4,007 research outputs found

    Entanglement in the classical limit: quantum correlations from classical probabilities

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    We investigate entanglement for a composite closed system endowed with a scaling property allowing to keep the dynamics invariant while the effective Planck constant hbar_eff of the system is varied. Entanglement increases as hbar_eff goes to 0. Moreover for sufficiently low hbar_eff the evolution of the quantum correlations, encapsulated for example in the quantum discord, can be obtained from the mutual information of the corresponding \emph{classical} system. We show this behavior is due to the local suppression of path interferences in the interaction that generates the entanglement. This behavior should be generic for quantum systems in the classical limit.Comment: 10 pages 3 figure

    Multiscale quantum-defect theory for two interacting atoms in a symmetric harmonic trap

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    We present a multiscale quantum-defect theory (QDT) for two identical atoms in a symmetric harmonic trap that combines the quantum-defect theory for the van der Waals interaction [B. Gao, Phys. Rev. A \textbf{64}, 010701(R) (2001)] at short distances with a quantum-defect theory for the harmonic trapping potential at large distances. The theory provides a systematic understanding of two atoms in a trap, from deeply bound molecular states and states of different partial waves, to highly excited trap states. It shows, e.g., that a strong pp wave pairing can lead to a lower energy state around the threshold than a ss wave pairing.Comment: 10 pages, 6 figure

    Influence of Coulomb distortion on polarization observables in elastic electromagnetic lepton hadron scattering at low energies

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    The formal expression for the most general polarization observable in elastic electromagnetic lepton hadron scattering at low energies is derived for the nonrelativistic regime. For the explicit evaluation the influence of Coulomb distortion on various polarization observables is calculated in a distorted wave Born approximation. Besides the hyperfine interaction also the spin-orbit interactions of lepton and hadron are included. For like charges the Coulomb repulsion reduces strongly the size of polarization observables compared to the plane wave Born approximation whereas for opposite charges the Coulomb attraction leads to a substantial increase of these observables for hadron lab kinetic energies below about 20 keV.Comment: 32 pages, 26 figures. Typos corrected, notation slightly changed, figures redrawn, one figure and references added. A condensed version is in press in Physical Review

    Entanglement, Mixedness, and Spin-Flip Symmetry in Multiple-Qubit Systems

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    A relationship between a recently introduced multipartite entanglement measure, state mixedness, and spin-flip symmetry is established for any finite number of qubits. It is also shown that, within those classes of states invariant under the spin-flip transformation, there is a complementarity relation between multipartite entanglement and mixedness. A number of example classes of multiple-qubit systems are studied in light of this relationship.Comment: To appear in Physical Review A; submitted 14 May 200

    Identification of the Beutler-Fano formula in eigenphase shifts and eigentime delays near a resonance

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    Eigenphase shifts and eigentime delays near a resonance for a system of one discrete state and two continua are shown to be functionals of the Beutler- Fano formulas using appropriate dimensionless energy units and line profile indices. Parameters responsible for the avoided crossing of eigenphase shifts and eigentime delays are identified. Similarly, parameters responsible for the eigentime delays due to a frame change are identified. With the help of new parameters, an analogy with the spin model is pursued for the S matrix and time delay matrix. The time delay matrix is shown to comprise three terms, one due to resonance, one due to a avoided crossing interaction, and one due to a frame change. It is found that the squared sum of time delays due to the avoided crossing interaction and frame change is unity.Comment: 17 pages, 3 figures, RevTe

    The Optimal Inhomogeneity for Superconductivity: Finite Size Studies

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    We report the results of exact diagonalization studies of Hubbard models on a 4×44\times 4 square lattice with periodic boundary conditions and various degrees and patterns of inhomogeneity, which are represented by inequivalent hopping integrals tt and t′t^{\prime}. We focus primarily on two patterns, the checkerboard and the striped cases, for a large range of values of the on-site repulsion UU and doped hole concentration, xx. We present evidence that superconductivity is strongest for UU of order the bandwidth, and intermediate inhomogeneity, 0<t′<t0 <t^\prime< t. The maximum value of the ``pair-binding energy'' we have found with purely repulsive interactions is Δpb=0.32t\Delta_{pb} = 0.32t for the checkerboard Hubbard model with U=8tU=8t and t′=0.5tt^\prime = 0.5t. Moreover, for near optimal values, our results are insensitive to changes in boundary conditions, suggesting that the correlation length is sufficiently short that finite size effects are already unimportant.Comment: 8 pages, 9 figures; minor revisions; more references adde

    Resonance structures in the multichannel quantum defect theory for the photofragmentation processes involving one closed and many open channels

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    The transformation introduced by Giusti-Suzor and Fano and extended by Lecomte and Ueda for the study of resonance structures in the multichannel quantum defect theory (MQDT) is used to reformulate MQDT into the forms having one-to-one correspondence with those in Fano's configuration mixing (CM) theory of resonance for the photofragmentation processes involving one closed and many open channels. The reformulation thus allows MQDT to have the full power of the CM theory, still keeping its own strengths such as the fundamental description of resonance phenomena without an assumption of the presence of a discrete state as in CM.Comment: 7 page
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