Search results for "High Energy Physics::Phenomenology"

showing 10 items of 5791 documents

Direct limits on the $B_s^0$ oscillation frequency

2006

Made available in DSpace on 2022-04-28T20:09:59Z (GMT). No. of bitstreams: 0 Previous issue date: 2006-01-01 We report results of a study of the Bs0 oscillation frequency using a large sample of Bs0 semileptonic decays corresponding to approximately 1fb-1 of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider in 2002-2006. The amplitude method gives a lower limit on the Bs0 oscillation frequency at 14.8ps-1 at the 95% C.L. At Δms=19ps-1, the amplitude deviates from the hypothesis A=0 (1) by 2.5 (1.6) standard deviations, corresponding to a two-sided C.L. of 1% (10%). A likelihood scan over the oscillation frequency, Δms, gives a most probable value of 19ps…

Semileptonic decayPhysicsParticle physicsMuonMeson010308 nuclear & particles physicsOscillationHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyCharge (physics)01 natural sciencesNuclear physicsAmplitude0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Production (computer science)High Energy Physics::Experiment14.40.Nd 12.15.Ff 12.15.Hh 13.20.He010306 general physics
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Semileptonic decays ofBcmesons into charmonium states in a relativistic quark model

2005

We use the framework of a relativistic constituent quark model to study the semileptonic transitions of the ${B}_{c}$ meson into $(\overline{c}c)$ charmonium states where $(\overline{c}c)={\ensuremath{\eta}}_{c}(^{1}S_{0})$, $J/\ensuremath{\psi}(^{3}S_{1})$, ${\ensuremath{\chi}}_{c0}(^{3}P_{0})$, ${\ensuremath{\chi}}_{c1}(^{3}P_{1})$, ${h}_{c}(^{1}P_{1})$, ${\ensuremath{\chi}}_{c2}(^{3}P_{2})$, $\ensuremath{\psi}(^{3}D_{2})$. We compute the ${q}^{2}$ dependence of all relevant form factors and give predictions for their semileptonic ${B}_{c}$ decay modes including also their $\ensuremath{\tau}$ modes. We derive a formula for the polar angle distribution of the charged lepton in the $(l{\ens…

Semileptonic decayScattering cross-sectionPhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyQuark modelHelicityHeavy Meson DecayAngular distributionEffective Field TheoryEffective lagrangianQuark modelHigh Energy Physics::ExperimentParticle Physics - PhenomenologyLeptonPhysical Review D
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The Isgur-Wise function from the lattice

1995

We calculate the Isgur-Wise function by measuring the elastic scattering amplitude of a $D$ meson in the quenched approximation on a $24^3\times48$ lattice at $\beta=6.2$, using an $O(a)$-improved fermion action. Fitting the resulting chirally-extrapolated Isgur-Wise function to Stech's relativistic-oscillator parametrization, we obtain a slope parameter $\rho^2=1.2+7-3. We then use this result, in conjunction with heavy-quark symmetry, to extract $V_{cb}$\ from the experimentally measured $\bar B\to D^*l\bar\nu\,$\ differential decay width. We find $|V_{cb}|\sqrt{\tau_B/1.48{\mathrm ps}}= 0.038 +2-2 +8-3, where the first set of errors is due to experimental uncertainties, while the second …

Semileptonic decayStatistics::TheoryParticle physicsEXTRACTIONMesonFORM-FACTORSHigh Energy Physics::LatticeHadronQUARK EFFECTIVE THEORYGeneral Physics and AstronomyFOS: Physical sciencesQuenched approximationElementary particleFaculty of Science\Computer ScienceParticle decayHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)B-MESON DECAYSD mesonB mesonMathematical physicsPhysicsStatistics::ApplicationsHEAVY MESONSHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaVCBQCDHigh Energy Physics - PhenomenologyWILSONHigh Energy Physics::Experiment
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Josephson-junction-based axion detection through resonant activation

2022

We discuss the resonant activation phenomenon on a Josephson junction due to the coupling of the Josephson system with axions. We show how such an effect can be exploited for axion detection. A nonmonotonic behavior, with a minimum, of the mean switching time from the superconducting to the resistive state versus the ratio of the axion energy and the Josephson plasma energy is found. We demonstrate how variations in switching times make it possible to detect the presence of the axion field. An experimental protocol for observing axions through their coupling with a Josephson system is proposed.

Settore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciCondensed Matter - Mesoscale and Nanoscale PhysicsFieldsPhysics::Instrumentation and DetectorsCondensed Matter - SuperconductivityHigh Energy Physics::PhenomenologyFOS: Physical sciencesStatistical PhysicsNonlinear DynamicsAstrophysicsParticlesResonant activationCondensed MatterCondensed Matter; Materials ; Applied Physics; Statistical PhysicsNonlinear Dynamics; Gravitation; Cosmology ; AstrophysicsParticles ; FieldsCosmologySuperconductivity (cond-mat.supr-con)High Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AxionCondensed Matter::SuperconductivityJosephson junctionMesoscale and Nanoscale Physics (cond-mat.mes-hall)Dark matterMaterialsApplied PhysicsGravitation
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"Table 63" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Heavy Jet Mass (RHO) distribution at c.m. energy 133.00 GeV.

Single Differential Cross Section133.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- ScatteringHigh Energy Physics::PhenomenologyDSIG/RHOExclusiveHigh Energy Physics::ExperimentDSIG/DRHONuclear Experiment
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"Table 67" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Heavy Jet Mass (RHO) distribution at c.m. energy 189.00 GeV.

Single Differential Cross Section189.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- ScatteringHigh Energy Physics::PhenomenologyDSIG/RHOExclusiveHigh Energy Physics::ExperimentDSIG/DRHONuclear Experiment
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"Table 69" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Heavy Jet Mass (RHO) distribution at c.m. energy 206.00 GeV.

Single Differential Cross Section206.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- ScatteringHigh Energy Physics::PhenomenologyDSIG/RHOExclusiveHigh Energy Physics::ExperimentDSIG/DRHONuclear Experiment
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"Table 62" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Heavy Jet Mass (RHO) distribution at c.m. energy 91.20 GeV.

Single Differential Cross SectionAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- ScatteringHigh Energy Physics::PhenomenologyDSIG/RHOExclusiveHigh Energy Physics::ExperimentDSIG/DRHO91.2Nuclear Experiment
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"Table 64" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Heavy Jet Mass (RHO) distribution at c.m. energy 161.00 GeV.

Single Differential Cross SectionAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- ScatteringHigh Energy Physics::PhenomenologyDSIG/RHOExclusiveHigh Energy Physics::ExperimentDSIG/DRHONuclear Experiment161.0
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"Table 65" of "Studies of QCD at e+ e- centre-of-mass energies between 91-GeV and 209-GeV."

2004

Heavy Jet Mass (RHO) distribution at c.m. energy 172.00 GeV.

Single Differential Cross SectionAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- ScatteringHigh Energy Physics::PhenomenologyDSIG/RHOExclusiveHigh Energy Physics::ExperimentDSIG/DRHONuclear Experiment172.0
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