Search results for "moment"

showing 10 items of 3027 documents

Unpolarized and polarized elementary kaon electroproduction cross sections measured at MAMI

2012

Present and future research into the electroproduction of kaons plays an im- portant role at Mainz Microtron MAMI. With the Kaos spectrometer employed for kaon detection in the multi-spectrometer facility, cross section measurements of the exclusive p(e;e 0 K + ); 0 reactions at low momentum transfers have been performed. Isobar and Regge-plus-resonance models were compared with the data. These measurements have clearly discriminated between e ective Lagrangian models for photo- and electroproduc- tion of strangeness. New experiments with polarized beam at low four-momentum transfer are addressing the imaginary part of the longitudinal-transverse response in this process, that can be separa…

Coupling constantPhysicsParticle physicsPhysicsQC1-999HadronNuclear TheoryStrangenessHelicityMomentumNuclear physicsIsobarHigh Energy Physics::ExperimentNuclear ExperimentMicrotronBeam (structure)EPJ Web of Conferences
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Prediction of the out-of-plane response of infilled frames under seismic loads by a new fiber-section macro-model

2016

This chapter suggests that an extension of the capability of the traditional inplane macro-models to capture the simultaneous in-plane and Out-Of-Plane (OOP) response of infills. A new simplified macro-model for the assessment of both in plane and out-of-plane responses of infilled frames was developed and validated. The possibility to simulate the arching action is achieved by using distributed plasticity fiber-section elements, able to directly account for the coupling between axial load and bending moment. The arching action is explicitly introduced by the use of fiber-section beam-column elements, which can model the coupling between axial-load and bending moment. The model presented is…

CouplingEngineeringbusiness.industryMaterials Science (miscellaneous)Seismic loadingBuilding and ConstructionStructural engineeringPlasticitymaronry infills. reinforced concrete frames in-plane out-of-plane equivalent strutDisplacement (vector)Mechanism (engineering)Settore ICAR/09 - Tecnica Delle Costruzioniequivalent strutmaronry infills. reinforced concrete framesBending momentMacroout-of-planebusinessin-planeJoint (geology)
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HP-Xe to go: Storage and Transportation of Hyperpolarized 129-Xe

2016

Abstract Recently the spin–lattice relaxation time T 1 of hyperpolarized (HP)- 129 Xe was significantly improved by using uncoated and Rb-free storage vessels of GE180 glass. For these cells, a simple procedure was established to obtain reproducible wall relaxation times of about 18 h. Then the limiting relaxation mechanism in pure Xe is due to the coupling between the nuclear spins and the angular momentum of the Xe–Xe van-der-Waals-molecules. This mechanism can be significantly reduced by using different buffer gases of which CO 2 was discovered to be the most efficient so far. From these values, it was estimated that for a 1:1 mixture of HP-Xe with CO 2 a longitudinal relaxation time of …

CouplingNuclear and High Energy PhysicsAngular momentumSpinsCondensed matter physicsChemistryRelaxation (NMR)BiophysicsAnalytical chemistrychemistry.chemical_element010402 general chemistryCondensed Matter Physics01 natural sciencesBiochemistry0104 chemical sciencessymbols.namesakeXenon0103 physical sciencessymbolsvan der Waals forceTotal pressure010306 general physicsLongitudinal Relaxation Time
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Quantum capture of charged particles by rapidly rotating symmetric top molecules with small dipole moments: analytical comparison of the fly-wheel an…

2013

The rate coefficients for capture of charged particles by spherical top molecules, which by isotopic substitution become symmetric top molecules with small dipole moment, are expressed analytically for the two limiting cases of weak coupling of the molecular angular momentum to the collision axis (dominating Coriolis interaction, the fly-wheel [FW] approximation) and strong coupling (negligible Coriolis interaction, the adiabatic channel [AC] approximation). The comparison leads to relations between rate coefficients for ultra-low (FW) and moderate (AC) temperatures and defines the range of parameters for which the analytical expressions become insufficient and a numerical treatment is nece…

CouplingPhysicsAngular momentumRange (particle radiation)BiophysicsCondensed Matter PhysicsCharged particleDipoleMoment (physics)Physical and Theoretical ChemistryAtomic physicsAdiabatic processMolecular BiologyQuantumMolecular Physics
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Production of a tensor glueball in the reaction γγ → G2π0 at large momentum transfer

2018

Abstract We study the production of a tensor glueball in the reaction γ γ → G 2 π 0 . We compute the cross section at higher momentum transfer using the collinear factorisation approach. We find that for a value of the tensor gluon coupling of f g T ∼ 100 MeV, the cross section can be measured in the near future by the Belle II experiment.

CouplingPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsGlueballMomentum transfer01 natural scienceslcsh:QC1-999GluonCross section (physics)Factorization0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)TensorNuclear Experiment010306 general physicslcsh:PhysicsPhysics Letters B
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Beam matching with space charge in energy recovery linacs

2019

Abstract Matching with space charge of an Energy-Recovery Linac (ERL) arc into the subsequent RF structure is essential to preserve beam quality. We show how to match beam envelopes and dispersion along the bends and recirculation arcs of an ERL, including space charge forces, in order to adjust the beam to the parameters of the subsequent RF structure. For a qualitative analysis, we show that one can use a beam matrix approach together with the smooth focusing approximation but with longitudinal–transverse coupling. It is also shown that the space-charge-modified dispersion plays a key role for the adjustment of the momentum compaction R 56 required for both the isochronous and the non-iso…

CouplingPhysicsNuclear and High Energy Physicsbusiness.industryMomentum compactionTracking (particle physics)Space chargeLinear particle acceleratorOpticsDispersion (optics)Physics::Accelerator PhysicsLaser beam qualitybusinessInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Axionlike Particles, Lepton-Flavor Violation, and a New Explanation of aμ and ae

2020

Axionlike particles (ALPs) with lepton-flavor-violating couplings can be probed in exotic muon and tau decays. The sensitivity of different experiments depends strongly on the ALP mass and its couplings to leptons and photons. For ALPs that can be resonantly produced, the sensitivity of three-body decays such as μ→3e and τ→3μ exceeds by many orders of magnitude that of radiative decays like μ→eγ and τ→μγ. Searches for these two types of processes are therefore highly complementary. We discuss experimental constraints on ALPs with a single dominant lepton-flavor-violating coupling. Allowing for one or more such couplings offers qualitatively new ways to explain the anomalies related to the m…

CouplingPhysicsParticle physicsMuonPhotonHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyElectronElectron magnetic dipole momentPhysics::GeophysicsOrders of magnitude (time)Radiative transferHigh Energy Physics::ExperimentLeptonPhysical Review Letters
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Experimental constraints on the coupling of the Higgs boson to electrons

2015

In the standard model (SM), the coupling of the Higgs boson to electrons is real and very small, proportional to the electron mass. New physics could significantly modify both real and imaginary parts of this coupling. We discuss experiments which are sensitive to the Higgs-electron coupling and derive the current bounds on new physics contributing to this coupling. The strongest constraint follows from the ACME bound on the electron electric dipole moment (EDM). We calculate the full analytic two-loop result for the electron EDM and show that it bounds the imaginary part of the Higgs-electron coupling to be less than 1.7 x 10^-2 times the SM electron Yukawa coupling. Deviations of the real…

CouplingPhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron ColliderAnomalous magnetic dipole momentPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesElectron electric dipole momentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentJournal of High Energy Physics
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Search for anomalous Wtb couplings in single top quark production

2008

Made available in DSpace on 2022-04-28T20:46:40Z (GMT). No. of bitstreams: 0 Previous issue date: 2008-11-25 Science and Technology Facilities Council In 0.9fb-1 of pp̄ collisions, the D0 Collaboration presented evidence for single top quark production in events with an isolated lepton, missing transverse momentum, and two to four jets. We examine these data to study the Lorentz structure of the Wtb coupling. The standard model predicts a left-handed vector coupling at the Wtb vertex. The most general lowest dimension, CP-conserving Lagrangian admits right-handed vector and left- or right-handed tensor couplings as well. We find that the data prefer the left-handed vector coupling and set u…

CouplingPhysicsTop quarkParticle physics010308 nuclear & particles physicsLorentz transformationGeneral Physics and Astronomy01 natural sciencesVertex (geometry)symbols.namesake0103 physical sciencesTransverse momentumsymbols010306 general physicsLagrangianLeptonPhysical Review Letters
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Fatigue Crack Growth for Different Ratios of Bending to Torsion in AlCu4Mg1

2008

The paper contains the fatigue crack growth test results obtained under proportional bending with torsion in AlCu4Mg1 aluminium alloy [1]. Specimens with rectangular cross sections and dimensions: length l = 90 mm, height w = 10 mm and thickness g = 8 mm were tested [2]. Each specimen had an external unilateral notch with depth 2 mm and radius ρ = 0.2 mm. The tests were performed under the stress ratio R = −1. The notches in the specimens were cut with a milling cutter and their surfaces were polished after grinding. The tests were realized on a fatigue test stand MZGS-100 where the ratio of torsion moment to bending moment was \( M_T (t)/M_B (t) = tg\alpha = \sqrt 3 /3,1{\text{ }}and\sqrt …

Crack closureMaterials scienceStress ratiovisual_artBending momentAluminium alloyvisual_art.visual_art_mediumTorsion (mechanics)Fatigue testingParis' lawComposite material
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