Search results for "coupling [Higgs particle]"

showing 10 items of 443 documents

Experimental evidence for chirality in the odd-A 105Rh

2004

Abstract High-spin states in 105 Rh were populated by the 96 Zr( 13 C, p3n) reaction at beam energies of 51 and 58 MeV, and studied using the EUROBALL IV γ -ray spectrometer and the DIAMANT charged particle array. A pair of nearly degenerate Δ I = 1 three-quasiparticle bands with the same spins and parity have been observed. Comparison of the experimental results with tilted axis cranking calculations confirms the chiral character of the two bands, while arguments based on the excitation of particles within the π g 9 / 2 ν ( h 11 / 2 ) 2 configuration of the yrast band and comparison with the previously observed γ band exclude the other possible interpretations. This is the first experiment…

PhysicsNuclear and High Energy PhysicsSpins010308 nuclear & particles physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Chiral partner bandsYrastDegenerate energy levelsParity (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Tilted axis cranking01 natural sciences21.10.Re; 21.60.-n; 23.20.Lv; 27.60.+jCore-quasiparticle coupling calculationsCharged particleThree-quasiparticle configuration0103 physical sciencesQuasiparticleAtomic physics010306 general physicsChirality (chemistry)ExcitationPhysics Letters B
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K+Λ photoproduction amplitudes incorporating absorptive effects and hypernuclear formation

1989

Incorporating final-state absorptive effects, we have reexamined the γp→K+Λ elementary process to obtain amplitudes which are used for describing photoproduction of hypernuclei. Our model not only resolves the persisting trouble of the small KNΛ coupling constant, but also yields agreement with cross-section data at higher energies. Using our amplitudes, we calculate angular distributions for the reaction16O(γ, K+)Λ16N. While the forward cross-section increases with increasing energy, the total cross-section is found to remain almost constant fromEγ=1.2 GeV through 2 GeV, which suggests that rather low photon energies hold promise for exploration of hypernuclear excitations.

PhysicsNuclear physicsCoupling constantParticle physicsPhotonAmplitudeNuclear ExperimentConstant (mathematics)Il Nuovo Cimento A
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Dynamical Dark sectors and Neutrino masses and abundances

2020

We investigate generalized interacting dark matter-dark energy scenarios with a time-dependent coupling parameter, allowing also for freedom in the neutrino sector. The models are tested in the phantom and quintessence regimes, characterized by an equation of state $w_x-1$, respectively. Our analyses show that for some of the scenarios the existing tensions on the Hubble constant $H_0$ and on the clustering parameter $S_8$ can be significantly alleviated. The relief is either due to \textit{(a)} a dark energy component which lies within the phantom region; or \textit{(b)} the presence of a dynamical coupling in quintessence scenarios. The inclusion of massive neutrinos into the interaction …

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsDegrees of freedom (physics and chemistry)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Astrophysics::Cosmology and Extragalactic AstrophysicsCoupling (probability)01 natural sciences7. Clean energyGeneral Relativity and Quantum Cosmologysymbols.namesakeCoupling parameter0103 physical sciencesDark energysymbolsNeutrino010303 astronomy & astrophysicsEnergy (signal processing)Hubble's lawQuintessenceAstrophysics - Cosmology and Nongalactic Astrophysics
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Transfer coefficients for evaporation of a system with a Lennard-Jones long-range spline potential

2007

International audience; Surface transfer coefficients are determined by nonequilibrium molecular dynamics simulations for a Lennard-Jones fluid with a long-range spline potential. In earlier work A. Røsjorde et al., J. Colloid Interface Sci. 240, 355 2001; J. Xu et al., ibid. 299, 452 2006, using a short-range Lennard-Jones spline potential, it was found that the resistivity coefficients to heat and mass transfer agreed rather well with the values predicted by kinetic theory. For the long-range Lennard-Jones spline potential considered in this paper we find significant discrepancies from the values predicted by kinetic theory. In particular the coupling coefficient, and as a consequence the…

PhysicsPhase transitionThermodynamics02 engineering and technologyNonequilibrium molecular dynamics021001 nanoscience & nanotechnology01 natural sciencesTheorem of corresponding states[PHYS.PHYS.PHYS-CHEM-PH] Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph][CHIM.THEO]Chemical Sciences/Theoretical and/or physical chemistry[ PHYS.PHYS.PHYS-CHEM-PH ] Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Spline (mathematics)Colloid[CHIM.THEO] Chemical Sciences/Theoretical and/or physical chemistryElectrical resistivity and conductivityMass transfer0103 physical sciences[ CHIM.THEO ] Chemical Sciences/Theoretical and/or physical chemistry[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]010306 general physics0210 nano-technologyCoupling coefficient of resonatorsComputingMilieux_MISCELLANEOUS
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Three-loop relation of quark $$\overline {MS} $$ and pole masses

1990

We calculate, exactly, the next-to-leading correction to the relation between the $$\overline {MS} $$ quark mass, $$\bar m$$ , and the scheme-independent pole mass,M, and obtain $$\begin{gathered} \frac{M}{{\bar m(M)}} \approx 1 + \frac{4}{3}\frac{{\bar \alpha _s (M)}}{\pi } + \left[ {16.11 - 1.04\sum\limits_{i = 1}^{N_F - 1} {(1 - M_i /M)} } \right] \hfill \\ \cdot \left( {\frac{{\bar \alpha _s (M)}}{\pi }} \right)^2 + 0(\bar \alpha _s^3 (M)), \hfill \\ \end{gathered} $$ as an accurate approximation forN F−1 light quarks of massesM i <M. Combining this new result with known three-loop results for $$\overline {MS} $$ coupling constant and mass renormalization, we relate the pole mass to the…

