Search results for "The Standard Model"

showing 10 items of 466 documents

Lepton universality violation with lepton flavor conservation in B-meson decays

2015

Anomalies in semileptonic B-meson decays present interesting patterns that might be revealing the shape of the new physics to come. Under the assumption that neutrino and charged lepton mass terms are the only sources of flavor violation and given the hierarchy between the two, we find that charged lepton universality violation without charged lepton flavor violation naturally arises. This can account for a deficit of B + → K + μμ over B + → K + ee decays with new physics coupled predominantly to muons and a new physics scale of a few TeV. A generic prediction of this scenario is a large enhacement of tauonic B decay rates that, in particular, could accommodate an excess in B → D (∗) τ ν. F…

Particle physicsNuclear and High Energy PhysicsPhysics beyond the Standard ModelB-PhysicsAtomicMathematical SciencesParticle and Plasma PhysicsEffective field theoryLeptoquarkB mesonNuclearMathematical PhysicsPhysicsQuantum PhysicsMuonRare DecaysHigh Energy Physics::PhenomenologyMolecularObservablehep-phNuclear & Particles PhysicsPhysical SciencesBeyond Standard ModelHigh Energy Physics::ExperimentNeutrinoLeptonJournal of High Energy Physics
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Global effective-field-theory analysis of new-physics effects in (semi)leptonic kaon decays

2016

We analyze the decays $K\to\pi\ell\nu$ and $P\to\ell\nu$ ($P=K,\pi$, $\ell=e,\,\mu$) using a low-energy Effective-Field-Theory approach to parametrize New Physics and study the complementarity with baryon $\beta$ decays. We then provide a road map for a global analysis of the experimental data, with all the Wilson coefficients simultaneously, and perform a fit leading to numerical bounds for them and for $V_{us}$. A prominent result of our analysis is a reinterpretation of the well-known $V_{ud}-V_{us}$ diagram as a strong constraint on new physics. Finally, we reinterpret our bounds in terms of the $SU(2)_L\times~U(1)_Y$-invariant operators, provide bounds to the corresponding Wilson coeff…

Particle physicsNuclear and High Energy PhysicsPhysics beyond the Standard ModelFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective lagrangian[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Effective field theoryComputer Science::Symbolic Computation010306 general physicsParticle Physics - PhenomenologyPhysicsLarge Hadron Collider[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics - Lattice (hep-lat)Renormalization groupBaryonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Journal of High Energy Physics
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Sensitivities to neutrino electromagnetic properties at the TEXONO experiment

2015

18 pages.- 4 figures.- 1 table

Particle physicsNuclear and High Energy PhysicsQuenching factorCoherent elastic neutrino-nucleus scatteringReactor neutrinosPhysics beyond the Standard ModelFOS: Physical sciencesWeak interactionNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Charge radiusNeutrino oscillationPhysicsNeutral currentScatteringFísicalcsh:QC1-999Neutrino magnetic momentHigh Energy Physics - PhenomenologyCoherent elastic neutrino–nucleus scattering (CENNS)Neutrino charge radiusNeutrinoRandom phase approximationWeak mixing anglelcsh:PhysicsPhysics Letters B
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Observing Higgs boson production through its decay into gamma-rays: A messenger for Dark Matter candidates

2012

In this Letter, we study the gamma-ray signatures subsequent to the production of a Higgs boson in space by dark matter annihilations. We investigate the cases where the Higgs boson is produced at rest or slightly boosted and show that such configurations can produce characteristic bumps in the gamma-ray data. These results are relevant in the case of the Standard Model-like Higgs boson provided that the dark matter mass is about 63 GeV, 109 GeV or 126 GeV, but can be generalized to any other Higgs boson masses. Here, we point out that it may be worth looking for a 63 GeV line since it could be the signature of the decay of a Standard Model-like Higgs boson produced in space, as in the case…

Particle physicsNuclear and High Energy Physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Physics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaDark matterFOS: Physical sciencesNeutralino annihilationElementary particle7. Clean energy01 natural sciencesNuclear physicssymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsLight dark matterBosonPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)010308 nuclear & particles physics[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]High Energy Physics::PhenomenologyScalar bosonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Higgs bosonsymbolsHigh Energy Physics::ExperimentAstrophysics - High Energy Astrophysical PhenomenaHiggs mechanismRoot-s=7 tev
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Search for charged lepton flavor violation in narrow Y decays

2010

Charged-lepton flavor-violating processes are unobservable in the standard model, but they are predicted to be enhanced in several extensions to the standard model, including supersymmetry and models with leptoquarks or compositeness. We present a search for such processes in a sample of 99 × 10 6 Υ ( 2 S ) decays and 117 × 10 6 Υ ( 3 S ) decays collected with the BABAR detector. We place upper limits on the branching fractions B ( Υ ( n S ) → e ± τ ∓ ) and B ( Υ ( n S ) → μ ± τ ∓ ) ( n = 2 , 3 ) at the 10 − 6 level and use these results to place lower limits of order 1 TeV on the mass scale of charged-lepton flavor-violating effective operators.

