Search results for "Muon"

showing 10 items of 1376 documents

Quantum critical point in the itinerant ferromagnet Ni$_{1-x}$Rh$_x$

2020

We report a chemical substitution-induced ferromagnetic quantum critical point in polycrystalline Ni$_{1-x}$Rh$_x$ alloys. Through magnetization and muon spin relaxation measurements, we show that the ferromagnetic ordering temperature is suppressed continuously to zero at $x_{crit} = 0.375$ while the magnetic volume fraction remains 100% up to $x_{crit}$, pointing to a second order transition. Non-Fermi liquid behavior is observed close to $x_{crit}$, where the electronic specific heat $C_{el}/T$ diverges logarithmically, while immediately above $x_{crit}$ the volume thermal expansion coefficient $\alpha_{V}/T$ and the Gr\"uneisen ratio $\Gamma = \alpha_{V}/C_{el}$ both diverge logarithmic…

PhysicsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Relaxation (NMR)Zero (complex analysis)General Physics and AstronomyOrder (ring theory)FOS: Physical sciencesMuon spin spectroscopy01 natural sciencesCondensed Matter - Strongly Correlated ElectronsMagnetizationFerromagnetismQuantum critical point0103 physical sciences010306 general physicsTemperature limit
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Testing WWγ vertex in radiative muon decay

2019

Large numbers of muons will be produced at facilities developed to probe the lepton-flavor-violating process μ→eγ. We show that by constructing a suitable asymmetry, radiative muon decay μ→eγνμν̄e can also be used to test the WWγ vertex at such facilities. The process has two missing neutrinos in the final state, and upon integrating their momenta the partial differential decay rate shows no radiation-amplitude zero. However, we establish that an easily separable part of the normalized differential decay rate that is odd under the exchange of photon and electron energies does have a zero in the case of the standard model (SM). This new type of zero has hitherto not been studied in the liter…

PhysicsConservation lawParticle physicsPhotonMuon010308 nuclear & particles physicsmedia_common.quotation_subjectElectronComputer Science::Digital Libraries01 natural sciencesAsymmetryVertex (geometry)Separable space0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsmedia_commonPhysical Review D
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A numerical method to calculate the muon relaxation function in the presence of diffusion

2014

We present an accurate and efficient method to calculate the effect of random fluctuations of the local field at the muon, for instance in the case muon diffusion, within the framework of the strong collision approximation. The method is based on a reformulation of the Markovian process over a discretized time base, leading to a summation equation for the muon polarization function which is solved by discrete Fourier transform. The latter is formally analogous, though not identical, to the integral equation of the original continuous-time model, solved by Laplace transform. With real-case parameter values, the solution of the discrete-time strong collision model is found to approximate the …

PhysicsCooley–Tukey FFT algorithmMuonDiscretizationLaplace transformNumerical analysisMathematical analysisFOS: Physical sciencesSummation equationCondensed Matter PhysicsIntegral equationAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterLocal fieldMathematical PhysicsOther Condensed Matter (cond-mat.other)Physica Scripta
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A measurement of the tau lifetime

1993

The tau lepton lifetime is measured using four different methods with the DELPHI detector. Three measurements using one prong decays are combined, accounting for correlations, resulting in tau(tau) = 298 +/- 7 (stat.) +/- 4 (syst.) fs while the decay length distribution of three prong decays gives tau(tau) = 298 +/- 13 (stat.) +/- 5 (syst.) fs. The combined result is tau(tau) = 298 +/- 7 fs. The ratio of the Fermi coupling constant from tau decay relative to that from muon decay is found to be 0.985 +/- 0.013, compatible with lepton universality.

PhysicsCoupling constantParticle physicsArgusNuclear and High Energy PhysicsMuonPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsElectron–positron annihilation01 natural sciences7. Clean energyNuclear physics0103 physical sciencesDecay lengthLEPTONS[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentFísica nuclearCombined result010306 general physicscomputerParticle Physics - ExperimentFermi Gamma-ray Space TelescopeLeptoncomputer.programming_language
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Footprints of a left-right symmetric model in a muon collider

2000

Abstract The double charged Higgs bosons, Δ ±± , are one of the benchmarks of left-right symmetric models. We discuss their production and demonstrate that even for small values of the Δ ++ l − l − coupling, they would produce observable signals at muon colliders.

