Results 91 to 100 of about 4,794 (202)
Abstract Within the assumption of Left‐Handed (LH) New Physics (NP), the relations between B(B→K(*)τ+τ−)$\mathcal {B}(B\rightarrow K^{(\ast )} \tau ^+\tau ^-)$ and B(B→K(*)νν¯)$\mathcal {B}(B\rightarrow K^{(\ast )} \nu \bar{\nu })$ for several Beyond the Standard Model (BSM) scenarios are reviewed, commonly considered to explain the Lepton flavor ...
Arturo de Giorgi, Gioacchino Piazza
wiley +1 more source
Interpreting W mass measurements in the SMEFT [PDF]
6pp, 4 figures V2: minor typo corrections and text clarifications, matches journal ...
Bjørn, Mikkel, Trott, Michael
openaire +4 more sources
Top Quark Flavor Changing Couplings at a Muon Collider
There is growing interest in the development of a muon collider that would make it possible to produce lepton collisions at energies of several TeV. Among others, there can be significant contributions to electroweak gauge boson, Higgs boson, and top quark physics.
Daniel Ake +3 more
wiley +1 more source
Addendum to: Scheming in the SMEFT. . . and a reparameterization invariance! [PDF]
Abstract We allow two independent flavor contractions for the operator $$ {\mathcal{Q}}_{ll} $$ Q l l
Ilaria Brivio, Michael Trott
openalex +6 more sources
Constraints on anomalous quartic gauge couplings via $W\gamma jj$ production at the LHC
The vector boson scattering at the Large Hadron Collider (LHC) is sensitive to anomalous quartic gauge couplings (aQGCs). In this paper, we investigate the aQGC contribution to $ W \gamma jj$ production at the LHC with $\sqrt{s}=13$ TeV in the context of
Guo, Yu-Chen +3 more
core +2 more sources
Incorporating doubly resonant $W^\pm$ data in a global fit of SMEFT parameters to lift flat directions [PDF]
We calculate the double pole contribution to two to four fermion scattering through $W^{\pm}$ currents at tree level in the Standard Model Effective Field Theory (SMEFT).
Berthier, Laure +2 more
core +2 more sources
Missing energy plus jet in the SMEFT [PDF]
We study the production of dineutrinos in proton-proton collisions, with large missing transverse energy and an energetic jet as the experimental signature.
Gudrun Hiller, Daniel Wendler
semanticscholar +1 more source
Field reparametrization in SMEFT [PDF]
Debate topic for effective field theory (EFT) is the choice of a “basis” for ${\rm dim}= 6$ operators. Clearly all bases are equivalent as long as they are a “basis”, containing a minimal set of operators ...
openaire +3 more sources
We develop Standard Model Effective Field Theory (SMEFT) predictions of σ( GG $$ \mathcal{GG} $$ → h), Γ(h → GG $$ \mathcal{GG} $$ ), Γ(h → AA $$ \mathcal{AA} $$ ) to incorporate full two loop Standard Model results at the amplitude level, in conjunction
Adam Martin, Michael Trott
doaj +1 more source
Higgs associated production with a vector decaying to two fermions in the geoSMEFT
We present the inclusive calculations of a Higgs boson produced in association with massive vector bosons in the Standard Model Effective Field Theory (SMEFT) to order $1/\Lambda^4$ for the 13 TeV LHC.
Tyler Corbett, Adam Martin
doaj +1 more source

