Search results for "RENORMALIZATION"

showing 10 items of 470 documents

The one loop gluon emission light cone wave function

2017

Light cone perturbation theory has become an essential tool to calculate cross sections for various small-$x$ dilute-dense processes such as deep inelastic scattering and forward proton-proton and proton-nucleus collisions. Here we set out to do one loop calculations in an explicit helicity basis in the four dimensional helicity scheme. As a first process we calculate light cone wave function for one gluon emission to one-loop order in Hamiltonian perturbation theory on the light front. We regulate ultraviolet divergences with transverse dimensional regularization and soft divergences with using a cut-off on longitudinal momentum. We show that when all the renormalization constants are comb…

COLLISIONSParticle physicsNuclear TheoryRENORMALIZATIONQUANTUM ELECTRODYNAMICSGeneral Physics and AstronomyFOS: Physical sciencesloop calculations114 Physical sciences01 natural scienceslight cone perturbation theoryRenormalizationNuclear Theory (nucl-th)Dimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)INFINITE-MOMENTUMLight cone0103 physical sciencesSCATTERINGHelicity basis010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsCoupling constantgluon emissionta114010308 nuclear & particles physicsCOLOR GLASS CONDENSATEDeep inelastic scatteringFRONT QCDHelicityEVOLUTIONHigh Energy Physics - PhenomenologyCHROMODYNAMICSQuantum electrodynamicsgluon saturation
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Monte Carlo Simulation of Alloy Phase Diagrams and Short-Range Order

1986

As a prototype model for order-disorder phenomena in binary alloys, a face-centered cubic lattice is considered,the sites of which can be taken by either A-atoms or B-atoms, assuming pair-wise interactions between nearest (J) and next nearest neighbours (J). The phase diagram is constructed from Monte Carlo calculations. Some technical aspects essential for the success of such calculations are briefly mentioned (use of grand-canonical rather than canonical ensemble, how to obtain the free energy needed to locate first-order phase transitions, etc.). It is shown that the topology of the phase diagram changes when the ratio R = Jnnn/Jnn is varied, and this behaviour is discussed in the contex…

Canonical ensemblePhase transitionMean field theoryLattice (order)Monte Carlo methodBinary numberStatistical physicsRenormalization groupMathematicsPhase diagram
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Chiral expansion of the nucleon mass to order q^6

2006

We present the results of a complete two-loop calculation at order q^6 of the nucleon mass in manifestly Lorentz-invariant chiral perturbation theory. The renormalization is performed using the reformulated infrared renormalization, which allows for the treatment of two-loop integrals while preserving all relevant symmetries, in particular chiral symmetry.

Chiral anomalyPhysicsNuclear and High Energy PhysicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLorentz covarianceRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQuantum mechanicsHomogeneous spacePerturbation theoryChiral symmetry breakingNucleonMathematical physics
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Rigidity transition in two-dimensional random fiber networks

2000

Rigidity percolation is analyzed in two-dimensional random fibrous networks. The model consists of central forces between the adjacent crossing points of the fibers. Two strategies are used to incorporate rigidity: adding extra constraints between second-nearest crossing points with a probability p(sn), and "welding" individual crossing points by adding there four additional constraints with a probability p(weld), and thus fixing the angles between the fibers. These additional constraints will make the model rigid at a critical probability p(sn)=p(sn)(c) and p(weld)=p(weld)(c), respectively. Accurate estimates are given for the transition thresholds and for some of the associated critical e…

CombinatoricsRigidity (electromagnetism)Central forcelawMathematical analysisWeldingRenormalization groupCritical probabilityCritical exponentMathematicslaw.inventionPhysical Review E
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Rigidity of random networks of stiff fibers in the low-density limit.

2001

Rigidity percolation is analyzed in two-dimensional random networks of stiff fibers. As fibers are randomly added to the system there exists a density threshold ${q=q}_{\mathrm{min}}$ above which a rigid stress-bearing percolation cluster appears. This threshold is found to be above the connectivity percolation threshold ${q=q}_{c}$ such that ${q}_{\mathrm{min}}=(1.1698\ifmmode\pm\else\textpm\fi{}{0.0004)q}_{c}.$ The transition is found to be continuous, and in the universality class of the two-dimensional central-force rigidity percolation on lattices. At percolation threshold the rigid backbone of the percolating cluster was found to break into rigid clusters, whose number diverges in the…

CombinatoricsRigidity (electromagnetism)Condensed matter physicsAverage sizeCluster (physics)ExponentLow densityPercolation thresholdRenormalization groupScalingMathematicsPhysical review. E, Statistical, nonlinear, and soft matter physics
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An example of cancellation of infinities in the star-quantization of fields

1993

Within the *-quantization framework, it is shown how to remove some of the divergences occurring in theλo 2 4 -theory by introducing aλ-dependent *-product cohomologically equivalent to the normal *-product.

