(0.08, -1), 0) self.assertEqual(len(amplitudes(par, wc, 'Bs', 'mu', 'mu')), 2) # ADeltaGamma should be +1.0 in the SM self.assertEqual(ADeltaGamma(par, wc, 'Bs', 'mu'), 1.0) self.assertEqual(flavio.sm_prediction('ADeltaGamma(Bs->mumu)'), 1.0) # BR should be around 3.5e-9 self.assertAlmostEqual(br_inst(par, wc, 'Bs', 'mu', 'mu')*1e9, 3.5, places=0) # correction factor should enhance the BR by roughly 7% self.assertAlmostEqual(br_timeint(par, wc, 'Bs', 'mu', 'mu')/br_inst(par, wc, 'Bs', 'mu', 'mu'), 1.07, places=2) # ratio of Bs->mumu and Bs->ee BRs should be roughly given by ratio of squared masses self.assertAlmostEqual( br_timeint(par, wc_e, 'Bs', 'e', 'e')/br_timeint(par, wc, 'Bs', 'mu', 'mu')/par['m_e']**2*par['m_mu']**2, 1., places=2) # comparison to 1311.0903 self.assertAlmostEqual(abs(ckm.xi('t','bs')(par))/par['Vcb'], 0.980, places=3) self.assertAlmostEqual(br_timeint(par, wc, 'Bs', 'mu', 'mu')/3.65e-9, 1, places=1) self.assertAlmostEqual(br_timeint(par, wc_e, 'Bs', 'e', 'e')/8.54e-14, 1, places=1) self.assertAlmostEqual(br_timeint(par, wc_tau, 'Bs', 'tau', 'tau')/7.73e-7, 1, places=1) def test_bsll_classes(self): par_default = default_parameters.get_central_all() self.assertAlmostEqual(br_timeint(par_default, wc_tau, 'Bs', 'tau', 'tau')/Observable['BR(Bs->tautau)'].prediction_central(default_parameters, wc_obj), 1, places=4) self.assertAlmostEqual(br_timeint(par_default, wc_e, 'Bs', 'e', 'e')/Observable['BR(Bs->ee)'].prediction_central(default_parameters, wc_obj), 1, places=4) self.assertAlmostEqual(br_timeint(par_default, wc, 'Bs', 'mu', 'mu')/Observable['BR(Bs->mumu)'].prediction_central(default_parameters, wc_obj), 1, places=4) def test_bsll_lfv(self): # test for errors self.assertEqual(flavio.sm_prediction('BR(B0->emu)'), 0) self.assertEqual(flavio.sm_prediction('BR(Bs->taumu)'), 0) self.assertEqual(flavio.sm_prediction('BR(B0->emu,mue)'), 0) self.assertEqual(flavio.sm_prediction('BR(Bs->mutau,taumu)'), 0) wc = flavio.WilsonCoefficients() wc.set_initial({'C10_bdemu': 1, 'C10_bdmue': 2}, scale=4.8) self.assertAlmostEqual(flavio.np_prediction('BR(B0->mue)', wc) /flavio.np_prediction('BR(B0->emu)', wc), 4) self.assertAlmostEqual(flavio.np_prediction('BR(B0->emu,mue)', wc) /flavio.np_prediction('BR(B0->emu)', wc), 5) def test_EffectiveLifetimes(self): # In this test we trivially check that the prefactors in (22) and (28) of arXiv:1204.1737 are the same ys = .5*par['DeltaGamma/Gamma_Bs'] tau_Bs = par['tau_Bs'] wc_dict = {'e': wc_e, 'mu': wc, 'tau': wc_tau} for l in ['e', 'mu', 'tau']: ADG = ADeltaGamma(par, wc_dict[l], 'Bs', l) tau = tau_ll(wc_dict[l], par, 'Bs', l) prefactor1 = br_lifetime_corr(ys, ADG) # eq. (22) of arXiv:1204.1737 prefactor2 = 2. - (1.-ys**2) * tau / tau_Bs # eq. (28) of arXiv:1204.1737 self.assertAlmostEqual(prefactor1, prefactor2, places=8) def test_BR_Bs_to_mumu(self): # cross check formula with 2nd implementation # use formula (1.2) and (1.3) of 1407.2771 def amplitudes_Amsterdam_Bs_mumu(par, wc): # masses scale = flavio.config['renormalization scale']['bll'] mmu = par['m_mu'] mB = par['m_Bs'] mb = running.get_mb(par, scale, nf_out=5) ms = running.get_ms(par, scale, nf_out=5) # Wilson coefficients C10SM = -4.188642825319258 #SM value for C10 -4.134# C10m = (C10SM+wc['C10_bsmumu']) - wc['C10p_bsmumu'] CPm = wc['CP_bsmumu'] - wc['CPp_bsmumu'] CSm = wc['CS_bsmumu'] - wc['CSp_bsmumu'] P = C10m/C10SM + mB**2/(2.*mmu) * (mb / (mb + ms)) * CPm/C10SM S = math.sqrt(1. - 4*mmu**2/mB**2) * mB**2/(2.*mmu) * (mb / (mb + ms)) * CSm/C10SM return P, S def BR_inst_Amsterdam_Bs_mumu(par, wc): # eq.