Search results for "equality"

showing 10 items of 1338 documents

Super-entropic black hole with Immirzi hair

2020

In the context of $f(R)$ generalizations to the Holst action, endowed with a dynamical Immirzi field, we derive an analytic solution describing asymptotically anti--de Sitter black holes with hyperbolic horizon. These exhibit a scalar hair of the second kind, which ultimately depends on the Immirzi field radial behavior. In particular, we show how the Immirzi field modifies the usual entropy law associated to the black hole. We also verify that the Immirzi field boils down to a constant value in the asymptotic region, thus restoring the standard loop quantum gravity picture. We finally prove the violation of the reverse isoperimetric inequality, resulting in the superentropic nature of the …

PhysicsHigh Energy Physics - TheoryField (physics)HorizonScalar (mathematics)FOS: Physical sciencesContext (language use)Loop quantum gravityGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyBlack holeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)Isoperimetric inequalityEntropy (arrow of time)Mathematical physics
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On the observability of Bell's inequality violation in the two-atoms optical Stern-Gerlach model

2005

Using the optical Stern-Gerlach model, we have recently shown that the non-local correlations between the internal variables of two atoms that successively interact with the field of an ideal cavity in proximity of a nodal region are affected by the atomic translational dynamics. As a consequence, there can be some difficulties in observing violation of the Bell's inequality for the atomic internal variables. These difficulties persist even if the atoms travel an antinodal region, except when the spatial wave packets are exactly centered in an antinodal point.

PhysicsMECHANICAL DESCRIPTIONTRANSLATIONAL DYNAMICSStern–Gerlach experimentIdeal (set theory)Field (physics)InequalityWave packetmedia_common.quotation_subjectDETERMINISTIC QUANTUM TELEPORTATIONCOMPLEMENTARITYAtomic and Molecular Physics and OpticsRABI OSCILLATIONSATOMSSCALAR PRODUCTHILBERT-SPACEQuantum mechanicsPhysics::Atomic and Molecular ClustersInternal variablePoint (geometry)Physics::Atomic PhysicsObservabilityPHYSICAL REALITYINTERFEROMETERmedia_common
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Couplings in coupled channels versus wave functions: Application to theX(3872)resonance

2010

We perform an analytical study of the scattering matrix and bound states in problems with many physical coupled channels. We establish the relationship of the couplings of the states to the different channels, obtained from the residues of the scattering matrix at the poles, with the wave functions for the different channels. The couplings basically reflect the value of the wave functions around the origin in coordinate space. In the concrete case of the $X(3872)$ resonance, understood as a bound state of ${D}^{0}{\overline{D}}^{*0}$ and ${D}^{+}{D}^{*\ensuremath{-}}$ (and $c.c.$ From now on, when we refer to ${D}^{0}{\overline{D}}^{*0}$ , ${D}^{+}{D}^{*\ensuremath{-}}$, or $D{\overline{D}}…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsForm factor (quantum field theory)Order (ring theory)Elementary particle01 natural sciencesResonance (particle physics)IsospinQuantum mechanics0103 physical sciencesBound state10. No inequality010306 general physicsWave functionS-matrixPhysical Review D
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Molecular picture for the X0(2866) as a D⁎K¯⁎ J = 0+ state and related 1+,2+ states

2020

Abstract We recall the predictions made ten years ago about a bound state of J P = 0 + in I = 0 of the D ⁎ K ¯ ⁎ system, which is manifestly exotic, and we associate it to the X 0 ( 2866 ) state reported in the recent LHCb experiment. Fine tuning the parameters to reproduce exactly the mass and width of the X 0 ( 2866 ) state, we report two more states stemming from the same interaction, one with 1 + and the other with 2 + . For reasons of parity, the 1 + state cannot be observed in D K ¯ decay, and we suggest to observe it in the D ⁎ K ¯ spectrum. On the other hand, the 2 + state can be observed in D K ¯ decay but the present experiment has too small statistics in the region of its mass to…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physics0103 physical sciencesBound stateParity (physics)010306 general physics10. No inequality01 natural sciencesPhysics Letters B
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Models for neutrino mass with discrete symmetries

2010

Discrete non-abelian flavor symmetries give in a natural way tri-bimaximal (TBM) mixing as showed in a prototype model. However neutrino mass matrix pattern may be very different from the tri-bimaximal one if small deviations of TBM will be observed. We give the result of a model independent analysis for TBM neutrino mass pattern.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSmall deviationsFOS: Physical sciencesMass matrix01 natural sciencesAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceNeutrino10. No inequality010306 general physicsMixing (physics)Nuclear Physics B - Proceedings Supplements
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Observation ofJ/ψpResonances Consistent with Pentaquark States inΛb0→J/ψK−pDecays

