Search results for "coupling [Higgs particle]"

showing 10 items of 443 documents

The spin-dependent structure function of the proton g1p and a test of the Bjorken sum rule

2010

Abstract The inclusive double-spin asymmetry, A 1 p , has been measured at COMPASS in deep-inelastic polarised muon scattering off a large polarised NH3 target. The data, collected in the year 2007, cover the range Q 2 > 1 ( GeV / c ) 2 , 0.004 x 0.7 and improve the statistical precision of g 1 p ( x ) by a factor of two in the region x 0.02 . The new proton asymmetries are combined with those previously published for the deuteron to extract the non-singlet spin-dependent structure function g 1 NS ( x , Q 2 ) . The isovector quark density, Δ q 3 ( x , Q 2 ) , is evaluated from a NLO QCD fit of g 1 NS . The first moment of Δ q 3 is in good agreement with the value predicted by the Bjorken su…

Quantum chromodynamicsPhysicsCoupling constantNuclear and High Energy PhysicsParticle physicsMuonIsovectorProton010308 nuclear & particles physicsDeep inelastic scattering01 natural sciencesNuclear physics0103 physical sciencesSum rule in quantum mechanics010306 general physicsSpin-½Physics Letters B
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Neutrinoless double beta decay and QCD running at low energy scales

2018

There is a common belief that the main uncertainties in the theoretical analysis of neutrinoless double beta ($0\nu\beta\beta$) decay originate from the nuclear matrix elements. Here, we uncover another previously overlooked source of potentially large uncertainties stemming from non-perturbative QCD effects. Recently perturbative QCD corrections have been calculated for all dimension 6 and 9 effective operators describing $0\nu\beta\beta$-decay and their importance for a reliable treatment of $0\nu\beta\beta$-decay has been demonstrated. However, these perturbative results are valid at energy scales above $\sim 1$ GeV, while the typical $0\nu\beta\beta$-scale is about $\sim 100$ MeV. In vi…

Quantum chromodynamicsPhysicsCoupling constantParticle physics010308 nuclear & particles physicsScalar (mathematics)Perturbative QCDFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesTensorPerturbation theory (quantum mechanics)010306 general physicsPhysical Review
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Screening effects in Relativistic Models of Dense Matter at Finite Temperature

1998

We investigate screening effects of the medium on the potential interaction between two static 'charges' for different models of dense plasmas in the one-boson exchange approximation. The potential can exhibit an oscillatory behavior, which is related to the analytic structure of the corresponding boson propagators in the complex $q$-plane. We have first revisited the one-pion exchange in a nuclear medium. In addition to Friedel oscillations, which are associated to branch cuts in the $q$-plane, there appears another oscillatory component, which arises from a pole on the pion propagator. This pole is located appart from the axes, giving rise to an oscillating Yukawa-like potential. Therefor…

Quantum chromodynamicsPhysicsFriedel oscillationsCoupling constantParticle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyYukawa potentialPerturbative QCDPropagatorFísicaFOS: Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicssymbolsBosonDebye
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Four-quark operators and non-leptonic weak transitions

1991

72 páginas, 12 figuras, 6 tablas.-- CERN-TH-5906-90 ; CPT-2393.

Quantum chromodynamicsPhysicsQuarkCoupling constantNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyFísicaPerturbative QCDQuantum field theoryChiral symmetry breakingEffective actionParticle Physics - Theory
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DETERMINATION OF ALPHA(S) FOR B-QUARKS AT THE Z(0) RESONANCE

1993

The strong coupling constant for b quarks has been determined, and its flavour independence, as predicted by QCD, investigated. The analysis involved events with lepton candidates selected from approximately 356 000 hadronic decays of the Z0, collected by the DELPHI detector at LEP in 1990 and 199 1. A method based on a direct comparison of the three-jet fraction in a b enriched sample, selected by requiring leptons with large momenta and transverse momenta, to that of the entire hadronic sample, illustrated the significant effect of the b quark mass on the multi-jet cross section, and verified the flavour independence of the strong coupling constant to an accuracy of +/- 6%. A second proce…

QuarkCHARMED MESONSNuclear and High Energy PhysicsParticle physicsHEAVY FLAVOR PRODUCTIONElectron–positron annihilationHigh Energy Physics::LatticeFRAGMENTATION FUNCTIONSFlavourHadron01 natural sciencesBottom quarkNuclear physicsMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentZ DECAYSPhysicsCoupling constantQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyJET PRODUCTION-RATESQCDSTRING MODELHigh Energy Physics::ExperimentFísica nuclearHEAVY FLAVOR PRODUCTION; JET PRODUCTION-RATES; E+ E ANNIHILATION; Z0 RESONANCE; FRAGMENTATION FUNCTIONS; CHARMED MESONS; STRING MODEL; MONTE-CARLO; Z DECAYS; QCDE+ E ANNIHILATIONZ0 RESONANCEParticle Physics - ExperimentLepton
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Spectrum of SU(2) lattice gauge theory with two adjoint Dirac flavours

2008

An SU(2) gauge theory with two fermions transforming under the adjoint representation of the gauge group may appear conformal or almost conformal in the infrared. We use lattice simulations to study the spectrum of this theory and present results on the masses of several gauge singlet states as a function of the physical quark mass determined through the axial Ward identity and find indications of a change from chiral symmetry breaking to a phase consistent with conformal behaviour at beta_L ~ 2. However, the measurement of the spectrum is not alone sufficient to decisively confirm the existence of conformal fixed point in this theory as we show by comparing to similar measurements with fun…

QuarkCoupling constantPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciences01 natural sciencesTheoretical physicsHigh Energy Physics - LatticeGauge groupLattice gauge theory0103 physical sciencesGauge theory010306 general physicsChiral symmetry breakingSpecial unitary group
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Unified QCD determination of all vector meson coupling constants

1992

Coupling constants of all vector mesons are determined in QCD by means of a new QCD sum-rule method. The results are found to be sensitive to the binding energy (i.e. meson and quark mass differences). For standard values of quark masses we obtainf ϱ=202 MeV,f K*=216 MeV,f D*=212±22 MeV,f B*=138±42 MeV, $$f_{D_s^* } = 238 \pm 21\,MeV$$ and $$f_{B_s^* } = 163 \pm 45\,MeV$$ . Based on this approach the spin-flavour symmetry for the heavy quark systems are also discussed.

