Search results for "High Energy Physics - Lattice"

showing 10 items of 466 documents

Non Perturbative One Gluon Exchange Potential from Dyson-Schwinger Equations

2012

Recent progress in the solution of Dyson-Schwinger equations of QCD allows for a non perturbative evaluation of the One Gluon Exchange (OGE) interaction. We calculate the interquark static potential for heavy mesons by assuming that it is given by this OGE interaction and we apply it to the description of charmonium.

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::ExperimentNuclear Experiment
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QCD and Strongly Coupled Gauge Theories: Challenges and Perspectives

2014

We dedicate this document to the memory of Mikhail Polikarpov, who passed away in July 2013. Misha worked with us for decades as a convener of the “Confinement” section of the Quark Confinement and Hadron Spectrum Series. He guided and expanded the scientific discussion of that topic, inspiring and under taking new research avenues. From its initial conception, he supported the enterprise of this document and organized Sect. 8, writing the part on confinement himself. He attracted the XIth Conference on Quark Confinement and the Hadron Spectrum to St. Petersburg (September 8-12, 2014; see http://phys.spbu.ru/confxi.html). His warm and kind personality, his high sense of humor, his ideas in …

High Energy Physics - TheoryEFFECTIVE-FIELD-THEORYNuclear TheoryPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelReviewHEAVY-ION COLLISIONSnucl-ex7. Clean energyCosmologyHigh Energy Physics - ExperimentQUARK-GLUON PLASMADEEP-INELASTIC SCATTERINGHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Gauge theoryNuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]hep-thHigh Energy Physics - Lattice (hep-lat)hep-phddc:High Energy Physics - PhenomenologyYANG-MILLS THEORYastro-ph.COAstrophysics - Cosmology and Nongalactic AstrophysicsPB-PB COLLISIONSParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)nucl-th[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]530 PhysicsStrong interactionComplex systemFOS: Physical scienceshep-lat[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]CHIRAL PERTURBATION-THEORY114 Physical sciencesELECTRIC-DIPOLE MOMENTNuclear Theory (nucl-th)Theoretical physicsHigh Energy Physics - Latticeddc:530Engineering (miscellaneous)Particle Physics - Phenomenologyhep-ex[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]NUCLEUS-NUCLEUS COLLISIONSPerspective (graphical)FísicaRADIATIVE ENERGY-LOSSFlow (mathematics)High Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]European Physical Journal C
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Corrections to the ${\bf SU(3)\times SU(3)}$ Gell-Mann-Oakes-Renner relation and chiral couplings $L^r_8$ and $H^r_2$

2012

Next to leading order corrections to the $SU(3) \times SU(3)$ Gell-Mann-Oakes-Renner relation (GMOR) are obtained using weighted QCD Finite Energy Sum Rules (FESR) involving the pseudoscalar current correlator. Two types of integration kernels in the FESR are used to suppress the contribution of the kaon radial excitations to the hadronic spectral function, one with local and the other with global constraints. The result for the pseudoscalar current correlator at zero momentum is $\psi_5(0) = (2.8 \pm 0.3) \times 10^{-3} GeV^{4}$, leading to the chiral corrections to GMOR: $\delta_K = (55 \pm 5)%$. The resulting uncertainties are mostly due to variations in the upper limit of integration in…

High Energy Physics - TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciences
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Transport coefficients from in medium quarkonium dynamics

2019

The in medium dynamics of heavy particles are governed by transport coefficients. The heavy quark momentum diffusion coefficient, $\kappa$, is an object of special interest in the literature, but one which has proven notoriously difficult to estimate, despite the fact that it has been computed by weak-coupling methods at next-to-leading order accuracy, and by lattice simulations of the pure SU(3) gauge theory. Another coefficient, $\gamma$, has been recently identified. It can be understood as the dispersive counterpart of $\kappa$. Little is known about $\gamma$. Both $\kappa$ and $\gamma$ are, however, of foremost importance in heavy quarkonium physics as they entirely determine the in an…

High Energy Physics - TheoryNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Nuclear TheoryHigh Energy Physics - Theory (hep-th)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical scienceshiukkasfysiikka
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Heavy quarkonium suppression in a fireball

2018

We perform a comprehensive study of the time evolution of heavy-quarkonium states in an expanding hot QCD medium by implementing effective field theory techniques in the framework of open quantum systems. The formalism incorporates quarkonium production and its subsequent evolution in the fireball including quarkonium dissociation and recombination. We consider a fireball with a local temperature that is much smaller than the inverse size of the quarkonium and much larger than its binding energy. The calculation is performed at an accuracy that is leading-order in the heavy-quark density expansion and next-to-leading order in the multipole expansion. Within this accuracy, for a smooth varia…

High Energy Physics - TheoryNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesquarkoniaComputer Science::Digital LibrariesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentNuclear Experimentrelativistic heavy-ion collisions
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Heavy quarkonium: progress, puzzles, and opportunities

2011

A golden age for heavy quarkonium physics dawned a decade ago, initiated by the confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of related experimental activity. The early years of this period were chronicled in the Quarkonium Working Group (QWG) CERN Yellow Report (YR) in 2004, which presented a comprehensive review of the status of the field at that time and provided specific recommendations for further progress. However, the broad spectrum of subsequent breakthroughs, surprises, and continuing puzzles could only be partially anticipated. Since the release of the YR, the BESII program concluded only to give birth to BESIII; the $B$-factories and CLEO-c flo…

