Search results for "model [interaction]"

showing 10 items of 1495 documents

Mass of astrophysically relevantCl31and the breakdown of the isobaric multiplet mass equation

2016

The mass of $^{31}\mathrm{Cl}$ has been measured with the JYFLTRAP double-Penning-trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility. The determined mass-excess value, $\ensuremath{-}7034.7(34)$ keV, is 15 times more precise than in the Atomic Mass Evaluation 2012. The quadratic form of the isobaric multiplet mass equation for the $T=3/2$ quartet at $A=31$ fails $({\ensuremath{\chi}}_{n}^{2}=11.6)$ and a nonzero cubic term, $d=\ensuremath{-}3.5(11)$ keV, is obtained when the new mass value is adopted. $^{31}\mathrm{Cl}$ has been found to be less proton-bound, with a proton separation energy of ${S}_{p}=264.6(34)$ keV. Energies for the excited states in $^{31…

PhysicsProton010308 nuclear & particles physicsQuadratic form (statistics)Type (model theory)7. Clean energy01 natural sciencesAtomic massNuclear physicsMass formulaPhotodisintegration0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsMultipletEnergy (signal processing)Physical Review C
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Oscillatory Solutions of Boundary Value Problems

2016

We consider boundary value problems of the form $$\displaystyle\begin{array}{rcl} & x'' = f(t,x,x'), & {}\\ & x(a) = A,\quad x(b) = B,& {}\\ \end{array}$$ assuming that f is continuous together with f x and fx′. We study also equations in a quasi-linear form $$\displaystyle{x'' + p(t)x' + q(t)x = F(t,x,x').}$$ Introducing types of solutions of boundary value problems as an oscillatory type of the respective equation of variations, we show that for a solution of definite type, the problem can be reformulated in a quasi-linear form. Resonant problems are considered separately. Any resonant problem that has no solutions of indefinite type is in fact nonresonant. The ways of how to detect solut…

PhysicsPure mathematicsBoundary value problemType (model theory)Dynamical system (definition)
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A direct method to find solutions of some type of coupled Korteweg-de Vries equations using hyperelliptic functions of genus two

2008

Abstract We suggest how one can obtain exact solutions of some type of coupled Korteweg–de Vries equations by means of hyperelliptic functions of genus two.

PhysicsPure mathematicsPartial differential equationDirect methodMathematics::Analysis of PDEsGeneral Physics and AstronomyType (model theory)Nonlinear systemMathematics::Algebraic GeometryNonlinear Sciences::Exactly Solvable and Integrable SystemsGenus (mathematics)Nonlinear Sciences::Pattern Formation and SolitonsHyperelliptic curveComputer Science::Databases
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Multiparticle breathers for a chain with double-quadratic on-site potential

1999

We investigate the existence and properties of multiparticle breathers for a one-dimensional model with harmonic nearest neighbor interactions where a group of r particles $(r=1,2,3,\dots{})$ perform interwell oscillations between both wells of a double-quadratic on-site potiential. We find two types of such breathers. For the first type the breather frequency $\ensuremath{\Omega}$ is within the single-particle oscillator spectrum, and the ``residence'' time of each breather particle in the left and right well is about the same. For the second breather $\ensuremath{\Omega}$ is below that spectrum, and the ratio ${\ensuremath{\tau}}_{L}/{\ensuremath{\tau}}_{R}$ of the residence time in the l…

PhysicsQuadratic equationGroup (mathematics)BreatherQuantum mechanicsSpectrum (functional analysis)Zero (complex analysis)Type (model theory)Nonlinear Sciences::Pattern Formation and SolitonsOmegak-nearest neighbors algorithmPhysical Review E
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Susy for non-Hermitian Hamiltonians, with a view to coherent states

2020

We propose an extended version of supersymmetric quantum mechanics which can be useful if the Hamiltonian of the physical system under investigation is not Hermitian. The method is based on the use of two, in general different, superpotentials. Bi-coherent states of the Gazeau-Klauder type are constructed and their properties are analyzed. Some examples are also discussed, including an application to the Black-Scholes equation, one of the most important equations in Finance.

PhysicsQuantum Physics010308 nuclear & particles physicsPhysical systemFOS: Physical sciencesSupersymmetic quantum mechanics Ladder operators Non self-adjoint hamiltonian Gazeau-Klauder coherent states 81SxxSupersymmetryMathematical Physics (math-ph)Type (model theory)01 natural sciencesHermitian matrixsymbols.namesakeTheoretical physicsLadder operator0103 physical sciencessymbolsCoherent statesGeometry and TopologySupersymmetric quantum mechanics010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical Physics
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Proof of a Conjecture on Contextuality in Cyclic Systems with Binary Variables

