Search results for "Particle physics"

showing 10 items of 6826 documents

Top-pair forward-backward asymmetry beyond next-to-leading order

2011

We make use of recent results in effective theory and higher-order perturbative calculations to improve the theoretical predictions of the QCD contribution to the top-quark pair production forward-backward asymmetry at the Tevatron. In particular, we supplement the fixed-order next-to-leading order calculation with higher-order corrections from soft-gluon resummation at next-to next-to-leading order accuracy performed in two different kinematic schemes, which allows us to make improved predictions for the asymmetry in the $p\overline{p}$ and $t\overline{t}$ rest frames as a function of the rapidity and invariant mass of the $t\overline{t}$ pair. Furthermore, we provide binned results which …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics530 Physics010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyOrder (ring theory)01 natural sciencesAsymmetryGluonNuclear physicsPair production10231 Institute for Computational Science0103 physical sciencesHigh Energy Physics::ExperimentRapidityInvariant mass3106 Nuclear and High Energy Physics3101 Physics and Astronomy (miscellaneous)Resummation010306 general physicsmedia_commonPhysical Review D
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Exclusive production of pion and kaon meson pairs in two photon collisions at LEP

2003

Exclusive production of pi and K meson pairs in two photon collisions is measured with ALEPH data collected between 1992 and 2000. Cross-sections are presented as a function of cos theta* and invariant mass, for \ cos theta* \ < 0.6 and invariant masses between 2.0 and 6.0 GeV/c(2) (2.25 and 4.0 GeV/c(2)) for pions (kaons). The shape of the distributions are found to be well described by QCD predictions but the data have a significantly higher normalization. (C) 2003 Published by Elsevier B.V.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAlephMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeInvariant (physics)16. Peace & justice01 natural sciencesNuclear physicsAngular distributionPion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Mass spectrumHigh Energy Physics::ExperimentInvariant massNuclear Experiment010306 general physicsParticle Physics - ExperimentPhysics Letters B
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The decay

2010

In this paper the potential for the discovery of new physics in the exclusive decay B ¯ d → K ¯ ⁎ 0 μ + μ − is discussed. Attention is paid to constructing observables which are protected from uncertainties in QCD form factors and at the same time observe the symmetries of the angular distribution. We discuss the sensitivity to new physics in the observables including the effect of CP-violating phases.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAngular distributionPhysics beyond the Standard ModelHomogeneous spaceObservableSensitivity (control systems)Atomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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Charged particle multiplicity in e^{+}e_{-}$ → q[L:q] events at 161 and 172 GeV and from the decay of the W boson

1998

The data collected by DELPHI in 1996 have been used to measure the average charged particle multiplicities and dispersions in $q\bar{q}$ events at centre-of-mass energies of $\sqrt{s}=161$~GeV and $\sqrt{s}=172$~GeV, and the average charge multiplicity in WW events at $\sqrt{s}=172$~GeV. The multiplicities in $q\bar{q}$ events are consistent with the evolution predicted by QCD. The dispersions in the multiplicity distributions are consistent with Koba-Nielsen-Olesen (KNO) scaling. The average multiplicity of charged particles in hadronic W decays has been measured for the first time; its value, $19.23 \pm 0.74 (stat+syst)$, is consistent with that expected for an $e^+e^-$ interaction at a c…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsElectron–positron annihilationHadronMultiplicity (mathematics)PartonCharge (physics)01 natural sciencesCharged particleNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysics letters: B
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Observation ofe+e−→ρ+ρ−nears=10.58  GeV

2008

We report the first observation of e^+e^- → ρ^+ρ^-, in a data sample of 379 fb^(-1) collected with the BABAR detector at the PEP-II e+e- storage ring at center-of-mass energies near √s = 10:58 GeV. We measure a cross section of σ(e^+e^- → ρ^+ρ^-)= 8:3 ± 0:7(stat)± 0:8(syst) fb within the range of │cosθ^*│ < 0:8 and │ cosθ_±│ < 0:85, where θ^* is the center-of-mass polar angle of the ρ^± meson and θ_± are the angles in the ρ^± rest frame between the direction of the boost from the laboratory frame and the direction of the π^±. Assuming production through single-photon annihilation, there are three independent helicity amplitudes. We measure the ratios of their squared moduli to be │F_(00)│^2…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsElectron–positron annihilationRest frame01 natural sciencesHelicityAmplitudeAngular distribution0103 physical sciences010306 general physicsPhysical Review D
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Ds+ meson production at central rapidity in proton–proton collisions at s=7 TeV

