-
1741
Unitarity bounds on the massive spin-2 particle explanation of muon $$g-2$$ g - 2 anomaly
Published 2024-03-01“…We calculate the s-wave projected amplitudes for two-body elastic scatterings of charged leptons and photons mediated by G at high energies for all possible initial and final helicity states. …”
Get full text
Article -
1742
Dispersive analysis of Λ b → Λ(1520) local form factors
Published 2023-02-01“…Finally, we use our results to obtain predictions for some observables in Λ b → Λ(1520)ℓ + ℓ − decays, as the differential branching ratio, the forward-backwards lepton asymmetry and the branching ratio of Λ b → Λ(1520)γ. …”
Get full text
Article -
1743
Explanation of electron and muon g − 2 anomalies in AMSB
Published 2022-10-01“…Two Yukawa deflected AMSB models are proposed and discussed in depth: one with lepton-specific interactions and the other one with messenger-matter interactions. …”
Get full text
Article -
1744
Neutrinoless double β decay and low scale leptogenesis
Published 2016-12-01“…This implies that neutrinoless double β decay experiments have already started to rule out part of the leptogenesis parameter space that is not constrained by any other experiment, and the lepton number violation that is responsible for the origin of baryonic matter in the universe may be observed in the near future.…”
Get full text
Article -
1745
Photon splitting corrections to soft-photon resummation
Published 2023-03-01“…We introduce different lepton dressing strategies which incorporate further leptons and hadrons in addition to the customary photons, and discuss their sensitivity to dressing parameters such as the cone size. …”
Get full text
Article -
1746
All-optical ultrafast spin rotation for relativistic charged particle beams
Published 2023-04-01“…An all-optical method of ultrafast spin rotation is put forward to precisely manipulate the polarization of relativistic charged particle beams of leptons or ions. Laser-driven dense ultrashort beams are manipulated via single-shot interaction with a copropagating temporally asymmetric laser pulse of moderate intensity. …”
Get full text
Article -
1747
Light neutrinophilic dark matter from a scotogenic model
Published 2023-10-01“…Due to minimality and the interplay between obtaining the correct DM relic abundance and neutrino oscillation data, the model predicts (i) a massless lightest neutrino, (ii) enhanced rate of 0νββ decay due to loop corrections involving light DM exchange, and (iii) testable lepton flavor-violating signal μ→eγ. Detecting monoenergetic neutrinos from DM annihilation in next-generation neutrino detectors offers a promising way to test this scenario.…”
Get full text
Article -
1748
Strange Hadron Production in Au+Au Collisions at RHIC Beam Energy Scan
Published 2023-01-01Get full text
Article -
1749
Dynamical inflation stimulated cogenesis
Published 2024-02-01“…The singlet fermions couple to SM leptons and generate neutrino masses via the inverse seesaw mechanism. …”
Get full text
Article -
1750
Leptogenesis in SO(10) models with A4 modular symmetry
Published 2022-10-01“…The predictions for the light neutrino masses, the effective mass in neutrinoless double beta decay and the leptonic CP violation phases are discussed.…”
Get full text
Article -
1751
A Brief Review of Chiral Chemical Potential and Its Physical Effects
Published 2020-12-01Get full text
Article -
1752
Renormalisation of SMEFT bosonic interactions up to dimension eight by LNV operators
Published 2023-06-01“…Abstract We present the renormalisation group running of the bosonic operators of the Standard Model effective field theory (SMEFT) by the Lepton Number Violating operators (LNVs) at 1-loop order up to O $$ \mathcal{O} $$ (v 4 /Λ4), with v ∼ 246 GeV as the electroweak scale and Λ as the SMEFT cut-off. …”
Get full text
Article -
1753
Absolute neutrino mass scale and dark matter stability from flavour symmetry
Published 2022-10-01“…In addition, Σ(81) leads to striking predictions in the lepton sector: only Inverted Ordering is realised, the absolute neutrino mass scale is predicted to be m lightest ≈ 7.5×10 −4 eV and the Majorana phases are correlated in such a way that |m ee | ≈ 0.018 eV. …”
Get full text
Article -
1754
SMEFT goes dark: Dark Matter models for four-fermion operators
Published 2023-09-01“…We also briefly discuss how our DM models could be constrained by reinterpretations of LHC searches and the prospects for HL-LHC and future lepton colliders.…”
Get full text
Article -
1755
Analysis of some b→cτν¯τ decay modes beyond the standard model
Published 2023-09-01“…We explore the q2-dependency of different observables, such as the differential branching fraction, ratio of branching fractions, forward-backward asymmetry, convexity parameter, and longitudinal polarization of the charged lepton, related to these decay processes in the standard model and beyond.…”
Get full text
Article -
1756
Complete NLO corrections to off-shell t t ¯ Z $$ \textrm{t}\overline{\textrm{t}}\textrm{Z} $$ production at the LHC
Published 2023-09-01“…In this work we present NLO-accurate predictions for the production and decay of a top-antitop pair in association with a Z boson at the LHC, in the multi-lepton decay channel. The complete set of LO contributions and NLO corrections of EW and QCD origin is included. …”
Get full text
Article -
1757
Local analytic sector subtraction for initial- and final-state radiation at NLO in massless QCD
Published 2022-12-01“…A numerical validation is provided for a variety of processes relevant to lepton as well as hadron colliders. This work constitutes a relevant step in view of the application of our subtraction method to processes involving initial-state radiation at next-to-next-to-leading order in QCD.…”
Get full text
Article -
1758
Spin studies via Drell-Yan processes at PANDA
Published 2014-06-01“…One of the main goals of the forthcoming experiments at FAIR is the study of Drell-Yan lepton pairs by means of proton-antiproton annihilations, taking also advantage of the expected high luminosity. …”
Get full text
Article -
1759
Dark Gauge U(1) symmetry for an alternative left–right model
Published 2018-02-01“…Abstract An alternative left–right model of quarks and leptons, where the $$SU(2)_R$$ SU(2)R lepton doublet $$(\nu ,l)_R$$ (ν,l)R is replaced with $$(n,l)_R$$ (n,l)R so that $$n_R$$ nR is not the Dirac mass partner of $$\nu _L$$ νL , has been known since 1987. …”
Get full text
Article -
1760
Search for a Heavy Toplike Quark in p p ¯ Collisions at √ s = 1.96 TeV
Published 2021“…We perform parallel searches for t ′→Wb and t ′→Wq (where q is a generic down-type quark) in events containing a lepton and four or more jets. By performing a fit to the two-dimensional distribution of total transverse energy versus reconstructed t ′ quark mass, we set upper limits on the t ′t ̄′ production cross section and exclude a standard model fourth-generation t ′ quark decaying to Wb (Wq) with mass below 358 (340)GeV/c2 at 95% C.L. © 2011 American Physical Society.…”
Get full text
Article