2015

We present a proof for a conjecture previously formulated by Dzhafarov, Kujala, and Larsson (Foundations of Physics, in press, arXiv:1411.2244). The conjecture specifies a measure for the degree of contextuality and a criterion (necessary and sufficient condition) for contextuality in a broad class of quantum systems. This class includes Leggett-Garg, EPR/Bell, and Klyachko-Can-Binicioglu-Shumovsky type systems as special cases. In a system of this class certain physical properties $q_{1},...,q_{n}$ are measured in pairs $(q_{i},q_{j})$; every property enters in precisely two such pairs; and each measurement outcome is a binary random variable. Denoting the measurement outcomes for a proper…

PhysicsQuantum PhysicsConjectureDegree (graph theory)Probability (math.PR)05 social sciencesBinary random variableFOS: Physical sciencesGeneral Physics and AstronomyBinary numberType (model theory)01 natural sciencesMeasure (mathematics)050105 experimental psychologyCombinatorics0103 physical sciencesFOS: Mathematics0501 psychology and cognitive sciencesQuantum Physics (quant-ph)81P13 81Q99 60A99010306 general physicsRandom variableMathematics - ProbabilityFoundations of Physics
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Comparative investigation of the freezing phenomena for quantum correlations under nondissipative decoherence

2013

We show that the phenomenon of frozen discord, exhibited by specific classes of two-qubit states under local nondissipative decoherent evolutions, is a common feature of all known bona fide measures of general quantum correlations. All those measures, despite inducing typically inequivalent orderings on the set of nonclassically correlated states, return a constant value in the considered settings. Every communication protocol which relies on quantum correlations as resource will run with a performance completely unaffected by noise in the specified dynamical conditions. We provide a geometric interpretation of this

PhysicsQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciQuantum decoherenceStatistical Mechanics (cond-mat.stat-mech)FOS: Physical sciencesMathematical Physics (math-ph)Noise (electronics)Atomic and Molecular Physics and OpticsInterpretation (model theory)Measurement theoryQuantum mechanicsStatistical physicsQuantum Physics (quant-ph)Constant (mathematics)ENTANGLEMENTValue (mathematics)QuantumCondensed Matter - Statistical MechanicsMathematical PhysicsDISCORDPhysics - OpticsOptics (physics.optics)Physical Review A
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Quantum walks and non-Abelian discrete gauge theory

2016

A new family of discrete-time quantum walks (DTQWs) on the line with an exact discrete $U(N)$ gauge invariance is introduced. It is shown that the continuous limit of these DTQWs, when it exists, coincides with the dynamics of a Dirac fermion coupled to usual $U(N)$ gauge fields in $2D$ spacetime. A discrete generalization of the usual $U(N)$ curvature is also constructed. An alternate interpretation of these results in terms of superimposed $U(1)$ Maxwell fields and $SU(N)$ gauge fields is discussed in the Appendix. Numerical simulations are also presented, which explore the convergence of the DTQWs towards their continuous limit and which also compare the DTQWs with classical (i.e. non-qu…

PhysicsQuantum PhysicsSpacetimeHigh Energy Physics::LatticeFOS: Physical sciencesGauge (firearms)01 natural sciences[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]010305 fluids & plasmasInterpretation (model theory)symbols.namesakeDirac fermion[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Quantum mechanics0103 physical sciencessymbols[ PHYS.PHYS.PHYS-GEN-PH ] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Quantum walkGauge theoryAbelian group010306 general physicsQuantum Physics (quant-ph)QuantumComputingMilieux_MISCELLANEOUSMathematical physics
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Pentaquark and diquark–diquark clustering: a QCD sum rule approach

2004

In this work we study the Theta(1540) in the framework of QCD sum rules based on (ud)^2\bar{s} diquark clustering as suggested by Jaffe and Wilczek. Within errors, the mass of the pentaquark is compatible with the experimentally measured value. The mass difference between the Theta and the pentaquark with the quantum numbers of the nucleon amounts to 70 MeV, consistent with the interpretation of the N(1440) as a pentaquark.

PhysicsQuantum chromodynamicsParticle physicsQCD sum rulesNuclear and High Energy PhysicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesQuantum numberQCD sum rulesPentaquarkPentaquarkInterpretation (model theory)DiquarkNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSum rule in quantum mechanicsNucleonNuclear ExperimentPhysics Letters B
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Effective Lagrangian approach to neutrinoless double beta decay and neutrino masses

2012

Neutrinoless double beta ($0\nu\beta\beta$) decay can in general produce electrons of either chirality, in contrast with the minimal Standard Model (SM) extension with only the addition of the Weinberg operator, which predicts two left-handed electrons in the final state. We classify the lepton number violating (LNV) effective operators with two leptons of either chirality but no quarks, ordered according to the magnitude of their contribution to \znbb decay. We point out that, for each of the three chirality assignments, $e_Le_L, e_Le_R$ and $e_Re_R$, there is only one LNV operator of the corresponding type to lowest order, and these have dimensions 5, 7 and 9, respectively. Neutrino masse…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Lepton numberPartícules (Física nuclear)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decayBeyond Standard ModelNeutrino PhysicsHigh Energy Physics::ExperimentNeutrinoLepton
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