2012

The pt-differential inclusive production cross section of the prompt charm-strange meson D_s in the rapidity range |y| phi pi, with phi -> KK, and its charge conjugate, about 480 D_s mesons were counted, after selection cuts, in the transverse momentum range 2

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAntiparticleLarge Hadron ColliderMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadronElementary particle7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsLeptonPhysics Letters B
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Mass Hierarchy, Mixing, CP-Violation and Higgs Decay---or Why Rotation is Good for Us

2011

The idea of a rank-one rotating mass matrix (R2M2) is reviewed detailing how it leads to ready explanations both for the fermion mass hierarchy and for the distinctive mixing patterns between up and down fermion states, which can be and have been tested against experiment and shown to be fully consistent with existing data. Further, R2M2 is seen to offer, as by-products: (i) a new solution of the strong CP problem in QCD by linking the theta-angle there to the Kobayashi-Maskawa CP-violating phase in the CKM matrix, and (ii) some novel predictions of possible anomalies in Higgs decay observable in principle at the LHC. A special effort is made to answer some questions raised.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsObservableMass matrixAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonCP violationStrong CP problemHigh Energy Physics::ExperimentMixing (physics)
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Nucleon andΔ(1232)form factors at low momentum transfer and small pion masses

2012

An expansion of the electromagnetic form factors of the nucleon and $\ensuremath{\Delta}(1232)$ in small momentum transfer and pion mass is performed in a manifestly covariant EFT framework consistent with chiral symmetry and analyticity. We present the expressions for the nucleon and $\ensuremath{\Delta}(1232)$ electromagnetic form factors, charge radii, and electromagnetic moments in the framework of $SU(2)$ baryon chiral perturbation theory, with nucleon and $\ensuremath{\Delta}$-isobar degrees of freedom, to next-to-leading order. Motivated by the results for the proton electric radius obtained from the muonic-hydrogen atom and electron-scattering process, we extract values for the seco…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsNuclear TheoryMomentum transferElectric form factorLattice QCD01 natural sciences7. Clean energyBaryonPion0103 physical sciencesNuclear Experiment010306 general physicsNucleonPhysical Review D
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Chiral sum rules and vacuum condensates from tau-lepton decay data

2015

QCD finite energy sum rules, together with the latest updated ALEPH data on hadronic decays of the tau-lepton are used in order to determine the vacuum condensates of dimension $d=2$ and $d=4$. These data are also used to check the validity of the Weinberg sum rules, and to determine the chiral condensates of dimension $d=6$ and $d=8$, as well as the chiral correlator at zero momentum, proportional to the counter term of the ${\cal{O}}(p^4)$ Lagrangian of chiral perturbation theory, $\bar{L}_{10}$. Suitable (pinched) integration kernels are introduced in the sum rules in order to suppress potential quark-hadron duality violations. We find no compelling indications of duality violations in t…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryDimension (graph theory)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyDuality (optimization)Order (ring theory)FOS: Physical sciencesMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentEnergy (signal processing)LeptonJournal of High Energy Physics
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From Hadronic τ Decays to the Chiral Couplings and

2009

A sum rule analysis of the hadronic τ -decay data can be used to determine the low-energy constants L 10 r ( μ ) and C 87 r ( μ ) . These constants are QCD chiral-order parameters, which appear at order p 4 and p 6 , respectively, in the chiral perturbation theory expansion of the V − A correlator. At order p 4 we obtain L 10 r ( M ρ ) = − ( 5.22 ± 0.06 ) ⋅ 10 − 3 . Including in the analysis the order p 6 contributions, we get L 10 r ( M ρ ) = − ( 4.06 ± 0.39 ) ⋅ 10 − 3 and C 87 r ( M ρ ) = ( 4.89 ± 0.19 ) ⋅ 10 − 3 GeV − 2 .

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHadronOrder (group theory)Sum rule in quantum mechanicsAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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