(1.2) from 1407.2771 scale = flavio.config['renormalization scale']['bll'] GF = par['GF'] alphaem = running.get_alpha(par, scale)['alpha_e'] mW = par['m_W'] mB = par['m_Bs'] mmu = par['m_mu'] tauB = par['tau_Bs'] fB = par['f_Bs'] xi_ts_tb = ckm.xi('t','bs')(par) s2w = par['s2w'] # Wilson coefficients C10SM = -4.188642825319258 #SM value for C10 P,S = amplitudes_Amsterdam_Bs_mumu(par, wc) return (GF**2 * alphaem**2 * mB)/(16. * math.pi**3) * math.sqrt(1.-4.*mmu**2/mB**2) * C10SM**2 * abs(xi_ts_tb)**2 * tauB * fB**2 * mmu**2 * (abs(P)**2 + abs(S)**2) def ADG_Amsterdam(par, wc): P, S = amplitudes_Amsterdam_Bs_mumu(par, wc) return ((P**2).real - (S**2).real)/(abs(P)**2 + abs(S)**2) def corr_factor(par, wc): ADG = ADG_Amsterdam(par, wc) y = par['DeltaGamma/Gamma_Bs']/2. corr = (1 - y**2)/(1 + ADG*y) return corr def BR_Amsterdam_Bs_mumu(par, wc): BR_inst = BR_inst_Amsterdam_Bs_mumu(par, wc) corr = corr_factor(par, wc) return BR_inst / corr # define function that calculates the BR in both implementations def BR(c10, c10p, cS, cSp, cP, cPp): list_wc = {'C10_bsmumu' : c10, 'C10p_bsmumu': c10p, 'CS_bsmumu' : cS, 'CSp_bsmumu' : cSp, 'CP_bsmumu' : cP, 'CPp_bsmumu' : cPp, 'C9_bsmumu' : 0., 'C9p_bsmumu' : 0.} wc = flavio.WilsonCoefficients() wc.set_initial(list_wc, scale=160 ) BR_flavio = flavio.np_prediction('BR(Bs->mumu)', wc) BR_Amsterdam = BR_Amsterdam_Bs_mumu(par, list_wc) return {'flavio': BR_flavio, 'Amsterdam': BR_Amsterdam} # test SM value br_SM = BR(0,0,0,0,0,0) self.assertAlmostEqual(br_SM['flavio'] / br_SM['Amsterdam'], 1., delta=0.02) # test some values for WC's br = BR(-.4,0,0,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(-.5*1j,0,0,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(0,0,0.01,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(0,0,0,-0.01*1j,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=2) br = BR(0,0,0,0,0.01,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.05) br = BR(0,0,0,0,0,-0.02*1j) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.04) br = BR(-.5*1j,0,0.01,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(-.5*1j,0,0,0,-0.03,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.04)A class whose instances are single test cases.
By default, the test code itself should be placed in a method named 'runTest'.
If the fixture may be used for many test cases, create as many test methods as are needed. When instantiating such a TestCase subclass, specify in the constructor arguments the name of the test method that the instance is to execute.
Test authors should subclass TestCase for their own tests. Construction and deconstruction of the test's environment ('fixture') can be implemented by overriding the 'setUp' and 'tearDown' methods respectively.
If it is necessary to override the init method, the base class init method must always be called. It is important that subclasses should not change the signature of their init method, since instances of the classes are instantiated automatically by parts of the framework in order to be run.
When subclassing TestCase, you can set these attributes: * failureException: determines which exception will be raised when the instance's assertion methods fail; test methods raising this exception will be deemed to have 'failed' rather than 'errored'. * longMessage: determines whether long messages (including repr of objects used in assert methods) will be printed on failure in addition to any explicit message passed. * maxDiff: sets the maximum length of a diff in failure messages by assert methods using difflib. It is looked up as an instance attribute so can be configured by individual tests if required.