Complex systemStatistical and Nonlinear PhysicsTopologyRenormalizationsymbols.namesakeTheoretical physicsSingularityHamiltonian formalismRegularization (physics)symbolsQuantum field theoryHamiltonian (quantum mechanics)Mathematical PhysicsMathematicsLetters in Mathematical Physics
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Parallelization strategies for density matrix renormalization group algorithms on shared-memory systems

2003

Shared-memory parallelization (SMP) strategies for density matrix renormalization group (DMRG) algorithms enable the treatment of complex systems in solid state physics. We present two different approaches by which parallelization of the standard DMRG algorithm can be accomplished in an efficient way. The methods are illustrated with DMRG calculations of the two-dimensional Hubbard model and the one-dimensional Holstein-Hubbard model on contemporary SMP architectures. The parallelized code shows good scalability up to at least eight processors and allows us to solve problems which exceed the capability of sequential DMRG calculations.

Condensed Matter::Quantum GasesDensity matrixNumerical AnalysisStrongly Correlated Electrons (cond-mat.str-el)Physics and Astronomy (miscellaneous)Hubbard modelApplied MathematicsDensity matrix renormalization groupComplex systemFOS: Physical sciencesParallel computingRenormalization groupComputer Science ApplicationsCondensed Matter - Strongly Correlated ElectronsComputational MathematicsShared memoryModeling and SimulationScalabilityCode (cryptography)Condensed Matter::Strongly Correlated ElectronsAlgorithmMathematicsJournal of Computational Physics
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Fulde-Ferrell-Larkin-Ovchinnikov pairing in one-dimensional optical lattices

2008

Spin-polarized attractive Fermi gases in one-dimensional (1D) optical lattices are expected to be remarkably good candidates for the observation of the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) phase. We model these systems with an attractive Hubbard model with population imbalance. By means of the density-matrix renormalization-group method, we compute the pairing correlations as well as the static spin and charge structure factors in the whole range from weak to strong coupling. We demonstrate that pairing correlations exhibit quasi-long-range order and oscillations at the wave number expected from the FFLO theory. However, we also show by numerically computing the mixed spin-charge static …

Condensed Matter::Quantum GasesDensity matrixPhysicseducation.field_of_studyHubbard modelCondensed matter physicsLattice field theoryPopulationCondensed Matter Physics01 natural sciences010305 fluids & plasmasElectronic Optical and Magnetic MaterialsATOMSRenormalizationPairingQuantum mechanicsTONKS-GIRARDEAU GAS0103 physical sciencesTHEOREMATTRACTIVE HUBBARD-MODEL010306 general physicsFermi gasStructure factoreducationPhysical Review B
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Supersolid-superfluid phase separation in the extended Bose-Hubbard model

2021

Recent studies have suggested a new phase in the extended Bose-Hubbard model in one dimension at integer filling [1,2]. In this work, we show that this new phase is phase-separated into a supersolid and superfluid part, generated by mechanical instability. Numerical simulations are performed by means of the density matrix renormalization group algorithm in terms of matrix product states. In the phase-separated phase and the adjacent homogeneous superfluid and supersolid phases, we find peculiar spatial patterns in the entanglement spectrum and string-order correlation functions and show that they survive in the thermodynamic limit. In particular, we demonstrate that the elementary excitatio…

Condensed Matter::Quantum GasesPhysicsDensity matrixQuantum PhysicsHubbard modelSuperfluïdesaDensity matrix renormalization groupCondensed matterFOS: Physical sciencesBose–Hubbard modelMatèria condensada01 natural sciences010305 fluids & plasmasSuperfluiditySupersolidQuantum Gases (cond-mat.quant-gas)SuperfluidityLuttinger liquidQuantum mechanics0103 physical sciencesThermodynamic limitCondensed Matter - Quantum GasesQuantum Physics (quant-ph)010306 general physicsLuttinger parameterPhysical Review B
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Exact Numerical Treatment of Finite Quantum Systems Using Leading-Edge Supercomputers

2005

Using exact diagonalization and density matrix renormalization group techniques a finite-size scaling study in the context of the Peierls-insulator Mott-insulator transition is presented. Program implementation on modern supercomputers and performance aspects are discussed.

Condensed Matter::Quantum GasesPhysicsLeading edgeDensity matrix renormalization groupCondensed Matter::Strongly Correlated ElectronsContext (language use)Statistical physicsScalingQuantum
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