Search results for "normalization"

showing 10 items of 632 documents

QCD sum rules for heavy baryons

2001

We construct the heavy baryonic currents by using the Bethe-Salpeter wave functions in the heavy quark limit. We discuss the one-loop renormalization of these heavy baryonic currents as well as their two-point correlators up to the order $1/M_h$. For a special case, we do the QCD sum rule for masses of the doublet (3/2,5/2).

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsQCD sum rulesBethe–Salpeter equationHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsNuclear physicsRenormalizationBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentWave functionSpin-½Physical Review D
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Phase diagram of the two-channel kondo lattice model in one dimension.

2004

Employing the density matrix renormalization group method and strong-coupling perturbation theory, we study the phase diagram of the $\mathrm{SU}(2)\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(2)$ Kondo lattice model in one dimension. We show that, at quarter filling, the system can exist in two phases depending on the coupling strength. The weak-coupling phase is dominated by RKKY exchange correlations, while the strong-coupling phase is characterized by strong antiferromagnetic correlations of the channel degree of freedom. These two phases are separated by a quantum critical point. For conduction-band fillings of less than one-quarter, we find a paramagnetic metallic phase at weak coupl…

PhysicsQuantum phase transitionRKKY interactionCondensed matter physicsDensity matrix renormalization groupQuantum critical pointQuantum mechanicsGeneral Physics and AstronomyCondensed Matter::Strongly Correlated ElectronsKondo effectCoupling (probability)Lattice model (physics)Phase diagramPhysical review letters
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Holographic encoding of universality in corner spectra

2017

In numerical simulations of classical and quantum lattice systems, 2d corner transfer matrices (CTMs) and 3d corner tensors (CTs) are a useful tool to compute approximate contractions of infinite-size tensor networks. In this paper we show how the numerical CTMs and CTs can be used, {\it additionally\/}, to extract universal information from their spectra. We provide examples of this for classical and quantum systems, in 1d, 2d and 3d. Our results provide, in particular, practical evidence for a wide variety of models of the correspondence between $d$-dimensional quantum and $(d+1)$-dimensional classical spin systems. We show also how corner properties can be used to pinpoint quantum phase …

PhysicsQuantum phase transitionStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciencesObservable02 engineering and technologyQuantum entanglement021001 nanoscience & nanotechnology01 natural sciencesUniversality (dynamical systems)RenormalizationCondensed Matter - Strongly Correlated ElectronsQuantum stateQuantum mechanics0103 physical sciencesTensor010306 general physics0210 nano-technologyQuantum
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Renormalization Constants of Quark Operators for the Non-Perturbatively Improved Wilson Action

2004

We present the results of an extensive lattice calculation of the renormalization constants of bilinear and four-quark operators for the non-perturbatively O(a)-improved Wilson action. The results are obtained in the quenched approximation at four values of the lattice coupling by using the non-perturbative RI/MOM renormalization method. Several sources of systematic uncertainties, including discretization errors and final volume effects, are examined. The contribution of the Goldstone pole, which in some cases may affect the extrapolation of the renormalization constants to the chiral limit, is non-perturbatively subtracted. The scale independent renormalization constants of bilinear quark…

PhysicsQuarkNONPERTURBATIVE RENORMALIZATIONNuclear and High Energy PhysicsDiscretizationHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)ExtrapolationFOS: Physical sciencesBilinear interpolationFísicaQuenched approximationRenormalizationHigh Energy Physics - LatticeLattice (order)visual_artvisual_art.visual_art_mediumGoldstoneMathematical physics
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Constituent quarks and parton distributions

1997

Abstract The high energy parton distribution when evolved to a low energy scale appears to indicate that a valence picture of hadron structure arises. We have developed a formalism based on a laboratory partonic description which connects the parton distributions with the momentum distributions of a quark model. The formalism uses Next to Leading Order evolution and has been defined to produce the right support for the parton distributions. In this scheme we have analyzed the polarized and unpolarized data and shown that well-known Quark Models lead to a qualitative description of the data. However, if one aims at a quantitative agreement, these conventional low energy models have to be cha…