Create an instance of the class that will use the named test method when executed. Raises a ValueError if the instance does not have a method with the specified name.
Ancestors
- unittest.case.TestCase
Methods
def test_BR_Bs_to_mumu(self)-
Expand source code
def test_BR_Bs_to_mumu(self): # cross check formula with 2nd implementation # use formula (1.2) and (1.3) of 1407.2771 def amplitudes_Amsterdam_Bs_mumu(par, wc): # masses scale = flavio.config['renormalization scale']['bll'] mmu = par['m_mu'] mB = par['m_Bs'] mb = running.get_mb(par, scale, nf_out=5) ms = running.get_ms(par, scale, nf_out=5) # Wilson coefficients C10SM = -4.188642825319258 #SM value for C10 -4.134# C10m = (C10SM+wc['C10_bsmumu']) - wc['C10p_bsmumu'] CPm = wc['CP_bsmumu'] - wc['CPp_bsmumu'] CSm = wc['CS_bsmumu'] - wc['CSp_bsmumu'] P = C10m/C10SM + mB**2/(2.*mmu) * (mb / (mb + ms)) * CPm/C10SM S = math.sqrt(1. - 4*mmu**2/mB**2) * mB**2/(2.*mmu) * (mb / (mb + ms)) * CSm/C10SM return P, S def BR_inst_Amsterdam_Bs_mumu(par, wc): # eq.(1.2) from 1407.2771 scale = flavio.config['renormalization scale']['bll'] GF = par['GF'] alphaem = running.get_alpha(par, scale)['alpha_e'] mW = par['m_W'] mB = par['m_Bs'] mmu = par['m_mu'] tauB = par['tau_Bs'] fB = par['f_Bs'] xi_ts_tb = ckm.xi('t','bs')(par) s2w = par['s2w'] # Wilson coefficients C10SM = -4.188642825319258 #SM value for C10 P,S = amplitudes_Amsterdam_Bs_mumu(par, wc) return (GF**2 * alphaem**2 * mB)/(16. * math.pi**3) * math.sqrt(1.-4.*mmu**2/mB**2) * C10SM**2 * abs(xi_ts_tb)**2 * tauB * fB**2 * mmu**2 * (abs(P)**2 + abs(S)**2) def ADG_Amsterdam(par, wc): P, S = amplitudes_Amsterdam_Bs_mumu(par, wc) return ((P**2).real - (S**2).real)/(abs(P)**2 + abs(S)**2) def corr_factor(par, wc): ADG = ADG_Amsterdam(par, wc) y = par['DeltaGamma/Gamma_Bs']/2. corr = (1 - y**2)/(1 + ADG*y) return corr def BR_Amsterdam_Bs_mumu(par, wc): BR_inst = BR_inst_Amsterdam_Bs_mumu(par, wc) corr = corr_factor(par, wc) return BR_inst / corr # define function that calculates the BR in both implementations def BR(c10, c10p, cS, cSp, cP, cPp): list_wc = {'C10_bsmumu' : c10, 'C10p_bsmumu': c10p, 'CS_bsmumu' : cS, 'CSp_bsmumu' : cSp, 'CP_bsmumu' : cP, 'CPp_bsmumu' : cPp, 'C9_bsmumu' : 0., 'C9p_bsmumu' : 0.} wc = flavio.WilsonCoefficients() wc.set_initial(list_wc, scale=160 ) BR_flavio = flavio.np_prediction('BR(Bs->mumu)', wc) BR_Amsterdam = BR_Amsterdam_Bs_mumu(par, list_wc) return {'flavio': BR_flavio, 'Amsterdam': BR_Amsterdam} # test SM value br_SM = BR(0,0,0,0,0,0) self.assertAlmostEqual(br_SM['flavio'] / br_SM['Amsterdam'], 1., delta=0.02) # test some values for WC's br = BR(-.4,0,0,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(-.5*1j,0,0,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(0,0,0.01,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(0,0,0,-0.01*1j,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=2) br = BR(0,0,0,0,0.01,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.05) br = BR(0,0,0,0,0,-0.02*1j) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.04) br = BR(-.5*1j,0,0.01,0,0,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.02) br = BR(-.5*1j,0,0,0,-0.03,0) self.assertAlmostEqual(br['flavio'] / br['Amsterdam'], 1., delta=0.04) def test_EffectiveLifetimes(self)-
