REVIEW OF PARTICLE PHYSICS

By J. Beringer. 2013

361 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/a8208df5e7e2c4bdfb972b624729fb08bf5bcca8

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Citations in the corpus

Measurement of the fragmentation fraction ratio fs/fd and its dependence on B meson kinematics (2013, methodology): “ching the highest sensitivity in the search for physics beyond the Standard Model. The branching fractions of a large number of B0 and B+ decays have been measured to high precision at the Bfactories [2], but no B0 s branching fraction is yet known with suciently high precision to be used as a norma”
Updated fit to three neutrino mixing: status of leptonic CP violation (2014, background): “third vertex is not too much aected by the uncertainty of the normalization side. Note that the most common unitarity triangle in the quark sector is the one based on the d-quark and b-quark columns [7], which corresponds to the 1st and 3rd column in the leptonic matrix, i.e., to the triangle in the”
Differential branching fraction and angular analysis of the decay $B_s^0\to\phi\mu^{+}\mu^{-}$ (2013, methodology): “nd is strongly suppressed by particle identication criteria. In the narrow ˚ mass window, 2:4 00:5 misidentied B0 !K + candidates are expected within 250MeV=c of the known B0 s mass of 5366MeV=c2 [11]. The resonant decay B0 s !J= ˚ can also constitute a source of peaking background if the K+ (K ) is”
Test of lepton universality using b+ → K+ℓ+ℓ- decays. (2014, background): “ction to cancel potential sources of systematic uncertainty between the B +!K ‘ +‘ and B !J= (!‘+‘ )K decays as the eciencies are correlated and the branching fraction to B +!J= K is known precisely [11]. This is achieved by using the same selection for B +!K ‘+‘ and B !J= (!‘+‘ )K+ decays for each ”
Hunting for topological dark matter with atomic clocks (2013, methodology): “3 GeV/cm(3) in Solar system neighborhood [7]), its relation to particles and fields of the Standard Model (SM) remains a mystery.”
Differential branching fraction and angular analysis of the decay B0 → K∗0μ+μ− (2013, background): “dB dq2 = 1 q2 max q2 min Nsig N K 0J= "K 0J= " 0 + B (B0 !K0J= ) B (J= !+ ) : (5) The branching fractions B(B0 !K0J= ) and B(J= !+ ) are (1:31 0:03 0:08) 10 3 [24] and (5:93 0:06) 10 2 [23], respectively. The eciency ratio, "K 0J= ="K 0+ , depends on the unknown angular distribut”