Search results for "symmetry"

showing 10 items of 3576 documents

Single π0 production off neutrons bound in deuteron with linearly polarized photons

2021

The quasifree γ→d→π0n(p) photon beam asymmetry, Σ, has been measured at photon energies, Eγ, from 390 to 610 MeV, corresponding to center of mass energy from 1.271 to 1.424 GeV, for the first time. The data were collected in the A2 hall of the MAMI electron beam facility with the Crystal Ball and TAPS calorimeters covering pion center-of-mass angles from 49∘ to 148∘. In this kinematic region, polarization observables are sensitive to contributions from the Δ(1232) and N(1440) resonances. The extracted values of Σ have been compared to predictions based on partial-wave analyses (PWAs) of the existing pion photoproduction database. Our comparison includes the SAID, MAID and Bonn–Gatchina anal…

deuteronpolarizationN(1440)partial waveNuclear Theoryphoton: energyDelta(1232)beam: asymmetryMainz Linackinematicsisospin: symmetrycalorimeterelectron: beampi0: photoproductionNuclear Experimentphoton: beamCrystal Ball
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Measurement of the spin-dependent structure function g1(x) of the deuteron

1993

We report on the first measurement of the spin-dependent structure function g1d of the deuteron in the deep inelastic scattering of polarised muons off polarised deuterons, in the kinematical range 0.006<x<0.6, 1 GeV2<Q2<30 GeV2. The first moment, Γ1d=sh{phonetic}01 g1d dx=0.023±0.020 (stat.) ± 0.015 (syst.), is smaller than the prediction of the Ellis-Jaffe sum rules. Using earlier measurements of g1p, we infer the first moment of the spin-dependent neutron structure function g1n. The difference Γ1p-Γ1n=0.20 ±0.05 (stat.) ± 0.04 (syst.) agrees with the prediction of the Bjorken sum rule, Γ1p-Γ1n=0.191 ±0.002.

deuteron: polarized targetNuclear and High Energy PhysicsINELASTIC E-P; POLARIZED PROTONS; SUM-RULE; SCATTERING; ELECTROPRODUCTION; ASYMMETRYINELASTIC E-PProtonpolarized target: deuterondeep inelastic scattering: muon deuteronstructure function: spinmuon deuteron: deep inelastic scatteringSUM-RULE530Nuclear physicsINELASTIC E-P; POLARIZED PROTONS; SUM-RULE; SCATTERING; ELECTROPRODUCTION; ASYMMETRY; MODELTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYSCATTERINGNeutronpolarized beam: muonSpin-½PhysicsQuantum chromodynamicsspin: structure functionMuonScatteringdeuteron: structure functionELECTROPRODUCTIONnucleon: structure functionCERN SPSDeep inelastic scatteringmomentmagnetic spectrometer: experimental resultsPOLARIZED PROTONSapprox. 100 GeVASYMMETRYSum rule in quantum mechanicsmuon: polarized beamParticle Physics - ExperimentPhysics Letters B
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Effective charge from lattice QCD

2020

Using lattice configurations for quantum chromodynamics (QCD) generated with three domain-wall fermions at a physical pion mass, we obtain a parameter-free prediction of QCD's renormalisation-group-invariant process-independent effective charge, $\hat\alpha(k^2)$. Owing to the dynamical breaking of scale invariance, evident in the emergence of a gluon mass-scale, this coupling saturates at infrared momenta: $\hat\alpha(0)/\pi=0.97(4)$. Amongst other things: $\hat\alpha(k^2)$ is almost identical to the process-dependent (PD) effective charge defined via the Bjorken sum rule; and also that PD charge which, employed in the one-loop evolution equations, delivers agreement between pion parton di…

dimension: 4Nuclear TheoryHigh Energy Physics::Latticesum rule: Bjorkenparton: distribution function01 natural sciencespi: massHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentInstrumentationQuantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)scalingdynamical symmetry breakinglattice field theoryLattice QCDDyson-Schwinger equationsEmergence of massHigh Energy Physics - Phenomenologyinfraredfermion: domain wallSum rule in quantum mechanicsRunning couplingNuclear and High Energy PhysicsParticle physicsLattice field theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Lattice field theoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Theory (nucl-th)High Energy Physics - Lattice0103 physical sciencesquantum chromodynamicsQuantum field theory010306 general physicsCoupling constant010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics::Phenomenologycoupling constantAstronomy and AstrophysicsgluonGluonDistribution functionevolution equation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentQuantum chromodynamicsConfinement
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Distraction osteogenesis in Goldenhar Syndrome: Case report and 8-year follow-up

