Search results for "Mathematica"

showing 10 items of 7971 documents

Quantum deformations of singletons and of free zero-mass fields

1993

We consider quantum deformations of the real symplectic (or anti-De Sitter) algebra sp(4), ℝ ≅ spin(3, 2) and of its singleton and (4-dimensional) zero-mass representations. For q a root of −1, these representations admit finite-dimensional unitary subrepresentations. It is pointed out that Uq(sp(4, ℝ)), unlike Uq(su(2, 2)), contains Uq(sl2) as a quantum subalgebra.

Quantum mechanicsSubalgebraGeneral Physics and AstronomyQuantum algebraLie groupQuantum field theoryMathematics::Representation TheorySL2(R)QuantumMathematicsSpin-½Symplectic geometryMathematical physicsFoundations of Physics
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When Casimir meets Kibble–Zurek

2012

Verification of the dynamical Casimir effect (DCE) in optical systems is still elusive due to the very demanding requirements for its experimental implementation. This typically requires very fast changes in the boundary conditions of the problem. We show that an ensemble of two-level atoms collectively coupled to the electromagnetic field of a cavity, driven at low frequencies and close to a quantum phase transition, stimulates the production of photons from the vacuum. This paves the way for an effective simulation of the DCE through a mechanism that has recently found experimental demonstration. The spectral properties of the emitted radiation reflect the critical nature of the system an…

Quantum phase transitionElectromagnetic fieldPhysicsPhotonCritical phenomenadynamical casimir effect cavity QEDCondensed Matter PhysicsAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaCasimir effectQuantum mechanicsAtomBoundary value problemMathematical PhysicsBoson
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Dynamical bifurcation as a semiclassical counterpart of a quantum phase transition

2011

We illustrate how dynamical transitions in nonlinear semiclassical models can be recognized as phase transitions in the corresponding -- inherently linear -- quantum model, where, in a Statistical Mechanics framework, the thermodynamic limit is realized by letting the particle population go to infinity at fixed size. We focus on lattice bosons described by the Bose-Hubbard (BH) model and Discrete Self-Trapping (DST) equations at the quantum and semiclassical level, respectively. After showing that the gaussianity of the quantum ground states is broken at the phase transition, we evaluate finite populations effects introducing a suitable scaling hypothesis; we work out the exact value of the…

Quantum phase transitionPhysicsQuantum Physicseducation.field_of_studyPhase transitionStatistical Mechanics (cond-mat.stat-mech)PopulationFOS: Physical sciencesSemiclassical physicsStatistical mechanicsAtomic and Molecular Physics and OpticsQuantum mechanicsThermodynamic limitQuantum Physics (quant-ph)educationCritical exponentQuantumCondensed Matter - Statistical MechanicsMathematical physicsPhysical Review A
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Probing Quantum Frustrated Systems via Factorization of the Ground State

2009

The existence of definite orders in frustrated quantum systems is related rigorously to the occurrence of fully factorized ground states below a threshold value of the frustration. Ground-state separability thus provides a natural measure of frustration: strongly frustrated systems are those that cannot accommodate for classical-like solutions. The exact form of the factorized ground states and the critical frustration are determined for various classes of nonexactly solvable spin models with different spatial ranges of the interactions. For weak frustration, the existence of disentangling transitions determines the range of applicability of mean-field descriptions in biological and physica…

Quantum phase transitionfrustrationmedia_common.quotation_subjectGeneral Physics and AstronomyFrustrationFOS: Physical sciences01 natural sciences010305 fluids & plasmasFactorizationQuantum mechanics0103 physical sciencesStatistical physicsPhysics - Biological Physics010306 general physicsQuantumCondensed Matter - Statistical MechanicsMathematical Physicsmedia_commonSpin-½PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Mathematical Physics (math-ph)Closed and exact differential formsCondensed Matter - Other Condensed MatterRange (mathematics)Biological Physics (physics.bio-ph)Condensed Matter::Strongly Correlated ElectronsGround stateQuantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)
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Flavour Conservation in Two Higgs Doublet Models

