Search results for "Invariant"

showing 10 items of 783 documents

Measurement of the W mass in e+e− collisions at 183 GeV

1999

Abstract The mass of the W boson is obtained from reconstructed invariant mass distributions in W-pair events. The sample of W pairs is selected from 57 pb−1 collected with the ALEPH detector in 1997 at a centre-of-mass energy of 183 GeV. The invariant mass distributions of reweighted Monte Carlo events are fitted separately to the experimental distributions in the q q q q and all lν q q channels to give the following W masses: m W hadronic =80.461±0.177 (stat.) ±0.045 (syst.) ±0.056 (theory) GeV /c 2 , m W semileptonic =80.326±0.184 (stat.) ±0.040 (syst.) GeV /c 2 , where the theory error represents the possible effects of final state interactions. The combination of these two measurements…

PhysicsNuclear and High Energy PhysicsParticle physicsAleph[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]010308 nuclear & particles physicsElectron–positron annihilationHadronMonte Carlo methodState (functional analysis)LEP01 natural sciencesNuclear physicsALEPH ExperimentPair productionALEPH Experiment; LEP; W boson0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]W bosonInvariant massHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentALEPH experimentParticle Physics - Experiment
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Do p annihilations at rest choose the Eightfold way?

1993

Dynamical selection rules observed in pp annihilation at rest are linked to relations between SU(3) invariant amplitudes. The ϱπ puzzle, the KK suppression in P wave, and the unexplained production rates of πa2 (1320) are shown to be manifestions of one SU(3) amplitude ratio. The dynamical selection rules observed in the production of strange mesons lead to symmetries in SU(3) amplitudes. We conjecture that these symmetries reflect the underlying quark-gluon dynamic. It is shown that the contribution of annihilation diagrams to important annihilation channels like ϱ0π0 or ηω is small or vanishes. Hence rearrangement must play an important role. The use of SU(3) relations in the context of N…

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationAmplitudeMesonBranching fractionEightfold WayHomogeneous spaceStrangeness productionInvariant (physics)Physics Letters B
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Study ofe+e−→pp¯via initial-state radiation atBABAR

2013

The e{sup +}e{sup -}{yields}pp cross section is determined over a range of pp masses, from threshold to 4.5 GeV/c{sup 2}, by studying the e{sup +}e{sup -}{yields}pp{gamma} process. The data set corresponds to an integrated luminosity of 232 fb{sup -1}, collected with the BABAR detector at the PEP-II storage ring, at an e{sup +}e{sup -} center-of-mass energy of 10.6 GeV. The mass dependence of the ratio of electric and magnetic form factors, G{sub E}/G{sub M}, is measured for pp masses below 3 GeV/c{sup 2}; its value is found to be significantly larger than 1 for masses up to 2.2 GeV/c{sup 2}. We also measure J/{psi}{yields}pp and {psi}(2S){yields}pp branching fractions and set an upper limi…

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationBranching fraction010308 nuclear & particles physicsElectron–positron annihilationmedia_common.quotation_subjectAnalytical chemistryRadiation01 natural sciences7. Clean energyAsymmetryParticle identificationNuclear physicsAngular distribution0103 physical sciencesHigh Energy Physics::ExperimentInvariant massTotal energyNuclear Experiment010306 general physicsBhabha scatteringmedia_commonPhysical Review D
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Invariant approach to flavor-dependent CP-violating phases in the MSSM

2004

We use a new weak basis invariant approach to classify all the observable phases in any extension of the Standard Model (SM). We apply this formalism to determine the invariant CP phases in a simplified version of the Minimal Supersymmetric SM with only three non-trivial flavour structures. We propose four experimental measures to fix completely all the observable phases in the model. After these phases have been determined from experiment, we are able to make predictions on any other CP-violating observable in the theory, much in the same way as in the Standard Model all CP-violation observables are proportional to the Jarlskog invariant.

PhysicsNuclear and High Energy PhysicsParticle physicsBasis (linear algebra)Formalism (philosophy)FlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableExtension (predicate logic)Standard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Invariant (mathematics)Particle Physics - Phenomenology
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The tau weak-magnetic dipole moment

1994

We calculate the prediction for the anomalous weak-magnetic form factor of the tau lepton at $q^2=M_Z^2$ within the Standard Model. With all particles on-shell, this is a electroweak gauge invariant quantity. Its value is $a_\tau^w (M_Z^2)= - \;(2.10 + 0.61\, i) \times 10^{-6}$. We show that the transverse and normal components of the single-tau polarization of tau pairs produced at $e^+e^-$ unpolarized collisions are sensitive to the real and absorptive parts of the anomalous weak-magnetic dipole moment of the tau. The sensitivity one can achieve at LEP in the measurement of this dipole moment is discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsCamps magnèticsMagnetic momentElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesInvariant (physics)Polarization (waves)Partícules (Física nuclear)Transverse planeDipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCamps Teoria quàntica deLeptonParticle Physics - Phenomenology
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Chiral approach to the two pion decay of the Roper

