Search results for "Phenomenological model"

showing 10 items of 68 documents

Cornering Colored Coannihilation

2018

In thermal dark matter models, allowing the dark matter candidate to coannihilate with another particle can considerably loosen the relic density constraints on the dark matter mass. In particular, introducing a single strongly interacting coannihilation partner in a dark matter model can bring the upper bound on the dark sector energy scale from a few TeV up to about 10 TeV. While these energies are outside the LHC reach, a large part of the parameter space for such coannihilating models can be explored by future hadron colliders. In this context, it is essential to determine whether the current bounds on dark matter simplified models also hold in non-minimal scenarios. In this paper, we s…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsDark matterHadronFOS: Physical sciencesContext (language use)Minimal modelsAstrophysics::Cosmology and Extragalactic AstrophysicsParameter space01 natural sciencesUpper and lower boundslaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)law0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsColliderPhenomenological Models
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Collider probes of axion-like particles.

2017

Axion-like particles (ALPs), which are gauge-singlets under the Standard Model (SM), appear in many well-motivated extensions of the SM. Describing the interactions of ALPs with SM fields by means of an effective Lagrangian, we discuss ALP decays into SM particles at one-loop order, including for the first time a calculation of the $a\to\pi\pi\pi$ decay rates for ALP masses below a few GeV. We argue that, if the ALP couples to at least some SM particles with couplings of order $(0.01-1) \mbox{TeV}^{-1}$, its mass must be above 1 MeV. Taking into account the possibility of a macroscopic ALP decay length, we show that large regions of so far unconstrained parameter space can be explored by se…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonLarge Hadron ColliderAnomalous magnetic dipole moment010308 nuclear & particles physicsBranching fractionElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesPhysics::GeophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsAxionPhenomenological ModelsLepton
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Inclusive and exclusive neutrino-nucleus cross sections and the reconstruction of the interaction kinematics

2021

Abstract We present a full kinematic analysis of neutrino-nucleus charged current quasielastic interactions based on the Local Fermi Gas model and the Random Phase Approximation. The model was implemented in the NEUT Monte Carlo framework, which allows us to investigate potentially measurable observables, including hadron distributions. We compare the predictions simultaneously to the most recent T2K and MINERvA charged current (CC) inclusive, CC0π and transverse kinematic-imbalance variable results. We pursuit a microscopic interpretation of the relevant reaction mechanisms, with the aim to achieving in neutrino oscillation experiments a correct reconstruction of the incoming neutrino kine…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsMonte Carlo methodFOS: Physical sciencesObservableKinematics01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCP violationlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino010306 general physicsNeutrino oscillationRandom phase approximationCharged currentPhenomenological ModelsJournal of High Energy Physics
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Parity violating pion electroproduction off the nucleon

1995

Parity violating (PV) contributions due to interference between $\gamma$ and $Z^0$ exchange are calculated for pion electroproduction off the nucleon. A phenomenological model with effective Lagrangians is used to determine the resulting asymmetry for the energy region between threshold and $\Delta(1232)$ resonance. The $\Delta$ resonance is treated as a Rarita-Schwinger field with phenomenological $N \Delta$ transition currents. The background contributions are given by the usual Born terms using the pseudovector $\pi N$ Lagrangian. Numerical results for the asymmetry are presented.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theorymedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesParity (physics)AsymmetryNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)PionPhenomenological modelsymbolsNuclear fusionHigh Energy Physics::ExperimentNucleonNuclear theoryLagrangianmedia_commonZeitschrift f�r Physik A Hadrons and Nuclei
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Emission patterns of neutral pions in40AMeV Ta+Au reactions

2010

Differential cross sections of neutral pions emitted in {sup 181}Ta+{sup 197}Au collisions at a beam energy of 39.5A MeV have been measured with the two-arm photon spectrometer (TAPS). The kinetic energy and transverse momentum spectra of neutral pions cannot be properly described in the framework of the thermal model, nor when the reabsorption of pions is accounted for in a phenomenological model. However, high energy and high momentum tails of the pion spectra can be well fitted through thermal distributions with unexpectedly soft temperature parameters below 10 MeV.

