8,512 research outputs found

    Optimal Measurements for Tests of EPR-Steering with No Detection Loophole using Two-Qubit Werner States

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    It has been shown in earlier works that the vertices of Platonic solids are good measurement choices for tests of EPR-steering using isotropically entangled pairs of qubits. Such measurements are regularly spaced, and measurement diversity is a good feature for making EPR-steering inequalities easier to violate in the presence of experimental imperfections. However, such measurements are provably suboptimal. Here, we develop a method for devising optimal strategies for tests of EPR-steering, in the sense of being most robust to mixture and inefficiency (while still closing the detection loophole of course), for a given number nn of measurement settings. We allow for arbitrary measurement directions, and arbitrary weightings of the outcomes in the EPR-steering inequality. This is a difficult optimization problem for large nn, so we also consider more practical ways of constructing near-optimal EPR-steering inequalities in this limit.Comment: 15 pages, 11 Figure

    The entanglement of indistinguishable particles shared between two parties

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    Using an operational definition we quantify the entanglement, EPE_P, between two parties who share an arbitrary pure state of NN indistinguishable particles. We show that EPEME_P \leq E_M, where EME_M is the bipartite entanglement calculated from the mode-occupation representation. Unlike EME_M, EPE_P is {\em super-additive}. For example, EP=0E_P =0 for any single-particle state, but the state 11\ket{1}\ket{1}, where both modes are split between the two parties, has EP=1/2E_P = 1/2. We discuss how this relates to quantum correlations between particles, for both fermions and bosons.Comment: 4 + epsilon pages. No figures. This published version is slightly modified from the origina

    Entanglement of identical particles and reference phase uncertainty

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    We have recently introduced a measure of the bipartite entanglement of identical particles, E_P, based on the principle that entanglement should be accessible for use as a resource in quantum information processing. We show here that particle entanglement is limited by the lack of a reference phase shared by the two parties, and that the entanglement is constrained to reference-phase invariant subspaces. The super-additivity of E_P results from the fact that this constraint is weaker for combined systems. A shared reference phase can only be established by transferring particles between the parties, that is, with additional nonlocal resources. We show how this nonlocal operation can increase the particle entanglement.Comment: 8 pages, no figures. Invited talk given at EQIS'03, Kyoto, September, 2003. Minor typos corrected, 1 reference adde

    Two-dimensional Site-Bond Percolation as an Example of Self-Averaging System

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    The Harris-Aharony criterion for a statistical model predicts, that if a specific heat exponent α0\alpha \ge 0, then this model does not exhibit self-averaging. In two-dimensional percolation model the index α=1/2\alpha=-{1/2}. It means that, in accordance with the Harris-Aharony criterion, the model can exhibit self-averaging properties. We study numerically the relative variances RMR_{M} and RχR_{\chi} for the probability MM of a site belongin to the "infinite" (maximum) cluster and the mean finite cluster size χ\chi. It was shown, that two-dimensional site-bound percolation on the square lattice, where the bonds play the role of impurity and the sites play the role of the statistical ensemble, over which the averaging is performed, exhibits self-averaging properties.Comment: 15 pages, 5 figure

    Adaptive Phase Measurements in Linear Optical Quantum Computation

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    Photon counting induces an effective nonlinear optical phase shift on certain states derived by linear optics from single photons. Although this no nlinearity is nondeterministic, it is sufficient in principle to allow scalable linear optics quantum computation (LOQC). The most obvious way to encode a qubit optically is as a superposition of the vacuum and a single photon in one mode -- so-called "single-rail" logic. Until now this approach was thought to be prohibitively expensive (in resources) compared to "dual-rail" logic where a qubit is stored by a photon across two modes. Here we attack this problem with real-time feedback control, which can realize a quantum-limited phase measurement on a single mode, as has been recently demonstrated experimentally. We show that with this added measurement resource, the resource requirements for single-rail LOQC are not substantially different from those of dual-rail LOQC. In particular, with adaptive phase measurements an arbitrary qubit state α0+β1\alpha \ket{0} + \beta\ket{1} can be prepared deterministically

    Entanglement under restricted operations: Analogy to mixed-state entanglement

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    We show that the classification of bi-partite pure entangled states when local quantum operations are restricted yields a structure that is analogous in many respects to that of mixed-state entanglement. Specifically, we develop this analogy by restricting operations through local superselection rules, and show that such exotic phenomena as bound entanglement and activation arise using pure states in this setting. This analogy aids in resolving several conceptual puzzles in the study of entanglement under restricted operations. In particular, we demonstrate that several types of quantum optical states that possess confusing entanglement properties are analogous to bound entangled states. Also, the classification of pure-state entanglement under restricted operations can be much simpler than for mixed-state entanglement. For instance, in the case of local Abelian superselection rules all questions concerning distillability can be resolved.Comment: 10 pages, 2 figures; published versio

    Ferreting out the Fluffy Bunnies: Entanglement constrained by Generalized superselection rules

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    Entanglement is a resource central to quantum information (QI). In particular, entanglement shared between two distant parties allows them to do certain tasks that would otherwise be impossible. In this context, we study the effect on the available entanglement of physical restrictions on the local operations that can be performed by the two parties. We enforce these physical restrictions by generalized superselection rules (SSRs), which we define to be associated with a given group of physical transformations. Specifically the generalized SSR is that the local operations must be covariant with respect to that group. Then we operationally define the entanglement constrained by a SSR, and show that it may be far below that expected on the basis of a naive (or ``fluffy bunny'') calculation. We consider two examples. The first is a particle number SSR. Using this we show that for a two-mode BEC (with Alice owning mode AA and Bob mode BB), the useful entanglement shared by Alice and Bob is identically zero. The second, a SSR associated with the symmetric group, is applicable to ensemble QI processing such as in liquid-NMR. We prove that even for an ensemble comprising many pairs of qubits, with each pair described by a pure Bell state, the entanglement per pair constrained by this SSR goes to zero for a large ensemble.Comment: 8 pages, proceedings paper for an invited talk at 16th International Conference on Laser Spectroscopy (2003

    State and dynamical parameter estimation for open quantum systems

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    Following the evolution of an open quantum system requires full knowledge of its dynamics. In this paper we consider open quantum systems for which the Hamiltonian is ``uncertain''. In particular, we treat in detail a simple system similar to that considered by Mabuchi [Quant. Semiclass. Opt. 8, 1103 (1996)]: a radiatively damped atom driven by an unknown Rabi frequency Ω\Omega (as would occur for an atom at an unknown point in a standing light wave). By measuring the environment of the system, knowledge about the system state, and about the uncertain dynamical parameter, can be acquired. We find that these two sorts of knowledge acquisition (quantified by the posterior distribution for Ω\Omega, and the conditional purity of the system, respectively) are quite distinct processes, which are not strongly correlated. Also, the quality and quantity of knowledge gain depend strongly on the type of monitoring scheme. We compare five different detection schemes (direct, adaptive, homodyne of the xx quadrature, homodyne of the yy quadrature, and heterodyne) using four different measures of the knowledge gain (Shannon information about Ω\Omega, variance in Ω\Omega, long-time system purity, and short-time system purity).Comment: 14 pages, 18 figure
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