scholarly journals The rare decay B→Xsℓ+ℓ− to NNLL precision for arbitrary dilepton invariant mass

2004 ◽  
Vol 685 (1-3) ◽  
pp. 351-392 ◽  
Author(s):  
A. Ghinculov ◽  
T. Hurth ◽  
G. Isidori ◽  
Y.-P. Yao
1997 ◽  
Vol 56 (6) ◽  
pp. R2920-R2923 ◽  
Author(s):  
R. Holzmann ◽  
M. Appenheimer ◽  
R. Averbeck ◽  
Y. Charbonnier ◽  
H. Delagrange ◽  
...  

2013 ◽  
Vol 87 (9) ◽  
Author(s):  
Bhaskar Dutta ◽  
Teruki Kamon ◽  
Nikolay Kolev ◽  
Kuver Sinha ◽  
Kechen Wang ◽  
...  

2021 ◽  
Vol 2021 (11) ◽  
Author(s):  
◽  
R. Aaij ◽  
A. S. W. Abdelmotteleb ◽  
C. Abellán Beteta ◽  
T. Ackernley ◽  
...  

Abstract An angular analysis of the rare decay $$ {B}_s^0 $$ B s 0 → ϕμ+μ− is presented, using proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7, 8 and 13 TeV, corresponding to an integrated luminosity of 8.4 fb−1. The observables describing the angular distributions of the decay $$ {B}_s^0 $$ B s 0 → ϕμ+μ− are determined in regions of q2, the square of the dimuon invariant mass. The results are consistent with Standard Model predictions.


2017 ◽  
Vol 32 (16) ◽  
pp. 1750094 ◽  
Author(s):  
Christian Gross ◽  
Oleg Lebedev ◽  
Jose Miguel No

The Standard Model (SM) extensions with vector-like states which have either zero hypercharge or zero weak isospin are rather poorly constrained by the electroweak precision measurements. Such new states would however modify the running of the gauge couplings at high energies. As a result, the Drell–Yan process [Formula: see text] at the LHC places useful constraints on these models. The relevant observables include both the dilepton invariant mass distribution [Formula: see text] and the forward–backward asymmetry [Formula: see text]. We find that the LHC Run 1 data and the initial data from Run 2 surpass the sensitivity of LEP and already put meaningful constraints on the existence of such particles, which will become progressively stronger with more data.


1998 ◽  
Vol 525 (1-2) ◽  
pp. 333-349 ◽  
Author(s):  
Gerhard Buchalla ◽  
Gino Isidori

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