High Energy Physics - TheoryNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeTevatronB-C MESON; QCD SUM-RULES; NUCLEUS COLLISIONSAtomic01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Broad spectrumHigh Energy Physics - Phenomenology (hep-ph)Particle and Plasma Physicseffective field theoryBatavia TEVATRON CollNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentBrookhaven RHIC CollQuantum chromodynamicsPhysicsQuantum PhysicsLarge Hadron ColliderHigh Energy Physics - Lattice (hep-lat)lattice field theoryHERAQuarkoniumNuclear & Particles PhysicsCLEOB-C MESONHigh Energy Physics - PhenomenologyDESY HERA Stordecay [quarkonium]Jefferson LabParticle physicsFOS: Physical sciencesnonrelativistic [quantum chromodynamics]DeconfinementB-factoryNuclear Theory (nucl-th)High Energy Physics - Latticescattering [heavy ion]QCD SUM-RULES0103 physical sciencesNuclearddc:530010306 general physicsEngineering (miscellaneous)Particle Physics - Phenomenologyproduction [quarkonium]BES010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyplasma [quark gluon]FísicaMoleculartetraquarkHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]hadron spectroscopy [meson]hadron spectroscopy [quarkonium]High Energy Physics::Experimentheavy [quarkonium]NUCLEUS COLLISIONSThe European Physical Journal C
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Constraints on Conformal Windows from Holographic Duals

2009

We analyze a beta function with the analytic form of Novikov-Shifman-Vainshtein-Zakharov result in the five dimensional gravity-dilaton environment. We show how dilaton inherits poles and fixed points of such beta function through the zeros and points of extremum in its potential. Super Yang-Mills and supersymmetric QCD are studied in detail and Seiberg's electric-magnetic duality in the dilaton potential is explicitly demonstrated. Non-supersymmetric proposals of similar functional form are tested and new insights into the conformal window as well as determinations of scheme-independent value of the anomalous dimension at the fixed point are presented.

High Energy Physics - TheoryNuclear and High Energy PhysicsGeneral Physics and AstronomyDuality (optimization)FOS: Physical sciencesConformal mapFixed point01 natural sciencesTheoretical physicssymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGauge theory010306 general physicsBeta functionPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Astronomy and AstrophysicsAdS/CFT correspondenceHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)symbolsSeiberg dualityDilaton
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A non-perturbative study of massive gauge theories

2013

We consider a non-perturbative formulation of an SU(2) massive gauge theory on a space-time lattice, which is also a discretised gauged non-linear chiral model. The lattice model is shown to have an exactly conserved global SU(2) symmetry. If a scaling region for the lattice model exists and the lightest degrees of freedom are spin one vector particles with the same quantum numbers as the conserved current, we argue that the most general effective theory describing their low-energy dynamics must be a massive gauge theory. We present results of a exploratory numerical simulation of the model and find indications for the presence of a scaling region where both a triplet vector and a scalar re…

High Energy Physics - TheoryNuclear and High Energy PhysicsHiggs PhysicsHigh Energy Physics::Latticehep-latFOS: Physical sciences01 natural sciencesTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)0103 physical sciencesEffective field theoryGauge theory010306 general physicsConserved currentScalingLattice Gauge Field TheoriesPhysics010308 nuclear & particles physicshep-thHigh Energy Physics - Lattice (hep-lat)Físicahep-phQuantum numberHigh Energy Physics - PhenomenologyChiral modelHigh Energy Physics - Theory (hep-th)Gauge SymmetryNon-perturbativeSigma Models
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On the zero crossing of the three-gluon vertex

2016

We report on new results on the infrared behaviour of the three-gluon vertex in quenched Quantum Chormodynamics, obtained from large-volume lattice simulations. The main focus of our study is the appearance of the characteristic infrared feature known as 'zero crossing', the origin of which is intimately connected with the nonperturbative masslessness of the Faddeev-Popov ghost. The appearance of this effect is clearly visible in one of the two kinematic configurations analyzed, and its theoretical origin is discussed in the framework of Schwinger-Dyson equations. The effective coupling in the momentum subtraction scheme that corresponds to the three-gluon vertex is constructed, revealing t…

High Energy Physics - TheoryNuclear and High Energy PhysicsLattice simulationsInfraredHigh Energy Physics::LatticeFOS: Physical sciencesThree-gluon vertexKinematicsnonperturbative01 natural sciencesSchwinger–Dyson equations[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQuantum mechanicsLattice (order)0103 physical sciencesddc:530Exact locationquantum chromodynamics: quenching010306 general physicsMathematical physicslatticeQuantum chromodynamicsPhysicsZero crossing010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat][PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)[ PHYS.HLAT ] Physics [physics]/High Energy Physics - Lattice [hep-lat]gluon: vertexcrossingZero crossingghostlcsh:QC1-999GluonDyson-Schwinger equationHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]infrared[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]lcsh:Physics
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Derivation of spontaneously broken gauge symmetry from the consistency of effective field theory II: Scalar field self-interactions and the electroma…

2019

We extend our study of deriving the local gauge invariance with spontaneous symmetry breaking in the context of an effective field theory by considering self-interactions of the scalar field and inclusion of the electromagnetic interaction. By analyzing renormalizability and the scale separation conditions of three-, four- and five-point vertex functions of the scalar field, we fix the two couplings of the scalar field self-interactions of the leading order Lagrangian. Next we add the electromagnetic interaction and derive conditions relating the magnetic moment of the charged vector boson to its charge and the masses of the charged and neutral massive vector bosons to each other and the tw…

High Energy Physics - TheoryNuclear and High Energy PhysicsNuclear TheorySpontaneous symmetry breakingFOS: Physical sciences01 natural sciencesStandard ModelVector bosonNuclear Theory (nucl-th)Theoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryddc:530Gauge theory010306 general physicsGauge symmetryPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics - Lattice (hep-lat)lcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Scalar fieldlcsh:Physics
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