QuarkCoupling constantPhysicsQuantum chromodynamicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyBinding energySymmetry (physics)Nuclear physicsHigh Energy Physics::ExperimentVector mesonNuclear ExperimentEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Exclusive heavy vector meson production at next-to-leading order in the dipole picture

2021

We calculate exclusive production of a longitudinally polarized heavy vector meson at next-to-leading order in the dipole picture. The large quark mass allows us to separately include both the first QCD correction proportional to the coupling constant $\alpha_s$, and the first relativistic correction suppressed by the quark velocity $v^2$. Both of these corrections are found to be numerically important in $\mathrm{J}/\psi$ production. The results obtained are directly suitable for phenomenological calculations. We also demonstrate how vector meson production provides complementary information to structure function analyses when one extracts the initial condition for the energy evolution of …

QuarkNuclear and High Energy PhysicsParticle physicsCOLLISIONSProtonJ/PSI MESONSQC1-999High Energy Physics::LatticeNuclear TheoryStructure (category theory)FOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesInitial value problemVector meson010306 general physicsNUCLEUSPhysicsCoupling constantQuantum chromodynamicskvarkit010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyELECTROPRODUCTIONEVOLUTIONDipoleHigh Energy Physics - PhenomenologyPHOTOPRODUCTIONHigh Energy Physics::Experiment
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DETERMINATION OF ALPHA-S FROM THE SCALING VIOLATION IN THE FRAGMENTATION FUNCTIONS IN E+E- ANNIHILATION

1993

A determination of the hadronic fragmentation functions of the Z0 boson is presented from a study of the inclusive hadron production with the DELPHI detector at LEP. These fragmentation functions were compared with the ones at lower energies, thus covering data in a large kinematic range: 196 less-than-or-equal-to Q2 less-than-or-equal-to 8312 GeV2 and x (= p(h)/E(beam)) > 0.08. A large scaling violation was observed, which was used to extract the strong coupling constant in second order QCD: alpha(s)(M(Z)) = 0.118 +/- 0.005. The corresponding QCD scale for five quark flavours is: LAMBDA(MS)(5)BAR = 230 +/- 60 MeV.

QuarkNuclear and High Energy PhysicsParticle physicsHADRONIC-Z-DECAYS; JET PRODUCTION-RATES; LUND MONTE-CARLO; LEADING ORDER; QUANTUM CHROMODYNAMICS; PERTURBATIVE QCD; PARTON DENSITIES; RESONANCE; SCATTERING; PHYSICSLUND MONTE-CARLOHigh Energy Physics::LatticeElectron–positron annihilationHadronElementary particlePARTON DENSITIES01 natural sciencesNuclear physicsPHYSICS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PERTURBATIVE QCDSCATTERING010306 general physicsNuclear ExperimentBosonQuantum chromodynamicsPhysicsCoupling constantAnnihilationQUANTUM CHROMODYNAMICS010308 nuclear & particles physicsJET PRODUCTION-RATESLEADING ORDERHigh Energy Physics::PhenomenologyRESONANCEFísica nuclearHigh Energy Physics::ExperimentParticle Physics - ExperimentHADRONIC-Z-DECAYSPHYSICS LETTERS B
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Quark and gluon distributions and $\alpha_{s}$ from nucleon structure functions at low $x$

1993

Abstract The Q2 dependence of the structure functions F2p and F2d recently measured by the NMC is compared with the predictions of perturbative QCD at next-to-leading order. Good agreement is observed, leading to accurate determinations of the quark and gluon distributions in the range 0.008 ⩽ × ⩽ 0.5. The strong coupling constant is measured from the low x data; the result agrees with previous determinations.

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::Latticedeep inelastic scattering: muon deuteronmuon deuteron: deep inelastic scatteringPARTON DENSITIESJet (particle physics)530CROSS-SECTIONSNuclear physicsnumerical calculations: interpretation of experimentsstrong interaction: coupling constant90: 280 GeVDEEP INELASTIC-SCATTERING; LEADING ORDER; QUANTUM CHROMODYNAMICS; PERTURBATION-THEORY; PARTON DENSITIES; CROSS-SECTIONS; FREEDOM; MSBAR; JET; NMCdeep inelastic scattering: muon pp: structure functionNMCCoupling constantQuantum chromodynamicsPhysicsQUANTUM CHROMODYNAMICSLEADING ORDERHigh Energy Physics::Phenomenologydeuteron: structure functiongluon: momentum spectrumperturbation theory: higher-orderPerturbative QCDDeep inelastic scatteringquark: momentum spectrumFREEDOMGluondependence: momentum transferJETMSBARmuon p: deep inelastic scatteringPERTURBATION-THEORYDEEP INELASTIC-SCATTERINGHigh Energy Physics::Experimentcoupling constant: strong interactionNucleonParticle Physics - Experiment
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