Search results for "Gauge"

showing 10 items of 710 documents

Towards leading isospin breaking effects in mesonic masses with $O(a)$ improved Wilson fermions

2017

We present an exploratory study of leading isospin breaking effects in mesonic masses using $O(a)$ improved Wilson fermions. Isospin symmetry is explicitly broken by distinct masses and electric charges of the up and down quarks. In order to be able to make use of existing isosymmetric QCD gauge ensembles we apply reweighting techniques. The path integral describing QCD+QED is expanded perturbatively in powers of the light quarks' mass deviations and the electromagnetic coupling. We employ QED$_{\mathrm{L}}$ as a finite volume formulation of QED.

Quantum chromodynamicsQuarkPhysicsParticle physics010308 nuclear & particles physicsPhysicsQC1-999Computer Science::Information RetrievalHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermionGauge (firearms)01 natural sciencesElectric chargeSymmetry (physics)High Energy Physics - LatticeIsospin0103 physical sciencesPath integral formulationHigh Energy Physics::Experiment010306 general physics
researchProduct

Electromagnetic lattice gauge invariance in two-dimensional discrete-time quantum walks

2018

International audience; Gauge invariance is one of the more important concepts in physics. We discuss this concept in connection with the unitary evolution of discrete-time quantum walks in one and two spatial dimensions, when they include the interaction with synthetic, external electromagnetic fields. One introduces this interaction as additional phases that play the role of gauge fields. Here, we present a way to incorporate those phases, which differs from previous works. Our proposal allows the discrete derivatives, that appear under a gauge transformation, to treat time and space on the same footing, in a way which is similar to standard lattice gauge theories. By considering two step…

Quantum informationHigh Energy Physics::Latticecurrent: conservation lawLattice field theoryFOS: Physical sciencescurrent: density01 natural sciences010305 fluids & plasmasrandom walksymbols.namesakeTheoretical physics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]electromagnetic field0103 physical sciencesunitarityinvariance: gaugeQuantum walkDirac equationcontinuum limitGauge theorydimension: 2010306 general physicsConserved currentComputingMilieux_MISCELLANEOUSQuantum walksPhysicsQuantum PhysicsSpacetimeUnitaritylattice field theoryInvariant (physics)[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]electromagneticDirac equationsymbolsgauge field theoryQuantum simulationQuantum Physics (quant-ph)transformation: gaugeLattice gauge theoriesPhysical Review A
researchProduct

Incommensurate phases of a bosonic two-leg ladder under a flux

2016

A boson two--leg ladder in the presence of a synthetic magnetic flux is investigated by means of bosonization techniques and Density Matrix Renormalization Group (DMRG). We follow the quantum phase transition from the commensurate Meissner to the incommensurate vortex phase with increasing flux at different fillings. When the applied flux is $\rho \pi$ and close to it, where $\rho$ is the filling per rung, we find a second incommensuration in the vortex state that affects physical observables such as the momentum distribution, the rung-rung correlation function and the spin-spin and charge-charge static structure factors.

Quantum phase transitionBosonizationBosonisation[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]IncommensurationsFOS: Physical sciencesGeneral Physics and Astronomychamps de jauge artificiels01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)Condensed Matter - Strongly Correlated ElectronsCorrelation functionGauge fieldsCondensed Matter::Superconductivity0103 physical sciencesBosonizationtranstion commensurable-incommensurable010306 general physicsCommensurate-Incommensurate transitions[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsartificial gauge fieldsDensity matrix renormalization groupGauge fields; Incommensurations; Meissner to vortex transition; Physics and Astronomy (all)Vortex stateMagnetic fluxVortexQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality.Quantum Gases (cond-mat.quant-gas)Meissner to vortex transitionCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality
researchProduct

Spectrum of SU(2) lattice gauge theory with two adjoint Dirac flavours

2008

An SU(2) gauge theory with two fermions transforming under the adjoint representation of the gauge group may appear conformal or almost conformal in the infrared. We use lattice simulations to study the spectrum of this theory and present results on the masses of several gauge singlet states as a function of the physical quark mass determined through the axial Ward identity and find indications of a change from chiral symmetry breaking to a phase consistent with conformal behaviour at beta_L ~ 2. However, the measurement of the spectrum is not alone sufficient to decisively confirm the existence of conformal fixed point in this theory as we show by comparing to similar measurements with fun…