PhysicsQuarkNuclear and High Energy PhysicsAngular momentumParticle physicsHigh Energy Physics::PhenomenologyQuark modelHadronConstituent quarkPartonRenormalization groupGluonNuclear physicsHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics A
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Minimally doubled fermions at one loop

2009

Minimally doubled fermions have been proposed as a cost-effective realization of chiral symmetry at non-zero lattice spacing. Using lattice perturbation theory at one loop, we study their renormalization properties. Specifically, we investigate the consequences of the breaking of hyper-cubic symmetry, which is a typical feature of this class of fermionic discretizations. Our results for the quark self-energy indicate that the four-momentum undergoes a renormalization which contains a linearly divergent piece. We also compute renormalization factors for quark bilinears, construct the conserved vector and axial-vector currents and verify that at one loop the renormalization factors of the lat…

PhysicsQuarkNuclear and High Energy PhysicsFermion doublingChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Lattice field theoryFOS: Physical sciencesFermionRenormalizationHigh Energy Physics - LatticeQuantum electrodynamicsFunctional renormalization groupChiral symmetry breakingMathematical physicsPhysics Letters B
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Non-perturbative renormalization of static-light four-fermion operators in quenched lattice QCD

2007

We perform a non-perturbative study of the scale-dependent renormalization factors of a multiplicatively renormalizable basis of $\Delta{B}=2$ parity-odd four-fermion operators in quenched lattice QCD. Heavy quarks are treated in the static approximation with various lattice discretizations of the static action. Light quarks are described by non-perturbatively ${\rm O}(a)$ improved Wilson-type fermions. The renormalization group running is computed for a family of Schroedinger functional (SF) schemes through finite volume techniques in the continuum limit. We compute non-perturbatively the relation between the renormalization group invariant operators and their counterparts renormalized in …

PhysicsQuarkNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Lattice field theoryFOS: Physical sciencesParticle Physics - LatticeLattice QCDFermionRenormalization groupRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)lattice gauge field theories; lattice qcd; lattice quantum field theoryNon-perturbativeMathematical physics
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Quark–lepton mass relation in a realistic A4 extension of the Standard Model

2013

We propose a realistic A4A4 extension of the Standard Model involving a particular quark–lepton mass relation, namely that the ratio of the third family mass to the geometric mean of the first and second family masses are equal for down-type quarks and charged leptons. This relation, which is approximately renormalization group invariant, is usually regarded as arising from the Georgi–Jarlskog relations, but in the present model there is no unification group or supersymmetry. In the neutrino sector we propose a simple modification of the so-called Zee–Wolfenstein mass matrix pattern which allows an acceptable reactor angle along with a deviation of the atmospheric and solar angles from thei…

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySupersymmetryInvariant (physics)Renormalization groupMass matrix01 natural sciences0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsLeptonPhysics Letters B
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Low-energy interactions of Nambu-Goldstone bosons with D mesons in covariant chiral perturbation theory

2010

We calculate the scattering lengths of Nambu-Goldstone bosons interacting with D mesons in a covariant formulation of chiral perturbation theory, which satisfies heavy-quark spin symmetry and analytical properties of loop amplitudes. We compare our results with previous studies performed using heavy-meson chiral perturbation theory and show that recoil corrections are sizable in most cases.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonHigh Energy Physics::ExperimentPerturbation theoryChiral symmetry breakingNuclear ExperimentBoson
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Magnetic moments of heavy baryons

2000

6 páginas, 2 figuras, 4 tablas.-- PACS number(s): 12.39.Fe, 12.39.Hg, 14.20.Lq, 14.20.Mr

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMagnetic momentHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartícules (Física nuclear)BaryonCharmed baryonsRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Order (group theory)Nuclear Experiment
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