Search results for "BOSONS"

showing 10 items of 83 documents

Testing for new physics with low-energy anti-neutrino sources: LAMA as a case study

1998

Some electroweak models with extended neutral currents, such as those based on the $E_6$ group, lead to an increase of the $\bar{\nu}-e$ scattering cross section at energies below 100 keV. We propose to search for the heavy Z' boson contribution in an experiment with a high-activity artificial neutrino source and with a large-mass detector. We present the case for the LAMA experiment with a large NaI(Tl) detector located at the Gran Sasso underground laboratory. The neutrino flux is known to within a one percent accuracy, in contrast to the reactor case and one can reach lower neutrino energies. Both features make our proposed experiment more sensitive to extended gauge models, such as the …

GAUGE BOSONSNuclear and High Energy PhysicsParticle physicsVIOLATIONPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelFOS: Physical sciencesFluxMASSSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Phenomenology (hep-ph)GAUGE BOSONS; MASS; CONSTRAINTS; SCATTERING; VIOLATION; SEARCHSEARCHSCATTERINGSensitivity (control systems)BosonPhysicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyElectroweak interactionDetectorCONSTRAINTSFísicaGauge (firearms)High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoNuclear Physics B
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Limits on neutral Higgs boson production in the forward region in $pp$ collisions at $\sqrt{s} = 7$ TeV

2013

Limits on the cross-section times branching fraction for neutral Higgs bosons, produced in p p collisions at root s = 7 TeV, and decaying to two tau leptons with pseudorapidities between 2.0 and 4.5, are presented. The result is based on a dataset, corresponding to an integrated luminosity of 1.0 fb(-1), collected with the LHCb detector. Candidates are identified by reconstructing final states with two muons, a muon and an electron, a muon and a hadron, or an electron and a hadron. A model independent upper limit at the 95% confidence level is set on a neutral Higgs boson cross-section times branching fraction. It varies from 8.6 pb for a Higgs boson mass of 90 GeV to 0.7 pb for a Higgs bos…

GravitacióSEARCH; MSSM; LHCHadronStandard-model Higgs boson7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Teoria quànticaNuclear ExperimentQCBosonPhysicsHiggs physicsQuantum field theoryHiggs bosonProduction (computer science)Física nuclearLHCHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified leptons photons or other nonhadronic particlesParticle Physics - ExperimentGravitationParticle physicsTeoria quàntica de campsNuclear and High Energy PhysicsFOS: Physical sciencesStandard-model Higgs bosons; Supersymmetric Higgs bosons; Hadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified leptons photons or other nonhadronic particlesHadronsPartícules (Física nuclear)Standard ModelSEARCH0103 physical sciences010306 general physicsLarge Hadron Collider (France and Switzerland)Standard-model Higgs bosonsMuonHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionComputer Science::Information RetrievalHadron-Hadron Scattering; Higgs physicsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsHiggs physicSupersymmetric Higgs bosonSupersymmetric Higgs bosonsQuantum theoryHadron-Hadron Scattering; Higgs physics; Nuclear and High Energy PhysicsHigh Energy Physics::ExperimentMSSMLepton
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Search for high-mass resonances decaying to dimuons at CDF.

2009

We present a search for high-mass neutral resonances using dimuon data corresponding to an integrated luminosity of 2.3 fb(-1) collected in pp collisions at s=1.96 TeV by the CDF II detector at the Fermilab Tevatron. No significant excess above the standard model expectation is observed in the dimuon invariant-mass spectrum. We set 95% confidence level upper limits on sigma BR(pp -> X ->mu mu), where X is a boson with spin-0, 1, or 2. Using these cross section limits, we determine lower mass limits on sneutrinos in R-parity-violating supersymmetric models, Z(') bosons, and Kaluza-Klein gravitons in the Randall-Sundrum model.

