FLAG review 2021
Y Aoki, T Blum, G Colangelo, S Collins… - The European Physical …, 2022 - Springer
We review lattice results related to pion, kaon, D-meson, B-meson, and nucleon physics with
the aim of making them easily accessible to the nuclear and particle physics communities …
the aim of making them easily accessible to the nuclear and particle physics communities …
Averages of b-hadron, c-hadron, and -lepton properties as of 2018: Heavy Flavor Averaging Group (HFLAV)
Y Amhis, S Banerjee, E Ben-Haim… - The European Physical …, 2021 - Springer
This paper reports world averages of measurements of b-hadron, c-hadron, and τ τ-lepton
properties obtained by the Heavy Flavour Averaging Group using results available through …
properties obtained by the Heavy Flavour Averaging Group using results available through …
Averages of -hadron, -hadron, and -lepton properties as of 2021
Y Amhis, S Banerjee, E Ben-Haim, E Bertholet… - Physical Review D, 2023 - APS
This paper reports world averages of measurements of b-hadron, c-hadron, and τ-lepton
properties obtained by the Heavy Flavor Averaging Group using results available before …
properties obtained by the Heavy Flavor Averaging Group using results available before …
FLAG review 2019: Flavour lattice averaging group (FLAG)
S Aoki, Y Aoki, D Bečirević, T Blum… - The European Physical …, 2020 - Springer
We review lattice results related to pion, kaon, D-meson, B-meson, and nucleon physics with
the aim of making them easily accessible to the nuclear and particle physics communities …
the aim of making them easily accessible to the nuclear and particle physics communities …
[HTML][HTML] 50 Years of quantum chromodynamics: Introduction and Review
F Gross, E Klempt, SJ Brodsky, AJ Buras… - The European Physical …, 2023 - Springer
Quantum Chromodynamics, the theory of quarks and gluons, whose interactions can be
described by a local SU (3) gauge symmetry with charges called “color quantum numbers” …
described by a local SU (3) gauge symmetry with charges called “color quantum numbers” …
Update of the global electroweak fit and constraints on two-Higgs-doublet models
Gfitter Group, J Haller, A Hoecker, R Kogler… - The European Physical …, 2018 - Springer
We present an update of the global fit of the Standard Model electroweak sector to latest
experimental results. We include new kinematic top quark and W boson mass …
experimental results. We include new kinematic top quark and W boson mass …
Measurement of the ratios of branching fractions and
LHCb Collaboration - arXiv preprint arXiv:2302.02886, 2023 - arxiv.org
The ratios of branching fractions $\mathcal {R}(D^{*})\equiv\mathcal {B}(\bar {B}\to
D^{*}\tau^{-}\bar {\nu} _ {\tau})/\mathcal {B}(\bar {B}\to D^{*}\mu^{-}\bar {\nu} _ {\mu}) $ and …
D^{*}\tau^{-}\bar {\nu} _ {\tau})/\mathcal {B}(\bar {B}\to D^{*}\mu^{-}\bar {\nu} _ {\mu}) $ and …
B-decay discrepancies after Moriond 2019
J Aebischer, W Altmannshofer, D Guadagnoli… - The European Physical …, 2020 - Springer
Following the updated measurement of the lepton flavour universality (LFU) ratio R_K RK in
B → K ℓ ℓ B→ K ℓ ℓ decays by LHCb, as well as a number of further measurements, eg R …
B → K ℓ ℓ B→ K ℓ ℓ decays by LHCb, as well as a number of further measurements, eg R …
Closing the window on single leptoquark solutions to the B-physics anomalies
A Angelescu, D Bečirević, DA Faroughy… - Journal of High Energy …, 2018 - Springer
We examine various scenarios in which the Standard Model is extended by a light
leptoquark state to solve for one or both B-physics anomalies, viz. RD* exp> RD* SM or/and …
leptoquark state to solve for one or both B-physics anomalies, viz. RD* exp> RD* SM or/and …
Measurement of the Lepton Polarization and in the Decay
S Hirose, T Iijima, I Adachi, K Adamczyk, H Aihara… - Physical review …, 2017 - APS
We report the first measurement of the τ lepton polarization P τ (D*) in the decay B¯→ D* τ-
ν¯ τ as well as a new measurement of the ratio of the branching fractions R (D*)= B (B¯→ D …
ν¯ τ as well as a new measurement of the ratio of the branching fractions R (D*)= B (B¯→ D …