Search results for "theoretical physics"

showing 10 items of 751 documents

New physics vs new paradigms: distinguishing CPT violation from NSI

2019

Our way of describing Nature is based on local relativistic quantum field theories, and then CPT symmetry, a natural consequence of Lorentz invariance, locality and hermiticity of the Hamiltonian, is one of the few if not the only prediction that all of them share. Therefore, testing CPT invariance does not test a particular model but the whole paradigm. Current and future long baseline experiments will assess the status of CPT in the neutrino sector at an unprecedented level and thus its distinction from similar experimental signatures arising from non-standard interactions is imperative. Whether the whole paradigm is at stake or just the standard model of neutrinos crucially depends on th…

Physics::General PhysicsPhysics and Astronomy (miscellaneous)CPT symmetryPhysics beyond the Standard ModelFOS: Physical scienceslcsh:AstrophysicsLorentz covariance01 natural sciencesPartícules (Física nuclear)High Energy Physics - Experimentsymbols.namesakeTheoretical physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuantum field theory010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsLocalityHigh Energy Physics::PhenomenologyHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentNeutrinoHamiltonian (quantum mechanics)
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Remarks on quantum groups

1991

We give a Poisson-bracket realization of SL q (2) in the phase space ℝ2. We then discuss the physical meaning of such a realization in terms of a modified (regularized) toy model, the nonregularized version of which is due to Klauder. Some general remarks and suggestions are also presented in this Letter.

Poisson bracketTheoretical physicsToy modelQuantum groupPhase spaceComplex systemStatistical and Nonlinear PhysicsMeaning (non-linguistic)QuantumRealization (systems)Mathematical PhysicsMathematicsMathematical physicsLetters in Mathematical Physics
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Use of a running coupling in the NLO calculation of forward hadron production

2018

We address and solve a puzzle raised by a recent calculation [1] of the cross-section for particle production in proton-nucleus collisions to next-to-leading order: the numerical results show an un- reasonably large dependence upon the choice of a prescription for the QCD running coupling, which spoils the predictive power of the calculation. Specifically, the results obtained with a prescription formulated in the transverse coordinate space differ by one to two orders of magnitude from those obtained with a prescription in momentum space. We show that this discrepancy is an artefact of the interplay between the asymptotic freedom of QCD and the Fourier transform from coordinate space to mo…

Position and momentum spaceQCD EVOLUTION01 natural sciencesAsymptotic freedomquantum chromodynamics: correctionhard scatteringHigh Energy Physics - Phenomenology (hep-ph)coupling constant: energy dependencestrong interaction: coupling constantEQUATIONkvanttifysiikkaComputingMilieux_MISCELLANEOUSPhysicsQuantum chromodynamicsQUARKhigher-order: 1nuclear physicssddc:12.39.StHigh Energy Physics - Phenomenology12.38.Bxsymbolsydinfysiikkahadron: forward productionFOS: Physical sciences114 Physical sciencesRENORMALIZATION-GROUP12.38.Cysymbols.namesakeCross section (physics)Theoretical physicsquantum chromodynamics0103 physical sciencessirontarelativistic heavy-ion collisionCoordinate spacenumerical calculations010306 general physicsp nucleus: scatteringcorrection: higher-orderCouplingta114010308 nuclear & particles physics25.75.-qCOLOR GLASS CONDENSATENONLINEAR GLUON EVOLUTIONRenormalization groupFourier transformasymptotic freedom[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical Review D
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Deformed quons and bi-coherent states

2017

We discuss how a q-mutation relation can be deformed replacing a pair of conjugate operators with two other and unrelated operators, as it is done in the construction of pseudo-fermions, pseudo-bosons and truncated pseudo-bosons. This deformation involves interesting mathematical problems and suggests possible applications to pseudo-hermitian quantum mechanics. We construct bi-coherent states associated to $\D$-pseudo-quons, and we show that they share many of their properties with ordinary coherent states. In particular, we find conditions for these states to exist, to be eigenstates of suitable annihilation operators and to give rise to a resolution of the identity. Two examples are discu…

Pseudo-bosonComputer Science::Machine LearningSimilarity (geometry)Mathematical problemGeneral MathematicsFOS: Physical sciencesGeneral Physics and AstronomyComputer Science::Digital Libraries01 natural sciencesPhysics and Astronomy (all)Statistics::Machine LearningTheoretical physicsIdentity (mathematics)Engineering (all)Quon0103 physical sciencesMathematics (all)0101 mathematics010306 general physicsSettore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsMathematical PhysicsPhysicsQuantum PhysicsAnnihilation010102 general mathematicsGeneral EngineeringMathematical Physics (math-ph)Bounded functionComputer Science::Mathematical SoftwareCoherent statesQuantum Physics (quant-ph)Coherent stateResolution (algebra)
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Pseudo-Bosons from Landau Levels

2010

We construct examples of pseudo-bosons in two dimensions arising from the Hamiltonian for the Landau levels. We also prove a no-go result showing that non-linear combinations of bosonic creation and annihilation operators cannot give rise to pseudo-bosons.