HIGH MASS RESONANCEParticle physicsFermilab TevatronTevatronGeneral Physics and AstronomyFOS: Physical sciencesddc:500.2114 Physical sciencesResonance7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsTellurium compoundsHigh Energy Physics - Experiment (hep-ex)Integrated luminosities0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsBosonsBosonPhysicsMuonMass spectrometryhep-ex010308 nuclear & particles physicsPhysicsInvariant-mass spectrum13.85.Rm 13.85.Qk 12.60.Cn 14.70.Pw 04.50.-hHigh Energy Physics::PhenomenologyConfidence levelsGravitonSupersymmetryUpper limitsSupersymmetric modelsCross sectionsRandall–Sundrum modelThe standard modelsMass spectrumCDFHigh Energy Physics::ExperimentPhysical review letters
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D-Pseudo-Bosons, Complex Hermite Polynomials, and Integral Quantization

2015

The D-pseudo-boson formalism is illustrated with two examples. The first one involves deformed complex Hermite polynomials built using finite-dimensional irreducible representations of the group GL(2, C) of invertible 2 × 2 matrices with complex entries. It reveals interesting aspects of these representations. The second example is based on a pseudo-bosonic generalization of operator-valued functions of a complex variable which resolves the identity. We show that such a generalization allows one to obtain a quantum pseudo-bosonic version of the complex plane viewed as the canonical phase space and to understand functions of the pseudo-bosonic operators as the quantized versions of functions…

Hermite polynomials010102 general mathematics01 natural scienceslaw.inventionClassical orthogonal polynomialsAlgebraQuantization (physics)Invertible matrixlawIrreducible representationPhase space0103 physical sciencesCoherent statespseudo-bosonsGeometry and Topology0101 mathematics010306 general physicsSettore MAT/07 - Fisica MatematicaComplex planeMathematical PhysicsAnalysisMathematics
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Elementary Goldstone Higgs boson and dark matter

2015

We investigate a perturbative extension of the Standard Model featuring elementary pseudo-Goldstone Higgs and dark matter particles. These are two of the five Goldstone bosons parametrising the SU(4)/Sp(4) coset space. They acquire masses, and therefore become pseudo-Goldstone bosons, due to the embedding of the Yukawa and the electroweak gauge interactions that do not preserve the full SU(4) symmetry. At the one-loop order the top corrections dominate and align the vacuum in the direction where the Higgs is mostly a pseudo-Goldstone boson. Because of the perturbative and elementary nature of the theory, the quantum corrections are precisely calculable. The remaining pseudo-Goldstone boson …

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsHiggs bosonHigh Energy Physics::LatticeFOS: Physical sciencesElementary particleTechnicolor01 natural sciencesdark matterStandard Modelsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosons0103 physical sciences010306 general physicsCondensed Matter::Quantum GasesPhysicsGauge bosonta114relic densityelectroweak interaction010308 nuclear & particles physicshep-thHigh Energy Physics::Phenomenologyhep-phHigh Energy Physics - PhenomenologyHiggs fieldscalar particleHigh Energy Physics - Theory (hep-th)symbolsHiggs bosonLHCHiggs mechanismMinimal Supersymmetric Standard ModelPhysical Review D
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Finite size spectrum of SU(N) principal chiral field from discrete Hirota dynamics

2016

Using recently proposed method of discrete Hirota dynamics for integrable (1+1)D quantum field theories on a finite space circle of length L, we derive and test numerically a finite system of nonlinear integral equations for the exact spectrum of energies of SU(N)xSU(N) principal chiral field model as functions of m L, where m is the mass scale. We propose a determinant solution of the underlying Y-system, or Hirota equation, in terms of determinants (Wronskians) of NxN matrices parameterized by N-1 functions of the spectral parameter, with the known analytical properties at finite L. Although the method works in principle for any state, the explicit equations are written for states in the …

High Energy Physics - TheoryNuclear and High Energy PhysicsSigma modelField (physics)FOS: Physical sciences2 dimensionsrepresentation-theory01 natural sciencesexcited-state energiesnonlinear integral-equationsQuantum mechanics0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. Radioactivityvolume dependenceQuantum field theory010306 general physicsS-matrixMathematical physicsPhysics[PHYS]Physics [physics][ PHYS ] Physics [physics]010308 nuclear & particles physicsWronskiano(n) sigma-modeln phase-transitionState (functional analysis)goldstone bosonsAdS/CFT correspondenceHigh Energy Physics - Theory (hep-th)lcsh:QC770-798tba equations
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Pinch Technique: Theory and Applications

2009

We review the theoretical foundations and the most important physical applications of the Pinch Technique (PT). This general method allows the construction of off-shell Green’s functions in non-Abelian gauge theories that are independent of the gauge-fixing parameter and satisfy ghost-free Ward identities. We first present the diagrammatic formulation of the technique in QCD, deriving, at one loop, the gauge independent gluon self-energy, quark–gluon vertex, and three-gluon vertex, together with their Abelian Ward identities. The generalization of the PT to theories with spontaneous symmetry breaking is carried out in detail, and the profound connection with the optical theorem and the disp…