2003

Abstract The analysis of Manley and collaborators [1] of the decay of the Roper into two pions requires the introduction of an effective scalar-isosclar ϵ or σ meson in order to describe the s-wave ππ interaction. Here we try to understand at a more fundamental level the origin of this effective channel. In our model the two pions are produced in single pion-baryon-baryon vertices and their re-scattering in the L=0, I=0 channel is explicitly evaluated. For that purpose we use unitarized chiral perturbation theory to obtain the Bethe-Salpeter amplitude for the two pion re-scattering in the appropriate channel. Our model produces invariant mass distributions in agreement with the ones obtaine…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryBethe–Salpeter equationMesonHigh Energy Physics::PhenomenologyNuclear TheoryHadronElementary particleParticle decayPionInvariant massNuclear ExperimentNuclear Physics A
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Chiral dynamics and the reactions pp↦dK+ and pp↦dπ+η

2001

We perform a study of the final-state interactions of the K+\(\) and the \(\)d systems in the reactions pp↦dK+\(\) and pp↦dπ+η. Since the two-meson system couples strongly to the a0(980) resonance, these reactions are expected to be an additional source of information about the controversial scalar sector. We also show that these reactions present peculiar features which can shed additional light on the much debated meson-baryon scalar sector with strangeness -1. We deduce the general structure of the amplitudes close to the dK+\(\) threshold, allowing for primary K+\(\) as well as π+η production with the two mesons in relative S- or P-wave. The interactions of the mesons are accounted for …

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonHigh Energy Physics::PhenomenologyHadronScalar (mathematics)Production (computer science)Invariant (mathematics)StrangenessResonance (particle physics)The European Physical Journal A
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Study of dipion bottomonium transitions and search for thehb(1P)state

2011

We study inclusive di-pion decays using a sample of 108 x 10{sup 6} {Upsilon}(3S) events recorded with the BABAR detector. We search for the decay mode {Upsilon}(3S) {yields} {pi}{sup +}{pi}{sup -}h{sub b} (1P) and find no evidence for the bottomonium spin-singlet state h{sub b}(1P) in the invariant mass distribution recoiling against the {pi}{sup +}{pi}{sup -} system. Assuming the h{sub b}(1P) mass to be 9.900 GeV/c{sup 2}, we measure the upper limit on the branching fraction {Beta}[{Upsilon}(3S) {yields} {pi}{sup +}{pi}{sup -}h{sub b}(1P)] < 1.2 x 10{sup -4}, at 90% confidence level. We also investigate the {chi}{sub bJ}(2P) {yields} {pi}{sup +}{pi}{sup -} {chi}{sub bJ}(1P), {Upsilon}(3S)…

PhysicsNuclear and High Energy PhysicsParticle physicsCrystallography010308 nuclear & particles physicsBranching fraction0103 physical sciencesInvariant massState (functional analysis)010306 general physics01 natural sciencesPhysical Review D
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Why a scalar explanation of the L3 events is implausible

1993

We investigate the question of whether an additional light neutral scalar can explain the $l^+ l^- \gamma \gamma$ events with high invariant mass photon pairs recently observed by the L3 collaboration. We parameterize the low energy effects of the unknown dynamics in terms of higher dimensional effective operators. We show that operators which allow for the scalar to be produced and decay into photon pairs will allow other observable processes that should have been seen in current experiments.

PhysicsNuclear and High Energy PhysicsParticle physicsCurrent (mathematics)PhotonScalar (mathematics)FOS: Physical sciencesFísicaObservablelcsh:QC1-999High Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)Invariant masslcsh:PhysicsPhysics Letters B
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Self-consistent variational approach to the minimal left-right symmetric model of electroweak interactions

2006

The problem of mass generation is addressed by a Gaussian variational method for the minimal left-right symmetric model of electroweak interactions. Without any scalar bidoublet, the Gaussian effective potential is shown to have a minimum for a broken symmetry vacuum with a finite expectation value for both the scalar Higgs doublets. The symmetry is broken by the fermionic coupling that destabilizes the symmetric vacuum, yielding a self consistent fermionic mass. In this framework a light Higgs is only compatible with the existence of a new high energy mass scale below 2 TeV.

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak gauge sector quantum field theoryMass generationScalar (mathematics)Electroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesSymmetry (physics)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Variational methodHiggs bosonInvariant massSymmetry breaking
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