Search results for "normalization"

showing 10 items of 632 documents

Nonperturbative renormalization of quark bilinears

1998

We compute non-perturbatively the renormalization constants of quark bilinears on the lattice in the quenched approximation at three values of the coupling beta=6/g_0^2=6.0,6.2,6.4 using both the Wilson and the tree-level improved SW-Clover fermion action. We perform a Renormalization Group analysis at the next-to-next-to-leading order and compute Renormalization Group invariant values for the constants. The results are applied to obtain a fully non-perturbative estimate of the vector and pseudoscalar decay constants.

QuarkPhysicsNuclear and High Energy Physicsgauge theory lattice non-perturbative renormalizationHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesQuenched approximationFermionRenormalization groupRenormalizationPseudoscalarFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeLattice (order)Non-perturbativeMathematical physics
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Nonperturbative renormalization and O(a) -improvement of the nonsinglet vector current with Nf=2+1 Wilson fermions and tree-level Symanzik improved g…

2019

In calculating hadronic contributions to precision observables for tests of the Standard Model in lattice QCD, the electromagnetic current plays a central role. Using a Wilson action with $\mathrm{O}(a)$ improvement in QCD with ${N}_{\mathrm{f}}$ flavors, a counterterm must be added to the vector current in order for its on-shell matrix elements to be $\mathrm{O}(a)$ improved. In addition, the local vector current, which has support on one lattice site, must be renormalized. At $\mathrm{O}(a)$, the breaking of the $\mathrm{SU}({N}_{\mathrm{f}})$ symmetry by the quark mass matrix leads to a mixing between the local currents of different quark flavors. We present a nonperturbative calculation…

QuarkPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryLattice QCDFermionMass matrix01 natural sciencesRenormalizationLattice (order)0103 physical sciences010306 general physicsMathematical physicsPhysical Review D
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Determination of m¯b/m¯c and m¯b from nf=4 lattice QCD+QED

2021

We extend HPQCD's earlier ${n}_{f}=2+1+1$ lattice-QCD analysis of the ratio of $\overline{\mathrm{MS}}$ masses of the $b$ and $c$ quark to include results from finer lattices (down to 0.03 fm) and a new calculation of QED contributions to the mass ratio. We find that ${\overline{m}}_{b}(\ensuremath{\mu})/{\overline{m}}_{c}(\ensuremath{\mu})=4.586(12)$ at renormalization scale $\ensuremath{\mu}=3\text{ }\text{ }\mathrm{GeV}$. This result is nonperturbative. Combining it with HPQCD's recent lattice $\mathrm{QCD}+\mathrm{QED}$ determination of ${\overline{m}}_{c}(3\text{ }\text{ }\mathrm{GeV})$ gives a new value for the $b$-quark mass: ${\overline{m}}_{b}(3\text{ }\text{ }\mathrm{GeV})=4.513(2…

QuarkQuantum chromodynamicsPhysicsParticle physics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)Lattice QCDMass ratio01 natural sciencesRenormalizationLattice (order)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Gauge-invariant on-shellZ 2 in QED, QCD and the effective field theory of a static quark

1991

We calculate theon-shell fermion wave-function renormalization constantZ 2 of a general gauge theory, to two loops, inD dimensions and in an arbitrary covariant gauge, and find it to be gauge-invariant. In QED this is consistent with the dimensionally regularized version of the Johnson-Zumino relation: d logZ 2/da 0=i(2π)−D e 0 2 ∫d D k/k 4=0. In QCD it is, we believe, a new result, strongly suggestive of the cancellation of the gauge-dependent parts of non-abelian UV and IR anomalous dimensions to all orders. At the two-loop level, we find that the anomalous dimension γ F of the fermion field in minimally subtracted QCD, withN L light-quark flavours, differs from the corresponding anomalou…

QuarkQuantum chromodynamicsPhysicsParticle physicsFermionic fieldPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFermionRenormalizationsymbols.namesakeEffective field theorysymbolsCovariant transformationGauge theoryEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
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Dimensional reduction methods in QCD

1994

We apply the technique of dimensional reduction to massless quantum chromodynamics. It is shown that compared to conventional dimensional regularization methods calculations of radiative corrections at the one-loop level are less involved. We discuss the use of helicity methods within this framework and as an application we evaluate the one-loop corrections to the parity-violating cross sections and to the quark forwardbackward asymmetric polarization in\(e^ + e^ - \to V \to q\bar q(g)\). Finally, we demonstrate that further simplifications occur in the computation of structure functions including the parity-violating structure function in quark- and gluoninitiated electroproduction process…

QuarkQuantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)Electron–positron annihilationHigh Energy Physics::PhenomenologyHelicityRenormalizationMassless particleDimensional regularizationDimensional reductionHigh Energy Physics::ExperimentEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Operator product expansion and quark condensate from Lattice QCD in coordinate space

2005

We present a lattice QCD determination of the chiral quark condensate based on a new method. We extract the quark condensate from the operator product expansion of the quark propagator at short euclidean distances, where it represents the leading contribution in the chiral limit. From this study we obtain MS( 2 GeV) = -( 265 +/- 5 +/- 22MeV)(3), in good agreement with determinations of this quantity based on different approaches. The simulation is performed by using the O( a)- improved Wilson action at beta = 6.45 on a volume 32(3) x 70 in the quenched approximation.

QuarkQuantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)Field (physics)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Lattice (group)FísicaPropagatorFOS: Physical sciencesRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentOperator product expansionCoordinate spaceEngineering (miscellaneous)
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Higher-order effects for the coupling constant in asymptotically free theories

1977

It is shown that the two-loop contribution to the Callan-Symanzik $\ensuremath{\beta}$ function leads to an effective coupling constant which may be quite different from the value obtained from the standard one-loop calculation. This correction is larger than that due to finite quark masses. Possible implications for the comparison between asymptotically free theories and experiment are discussed.

QuarkRenormalizationPhysicsCoupling constantQuantum mechanicsQuark modelOrder (ring theory)Function (mathematics)Gauge theoryQuantum field theoryPhysical Review D
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Renormalization of the effective theory for heavy quarks at small velocity

1995

The slope of the Isgur-Wise function at the normalization point, $\xi^{(1)}(1)$,is one of the basic parameters for the extraction of the $CKM$ matrix element $V_{cb}$ from exclusive semileptonic decay data. A method for measuring this parameter on the lattice is the effective theory for heavy quarks at small velocity $v$. This theory is a variant of the heavy quark effective theory in which the motion of the quark is treated as a perturbation. In this work we study the lattice renormalization of the slow heavy quark effective theory. We show that the renormalization of $\xi^{(1)}(1)$ is not affected by ultraviolet power divergences, implying no need of difficult non-perturbative subtraction…

QuarkSemileptonic decayPhysicsNuclear and High Energy Physicsheavy quark effective theory; small quark velocities; renormalizationComputationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Perturbation (astronomy)FísicaFOS: Physical sciencesRenormalizationHigh Energy Physics - LatticeLattice (order)Effective field theoryHeavy quark effective theoryMathematical physics
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Kaon mixing beyond the SM from N-f=2 tmQCD and model independent constraints from the UTA

2013

We present the first unquenched, continuum limit, lattice QCD results for the matrix elements of the operators describing neutral kaon oscillations in extensions of the Standard Model. Owing to the accuracy of our calculation on Delta S = 2 weak Hamiltonian matrix elements, we are able to provide a refined Unitarity Triangle analysis improving the bounds coming from model independent constraints on New Physics. In our non-perturbative computation we use a combination of N-f = 2 maximally twisted sea quarks and Osterwalder-Seiler valence quarks in order to achieve both O(a)-improvement and continuum-like renormalization properties for the relevant four-fermion operators. The calculation of t…

QuarkStrange quarkParticle physicsNuclear and High Energy PhysicsPhysics beyond the Standard ModelComputationHigh Energy Physics::LatticeFOS: Physical sciencesLattice QCD01 natural sciencesRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciences010306 general physicsPhysicsHamiltonian matrixUnitarity010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]Computer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)FísicaLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelBeyond the Standard Model Physics
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A combined molecular dynamics and Monte Carlo study of the approach towards phase separation in colloid-polymer mixtures.

2011

A coarse-grained model for colloid-polymer mixtures is investigated where both colloids and polymer coils are represented as point-like particles interacting with spherically symmetric effective potentials. Colloid-colloid and colloid-polymer interactions are described by Weeks-Chandler-Andersen potentials, while the polymer-polymer interaction is very soft, of strength k(B)T/2 for maximum polymer-polymer overlap. This model can be efficiently simulated both by Monte Carlo and molecular dynamics methods, and its phase diagram closely resembles that of the well-known Asakura-Oosawa model. The static and dynamic properties of the model are presented for systems at critical colloid density, va…

RENORMALIZATIONPolymersMonte Carlo methodBiophysicsThermodynamicsSOFT MATTERMolecular Dynamics SimulationDiffusionColloidMolecular dynamicsFLUIDSCritical point (thermodynamics)PARTICLESGeneral Materials ScienceComputer SimulationColloidsAnisotropyPhase diagramchemistry.chemical_classificationQuantitative Biology::BiomoleculesModels StatisticalChemistryPhysicsPolymerCondensed Matter PhysicsCondensed Matter::Soft Condensed MatterShear rateKineticsSIMULATIONPERTURBATION-THEORYAnisotropyStress MechanicalPAIR POTENTIALSMonte Carlo MethodBEHAVIORINTERFACESAlgorithmsJournal of physics. Condensed matter : an Institute of Physics journal
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