2018

In extensions of the Standard Model with two Higgs doublets, flavour changing Yukawa couplings of the neutral scalars may be present at tree level. In this work we consider the most general scenario in which those flavour changing couplings are absent. We re-analyse the conditions that the Yukawa coupling matrices must obey for such \emph{general flavour conservation} (gFC), and study the one loop renormalisation group evolution of such conditions in both the quark and lepton sectors. We show that gFC in the leptonic sector is one loop stable under the Renormalization Group Evolution (RGE) and in the quark sector we present some new Cabibbo like solution also one loop RGE stable. At a pheno…

QuarkCouplingPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesRenormalization group01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLepton
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Renormalization and Scale Evolution of the Soft-Quark Soft Function

2020

Soft functions defined in terms of matrix elements of soft fields dressed by Wilson lines are central components of factorization theorems for cross sections and decay rates in collider and heavy-quark physics. While in many cases the relevant soft functions are defined in terms of gluon operators, at subleading order in power counting soft functions containing quark fields appear. We present a detailed discussion of the properties of the soft-quark soft function consisting of a quark propagator dressed by two finite-length Wilson lines connecting at one point. This function enters in the factorization theorem for the Higgs-boson decay amplitude of the $h\to\gamma\gamma$ process mediated by…

QuarkHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeFOS: Physical sciencesPosition and momentum spaceRenormalizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)FactorizationPerturbative QCDRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. RadioactivityResummationMathematical physicsPhysicsHigh Energy Physics::PhenomenologyPropagatorEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Weierstrass factorization theoremsymbolslcsh:QC770-798High Energy Physics::ExperimentResummation
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Two-current correlations in the pion in the Nambu and Jona-Lasinio model

2020

We present an analysis of two-current correlations for the pion in the Nambu--Jona-Lasinio model, with Pauli--Villars regularization. We provide explicit expressions in momentum space for two-current correlations corresponding to the zeroth component of the vector Dirac bilinear in the quark vertices, which has been evaluated on the lattice. The numerical results show a remarkable qualitative agreement with recent lattice data. The factorization approximation into one-body currents is discussed.

QuarkNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeNuclear TheoryDirac (software)FOS: Physical scienceslcsh:AstrophysicsPosition and momentum spaceParton01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)PionFactorizationlcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Mathematical physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyLattice (module)Regularization (physics)lcsh:QC770-798The European Physical Journal C
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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
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Pentaquarks with anticharm or beauty revisited

2019

We use a constituent model to analyze the stability of pentaquark $\bar Q qqqq$ configurations with a heavy antiquark $\bar c$ or $\bar b$, and four light quarks $uuds$, $ddsu$ or $ssud$. The interplay between chromoelectric and chromomagnetic effects is not favorable, and, as a consequence, no bound state is found below the lowest dissociation threshold.

QuarkNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesdissociation01 natural sciencesDissociation (chemistry)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateInteracción entre cromoeléctico22 Física010306 general physicsconstituentpentaquarkPhysics010308 nuclear & particles physicschromoelectricstabilitymathematical methods: variationalEfectos cromomagnéticoslcsh:QC1-999Pentaquarkanti-charmConfiguraciones pentaquark QHigh Energy Physics - Phenomenologychromomagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]lcsh:Physics
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Classification of the hadronic decays of the Z$^0$ into b and c quark pairs using a neural network

1992

A classifier based on a feed-forward neural network has been used for separating a sample of about 123 500 selected hadronic decays of the Z 0 , collected by DELPHI during 1991, into three classes according to the flavour of the original quark pair: u u +d d +s s (unresolved), c c and b b . The classification has been used to compute the partial widths of the Z 0 into b and c quark pairs. This gave Γ c c /Γ h = 0.151 ± 0.008 ( stat. ) ± 0.041 ( syst. ) , Γ b b /Γ h = 0.232±0.005 ( stat. )±0.017 ( syst. ) .

QuarkNuclear and High Energy PhysicsParticle physicsLUND MONTE-CARLO; HEAVY FLAVOR PRODUCTION; JET FRAGMENTATION; PHYSICS; BOSONHEAVY FLAVOR PRODUCTIONLUND MONTE-CARLOElectron–positron annihilationFlavourHadronMathematicsofComputing_GENERALComputer Science::Digital Libraries01 natural sciencesJET FRAGMENTATIONCharm quarkPHYSICS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPhysicsArtificial neural network010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTheoryofComputation_GENERALBOSONMathMLComputer Science::Mathematical SoftwareHigh Energy Physics::ExperimentFísica nuclearClassifier (UML)Particle Physics - Experiment
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