2007

Goldenhar syndrome is a well-known condition featuring the following triad of anomalies: ocular abnormalities, microtia and vertebral anomalies. This syndrome involves structures arising from the first and second branchial arches. Craniofacial anomalies, including mandibular, zygomatic and/or maxillary hypoplasias are found in 50% of patients with Goldenhar syndrome. Patients with this syndrome may present unilateral or bilateral underdevelopment of the mandible. Several treatments for the correction of the dento-facial deformity have been described, among them distraction osteogenesis is one that shows promising results. Distraction osteogenesis is the process of bone formation that occurs…

distraction osteogenesisGoldenhar syndromeUNESCO::CIENCIAS MÉDICASeducation:CIENCIAS MÉDICAS [UNESCO]asymmetry
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On hidden heterogeneity in directional asymmetry – can systematic bias be avoided?

2006

8 pages; International audience; Directional asymmetry (DA) biases the analysis of fluctuating asymmetry (FA) mainly because among-individual differences in the predisposition for DA are difficult to detect. However, we argue that systematic bias mainly results from predictable associations between signed right-left asymmetry and other factors, i.e. from systematic variation in DA. We here demonstrate methods to test and correct for this, by analysing bilateral asymmetry in size and shape of an irregular sea urchin. Notably, in this model system, DA depended significantly on body length and geographic origin, although mean signed asymmetry (mean DA) was not significant in the sample as a wh…

echinoidmedia_common.quotation_subjectModel systemMESH : Analysis of VarianceSystematic variationEnvironmentBiologyAsymmetryFunctional LateralityStatistical powerFluctuating asymmetry[ SDV.BDD.MOR ] Life Sciences [q-bio]/Development Biology/Morphogenesiscase studySpecies SpecificityStatisticsAnimalsMESH : Species Specificitydevelopmental stabilityMESH : EvolutionMESH : FranceMESH : Functional LateralityEcology Evolution Behavior and Systematicsmedia_commonMESH : Sea UrchinsAnalysis of VarianceBilateral asymmetryMESH : Variation (Genetics)MESH : Reproducibility of Resultsfluctuating asymmetryGenetic VariationReproducibility of ResultsContrast (statistics)methodologyBiological EvolutionMESH : EnvironmentSea UrchinsGeographic originAbatus cordatusFranceMESH : Animalsdirectional asymmetry
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Spectroscopic signatures for planar equilibrium geometries in methyl-substituted oligothiophenes

2009

In recent studies it was demonstrated that temperature-dependent optical spectroscopy is a valuable tool for revealing the differences in the geometries of flexible molecules like oligothiophenes (OTs) in the ground (S0) and first excited (S1) electronic states, by examining the symmetry relations between the absorption and emission spectra: while at low temperature the spectra show mirror symmetry, pointing to planar geometries in S0 and S1, the symmetry relation breaks down at ambient temperature due to thermal population of torsional modes. In the present joint spectroscopic and theoretical study, we demonstrate that this behavior is also observed for di- and tetramethyl-substituted OTs,…

education.field_of_studyAbsorption spectroscopyoligothiophenesChemistrybusiness.industryPopulationGeneral Physics and AstronomySymmetry (physics)Opticsmethyl-substituted oligothiophenesChemical physicsExcited stateMoleculeEmission spectrumPhysical and Theoretical ChemistryeducationbusinessSpectroscopyMirror symmetryFIS/03 - FISICA DELLA MATERIAPhys. Chem. Chem. Phys.
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(R)-(−)-Quinuclidin-3-ol