QuarkCoupling constantPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciences01 natural sciencesTheoretical physicsHigh Energy Physics - LatticeGauge groupLattice gauge theory0103 physical sciencesGauge theory010306 general physicsChiral symmetry breakingSpecial unitary group
researchProduct

Low-energy couplings of QCD from current correlators near the chiral limit

2004

We investigate a new numerical procedure to compute fermionic correlation functions at very small quark masses. Large statistical fluctuations, due to the presence of local ``bumps'' in the wave functions associated with the low-lying eigenmodes of the Dirac operator, are reduced by an exact low-mode averaging. To demonstrate the feasibility of the technique, we compute the two-point correlator of the left-handed vector current with Neuberger fermions in the quenched approximation, for lattices with a linear extent of L~1.5 fm, a lattice spacing a~0.09 fm, and quark masses down to the epsilon-regime. By matching the results with the corresponding (quenched) chiral perturbation theory expres…

QuarkNuclear and High Energy PhysicsChiral perturbation theoryCurrent (mathematics)High Energy Physics::LatticeFOS: Physical sciencesQuenched approximationStatistical fluctuationsDirac operatorsymbols.namesakechiral Lagrangianslattice QCDHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Latticelattice gauge field theoriesPhysicsQuantum chromodynamicsHigh Energy Physics - Lattice (hep-lat)FísicaFermionQCDFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyLattice gauge theoryQuantum electrodynamicssymbols
researchProduct

Renormalization group invariant matrix elements of Delta S = 2 and Delta I = 3/2 four fermion operators without quark masses

1999

We introduce a new parameterization of four-fermion operator matrix elements which does not involve quark masses and thus allows a reduction of systematic uncertainties. In order to simplify the matching between lattice and continuum renormalization schemes, we express our results in terms of renormalization group invariant B-parameters which are renormalization-scheme and scale independent. As an application of our proposal, matrix elements of DI=3/2 and SUSY DS =2 operators have been computed. The calculations have been performed using the tree-level improved Clover lattice action at two different values of the strong coupling constant (beta=6/g^2=6.0 and 6.2), in the quenched approximati…

QuarkNuclear and High Energy PhysicsHigh Energy Physics::LatticeSTANDARD MODELFOS: Physical sciencesWILSON FERMIONSQuenched approximationPartícules (Física nuclear)kaon decays gauge theory latticeLATTICE QCDRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKAON B-PARAMETERLattice (order)Mathematical physicsPhysicsHigh Energy Physics - Lattice (hep-lat)FísicaFermionSupersymmetryInvariant (physics)Renormalization groupFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
researchProduct

NNLO Unquenched Calculation of the b Quark Mass

2000

By combining the first unquenched lattice computation of the B-meson binding energy and the two-loop contribution to the lattice HQET residual mass, we determine the (\bar{{MS}}) (b)-quark mass, (\bar{m}_{b}(\bar{m}_{b})). The inclusion of the two-loop corrections is essential to extract (\bar{m}_{b}(\bar{m}_{b})) with a precision of ({\cal O}(\Lambda^{2}_{QCD}/m_{b})), which is the uncertainty due to the renormalon singularities in the perturbative series of the residual mass. Our best estimate is (\bar{m}_{b}(\bar{m}_{b}) = (4.26 \pm 0.09) {\rm GeV}), where we have combined the different errors in quadrature. A detailed discussion of the systematic errors contributing to the final number …

QuarkNuclear and High Energy PhysicsParticle physicsB physics gauge theory latticeComputationB physics QCD latticeHigh Energy Physics::LatticeBinding energyLattice field theoryFOS: Physical sciencesElementary particleBottom quarkPartícules (Física nuclear)RenormalonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)BibliographyPhysicsQuantum chromodynamicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)PropagatorFermionAtomic and Molecular Physics and OpticsFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyStrange matterHigh Energy Physics::Experiment
researchProduct

Light hadrons from lattice QCD with light (u, d), strange and charm dynamical quarks

