Search results for "BOSONS"

showing 10 items of 83 documents

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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Finding the Higgs boson through supersymmetry

2009

6 pages, 7 figures.-- PACS nrs.: 12.60.Jv; 13.85.Ni; 14.60.Pq; 14.80.Cp.-- ArXiv pre-print available at: http://arxiv.org/abs/0809.1637

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSupergravity[PACS] Non-standard-model Higgs bosonsElectroweak interactionBosón de HiggsHigh Energy Physics::Phenomenology[PACS] Supersymmetric unified modelsFOS: Physical sciencesFísicaSupersymmetry[PACS] Neutrino mass and mixingSupersymmetry breaking[PACS] Hadron-induced inclusive production with identified hadrons (energy > 10 GeV)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SupersimetríaHiggs bosonHigh Energy Physics::ExperimentNeutrino oscillationMinimal Supersymmetric Standard Model
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Spin and charge currents driven by the Higgs mode in high-field superconductors

2020

The Higgs mode in superconducting materials describes slowly decaying oscillations of the order parameter amplitude. We demonstrate that in superconductors with a built-in spin-splitting field the Higgs mode is strongly coupled to the spin degrees of freedom, allowing for the generation of time-dependent spin currents. Converting such spin currents to electric signals by spin-filtering elements provides a tool for the second-harmonic generation and the electrical detection of the Higgs mode generated by the external irradiation. The nonadiabatic spin torques generated by these spin currents allow for the magnetic detection of the Higgs mode by measuring the precession of the magnetic moment…

Work (thermodynamics)suprajohtavuusFerromagnetic superconductors02 engineering and technology01 natural sciencessuprajohteetTunnel junctionsCondensed Matter::SuperconductivitySpin current0103 physical sciencesmagnetismi010306 general physicsSpin-½PhysicsSuperconductivityHiggs bosonsCondensed matter physicsHigh Energy Physics::PhenomenologyDirect observationMode (statistics)Charge (physics)021001 nanoscience & nanotechnologyMultilayer thin filmsspin (kvanttimekaniikka)Higgs bosonCondensed Matter::Strongly Correlated ElectronsHigh field0210 nano-technologyPhysical Review Research
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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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Massive Spin One and Renormalizable Gauges

2015

For many decades of the last century, physicists were struggling to define consistent (renormalizable and unitarity preserving) models for spin-one massive particles (Proca fields). As we know, this was beautifully achieved by Weinberg, Salam and Glashow in 1967 when they proposed an electroweak unified theory which we now call the Standard Model. The electroweak symmetry breaking mechanism, among other things, generates mass terms for the W and Z bosons, while preserving renormalizability and unitarity. The longitudinal degrees of freedom of the massive spin-one particles are given by the Goldostone bosons. Choosing one gauge or another might seem just a matter of convenience and in most c…

PhysicsRenormalizationHigh Energy Physics::TheoryHiggs fieldTheoretical physicsStandard Model (mathematical formulation)UnitarityHigh Energy Physics::LatticeW and Z bosonsHigh Energy Physics::PhenomenologyElectroweak interactionUnified field theoryBoson
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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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Variational Bethe ansatz approach for dipolar one-dimensional bosons

2020

We propose a variational approximation to the ground state energy of a one-dimensional gas of interacting bosons on the continuum based on the Bethe Ansatz ground state wavefunction of the Lieb-Liniger model. We apply our variational approximation to a gas of dipolar bosons in the single mode approximation and obtain its ground state energy per unit length. This allows for the calculation of the Tomonaga-Luttinger exponent as a function of density and the determination of the structure factor at small momenta. Moreover, in the case of attractive dipolar interaction, an instability is predicted at a critical density, which could be accessed in lanthanide atoms.

[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Dipolar interactionsFOS: Physical sciences02 engineering and technologyGas atomici interagenti01 natural sciencesBethe ansatzVariational methods in quantum mechanicsCondensed Matter - Strongly Correlated ElectronsQuantum mechanics0103 physical sciencesLieb–Liniger model010306 general physicsWave function[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesLieb-Liniger modelStrongly Correlated Electrons (cond-mat.str-el)one dimensional bosonsFunction (mathematics)021001 nanoscience & nanotechnologyQuantum Gases (cond-mat.quant-gas)Exponent[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]0210 nano-technologyStructure factorGround stateCondensed Matter - Quantum Gases
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Ultracold atomic Bose and Fermi spinor gases in optical lattices

2006

We investigate magnetic properties of Mott-insulating phases of ultracold Bose and Fermi spinor gases in optical lattices. We consider in particular the F=2 Bose gas, and the F=3/2 and F=5/2 Fermi gases. We derive effective spin Hamiltonians for one and two atoms per site and discuss the possibilities of manipulating the magnetic properties of the system using optical Feshbach resonances. We discuss low temperature quantum phases of a 87Rb gas in the F=2 hyperfine state, as well as possible realizations of high spin Fermi gases with either 6Li or 132Cs atoms in the F=3/2 state, and with 173Yb atoms in the F=5/2 state.

Condensed Matter::Quantum GasesPhysicseinstein condensationSpinorBose gasCondensed matter physicsFOS: Physical sciencesGeneral Physics and Astronomyresonant lightQuantum phasesState (functional analysis)quantum phasesCondensed Matter - Other Condensed Matterground-statesone bosonssystemsddc:530Condensed Matter::Strongly Correlated ElectronsantiferromagnetsDewey Decimal Classification::500 | Naturwissenschaften::530 | PhysikHyperfine structureOther Condensed Matter (cond-mat.other)Spin-½Fermi Gamma-ray Space TelescopeNew Journal of Physics
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Pseudo-Bosons from Landau Levels

2010

We construct examples of pseudo-bosons in two dimensions arising from the Hamiltonian for the Landau levels. We also prove a no-go result showing that non-linear combinations of bosonic creation and annihilation operators cannot give rise to pseudo-bosons.

Pseudo-bosonFOS: Physical sciencesnon-hermitian HamiltoniansTheoretical physicssymbols.namesakeQuantum mechanicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsBosonPhysicsCondensed Matter::Quantum GasesQuantum Physicslcsh:MathematicsHigh Energy Physics::PhenomenologyCreation and annihilation operatorsAnalysiLandau quantizationMathematical Physics (math-ph)lcsh:QA1-939Non-hermitian HamiltonianLandau theorysymbolspseudo-bosonsGeometry and TopologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Analysis
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𝒟 $\mathcal {D}$ -Deformed Harmonic Oscillators

2015

We analyze systematically several deformations arising from two-dimensional harmonic oscillators which can be described in terms of $\cal{D}$-pseudo bosons. They all give rise to exactly solvable models, described by non self-adjoint hamiltonians whose eigenvalues and eigenvectors can be found adopting the quite general framework of the so-called $\cal{D}$-pseudo bosons. In particular, we show that several models previously introduced in the literature perfectly fit into this scheme.

PhysicsPhysics and Astronomy (miscellaneous)General MathematicsScheme (mathematics)pseudo-bosonsSettore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsHarmonic oscillatorBosonMathematical physicsInternational Journal of Theoretical Physics
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