PhysicsCouplingNuclear and High Energy PhysicsParticle physicsMuonPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologySymmetric modelObservableNuclear physicsMuon colliderHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentBosonPhysics Letters B
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An extension of two-Higgs-doublet model and the excesses of 750 GeV diphoton, muon g-2 and h → μτ

2016

In this paper we simultaneously explain the excesses of the 750 GeV diphoton, muon g-2 and $h\to \mu\tau$ in an extension of the two-Higgs-doublet model (2HDM) with additional vector-like fermions and a CP-odd scalar singlet ($P$) which is identified as the 750 GeV resonance. This 750 GeV resonance has a mixing with the CP-odd scalar ($A$) in 2HDM, which leads to a coupling between $P$ and the SM particles as well as a coupling between $A$ and the vector-like fermions. Such a mixing and couplings are strongly constrained by $\tau\to\mu\gamma$, muon g-2 and the 750 GeV diphoton data. We scan over the parameter space and find that such an extension can simultaneously account for the observed …

PhysicsCouplingParticle physicsNuclear and High Energy PhysicsMuon010308 nuclear & particles physicsScalar (mathematics)FermionParameter space01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyTwo-Higgs-doublet model0103 physical sciencesHigh Energy Physics::ExperimentSinglet state010306 general physicsNuclear ExperimentPhysics Letters B
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The spin-dependent structure function g1(x) of the deuteron from polarized deep-inelastic muon scattering

1997

We present a new measurement of the spin-dependent structure function $g_{1}^{\rm d}$ of the deuteron from deep inelastic scattering of 190 GeV polarized muons on polarized deuterons. The results are combined with our previous measurements of $g_{1}^{\rm d}$. A perturbative QCD evolution in next-to-leading order is used to compute $g_{1}^{\rm d}(x)$ at a constant $Q^{2}$. At $Q^{2} = 10$ GeV$^{2}$, we obtain a first moment $\Gamma_{1}^{\rm d} = \int_{0}^{1} g_{1}^{\rm d}{\rm d}x = 0.041 \pm 0.008$, a flavour-singlet axial charge of the nucleon $a_{0} = 0.30 \pm 0.08$, and an axial charge of the strange quark $a_{s} = -0.09 \pm 0.03$. Using our earlier determination of $\Gamma_{1}^{\rm p}$, …

PhysicsDISNuclear and High Energy PhysicsStrange quarkMuonSMCScatteringg1 structure functionSMC; DIS; g1 structure functionPerturbative QCDDeep inelastic scatteringNuclear physicsHigh Energy Physics::ExperimentSum rule in quantum mechanicsNucleonParticle Physics - ExperimentSpin-½Physics Letters B
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Restrictions for asymmetry and polarizations of recoil in muon capture

1975

Abstract Using the helicity formalism, we discuss muon capture by targets of spin-zero. Owing to the definite neutrino helicity, three independent observables define a complete experiment. The precise relation between asymmetry α and longitudinal polarization P L of recoil, α = 1 + 2 jP L , comes only from rotational invariance. When time-reversal invariance is inserted, there is an additional restriction between the average polarization P av and the longitudinal polarization P L . On the basis of the experimental result P av = 0.43 ± 0.10 for 12 C, we predict P L = −(0.99 +0.01 −0.04 .

PhysicsDensity matrixNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFísicaPolarization (waves)HelicityAsymmetryMuon captureNuclear physicsRecoilRotational invarianceHigh Energy Physics::ExperimentNeutrinomedia_commonNuclear Physics
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Comparative analysis of muon-capture and 0νββ -decay matrix elements

2020

Average matrix elements of ordinary muon capture (OMC) to the intermediate nuclei of neutrinoless double beta ($0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta}$) decays of current experimental interest are computed and compared with the corresponding energy and multipole decompositions of $0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta}$-decay nuclear matrix elements (NMEs). The present OMC computations are performed using the Morita-Fujii formalism by extending the original formalism beyond the leading order. The $0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta}$ NMEs include the appropriate short-range correlations, nuclear form factors, and higher-order nucleonic weak cu…

PhysicsFormalism (philosophy of mathematics)Particle physics010308 nuclear & particles physics0103 physical sciencesQuasiparticle010306 general physicsMultipole expansionWave function01 natural sciencesMuon capturePhysical Review C
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Search at the Mainz Microtron for light massive gauge bosons relevant for the muon g-2 anomaly.

2014

A massive, but light, Abelian U(1) gauge boson is a well-motivated possible signature of physics beyond the standard model of particle physics. In this Letter, the search for the signal of such a U(1) gauge boson in electron-positron pair production at the spectrometer setup of the A1 Collaboration at the Mainz Microtron is described. Exclusion limits in the mass range of 40  MeV/c^{2} to 300  MeV/c^{2}, with a sensitivity in the squared mixing parameter of as little as ε^{2}=8×10^{-7} are presented. A large fraction of the parameter space has been excluded where the discrepancy of the measured anomalous magnetic moment of the muon with theory might be explained by an additional U(1) gauge …

PhysicsGauge bosonParticle physicsMuonAnomalous magnetic dipole momentPhysics beyond the Standard ModelGeneral Physics and AstronomyDark photonNATURAL SCIENCES. Physics.Nuclear physicsPRIRODNE ZNANOSTI. Fizika.U(1)SPair productiondark photondark photon; U(1)SAnomaly (physics)Nuclear ExperimentMicrotronPhysical review letters
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