Search results for "Particle physics"

showing 10 items of 6826 documents

Neutrinoless double beta decay to excited collective 0+ states

2000

Abstract The many recently performed experiments to study the two-neutrino double beta (2 νββ ) decay to the first excited 0 + final state encourage similar experiments to be done for the neutrinoless double beta (0 νββ ) decay. Based on the accumulated theoretical and experimental information on the 2 νββ decays one could hope that the 0 νββ decay to the excited 0 + state would be very efficient in restricting the parameter space of modern particle-physics theories. In this article the 0 νββ decays of 76 Ge and 82 Se to excited collective 0 + states are studied within a realistic nuclear model. It is found that the lower limits for the half-lives of these decays are of the order of 10 27 y…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsDecay schemeExcited stateDouble beta decayHigh Energy Physics::ExperimentBeta (velocity)Parameter spaceBeta-decay stable isobarsPhysics Letters B
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Search for the decay KL → 3γ

1995

Abstract Data from the NA31 experiment at the CERN SPS have been used for the first search for the decay mode KL → 3γ. Seven events have been found with an estimated background of 6.7 ± 1.5 events. The corresponding upper limit for the branching ratio is Γ(K L → 3γ) Γ(K L → all ) = 2.4 × 10 −7 at the 90% confidence level, assuming a phase-space decay distribution.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsDistribution (mathematics)Branching fractionPhysics Letters B
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On the double-beta decays of 70Zn, 86Kr, 94Zr, 104Ru, 110Pd and 124Sn

2011

Abstract Double-beta decays of 70Zn, 86Kr, 94Zr, 104Ru, 110Pd and 124Sn to the final ground states and the decays of 110Pd and 124Sn to the excited states in 110Cd and 124Te are studied in the framework of the proton–neutron quasiparticle random-phase approximation (pnQRPA) combined with the multiple-commutator model (MCM) for description of decays to the excited final states. Reasonably large single-particle model spaces and G-matrix-based effective nuclear forces are used to compute the relevant nuclear matrix elements and decay half-lives. The present study is among the very few that have been dedicated to double-beta decays of these nuclei, although the associated double-beta Q values e…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsDouble beta decayExcited stateBeta (plasma physics)QuasiparticleBibliographyNuclear forceHigh Energy Physics::ExperimentGround stateNuclear Physics A
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Theory of double beta decay

2005

Basic features of the two-neutrino double beta ( 2 ν β β ) decay and neutrinoless double beta ( 0 ν β β ) decay are discussed. A short review of the most important nuclear models, used to describe the ββ decay, is given. A deeper survey of the nuclear matrix elements, related to the above-mentioned decay modes, is performed using the proton-neutron quasiparticle random-phase approximation (pnQRPA). In particular, the extraction of a proper value of the proton-neutron particle-particle interaction parameter in this theory is addressed. The relevance of different multipoles in the multipole decomposition of the 0 ν β β matrix element is also discussed in the pnQRPA framework.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsDouble beta decayQuasiparticleMatrix elementBeta (velocity)Flory–Huggins solution theoryNuclear ExperimentMultipole expansionNuclear Physics A
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Meson Decays with Crystal Ball at MAMI

2012

The Crystal Ball at MAMI setup offers excellent possibilities to study decays of light mesons like η , η ′ , and ω . Here, recent results on η and ω decays are presented. Furthermore, future perspectives in this field at MAMI are described.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsField (physics)MesonHigh Energy Physics::ExperimentNuclear ExperimentAtomic and Molecular Physics and OpticsCrystal BallNuclear Physics B - Proceedings Supplements
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Lepton flavour violating decay of the Z0 in the scalar triplet model

1987

Abstract The lepton flavour violating Z→μme, Z→μτ and Z→eτ decays are evaluated in the framework of the majoron triplet model of Gelmini and Roncadelli. The process is dominated by the diagrams with charged scalars in the loops, so the GIM cancellation is avoided. We obtain branching ratios for Z→μτ and Z→eτ which might be detectable at SLC and/or LEP.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsFlavourScalar (mathematics)High Energy Physics::PhenomenologyFísicaHigh Energy Physics::ExperimentLeptonMajoronParticle Physics - Phenomenology
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Test of lepton flavour universality in K+→ℓ+ν decays

2011

Abstract A precision test of lepton flavour universality has been performed by measuring the ratio R K of kaon leptonic decay rates K + → e + ν and K + → μ + ν in a sample of 59 813 reconstructed K + → e + ν candidates with ( 8.71 ± 0.24 ) % background contamination. The result R K = ( 2.487 ± 0.013 ) × 10 − 5 is in agreement with the Standard Model expectation.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsFlavourWidth ratioUniversality (dynamical systems)LeptonPhysics Letters B
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Hypernuclear Spectroscopy at JLab Hall C

2010

Abstract Since the 1st generation experiment, E89-009, which was successfully carried out as a pilot experiment of (e,e'K+) hypernuclear spectroscopy at JLab Hall C in 2000, precision hypernuclear spectroscopy by the (e,e'K+) reactions made considerable progress. It has evolved to the 2nd generation experiment, E01-011, in which a newly constructed high resolution kaon spectrometer (HKS) was installed and the “Tilt method” was adopted in order to suppress large electromagnetic background and to run with high luminosity. Preliminary high-resolution spectra of 7 Λ He and 28 Λ Al together with that of 12 Λ B that achieved resolution better than 500 keV(FWHM) were obtained. The third generation…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsFull width at half maximumLuminosity (scattering theory)Electron spectrometerSpectrometerResolution (electron density)Calibrationhypernuclear; electroproduction; kaon spectrometer; electron spectrometerSpectroscopySpectral lineNuclear Physics A
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Reanalysis of pion pion phase shifts from K -> pi pi decays

2009

We re-investigate the impact of isospin violation for extracting the s-wave pion pion scattering phase shift difference delta_0(M_K) - delta_2(M_K) from K -> pi pi decays. Compared to our previous analysis in 2003, more precise experimental data and improved knowledge of low-energy constants are used. In addition, we employ a more robust data-driven method to obtain the phase shift difference delta_0(M_K) - delta_2(M_K) = (52.5 \pm 0.8_{exp} \pm 2.8_{theor}) degrees.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyPionScatteringIsospinPhase (waves)PiFísica
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Search for high mass photon pairs in (f= e, μ, τ, v, q) at LEP

1993

Abstract The result of a search for high mass photon pairs from the processes e + e − → f f γγ (f = e, μ, τ, v and q) with the ALEPH detector is reported. The result for f = e , μ and τ is to be compared with the observation of 4 events by the L3 Collaboration with invariant masses, M γγ , of the two photons near 60 GeV. From a data sample approximately twice as large taken from 1990 to 1992, 6 events are found with M γγ distributed between 50 GeV and 72 GeV, while 4.9 events are expected from a QED calculation. There is no evidence for a mass peak; only one event ( μ + μ − γγ ) at M γγ = 59.4 ± 0.2 GeV is compatible with the L3 observation. In addition, for M γγ > 50 GeV, no event is found…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh energyPhotonElectron–positron annihilationHigh massALEPH experimentPhysics Letters B
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