2013

The structure of the title compound [alternatively called (R)-(−)-1-azabicyclo[2.2.2]octan-3-ol], C7H13NO, at 100 K has hexagonal (P61) symmetry. The structure shows a twist along the C—N pseudo-threefold axis. In the crystal, molecules are linkedviaO—H...N hydrogen bonds, forming infinite chains along thec-axis direction. The crystal studied was twinned by merohedry (twin law: 010, 100, 00-1; population: 0.925:0.075)

education.field_of_studyBicyclic moleculeHydrogen bondChemistryPopulationGeneral ChemistryCondensed Matter PhysicsBioinformaticsOrganic PapersCrystalCrystallographyGeneral Materials ScienceSymmetry (geometry)TwisteducationActa Crystallographica Section E Structure Reports Online
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Fluctuating asymmetry and immune function in a field cricket

2004

Recently, fluctuating asymmetry (FA) of morphological traits has attracted great attention as a short-cut measure of individual quality. Whereas there is some evidence that FA of sexual ornaments is negatively associated with immune function, studies concerning FA and immune function in non-ornamental traits are absent. Here, we tested whether FA of three non-ornamental traits in hind limbs is related to male immune function in a population of the Mediterranean field cricket, Gryllus bimaculatus. As different measures of male immune function, we used encapsulation rate and lytic activity. We found that a composite measure of FA (cFA) was negatively related to encapsulation rate. However, ly…

education.field_of_studybiologyEcologyGryllus bimaculatusPopulationZoologybiology.organism_classificationFluctuating asymmetryField cricketLower bodyImmune systemLytic cycleImmunocompetenceeducationEcology Evolution Behavior and SystematicsOikos
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Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian

2018

The electroweak sector of the Standard Model can be formulated in a way similar to Chiral Perturbation Theory (ChPT), but extended by a singlet scalar. The resulting effective field theory (EFT) is called Higgs-Electroweak Chiral Lagrangian (EWCh$\mathcal{L}$) and is the most general approach to new physics in the Higgs sector. It solely assumes the pattern of symmetry breaking leading to the three electroweak Goldstone bosons (i.e. massive $W$ and $Z$) and the existence of a Higgs-like scalar particle. The power counting of the EWCh$\mathcal{L}$ is given by a generalization of the momentum expansion of ChPT. It is connected to a loop expansion, making the theory renormalizable order by ord…

effective Lagrangian: chiralNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryelectroweak interaction: symmetry breakingHigh Energy Physics::LatticeScalar (mathematics)standard modelFOS: Physical sciencesTechnicolorsinglet: scalarHiggs particleexpansion: higher-order01 natural sciencesHiggs sectorStandard ModelrenormalizationRenormalizationTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)effective field theoryfluctuation: scalar0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. RadioactivityLimit (mathematics)010306 general physicsPhysicselectroweak interaction010308 nuclear & particles physicsnew physicsElectroweak interactionHigh Energy Physics::Phenomenologyhigher-order: 1perturbation theory: chiralGoldstone particleHiggs fieldHigh Energy Physics - Phenomenologyscalar particlebackground field[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Goldstone bosonHiggs bosonHiggs modellcsh:QC770-798expansion: heat kernelfield theory: renormalizableexpansion: momentum
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Measurement of the SMC muon beam polarisation using the asymmetry in the elastic scattering off polarised electrons

2000

A muon beam polarimeter was built for the SMC experiment at the CERN SPS, for beam energies of 100 and 190 GeV. The beam polarisation is determined from the asymmetry in the elastic scattering off the polarised electrons of a ferromagnetic target whose magnetisation is periodically reversed. At muon energies of 100 and 190 GeV the measured polarisation is P-mu = -0.80 +/- 0.03 (stat.) +/- 0.02 (syst.) and P-mu = - 0.797 +/- 0.011 (stat.) +/- 0.012 (syst.), respectively. These results agree with measurements of the beam polarisation using a shape analysis of the decay positron energy spectrum. (C) 2000 Elsevier Science B.V. All rights reserved.

electronNuclear and High Energy PhysicsSMC; DIS; muon polarimetermedia_common.quotation_subjectmuon beamElectronAsymmetryNuclear physicsMagnetizationpolarisation measurementDetectors and Experimental TechniquesNuclear ExperimentInstrumentationmedia_commonPhysicsElastic scatteringDISLarge Hadron ColliderMuonpolarised scatteringSMCmagnetised targetPolarimeterpolarised muonPolarization (waves)muon polarimeterPhysics::Accelerator PhysicsHigh Energy Physics::Experimentpolarised
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