2010

We present results of lattice QCD simulations with mass-degenerate up and down and mass-split strange and charm (N_f = 2+1+1) dynamical quarks using Wilson twisted mass fermions at maximal twist. The tuning of the strange and charm quark masses is performed at two values of the lattice spacing a~0.078 fm and a~0.086 fm with lattice sizes ranging from L~1.9 fm to L~2.8 fm. We measure with high statistical precision the light pseudoscalar mass m_PS and decay constant f_PS in a range 270 < m_PS < 510 MeV and determine the low energy parameters f_0, l_3 and l_4 of SU(2) chiral perturbation theory. We use the two values of the lattice spacing, several lattice sizes as well as different values of…

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHadronCharm quarkFOS: Physical sciencesLattice QCD2 FLAVORS01 natural sciencesCHIRAL PERTURBATION-THEORYCharm quarkLattice constantHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeTWISTED MASS FERMIONSChiral perturbation theoryWILSON QUARKS0103 physical sciencesddc:530ALGORITHM010306 general physicsSCALEPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFermionLattice QCDSIMULATIONSPseudoscalarHigh Energy Physics - PhenomenologyLattice gauge theoryChiral LagrangiansYANG-MILLS THEORYHigh Energy Physics::ExperimentPHASE-STRUCTUREMESONChiral lagrangiansLight hadronsJournal of High Energy Physics
researchProduct

Dynamical twisted mass fermions with light quarks

2007

We present results of dynamical simulations with 2 flavours of degenerate Wilson twisted mass quarks at maximal twist in the range of pseudo scalar masses from 300 to 550 MeV. The simulations are performed at one value of the lattice spacing a \lesssim 0.1 fm. In order to have O(a) improvement and aiming at small residual cutoff effects, the theory is tuned to maximal twist by requiring the vanishing of the untwisted quark mass. Precise results for the pseudo scalar decay constant and the pseudo scalar mass are confronted with chiral perturbation theory predictions and the low energy constants F, \bar{l}_3 and \bar{l}_4 are evaluated with small statistical errors.

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMONTE-CARLO ALGORITHMCHIRAL PERTURBATION-THEORY; MONTE-CARLO ALGORITHM; GROSS-NEVEU MODEL; YANG-MILLS THEORY; LATTICE QCD; PHASE-STRUCTURE; WILSON QUARKS; HMC ALGORITHM; GAUGE ACTIONS; 2 FLAVORSHigh Energy Physics::LatticeLattice field theoryScalar (mathematics)FOS: Physical sciences2 FLAVORSGAUGE ACTIONS01 natural sciences7. Clean energyCHIRAL PERTURBATION-THEORYLATTICE QCDHigh Energy Physics - LatticeGross–Neveu modelWILSON QUARKS0103 physical sciencesddc:530Twist010306 general physicsPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaGROSS-NEVEU MODELFermionLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciYANG-MILLS THEORYPHASE-STRUCTUREHMC ALGORITHM
researchProduct

Effective Theories for QCD-like at TeV Scale

2014

We study the Effective Field Theory of three QCD-like theories, which can be classified by having quarks in a complex, real or pseudo-real representations of the gauge group. The Lagrangians are written in a very similar way so that the calculations can be done using techniques from Chiral Perturbation Theory (ChPT). We calculated the vacuum-expectation-value, the mass and the decay constant of pseudo-Goldstone Bosons up to next-to-next-to leading order (NNLO) \cite{Bijnens:2009qm}. The various channels of general $n$ flavour meson-meson scattering of the three theories are systematically studied and calculated up to NNLO \cite{Bijnens:2011fm}. We also calculated the vector, axial-vector, s…

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryTechnicolorHigh Energy Physics::LatticeSpontaneous symmetry breakingNuclear TheoryFOS: Physical sciencesTechnicolorChiral Lagrangian01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeGauge group0103 physical sciencesEffective field theory010306 general physicsLattice Gauge Field TheoriesBosonPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologychiral extrapolationSpontaneous Symmetry BreakingHigh Energy Physics - PhenomenologyComposite ModelsHigh Energy Physics::ExperimentNuclear and Particle Physics Proceedings
researchProduct