PhysicsNuclear reactionNuclear and High Energy PhysicsPhotonMeson010308 nuclear & particles physicsNuclear TheoryHadronKinetic energy7. Clean energy01 natural sciencesSpectral lineNuclear physicsPion0103 physical sciencesPhenomenological modelAtomic physicsNuclear Experiment010306 general physicsPhysical Review C
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Small-polaron transport inLa0.67Ca0.33MnO3thin films

1998

We present a detailed study of the activated resistivity of ${\mathrm{La}}_{0.67}{\mathrm{Ca}}_{0.33}{\mathrm{MnO}}_{3}$ films up to 600 K under the influence of high magnetic fields. Data in zero field can be explained by small polaron hopping as treated in the Friedman-Holstein theory. Based on the spin orientation of ferromagnetic clusters in a magnetic field, we develop a phenomenological model describing the temperature and field dependence of the resistivity with a minimum of free parameters. We find that the polarons have a magnetic contribution to their activation energy for hopping which depends on the variation of the spin order with increasing temperature and can be modified by a…

PhysicsOrientation (vector space)Condensed matter physicsField (physics)FerromagnetismElectrical resistivity and conductivityPhenomenological modelOrder (ring theory)Condensed Matter::Strongly Correlated ElectronsPolaronMagnetic fieldPhysical Review B
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Singlet ground state magnetism: II. magnetic excitons in paramagnetic TbP

1979

The magneticΓ 1 –Γ 4 exciton of the singlet ground state system TbP has been studied by inelastic neutron scattering above the antiferromagnetic ordering temperature. Considerable dispersion and a pronounced splitting was found in the [100] and [110] directions. Both the band width and the splitting increased rapidly as the transition temperature was approached in accordance with the predictions of the RPA-theory. The dispersion is analysed in terms of a phenomenological model using interactions up to the fourth nearest neighbour.

PhysicsParamagnetismCondensed matter physicsMagnetismTransition temperatureExcitonPhenomenological modelAntiferromagnetismCondensed Matter PhysicsDispersion (chemistry)Inelastic neutron scatteringElectronic Optical and Magnetic MaterialsZeitschrift f�r Physik B Condensed Matter and Quanta
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The coannihilation codex

2015

We present a general classification of simplified models that lead to dark matter (DM) coannihilation processes of the form DM + X $\rightarrow$ SM$_1$ + SM$_2$, where X is a coannihilation partner for the DM particle and SM$_1$, SM$_2$ are Standard Model fields. Our classification also encompasses regular DM pair annihilation scenarios if DM and X are identical. Each coannhilation scenario motivates the introduction of a mediating particle M that can either belong to the Standard Model or be a new field, whereby the resulting interactions between the dark sector and the Standard Model are realized as tree-level and dimension-four couplings. We construct a basis of coannihilation models, cl…

PhysicsParticle physicsNuclear and High Energy PhysicsAnnihilationLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionDark matterFOS: Physical sciencesFermionQuantum number01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Hadronic CollidersSymmetry breaking010306 general physicsPhenomenological ModelsJournal of High Energy Physics
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Neutral Pion Threshold Production atQ2=0.05GeV2/c2and Chiral Perturbation Theory

2001

New data are presented on the $p({e,e}^{\ensuremath{'}}p){\ensuremath{\pi}}^{0}$ reaction at threshold at a four-momentum transfer of ${Q}^{2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.05{\mathrm{GeV}}^{2}{/c}^{2}$. The data were taken with the three-spectrometer setup of the A1 Collaboration at the Mainz Microtron MAMI. The complete center of mass solid angle was covered up to a center of mass energy of 4 MeV above threshold. Combined with measurements at three different values of the virtual photon polarization $\ensuremath{\epsilon}$, the structure functions ${\ensuremath{\sigma}}_{T}$, ${\ensuremath{\sigma}}_{L}$, ${\ensuremath{\sigma}}_{\mathrm{TT}}$, and ${\ensuremath{\sigma…

PhysicsParticle physicsPionChiral perturbation theoryHeavy baryon chiral perturbation theoryPhenomenological modelStructure functionSolid angleGeneral Physics and AstronomySigmaVirtual particleNuclear ExperimentPhysical Review Letters
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Microscopic derivation of the Jaynes-Cummings model with cavity losses

2006

In this paper we provide a microscopic derivation of the master equation for the Jaynes-Cummings model with cavity losses. We single out both the differences with the phenomenological master equation used in the literature and the approximations under which the phenomenological model correctly describes the dynamics of the atom-cavity system. Some examples wherein the phenomenological and the microscopic master equations give rise to different predictions are discussed in detail.

PhysicsQuantum PhysicsQuantum decoherenceJaynes–Cummings modelSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciCavity quantum electrodynamicsFOS: Physical sciences01 natural sciencesAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della Materia010305 fluids & plasmas0103 physical sciencesPhenomenological modelMaster equationQUANTUM-ELECTRODYNAMICS:AYNES-CUMMINGS MODELStatistical physicsQuantum Physics (quant-ph)010306 general physics
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