Expand source code
def test_EffectiveLifetimes(self): # In this test we trivially check that the prefactors in (22) and (28) of arXiv:1204.1737 are the same ys = .5*par['DeltaGamma/Gamma_Bs'] tau_Bs = par['tau_Bs'] wc_dict = {'e': wc_e, 'mu': wc, 'tau': wc_tau} for l in ['e', 'mu', 'tau']: ADG = ADeltaGamma(par, wc_dict[l], 'Bs', l) tau = tau_ll(wc_dict[l], par, 'Bs', l) prefactor1 = br_lifetime_corr(ys, ADG) # eq. (22) of arXiv:1204.1737 prefactor2 = 2. - (1.-ys**2) * tau / tau_Bs # eq. (28) of arXiv:1204.1737 self.assertAlmostEqual(prefactor1, prefactor2, places=8) def test_bsll(self)-
Expand source code
def test_bsll(self): # just some trivial tests to see if calling the functions raises an error self.assertGreater(br_lifetime_corr(0.08, -1), 0) self.assertEqual(len(amplitudes(par, wc, 'Bs', 'mu', 'mu')), 2) # ADeltaGamma should be +1.0 in the SM self.assertEqual(ADeltaGamma(par, wc, 'Bs', 'mu'), 1.0) self.assertEqual(flavio.sm_prediction('ADeltaGamma(Bs->mumu)'), 1.0) # BR should be around 3.5e-9 self.assertAlmostEqual(br_inst(par, wc, 'Bs', 'mu', 'mu')*1e9, 3.5, places=0) # correction factor should enhance the BR by roughly 7% self.assertAlmostEqual(br_timeint(par, wc, 'Bs', 'mu', 'mu')/br_inst(par, wc, 'Bs', 'mu', 'mu'), 1.07, places=2) # ratio of Bs->mumu and Bs->ee BRs should be roughly given by ratio of squared masses self.assertAlmostEqual( br_timeint(par, wc_e, 'Bs', 'e', 'e')/br_timeint(par, wc, 'Bs', 'mu', 'mu')/par['m_e']**2*par['m_mu']**2, 1., places=2) # comparison to 1311.0903 self.assertAlmostEqual(abs(ckm.xi('t','bs')(par))/par['Vcb'], 0.980, places=3) self.assertAlmostEqual(br_timeint(par, wc, 'Bs', 'mu', 'mu')/3.65e-9, 1, places=1) self.assertAlmostEqual(br_timeint(par, wc_e, 'Bs', 'e', 'e')/8.54e-14, 1, places=1) self.assertAlmostEqual(br_timeint(par, wc_tau, 'Bs', 'tau', 'tau')/7.73e-7, 1, places=1) def test_bsll_classes(self)-
Expand source code
def test_bsll_classes(self): par_default = default_parameters.get_central_all() self.assertAlmostEqual(br_timeint(par_default, wc_tau, 'Bs', 'tau', 'tau')/Observable['BR(Bs->tautau)'].prediction_central(default_parameters, wc_obj), 1, places=4) self.assertAlmostEqual(br_timeint(par_default, wc_e, 'Bs', 'e', 'e')/Observable['BR(Bs->ee)'].prediction_central(default_parameters, wc_obj), 1, places=4) self.assertAlmostEqual(br_timeint(par_default, wc, 'Bs', 'mu', 'mu')/Observable['BR(Bs->mumu)'].prediction_central(default_parameters, wc_obj), 1, places=4) def test_bsll_lfv(self)-
Expand source code
def test_bsll_lfv(self): # test for errors self.assertEqual(flavio.sm_prediction('BR(B0->emu)'), 0) self.assertEqual(flavio.sm_prediction('BR(Bs->taumu)'), 0) self.assertEqual(flavio.sm_prediction('BR(B0->emu,mue)'), 0) self.assertEqual(flavio.sm_prediction('BR(Bs->mutau,taumu)'), 0) wc = flavio.WilsonCoefficients() wc.set_initial({'C10_bdemu': 1, 'C10_bdmue': 2}, scale=4.8) self.assertAlmostEqual(flavio.np_prediction('BR(B0->mue)', wc) /flavio.np_prediction('BR(B0->emu)', wc), 4) self.assertAlmostEqual(flavio.np_prediction('BR(B0->emu,mue)', wc) /flavio.np_prediction('BR(B0->emu)', wc), 5)