High Energy Physics - TheoryParticle physicsSpontaneous symmetry breakingGluonsHigh Energy Physics::LatticeFOS: Physical sciencesGeneral Physics and AstronomyDynamical mass generationGauge-invarianceSchwinger–Dyson equationsRenormalizationTheoretical physicsQuantization (physics)symbols.namesakeHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Non-Abelian gauge theoriesFeynman diagramGauge theoryGauge bosonsQuantum chromodynamicsPhysicsBackground field methodGreens functionsElectroweak interactionHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)symbols
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Bicoherent-State Path Integral Quantization of a non-Hermitian Hamiltonian

2020

We introduce, for the first time, bicoherent-state path integration as a method for quantizing non-hermitian systems. Bicoherent-state path integrals arise as a natural generalization of ordinary coherent-state path integrals, familiar from hermitian quantum physics. We do all this by working out a concrete example, namely, computation of the propagator of a certain quasi-hermitian variant of Swanson's model, which is not invariant under conventional $PT$-transformation. The resulting propagator coincides with that of the propagator of the standard harmonic oscillator, which is isospectral with the model under consideration by virtue of a similarity transformation relating the corresponding…

High Energy Physics - TheorySwanson modelFOS: Physical sciencesGeneral Physics and AstronomyPT symmetrysymbols.namesakeFeynman diagramHarmonic oscillatorMathematical PhysicsNon-hermitian hamiltoniansMathematical physicsPhysicsQuantum PhysicsQuantization (signal processing)PropagatorMathematical Physics (math-ph)Bicoherent statesHermitian matrixIsospectralHigh Energy Physics - Theory (hep-th)Path integral quantizationPath integral formulationsymbolsPseudo-bosonsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)
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Combining data from high-energy p p -reactions and neutrinoless double-beta decay: Limits on the mass of the right-handed boson

2016

From the recently established lower-limits on the nonobservability of the neutrinoless double-beta decay of 76Ge (GERDA collaboration) and 136Xe (EXO-200 and KamLAND-Zen collaborations), combined with the ATLAS and CMS data, we extract limits for the left-right (LR) mixing angle, of the SU(2)L ×SU(2)R electroweak Hamiltonian. For the theoretical analysis, which is a model dependent, we have adopted a minimal extension of the Standard Model (SM) of Electroweak Interactions belonging to the SU(2)L ×SU(2)R representation. The nuclear-structure input of the analysis consists of a set of matrix elements and phase-space factors, and the experimental lower-limits for the half-lives. The other inpu…

Nuclear and High Energy PhysicsHigh energyParticle physicsCiencias AstronómicasPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelCiencias FísicasGeneral Physics and Astronomy01 natural sciencesRIGHT-HANDED CURRENTS//purl.org/becyt/ford/1 [https]Nuclear physicssymbols.namesakeNEUTRINOLESS DOUBLE-BETA-DECAYDouble beta decay0103 physical sciences010306 general physicsMASS OF THE RIGHT-HANDED BOSONSBosonPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsAtlas (topology)Electroweak interactionMass of the right-handed bosonsRight-handed currents//purl.org/becyt/ford/1.3 [https]Minimal extension of the standard modelAstronomíasymbolsNeutrinoless double-beta-decayMINIMAL EXTENSION OF THE STANDARD MODELHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)CIENCIAS NATURALES Y EXACTAS
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NLO QCD+EW predictions for V+jets including off-shell vector-boson decays and multijet merging

2016

We present next-to-leading order (NLO) predictions including QCD and electroweak (EW) corrections for the production and decay of off-shell electroweak vector bosons in association with up to two jets at the 13 TeV LHC. All possible dilepton final states with zero, one or two charged leptons that can arise from off-shell W and Z bosons or photons are considered. All predictions are obtained using the automated implementation of NLO QCD+EW corrections in the OpenLoops matrix-element generator combined with the Munich and Sherpa Monte Carlo frameworks. Electroweak corrections play an especially important role in the context of BSM searches, due to the presence of large EW Sudakov logarithms a…

Nuclear and High Energy PhysicsParticle physics530 PhysicsFOS: Physical sciencesContext (language use)10192 Physics InstituteAstrophysics::Cosmology and Extragalactic AstrophysicsJet (particle physics)01 natural sciencesVector bosonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences3106 Nuclear and High Energy Physics010306 general physicsNuclear ExperimentQCBosonQuantum chromodynamicsPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyW′ and Z′ bosonsHigh Energy Physics::ExperimentLepton
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