Search results for "decays"

showing 10 items of 244 documents

Search for the rare decay Bs 0→μ+μ-

2010

We present the results of a search for the flavor changing neutral current decay B-s(0) -> mu(+)mu(-) using 6.1 fb(-1) of p (p) over bar collisions at root s = 1.96 TeV collected by the D0 experiment at the Fermilab Tevatron Collider. The observed number of B-s(0) candidates is consistent with background expectations. The resulting upper limit on the branching fraction is B(B-s(0) -> mu(+)mu(-)) < 5.1 x 10(-8) at the 95% C.L. This limit is a factor of 2.4 better than that of the previous DO analysis and the best limit to date. Published by Elsevier B.V.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionFlavor-changing neutral currentTevatronD0 experimentRare decays01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesCP violationB-quarksFermilab010306 general physicsColliderb-quarksBar (unit)
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Disentangling new physics contributions in lepton flavour violating τ decays

2016

Abstract The possibility to discriminate between different operators contributing to lepton flavour violating tau decays is discussed within an effective field theory framework. Correlations among decay rates in different channels as well as differential distributions in many-body decays are considered. Recent developments in the determination of the hadronic form factors for τ → l π π ( l = e , μ ) decays are incorporated in the analysis. The above issues are exemplified by considering a Higgs-like boson with lepton flavour violating couplings. Implications of the search for lepton flavour violating Higgs decays performed recently by the CMS collaboration are also discussed.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeFlavourHadronHigh Energy Physics::Phenomenologylepton flavour violationHiggs decays01 natural sciencesNuclear physics0103 physical sciencesHiggs bosonEffective field theoryHigh Energy Physics::Experiment010306 general physicstau decaysBosonLeptonNuclear and Particle Physics Proceedings
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Study of D0– mixing and D0 doubly Cabibbo-suppressed decays

1998

Abstract Using a sample of four million hadronic Z events collected in ALEPH from 1991 to 1995, the decays D ∗+ → D 0 π s + , with D0 decaying to K−π+ or to K+π−, are studied. The relative branching ratio B(D0→K+π−)/B(D0→K−π+) is measured to be 1.84±0.59( stat. ) ±0.34( syst. ) %. The two possible contributions to the D0→K+π− decay, doubly Cabibbo-suppressed decays and D0– D 0 mixing, are disentangled by measuring the proper-time distribution of the reconstructed D0's. Assuming no interference between the two processes, the upper limit obtained on the mixing rate is 0.92% at 95% CL . The possible effect of interference between the two amplitudes is also assessed.

PhysicsNuclear and High Energy PhysicsParticle physicsALEPH Experiment; LEP; Cabibbo suppressed decaysBranching fractionElectron–positron annihilationHadronLEPNuclear physicsALEPH ExperimentDistribution (mathematics)AmplitudeCabibbo suppressed decaysALEPH experimentMixing (physics)Bar (unit)
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Precision measurement of the mass of the tau lepton

2014

An energy scan near the $\tau$ pair production threshold has been performed using the BESIII detector. About $24$ pb$^{-1}$ of data, distributed over four scan points, was collected. This analysis is based on $\tau$ pair decays to $ee$, $e\mu$, $eh$, $\mu\mu$, $\mu h$, $hh$, $e\rho$, $\mu\rho$ and $\pi\rho$ final states, where $h$ denotes a charged $\pi$ or $K$. The mass of the $\tau$ lepton is measured from a maximum likelihood fit to the $\tau$ pair production cross section data to be $m_{\tau} = (1776.91\pm0.12 ^{+0.10}_{-0.13}$) MeV/$c^2$, which is currently the most precise value in a single measurement.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilation010308 nuclear & particles physicshep-exElectron–positron annihilationMaximum likelihoodSingle measurementDetectorBESIII01 natural sciencesDECAYSHigh Energy Physics - ExperimentNuclear physicsENERGYPair production0103 physical sciencesRADIATIVE-CORRECTIONSHigh Energy Physics::Experiment010306 general physicsANNIHILATIONDETECTORSYSTEMLepton
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Spectral distribution for the decay τ→ντKπ

2006

Abstract With the newly available data sets on hadronic τ decays from the B -factories BaBar and BELLE, and future data from BESIII, precise information on the decay distributions will soon become available. This calls for an improvement of the decay spectra also on the theoretical side. In this work, the distribution function for the decay τ → ν τ K π will be presented with the relevant Kπ vector and scalar form factors being calculated in the framework of the resonance chiral theory, also taking into account additional constraints from dispersion relations and short-distances. As a by-product the slope and curvature of the vector form factor F + K π ( s ) are determined to be λ + ′ = 25.6…

PhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionPartial wave analysisHadronScalar (mathematics)ResonanceDecays of tausNuclear physicsDistribution functionDispersion relationHigh Energy Physics::ExperimentB mesonChiral symmetriesDispersion relationsPhysics Letters B
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Charm mass dependence of the weak Hamiltonian in chiral perturbation theory

2004

Suppose that the weak interaction Hamiltonian of four-flavour SU(4) chiral effective theory is known, for a small charm quark mass m_c. We study how the weak Hamiltonian changes as the charm quark mass increases, by integrating it out within chiral perturbation theory to obtain a three-flavour SU(3) chiral theory. We find that the ratio of the SU(3) low-energy constants which mediate Delta I=1/2 and Delta I=3/2 transitions, increases rather rapidly with m_c, as \sim m_c ln (1/m_c). The logarithmic effect originates from "penguin-type" charm loops, and could represent one of the reasons for the Delta I=1/2 rule.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryLogarithmHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesWeak interactionweak decaysCharm quarksymbols.namesakeHigh Energy Physics - Phenomenologylattice QCDHigh Energy Physics - Phenomenology (hep-ph)kaon physicssymbolsEffective field theorychiral lagrangiansHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)
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Final State Interactions in Kaon Decays

2001

27 páginas, 1 figura, 2 tablas.-- PACS: 13.25.Es; 11.30.Er; 13.85.Fb; 11.55.Fv.-- arXiv:hep-ph/0007208v1

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Lattice (hep-lat)Phase (waves)FOS: Physical sciencesFísicaState (functional analysis)Final state interactionsStandard ModelHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics - LatticeKaon decays
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Search for the decay K-s -> pi(0)e(+)e(-)

2001

Abstract A search for the decay K S →π 0 e + e − has been made using the NA48 detector at the CERN SPS. Using data collected in 1999 during a 40-hour run with a high-intensity KS beam, an upper limit for the branching fraction B (K S →π 0 e + e − ) −7 at 90% confidence level has been obtained.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderBranching fractiondecadimentiDetectorpionKaonsCP VIOLATION; KAONKAONK mesonNuclear physicsmesoni Kmesoni K; decadimentiCP violationLimit (mathematics)CP VIOLATIONK meson; pionradiative decaysBeam (structure)Kaons; radiative decays; chiral perturbation theorychiral perturbation theory
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Predictions for η→ηπ+π− producing f0(500), f0(980) and a0(980)

2017

Abstract We perform calculations for the η c → η π + π − decay using elements of SU(3) symmetry to see the weight of different trios of pseudoscalars produced in this decay, prior to the final state interaction of the mesons. After that, the interaction of pairs of mesons, leading finally to η π + π − , is done using the chiral unitary approach. We evaluate the π + π − and πη mass distributions and find large and clear signals for f 0 ( 500 ) , f 0 ( 980 ) and a 0 ( 980 ) excitation. The reaction is similar to the χ c 1 → η π + π − , which has been recently measured at BESIII and its implementation and comparison with these predictions will be very valuable to shed light on the nature of th…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsScalar (mathematics)Scalar meson statesState (functional analysis)01 natural scienceslcsh:QC1-999Symmetry (physics)Dynamically generated resonances0103 physical sciencesCharmonium decays010306 general physicsLow Masslcsh:PhysicsExcitationPhysics Letters B
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Search for CP violation in ZmF ττ

1992

Abstract Using the 18.8 pb−1 of data accumulated at LEP in 1990 and 1991 with the ALEPH detector, a direct test of neutral current CP-invariance is performed by a search for CP-odd correlations in Z decays to τ pairs where both τ decay modes are identified. No evidence for CP-violation is observed. The weak dipole moment of the τ has been measured to be dτ(mZ) = (1.3 ± 1.4 ± 0.1) × 10−17 e·cm which results in an upper limit on the weak dipole moment of |dτ(mZ)| ⩽ 3.7 × 10−17 e·cm with 95% confidence level.

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentElectron–positron annihilationAPLANARITIEST-ODDNuclear physicsMoment (mathematics)DipoleTAU-LEPTONSDirect testTESTSCP violationE+E COLLIDERSZ-DECAYSPhysics Letters B
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