Particle physicsPACS: 13.20.Gd 11.30.Hv 14.40.NdPhysics beyond the Standard ModelBABARGeneral Physics and AstronomyElementary particle01 natural sciencesPARTICLE PHYSICS; PEP2; BABARParticle identificationParticle decay0103 physical sciencesPEP2Grand Unified Theory010306 general physicsPhysics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologySupersymmetryBABAR detectorHEPPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica de partículesExperimentsLepton
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Search for Production of Invisible Final States in Single-Photon Decays of Υ(1S)

2010

We search for single-photon decays of the Upsilon(1S) resonance, Upsilon->gamma+invisible, where the invisible state is either a particle of definite mass, such as a light Higgs boson A0, or a pair of dark matter particles, chi chi-bar. Both A0 and chi are assumed to have zero spin. We tag Upsilon(1S) decays with a dipion transition Upsilon(2S)->pi+pi-Upsilon(1S) and look for events with a single energetic photon and significant missing energy. We find no evidence for such processes in the mass range m_A0<=9.2 GeV and m_chi<=4.5 GeV in the sample of 98e6 Upsilon(2S) decays collected with the BaBar detector and set stringent limits on new physics models that contain light dark ma…

Particle physicsPhotonAstrophysics::High Energy Astrophysical PhenomenaPhysics beyond the Standard ModelElectron–positron annihilationDark matterFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)PACS: 13.20.Gd 12.60.Jv 14.80.Da 95.35.+d0103 physical sciencessingle-photon decays of Upsilon(1S)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsLight dark matterPhysicsMissing energy010308 nuclear & particles physicsParticle physicsBABAR detectorHEPBaBarHiggs bosonHigh Energy Physics::ExperimentFísica de partículesExperimentsBaBar detector at SLAC
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Photons, Photon Jets and Dark Photons at 750 GeV and Beyond

2016

In new physics searches involving photons at the LHC, one challenge is to distinguish scenarios with isolated photons from models leading to "photon jets". For instance, in the context of the 750 GeV diphoton excess, it was pointed out that a true diphoton resonance $S \to \gamma\gamma$ can be mimicked by a process of the form $p p \to S \to a a \to 4\gamma$, where $S$ is a new scalar with a mass of 750 GeV and $a$ is a light pseudoscalar decaying to two collinear photons. Photon jets can be distinguished from isolated photons by exploiting the fact that a large fraction of photons convert to an $e^+e^-$ pair inside the inner detector. In this note, we quantify this discrimination power, an…

Particle physicsPhotonPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaScalar (mathematics)collinearFOS: Physical sciencesPhysics::OpticsContext (language use)Jet (particle physics)01 natural sciencesDark photonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)jet [photon]0103 physical sciencesddc:530010306 general physicspseudoscalarEngineering (miscellaneous)two-photonlifetimePhysicsnew physics010308 nuclear & particles physics750 GeV diphoton excesssensitivityPseudoscalarHigh Energy Physics - PhenomenologyCERN LHC CollHigh Energy Physics::ExperimentRegular Article - Theoretical Physics
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Bottom-up approach within the electroweak effective theory: Constraining heavy resonances

2020

The LHC has confirmed the existence of a mass gap between the known particles and possible new states. Effective field theory is then the appropriate tool to search for low-energy signals of physics beyond the Standard Model. We adopt the general formalism of the electroweak effective theory, with a non-linear realization of the electroweak symmetry breaking, where the Higgs is a singlet with independent couplings. At higher energies we consider a generic resonance Lagrangian which follows the above-mentioned non-linear realization and couples the light particles to bosonic heavy resonances with $J^P=0^\pm$ and $J^P=1^\pm$. Integrating out the resonances and assuming a proper short-distance…

Particle physicsPhotonPhysics beyond the Standard ModelFOS: Physical sciencesMateria - Propiedades.01 natural sciencesColisiones (Física nuclear)Computer Science::Digital LibrariesHigh Energy Physics - Phenomenology (hep-ph)Collisions (Nuclear physics)0103 physical sciencesEffective field theoryPartículas (Física nuclear)Symmetry breakingElectromagnetismo010306 general physicsParticles (Nuclear physics)PhysicsMatter - Properties.010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyResonanceHigh Energy Physics - PhenomenologyHiggs bosonMass gapPhysical Review
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Electroweak Higgs production with HiggsPO at NLO QCD

2017

We present the HiggsPO UFO model for Monte Carlo event generation of electroweak $VH$ and VBF Higgs production processes at NLO in QCD in the formalism of Higgs pseudo-observables (PO). We illustrate the use of this tool by studying the QCD corrections, matched to a parton shower, for several benchmark points in the Higgs PO parameter space. We find that, while being sizable and thus important to be considered in realistic experimental analyses, the QCD higher-order corrections largely factorize. As an additional finding, based on the NLO results, we advocate to consider 2D distributions of the two-jet azimuthal-angle difference and the leading jet $p_T$ for new physics searches in VBF Higg…

Particle physicsPhysics and Astronomy (miscellaneous)530 PhysicsPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeMonte Carlo methodFOS: Physical scienceslcsh:Astrophysics10192 Physics InstituteParameter space01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Factorization0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity3101 Physics and Astronomy (miscellaneous)010306 general physicsParton showerEngineering (miscellaneous)PhysicsQuantum chromodynamics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyHiggs bosonlcsh:QC770-798High Energy Physics::Experiment2201 Engineering (miscellaneous)
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Fermion pair production in e+e- collisions at 189-209 GeV and constraints on physics beyond the Standard Model

2006

Cross sections, angular distributions and forward-backward asymmetries are presented, of two-fermion events produced in e+e- collisions at centre-of-mass energies from 189 to 209 GeV at LEP, measured with the ALEPH detector. Results for e+e-, mu+mu-, tau+tau-, qq, bb and cc production are in agreement with the Standard Model predictions. Constraints are set on scenarios of new physics such as four-fermion contact interactions, leptoquarks, Z' bosons, TeV-scale quantum gravity and R-parity violating squarks and sneutrinos.

Particle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelElectron–positron annihilationFOS: Physical sciences01 natural sciences7. Clean energyStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Leptoquark010306 general physicsEngineering (miscellaneous)BosonPhysicsSystematic Uncertainty Standard Model Prediction Aleph Collaboration Hadronic Cross Section Tematic Uncertainty010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFermionSupersymmetryPair productionHigh Energy Physics::ExperimentParticle Physics - Experiment
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