PhysicsQuantum chromodynamicsCoupling constantQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyPropagatorElementary particleLoop (topology)RenormalizationHigh Energy Physics::ExperimentEngineering (miscellaneous)Bar (unit)Zeitschrift für Physik C Particles and Fields
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Two-loop calculation of the anomalous dimension of the axial current with static heavy quarks

1992

Abstract A method to perform two-loop calculations in Eichten's effective field theory for heavy quarks is developed. The anomalous dimension of the axial current for static heavy quarks is calculated at two loops. For N = 3, we get γ A (2) = − 1 36 [ 127 2 +28ξ(2)−5N f ] . This result is very important to understand completely the physical significance of the lattice measurement of the decay constant of the B meson. The two-loop correction generated by γ A (2) turns out to be small, less than 1% for four quark flavours, so that the value of the decay constant of the B meson does not need in practice renormalization group improvement. As extra results, the self-energy renormalization consta…

PhysicsQuarkCoupling constantNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeQuark modelLattice field theoryHadronNuclear TheoryHigh Energy Physics::PhenomenologyFísicaGluonQuantum electrodynamicsB mesonHigh Energy Physics::Experiment
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Infra-Red Asymptotic Dynamics of Gauge Invariant Charged Fields: QED versus QCD

1999

The freedom one has in constructing locally gauge invariant charged fields in gauge theories is analyzed in full detail and exploited to construct, in QED, an electron field whose two-point function W(p), up to the fourth order in the coupling constant, is normalized with on-shell normalization conditions and is, nonetheless, infra-red finite; as a consequence the radiative corrections vanish on the mass shell $p^2=\mu^2$ and the free field singularity is dominant, although, in contrast to quantum field theories with mass gap, the eigenvalue $\mu^2$ of the mass operator is not isolated. The same construction, carried out for the quark in QCD, is not sufficient for cancellation of infra-red …

PhysicsQuarkCoupling constantQuantum chromodynamicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsPropagatorFOS: Physical sciencesgauge theories QED QCD non local fieldsFactorizationHigh Energy Physics - Theory (hep-th)Quantum mechanicsGauge theoryQuantum field theoryMass gapMathematical physics
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Antiscreening of the Ampère force in QED and QCD plasmas

2013

The static forces between electric charges and currents are modified at the loop level by the presence of a plasma. While electric charges are screened, currents are not. The effective coupling constant at long distances is enhanced in both cases as compared to the vacuum, and by different amounts, a clear sign that Lorentz symmetry is broken. We investigate these effects quantitatively, first in a QED plasma and secondly using non-perturbative simulations of QCD with two light degenerate flavors of quarks.

PhysicsQuarkCoupling constantQuantum chromodynamicsNuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyDegenerate energy levelsFOS: Physical sciencesPlasmaElectric chargeNuclear Theory (nucl-th)High Energy Physics - PhenomenologyStatic forces and virtual-particle exchangeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQuantum electrodynamicsQuantum mechanicsQuark–gluon plasmaPhysical Review D
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Dynamics of Uniaxial Hard Ellipsoids

2007

We study the dynamics of monodisperse hard ellipsoids via a new event-driven molecular dynamics algorithm as a function of volume fraction $\phi$ and aspect ratio $X_0$. We evaluate the translational $D_{trans}$ and the rotational $D_{rot}$ diffusion coefficient and the associated isodiffusivity lines in the $\phi-X_0$ plane. We observe a decoupling of the translational and rotational dynamics which generates an almost perpendicular crossing of the $D_{trans}$ and $D_{rot}$ isodiffusivity lines. While the self intermediate scattering function exhibits stretched relaxation, i.e. glassy dynamics, only for large $\phi$ and $X_0 \approx 1$, the second order orientational correlator $C_2(t)$ sho…

PhysicsScattering functionCondensed matter physicsPlane (geometry)GLASS-TRANSITIONPHASEFOS: Physical sciencesGeneral Physics and AstronomyOrder (ring theory)Context (language use)Condensed Matter - Soft Condensed MatterEllipsoidSIMULATIONSGLASS-TRANSITION; HARD ELLIPSOIDS; EVENT-DRIVEN SIMULATIONS; MOLECULAR MODE COUPLING THEORYNuclear magnetic resonanceLIQUIDSPARTICLESSoft Condensed Matter (cond-mat.soft)Relaxation (physics)Rotational dynamicsPhysical Review Letters
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Impact of the quenching of gA on the sensitivity of 0νββ experiments

2017

Detection of the neutrinoless $\ensuremath{\beta}\ensuremath{\beta}$ ($0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta}$) decay is of high priority in the particle- and neutrino-physics communities. The detectability of this decay mode is strongly influenced by the value of the weak axial-vector coupling constant ${g}_{A}$. The recent nuclear-model analyses of $\ensuremath{\beta}$ and $\ensuremath{\beta}\ensuremath{\beta}$ decays suggest that the value of ${g}_{A}$ could be dramatically quenched, reaching ratios of ${g}_{A}^{\mathrm{free}}/{g}_{A}\ensuremath{\approx}4$, where ${g}_{A}^{\mathrm{free}}=1.27$ is the free, neutron-decay, value of ${g}_{A}$. The effects of this quenching ap…

PhysicsTurn (biochemistry)Coupling constantQuenching010308 nuclear & particles physicsFourth power0103 physical sciencesBeta (velocity)Sensitivity (control systems)Atomic physics010306 general physics01 natural sciencesNuclear theoryPhysical Review C
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