Search results for "QUANTUM MECHANICS"

showing 10 items of 2468 documents

Dual gauge-fixing property of the S matrix.

1996

The {ital S} matrix is known to be independent of the gauge-fixing parameter to all orders in perturbation theory. In this paper by employing the pinch technique we prove at one loop a stronger version of this independence. In particular, we show that one can use a gauge-fixing parameter for the gauge bosons inside quantum loops which is different from that used for the bosons outside loops, and the {ital S} matrix is independent of both. Possible phenomenological applications of this result are briefly discussed. {copyright} {ital 1996 The American Physical Society.}

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsGauge bosonComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyPropagatorFísicaMatrix (mathematics)Standard Model (mathematical formulation)Theoretical physicsQuantum mechanicsGauge fixingBosonS-matrixPhysical review. D, Particles and fields
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QCD sum rule analysis of the pentaquark

2005

We perform a QCD sum rule calculation to determine the mass and the parity of the lowest lying pentaquark state. We include operators up to dimension $d=13$ in the OPE and the direct instanton contributions. We find evidence for a positive parity state. The contribution from operators of dimension $d>5$ is instrumental in determining the parity of the state and achieving the convergence of the sum rule.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsInstantonParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesFísicaParity (physics)PentaquarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Invariant massOperator product expansionSum rule in quantum mechanics
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Factorization and N3LLp+NNLO predictions for the Higgs cross section with a jet veto

2013

We have recently derived a factorization formula for the Higgs-boson production cross section in the presence of a jet veto, which allows for a systematic resummation of large Sudakov logarithms of the form alpha_s^n ln^m(p_T^veto/m_H), along with the large virtual corrections known to affect also the total cross section. Here we determine the ingredients entering this formula at two-loop accuracy. Specifically, we compute the dependence on the jet-radius parameter R, which is encoded in the two-loop coefficient of the collinear anomaly, by means of a direct, fully analytic calculation in the framework of soft-collinear effective theory. We confirm the result obtained by Banfi et al. from a…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physics530 PhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesJet (particle physics)01 natural sciencesHigh Energy Physics - PhenomenologyCross section (physics)High Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesEffective field theoryHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Anomaly (physics)Resummation010306 general physics
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Perturbative chiral violations for domain-wall QCD with improved gauge actions

2006

We investigate, in the framework of perturbation theory at finite $N_s$, the effectiveness of improved gauge actions in suppressing the chiral violations of domain-wall fermions. Our calculations show substantial reductions of the residual mass when it is compared at the same value of the gauge coupling, the largest suppression being obtained when the DBW2 action is used. Similar effects can also be observed for a power-divergent mixing coefficient which is chirally suppressed. No significant reduction instead can be seen in the case of the difference between the vector and axial-vector renormalization constants when improved gauge actions are used in place of the plaquette action. We also …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFermionGauge (firearms)01 natural sciencesRenormalizationDomain wall (string theory)High Energy Physics - LatticeLattice gauge theory0103 physical sciencesPerturbation theory (quantum mechanics)010306 general physicsMixing (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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Results on longitudinal spin physics at COMPASS

2016

Abstract The COMPASS experiment at the CERN SPS has taken data for deep inelastic scattering of polarised muons off a polarised NH3 target in 2007 and 2011 and off a polarised 6LiD target in 2002–2004 and 2006. We present our new results on the longitudinal double spin asymmetry A 1 p and the spin-dependent structure function g 1 p obtained from the 2011 data set. These results are used in a NLO QCD fit to the world data to obtain the polarised parton distributions. Also an update on our results on the Bjorken sum rule, connecting the integral of the non-singlet spin-dependent structure function with the ratio of the weak coupling constants, is given. The gluon polarisation can be accessed …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsComputer science010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::PhenomenologyHadronPartonDeep inelastic scatteringEngineering physics01 natural sciencesGluonNuclear physicsCompass0103 physical sciencesCOMPASS experimentHigh Energy Physics::ExperimentSum rule in quantum mechanicsNuclear Experiment010306 general physicsParticle Physics - ExperimentNuclear and Particle Physics Proceedings
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Charm and bottom quark masses from QCD moment sum rules

2002

In this work the charm and bottom quark masses are determined from QCD moment sum rules for the charmonium and upsilon systems. In our analysis we include both the results from non-relativistic QCD and perturbation theory at next-next-to-leading order. For the pole masses we obtain $M_c=1.75\pm 0.15$ GeV and $M_b=4.98\pm 0.125$ GeV. Using the potential-subtracted mass in intermediate steps of the calculation the MS-masses are determined to $m_c(m_c) = 1.19 \pm 0.11$ GeV and $m_b(m_b) = 4.24 \pm 0.10$ GeV.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesBottom quarkAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Moment (physics)B mesonHigh Energy Physics::ExperimentCharm (quantum number)Perturbation theory (quantum mechanics)Astrophysics::Earth and Planetary AstrophysicsNuclear Experiment
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A Quark model analysis of the Sivers function.

2008

We develop a formalism to evaluate the Sivers function. The approach is well suited for calculations which use constituent quark models to describe the structure of the nucleon. A non-relativistic reduction of the scheme is performed and applied to the Isgur-Karl model of hadron structure. The results obtained are consistent with a sizable Sivers effect and the signs for the u and d flavor contributions turn out to be opposite. This pattern is in agreement with the one found analyzing, in the same model, the impact parameter dependent generalized parton distributions. The Burkardt Sum Rule turns out to be fulfilled to a large extent. We estimate the QCD evolution of our results from the mom…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryQuark modelHadronHigh Energy Physics::PhenomenologyConstituent quarkFísicaFOS: Physical sciencesPartonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Sum rule in quantum mechanicsImpact parameterNucleonParticle Physics - Phenomenology
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Bottomonium spectroscopy and radiative transitions involving theχbJ(1P,2P)states atBaBar

2014

We use (121±1) million Υ(3S) and (98±1) million Υ(2S) mesons recorded by the BABAR detector at the PEP-II e^+e^− collider at SLAC to perform a study of radiative transitions involving the χ_(bJ)(1P,2P) states in exclusive decays with μ^+μ^−γγ final states. We reconstruct twelve channels in four cascades using two complementary methods. In the first we identify both signal photon candidates in the electromagnetic calorimeter (EMC), employ a calorimeter timing-based technique to reduce backgrounds, and determine branching-ratio products and fine mass splittings. These results include the best observational significance yet for the χ_(b0)(2P)→γΥ(2S) and χ_(b0)(1P)→γΥ(1S) transitions. In the se…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsPhotonMeson010308 nuclear & particles physicsElectron–positron annihilation01 natural sciencesNuclear physicssymbols.namesakeExcited state0103 physical sciencessymbolsRadiative transferHigh Energy Physics::Experiment010306 general physicsSpectroscopyHamiltonian (quantum mechanics)Physical Review D
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New results on the spin structure function g1 of the proton and the deuteron from SMC

1998

Abstract New results from a measurement of the spin-dependent structure function g 1 p by the SMC are presented. A next-to-leading order QCD analysis of all published data is used to compute g 1 p at a fixed Q 2 of 10 GeV 2 . Two methods for the extrapolation towards x = 0 to determine the first moment are discussed. In both cases the violation of the Ellis-Jaffe sum rule is confirmed. Using the deuteron data in addition the Bjorken sum rule is tested.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsProtonDeuteriumQuantum electrodynamicsExtrapolationOrder (group theory)Function (mathematics)Sum rule in quantum mechanicsSpin structureAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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