2015

Observations of exotic structures in the J/ψp channel, that we refer to as pentaquark-charmonium states, in Λ0b→J/ψK−p decays are presented. The data sample corresponds to an integrated luminosity of 3/fb acquired with the LHCb detector from 7 and 8 TeV pp collisions. An amplitude analysis is performed on the three-body final-state that reproduces the two-body mass and angular distributions. To obtain a satisfactory fit of the structures seen in the J/ψp mass spectrum, it is necessary to include two Breit-Wigner amplitudes that each describe a resonant state. The significance of each of these resonances is more than 9 standard deviations. One has a mass of 4380±8±29 MeV and a width of 205±1…

PhysicsParticle physicsMeson010308 nuclear & particles physicsHadronGeneral Physics and AstronomyParity (physics)Exotic hadron01 natural sciencesPentaquarkBaryonNuclear physicsAmplitude0103 physical sciencesMass spectrumHigh Energy Physics::Experiment10. No inequality010306 general physicsPhysical Review Letters
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Bell's inequality violation for entangled generalized Bernoulli states in two spatially separate cavities

2005

We consider the entanglement of orthogonal generalized Bernoulli states in two separate single-mode high-$Q$ cavities. The expectation values and the correlations of the electric field in the cavities are obtained. We then define, in each cavity, a dichotomic operator expressible in terms of the field states which can be, in principle, experimentally measured by a probe atom that ``reads'' the field. Using the quantum correlations of couples of these operators, we construct a Bell's inequality which is shown to be violated for a wide range of the degree of entanglement and which can be tested in a simple way. Thus the cavity fields directly show quantum non-local properties. A scheme is als…

PhysicsQuantum PhysicsBell stateField (physics)Cavity quantum electrodynamicsFOS: Physical sciencesQuantum entanglementSettore FIS/03 - Fisica Della MateriaAtomic and Molecular Physics and OpticsEntanglementBernoulli's principleOperator (computer programming)Cavity radiation fieldBell's theoremQuantum mechanicsBell's inequalityBernoulli processQuantum Physics (quant-ph)Quantum
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Entanglement correlations, Bell inequalities, and the concurrence

2005

Probabilities of measurement outcomes of two-particle entangled states give a physically transparent interpretation of the concurrence and of the I-concurrence as entanglement measures. The (I)-concurrence can thus be measured experimentally. The tight connection between these measures and Bell inequalities is highlighted.

PhysicsQuantum PhysicsBell stateInequalitymedia_common.quotation_subjectGeneral Physics and AstronomyFOS: Physical sciencesConcurrenceQuantum entanglementQuantum PhysicsSquashed entanglementMultipartite entanglementLocal hidden variable theoryQuantum mechanicsComputer Science::Programming LanguagesBell test experimentsQuantum Physics (quant-ph)media_common
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Dynamics of Non Classically Reproducible Entanglement

2008

We investigate when the quantum correlations of a bipartite system, under the influence of environments with memory, are not reproducible with certainty by a classical local hidden variable model. To this purpose, we compare the dynamics of a Bell inequality with that of entanglement, as measured by concurrence. We find time regions when Bell inequality is not violated even in correspondence to high values of concurrence (up to $\approx 0.8$). We also suggest that these results may be observed by adopting a modification of a recent experimental optical setup. These findings indicate that even highly entangled systems cannot be exploited with certainty in contexts where the non classical rep…

PhysicsQuantum PhysicsBell stateSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciQuantum correlationCHSH inequalityFOS: Physical sciencesQuantum entanglementAtomic and Molecular Physics and OpticsQuantum nonlocalityLocal hidden variable theoryQuantum mechanicsBell test experimentsQuantum Physics (quant-ph)Quantum teleportationNon-locality entanglement Bell inequality open quantum systems
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CP symmetry and thermal effects on Dirac bi-spinor spin–parity local correlations

2018

Intrinsic quantum correlations supported by the $SU(2)\otimes SU(2)$ structure of the Dirac equation used to describe particle/antiparticle states, optical ion traps and bilayer graphene are investigated and connected to the description of local properties of Dirac bi-spinors. For quantum states driven by Dirac-like Hamiltonians, quantum entanglement and geometric discord between spin and parity degrees of freedom - sometimes mapped into equivalent low energy internal degrees of freedom - are obtained. Such \textit{spin-parity} quantum correlations and the corresponding nonlocal intrinsic structures of bi-spinor fermionic states can be classified in order to relate quantum observables to th…

PhysicsQuantum PhysicsFOS: Physical sciencesGeneral Physics and AstronomyCHSH inequalityObservableParity (physics)Quantum entanglement01 natural sciences010305 fluids & plasmassymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Local hidden variable theoryQuantum stateQuantum mechanicsDirac equation0103 physical sciencessymbolsQuantum Physics (quant-ph)010306 general physicsQuantum
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