Search results for " atom"

showing 10 items of 1526 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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Probing Higgs-portal dark matter with vector-boson fusion

2020

We constrain the Higgs-portal model employing the vector-boson fusion channel at the LHC. In particular, we include the phenomenologically interesting parameter region near the Higgs resonance, where the Higgs-boson mass is close to the threshold for dark-matter production and a running-width prescription has to be employed for the Higgs-boson propagator. Limits for the Higgs-portal coupling as a function of the dark-matter mass are derived from the CMS search for invisible Higgs-boson decays in vector-boson fusion at 13 TeV. Furthermore, we perform projections for the 14 TeV HL-LHC and the 27 TeV HE-LHC taking into account a realistic estimate of the systematic uncertainties. The respectiv…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHiggs PhysicsBranching fractionDark matterHigh Energy Physics::PhenomenologyPropagatorFOS: Physical sciences530Resonance (particle physics)Vector bosonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonlcsh:QC770-798ddc:530High Energy Physics::Experimentlcsh:Nuclear and particle physics. Atomic energy. RadioactivityBosonJournal of High Energy Physics
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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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Improved $K_{e3}$ radiative corrections sharpen the $K_{\mu 2}$--$K_{l3}$ discrepancy

2021

The measurements of $V_{us}$ in leptonic $(K_{\mu 2})$ and semileptonic $(K_{l3})$ kaon decays exhibit a $3\sigma$ disagreement, which could originate either from physics beyond the Standard Model or some large unidentified Standard Model systematic effects. Clarifying this issue requires a careful examination of all existing Standard Model inputs. Making use of a newly-proposed computational framework and the most recent lattice QCD results, we perform a comprehensive re-analysis of the electroweak radiative corrections to the $K_{e3}$ decay rates that achieves an unprecedented level of precision of $10^{-4}$, which improves the current best results by almost an order of magnitude. No larg…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsPhysics beyond the Standard ModelElectroweak interactionLattice QCDLattice QCDQC770-79801 natural sciencesStandard ModelHigh Energy Physics - ExperimentKaon PhysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesRadiative transferPrecision QEDHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentOrder of magnitude
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Nucleon polarizabilities: From Compton scattering to hydrogen atom

2016

We review the current state of knowledge of the nucleon polarizabilities and of their role in nucleon Compton scattering and in hydrogen spectrum. We discuss the basic concepts, the recent lattice QCD calculations and advances in chiral effective-field theory. On the experimental side, we review the ongoing programs aimed to measure the nucleon (scalar and spin) polarizabilities via the Compton scattering processes, with real and virtual photons. A great part of the review is devoted to the general constraints based on unitarity, causality, discrete and continuous symmetries, which result in model-independent relations involving nucleon polarizabilities. We (re-)derive a variety of such rel…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryUnitarityAtomic Physics (physics.atom-ph)010308 nuclear & particles physicsLattice field theoryCompton scatteringFOS: Physical sciencesVirtual particleLattice QCD01 natural sciencesPhysics - Atomic PhysicsLamb shiftNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentProgress in Particle and Nuclear Physics
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Sterile neutrinos with altered dispersion relations revisited

2020

In this paper we investigate neutrino oscillations with altered dispersion relations in the presence of sterile neutrinos. Modified dispersion relations represent an agnostic way to parameterize new physics. Models of this type have been suggested to explain global neutrino oscillation data, including deviations from the standard three-neutrino paradigm as observed by a few experiments. We show that, unfortunately, in this type of models new tensions arise turning them incompatible with global data.

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrino010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - Experiment3. Good healthHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Dispersion relationBeyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsNeutrino oscillationJournal of High Energy Physics
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Coherent Smith-Purcell radiation for minimally invasive bunch length measurement at the subpicosecond time scale

2021

Physical review accelerators and beams 24(4), 042803 (2021). doi:10.1103/PhysRevAccelBeams.24.042803

PhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsbusiness.industryScale (descriptive set theory)QC770-798Surfaces and InterfacesRadiation53001 natural sciencesMeasure (mathematics)Superconducting acceleratorSpace chargeLength measurementOpticsNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesCathode rayPhysics::Accelerator Physicsddc:530010306 general physicsbusinessBeam (structure)Physical Review Accelerators and Beams
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High brilliance uranium beams for the GSI FAIR

2017

The 40 years old GSI-UNILAC (Universal Linear Accelerator) as well as the heavy ion synchrotron SIS18 will serve as a high current heavy ion injector for the new FAIR (Facility for Antiproton and Ion Research) synchrotron SIS100. In the context of an advanced machine investigation program in combination with the ongoing UNILAC upgrade program, a new uranium beam intensity record (11.5 emA, ${\mathrm{U}}^{29+}$) at very high beam brilliance was achieved recently in a machine experiment campaign. This is an important step paving the way to fulfill the FAIR heavy ion high intensity beam requirements. Results of high current uranium beam measurements applying a newly developed pulsed hydrogen g…

PhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicschemistry.chemical_elementContext (language use)Surfaces and InterfacesUranium01 natural sciencesSynchrotronlaw.inventionNuclear physicsUpgradechemistrylawUniversal linear accelerator0103 physical sciencesPhysics::Accelerator PhysicsFacility for Antiproton and Ion Researchlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsIntensity (heat transfer)Beam (structure)Physical Review Accelerators and Beams
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Low-temperature X-ray detectors for precise Lamb shift measurements on hydrogen-like heavy ions

2000

The precise determination of the Lamb shift in heavy hydrogen-like ions provides a sensitive test of quantum electrodynamics in very strong Coulomb"elds, not accessible otherwise. For the investigation of the Lyman-a transitions in 208Pb81‘ or 238U91‘ with su$cient accuracy a high resolving calorimetric detector for hard X-rays (E)100 keV) is presently developed. The detector modules consist of arrays of silicon thermistors and of X-ray absorbers made of high Z material to optimize the absorption e$ciency. The detectors are housed in a specially designed 3He/4He dilution refrigerator with a side arm which "ts to the geometry of the internal target of the storage ring ESR at GSI Darmstadt. T…

PhysicsNuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsElectric potential energyBinding energyDetectorX-ray detectorHydrogen atomLamb shiftNuclear physicsCoulombAtomic physicsInstrumentationStorage ringNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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