Search results for "values."

showing 10 items of 1353 documents

A Quantum Mechanical Model of the Reissner-Nordstrom Black Hole

1997

We consider a Hamiltonian quantum theory of spherically symmetric, asymptotically flat electrovacuum spacetimes. The physical phase space of such spacetimes is spanned by the mass and the charge parameters $M$ and $Q$ of the Reissner-Nordstr\"{o}m black hole, together with the corresponding canonical momenta. In this four-dimensional phase space, we perform a canonical transformation such that the resulting configuration variables describe the dynamical properties of Reissner-Nordstr\"{o}m black holes in a natural manner. The classical Hamiltonian written in terms of these variables and their conjugate momenta is replaced by the corresponding self-adjoint Hamiltonian operator, and an eigenv…

PhysicsNuclear and High Energy PhysicsCanonical quantizationVacuum stateFOS: Physical sciencesCanonical transformationGeneral Relativity and Quantum Cosmology (gr-qc)WKB approximationGeneral Relativity and Quantum CosmologyBlack holesymbols.namesakeGeneral Relativity and Quantum CosmologyQuantum mechanicsPhase spacesymbolsHamiltonian (quantum mechanics)Eigenvalues and eigenvectors
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New approach for numerical solution of configuration-space Faddeev equations

1996

A new computational scheme for solving the bound state configuration-space Faddeev equations is applied. The scheme is based on the spline-approximation and the adiabatic limit of Faddeev equations. An ordering of variables being in agreement with the limit was chosen. As a result the matrix of the eigenvalue problem has a sparse block structure. Calculations of the bound states of µpp, µdd, µtt mesic molecules and ¯pdd, ¯ptt antiprotonic ones, were performed. To check the method, calculations of the binding energies for such systems as the positronium ion Ps−,3H and3He were carried out. The results are compared with the best results of other authors.

PhysicsNuclear and High Energy PhysicsFaddeev equationsCondensed Matter PhysicsAtomic and Molecular Physics and OpticsPositroniumMatrix (mathematics)Quantum mechanicsBound stateApplied mathematicsConfiguration spaceLimit (mathematics)Physical and Theoretical ChemistryAdiabatic processEigenvalues and eigenvectors
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Nuclear matrix elements of ββ decay from β-decay data

2005

Abstract The evaluation of the nuclear matrix elements (NME) of the two-neutrino double beta ( 2 ν β β ) decay and neutrinoless double beta ( 0 ν β β ) decay using the proton–neutron quasiparticle random-phase approximation (pnQRPA) is addressed. In particular, the extraction of a proper value of the proton–neutron particle–particle interaction parameter, g pp , of this theory is analyzed in detail. Evidence is shown, that it can be misleading to use the experimental half-life of the 2 ν β β decay to extract a value for g pp . Rather, arguments are given in favour of using the available data on single beta decay for this purpose.

PhysicsNuclear and High Energy PhysicsHalf-lifeProton–neutron interactionBeta decayDouble beta decayNuclear physicsDouble beta decayNuclear matrix elementsQuasiparticleQuasiparticle random-phase approximationBeta (velocity)High Energy Physics::ExperimentNeutrinoRandom phase approximationNuclear ExperimentEigenvalues and eigenvectorsPhysics Letters B
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The index theorem on the lattice with improved fermion actions

1998

We consider a Wilson-Dirac operator with improved chiral properties. We show that, for arbitrarily rough gauge fields, it satisfies the index theorem if we identify the zero modes with the small real eigenvalues of the fermion operator and use the geometrical definition of topological charge. This is also confirmed in a numerical study of the quenched Schwinger model. These results suggest that integer definitions of the topological charge based on counting real modes of the Wilson operator are equivalent to the geometrical definition. The problem of exceptional configurations and the sign problem in simulations with an odd number of dynamical Wilson fermions are briefly discussed. We consi…

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeOperator (physics)Zero (complex analysis)FísicaParticle Physics - LatticeFermionIntegerAtiyah–Singer index theoremTopological quantum numberEigenvalues and eigenvectorsMathematical physicsSign (mathematics)Nuclear Physics B
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New information on β-delayed neutron emission from Be-12, Be-14

1999

17 pages, 3 tables, 5 figures, 1 appendix.-- PACS nrs.: 23.40.Hc; 27.20.+n.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderRadioactivity: Be-12 Be-14 (from 1 GeV p on UC target selective mass separation)Astrophysics::High Energy Astrophysical PhenomenaConfidence intervalNuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Neutron long countersBe-12 Be-14 deduced P(n) values Be-14 deduced P(xn) valuesHigh Energy Physics::ExperimentNeutronMeasured βn nn time correlations[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentDelayed neutronRadioactive beam[PACS] Relation with nuclear matrix elements and nuclear structureBe-12 Be-14 (from 1 GeV p on UC target selective mass separation) [Radioactivity]
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Sweeping the Space of Admissible Quark Mass Matrices