Pseudo-bosonFOS: Physical sciencesnon-hermitian HamiltoniansTheoretical physicssymbols.namesakeQuantum mechanicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsBosonPhysicsCondensed Matter::Quantum GasesQuantum Physicslcsh:MathematicsHigh Energy Physics::PhenomenologyCreation and annihilation operatorsAnalysiLandau quantizationMathematical Physics (math-ph)lcsh:QA1-939Non-hermitian HamiltonianLandau theorysymbolspseudo-bosonsGeometry and TopologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Analysis
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Extended pseudo-fermions from non commutative bosons

2013

We consider some modifications of the two dimensional canonical commutation relations, leading to {\em non commutative bosons} and we show how biorthogonal bases of the Hilbert space of the system can be obtained out of them. Our construction extends those recently introduced by one of us (FB), modifying the canonical anticommutation relations. We also briefly discuss how bicoherent states, producing a resolution of the identity, can be defined.

Pure mathematicsFOS: Physical sciences01 natural sciencessymbols.namesakeIdentity (mathematics)Theoretical physicsMeasurement theory0103 physical sciences010306 general physicsSettore MAT/07 - Fisica MatematicaCommutative propertyMathematical PhysicsComputer Science::DatabasesComputingMilieux_MISCELLANEOUSMathematicsBoson[PHYS]Physics [physics]010308 nuclear & particles physicsHilbert spaceStatistical and Nonlinear PhysicsFermionMathematical Physics (math-ph)16. Peace & justiceBiorthogonal systemsymbolspseudo-bosons[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Resolution (algebra)
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Structure of the space of reducible connections for Yang-Mills theories

1990

Abstract The geometrical structure of the gauge equivalence classes of reducible connections are investigated. The general procedure to determine the set of orbit types (strata) generated by the action of the gauge group on the space of gauge potentials is given. In the so obtained classification, a stratum, containing generically certain reducible connections, corresponds to a class of isomorphic subbundles given by an orbit of the structure and gauge group. The structure of every stratum is completely clarified. A nonmain stratum can be understood in terms of the main stratum corresponding to a stratification at the level of a subbundle.

Pure mathematicsMathematics::Dynamical SystemsMathematical analysisStructure (category theory)General Physics and AstronomyYang–Mills existence and mass gapGauge (firearms)Space (mathematics)Mathematics::Algebraic GeometryGauge groupSubbundleGeometry and TopologyOrbit (control theory)Mathematics::Symplectic GeometryMathematical PhysicsGeneral Theoretical PhysicsMathematicsStratum
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The algebraic structure of cohomological field theory

1993

Abstract The algebraic foundation of cohomological field theory is presented. It is shown that these theories are based upon realizations of an algebra which contains operators for both BRST and vector supersymmetry. Through a localization of this algebra, we construct a theory of cohomological gravity in arbitrary dimensions. The observables in the theory are polynomial, but generally non-local operators, and have a natural interpretation in terms of a universal bundle for gravity. As such, their correlation functions correspond to cohomology classes on moduli spaces of Riemannian connections. In this uniformization approach, different moduli spaces are obtained by introducing curvature si…

Pure mathematicsTopological quantum field theoryDifferential formAlgebraic structureGeneral Physics and AstronomyCodimensionModuli spaceAlgebraOperator algebraQuantum gravityGeometry and TopologyOperator product expansionMathematical PhysicsGeneral Theoretical PhysicsMathematics
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Different operational meanings of continuous variable Gaussian entanglement criteria and Bell inequalities

2014

Entanglement, one of the most intriguing aspects of quantum mechanics, marks itself into different features of quantum states. For this reason different criteria can be used for verifying entanglement. In this paper we review some of the entanglement criteria casted for continuous variable states and link them to peculiar aspects of the original debate on the famous EPR paradox. Moreover, we give a handy expression for valuating Bell-type non-locality on Gaussian states. We also present the experimental measurement of a particular realization of the Bell operator over continuous variable entangled states produced by a sub-threshold type-II OPO.

Quantum PhysicsOperator (physics)GaussianFOS: Physical sciencesQuantum entanglementQuantum PhysicsCondensed Matter PhysicsIndustrial and Manufacturing EngineeringAtomic and Molecular Physics and OpticsExpression (mathematics)symbols.namesakeTheoretical physicsQuantum statesymbolsEPR paradoxLink (knot theory)Quantum Physics (quant-ph)InstrumentationRealization (probability)Mathematics
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2p x-ray absorption spectroscopy of 3d transition metal systems

2021

Abstract This review provides an overview of the different methods and computer codes that are used to interpret 2p x-ray absorption spectra of 3d transition metal ions. We first introduce the basic parameters and give an overview of the methods used. We start with the semi-empirical multiplet codes and compare the different codes that are available. A special chapter is devoted to the user friendly interfaces that have been written on the basis of these codes. Next we discuss the first principle codes based on band structure, including a chapter on Density Functional theory based approaches. We also give an overview of the first-principle multiplet codes that start from a cluster calculati…

Quantum chemistry calculationsComputer science02 engineering and technology01 natural sciencesTheoretical physicsAtomic and Molecular Physics0103 physical sciencesTaverneElectronicCluster (physics)Optical and Magnetic MaterialsPhysical and Theoretical ChemistryWave functionElectronic band structureMultipletComputingMilieux_MISCELLANEOUSDensity Functional TheorySpectroscopyX-ray absorption spectroscopy; Density Functional Theory; Quantum chemistry calculationsX-ray absorption spectroscopyRadiation010304 chemical physicsBasis (linear algebra)X-ray absorption spectroscopy021001 nanoscience & nanotechnologyCondensed Matter PhysicsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materials[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]First principleDensity functional theoryand Optics0210 nano-technologyDen kondenserade materiens fysik
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