2002

We propose a new and efficient method of reconstructing quark mass matrices from their eigenvalues and a complete set of mixing observables. By a combination of the principle of NNI (nearest neighbour interaction) bases which are known to cover the general case, and of the polar decomposition theorem that allows to convert arbitrary nonsingular matrices to triangular form, we achieve a parameterization where the remaining freedom is reduced to one complex parameter. While this parameter runs through the domain bounded by a circle with radius R determined by the up-quark masses around the origin in the complex plane one sweeps the space of all mass matrices compatible with the given set of d…

PhysicsNuclear and High Energy PhysicsMathematical analysisPolar decompositionFOS: Physical sciencesSpace (mathematics)Domain (mathematical analysis)High Energy Physics - PhenomenologyClassical mechanicsHigh Energy Physics - Phenomenology (hep-ph)Cover (topology)Mixing (mathematics)Bounded functionComplex planeEigenvalues and eigenvectors
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Measurement of in oscillation using quantum correlations in at

2015

We report a measurement of the parameter y(CP) in D-0-(D) over bar (0) oscillations performed by taking advantage of quantum coherence between pairs of D-0(D) over bar (0) mesons produced in e(+)e(-) annihilations near threshold. In this work, doubly-tagged D-0(D) over bar (0) events, where one D decays to a CP eigenstate and the other D decays in a semileptonic mode, are reconstructed using a data sample of 2.92 fb(-1) collected with the BESIII detector at the center-of-mass energy of root s = 3.773 GeV. We obtain y(CP) = (-2.0 +/- 1.3 +/- 0.7)%, where the first uncertainty is statistical and the second is systematic. This result is compatible with the current world average.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsOscillationQuantum correlation01 natural sciencesNuclear physicsPion0103 physical sciencesCP violationCoherence (signal processing)High Energy Physics::Experiment010306 general physicsEigenvalues and eigenvectors
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CP, T and CPT versus temporal asymmetries for entangled states of the B-system

1999

The observables used in the K-system to characterize T and CPT violation are no longer useful for the Bd-system, since the width difference between the physical states is vanishingly small. We show that only Im(epsilon) and Re(delta) can survive if Delta Gamma=0, and build alternative CP-odd, CPT-odd, T-odd and temporal asymmetries for the (B_CP -> B0, B0bar) transitions. These quantities enable us to test T and CPT invariances of the effective Hamiltonian for the B-system. The method needs the CP eigenstates B_CP, which can be tagged unambiguously to order lambda^3 from the entangled states of a B-factory.

PhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesFísicaObservableHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentHamiltonian (quantum mechanics)Eigenvalues and eigenvectorsParticle Physics - PhenomenologyPhysics Letters B
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Correlated neutral B meson decays into CP eigenstates

2003

In the two correlated $B$ meson decay experiment we propose to measure intensities relating CP eigenstate ($J/\psi K_{S,L}$) decays on $both$ sides, which will be measurable in future upgrades of KEK and PEP. As a CP-forbidden transition, we obtain $I(J/\psi K_S, J/\psi K_S, \Delta t) \sim \sin ^2 (2\beta)$. We calculate in a model independent way all the possible intensities relating final CP and flavour eigenstate decays. Under CPT-invariance, the asymmetries for processes related by CP$\Delta t$ vanish for $\Delta \Gamma =0$ and measure $\Delta \Gamma$ linearly. We notice the impossibility to isolate the sign of $\cos (2\bet a)$ without an independent knowledge of the sign of $\Delta \Ga…

PhysicsNuclear and High Energy PhysicsParticle physicsFlavourFOS: Physical sciencesFísicaObservableMeasure (mathematics)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)B mesonHigh Energy Physics::ExperimentEigenvalues and eigenvectorsSign (mathematics)
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Atmospheric neutrino anomaly without maximal mixing?

2000

We consider a pattern of neutrino masses in which there is an approximate mass degeneracy between the two mass eigenstates most coupled to the $\nu_\mu$ and $\nu_\tau$ flavour eigenstates. Earth-matter effects can lift this degeneracy and induce an effectively maximal mixing between these two generations. This occurs if $\nu_e$'s contain comparable admixtures of the degenerate eigenstates, even rather small ones. This provides an explanation of the atmospheric neutrino anomaly in which the {\it ab initio} introduction of a large mixing angle is not required. To test this possibility we perform a novel and detailed analysis of the 52 kiloton-year SuperKamiokande data, and we find that in a l…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyDegenerate energy levelsAb initioFOS: Physical sciencesFísicaCHOOZParameter spaceNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BibliographyHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationEigenvalues and eigenvectorsParticle Physics - PhenomenologyPhysical Review D
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