2,991 research outputs found

    A higher quantum bound for the V\'ertesi-Bene-Bell-inequality and the role of POVMs regarding its threshold detection efficiency

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    Recently, V\'{e}rtesi and Bene [Phys. Rev. A. {\bf 82}, 062115 (2010)] derived a two-qubit Bell inequality, ICH3I_{CH3}, which they show to be maximally violated only when more general positive operator valued measures (POVMs) are used instead of the usual von Neumann measurements. Here we consider a general parametrization for the three-element-POVM involved in the Bell test and obtain a higher quantum bound for the ICH3I_{CH3}-inequality. With a higher quantum bound for ICH3I_{CH3}, we investigate if there is an experimental setup that can be used for observing that POVMs give higher violations in Bell tests based on this inequality. We analyze the maximum errors supported by the inequality to identify a source of entangled photons that can be used for the test. Then, we study if POVMs are also relevant in the more realistic case that partially entangled states are used in the experiment. Finally, we investigate which are the required efficiencies of the ICH3I_{CH3}-inequality, and the type of measurements involved, for closing the detection loophole. We obtain that POVMs allow for the lowest threshold detection efficiency, and that it is comparable to the minimal (in the case of two-qubits) required detection efficiency of the Clauser-Horne-Bell-inequality.Comment: 11 Pages, 16 Figure

    Spin Josephson effect in ferromagnet/ferromagnet tunnel junctions

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    We consider the tunnel spin current between two ferromagnetic metals from a perspective similar to the one used in superconductor/superconductor tunnel junctions. We use fundamental arguments to derive a Josephson-like spin tunnel current IJspin∝sin⁥(Ξ1−ξ2)I_J^{\rm spin}\propto\sin(\theta_1-\theta_2). Here the phases are associated with the planar contribution to the magnetization, ∌eiΞ\sim e^{i\theta}. The crucial step in our analysis is the fact that the zz-component of the spin is canonically conjugate to the phase of the planar contribution: [Ξ,Sz]=i[\theta,S^z]=i. This is analogous to the commutation relation [ϕ,N]=i[\phi,N]=i in superconductors, where ϕ\phi is the phase associated to the superconducting order parameter and NN is the Cooper pair number operator. We briefly discuss the experimental consequences of our theoretical analysis.Comment: LaTex, seven pages, no figures; version to appear in Europhys. Lett.; in order to make room for a more extended microscopic analysis, the phenomenological discussion contained in v2 was remove

    Optical Bell-state analysis in the coincidence basis

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    Many quantum information protocols require a Bell-state measurement of entangled systems. Most optical Bell-state measurements utilize two-photon interference at a beam splitter. By creating polarization-entangled photons with spontaneous parametric down-conversion using a first-order Hermite-Gaussian pump beam, we invert the usual interference behavior and perform an incomplete Bell-state measurement in the coincidence basis. We discuss the possibility of a complete Bell-state measurement in the coincidence basis using hyperentangled states [Phys. Rev. A, \textbf{58}, R2623 (1998)].Comment: 5 pages, 5 figure

    Multimode Hong-Ou-Mandel Interferometry

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    We review some recent experiments based upon multimode two-photon interference of photon pairs created by spontaneous parametric down-conversion. The new element provided by these experiments is the inclusion of the transverse spatial profiles of the pump, signal and idler fields. We discuss multimode Hong-Ou-Mandel interference, and show that the transverse profile of the pump beam can be manipulated in order to control two-photon interference. We present the basic theory and experimental results as well as several applications to the field of quantum information.Comment: 20 pages, 14 figures, Brief Review to be published in Modern Physics Letters

    Long-distance distribution of genuine energy-time entanglement

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    Any practical realization of entanglement-based quantum communication must be intrinsically secure and able to span long distances avoiding the need of a straight line between the communicating parties. The violation of Bell's inequality offers a method for the certification of quantum links without knowing the inner workings of the devices. Energy-time entanglement quantum communication satisfies all these requirements. However, currently there is a fundamental obstacle with the standard configuration adopted: an intrinsic geometrical loophole that can be exploited to break the security of the communication, in addition to other loopholes. Here we show the first experimental Bell violation with energy-time entanglement distributed over 1 km of optical fibers that is free of this geometrical loophole. This is achieved by adopting a new experimental design, and by using an actively stabilized fiber-based long interferometer. Our results represent an important step towards long-distance secure quantum communication in optical fibers.Comment: 6 pages, 3 figures. Matches published versio

    Criticality in the 2+1-dimensional compact Higgs model and fractionalized insulators

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    We use a novel method of computing the third moment M_3 of the action of the 2+1-dimensional compact Higgs model in the adjoint representation with q=2 to extract correlation length and specific heat exponents nu and alpha, without invoking hyperscaling. Finite-size scaling analysis of M_3 yields the ratio (1+alpha)/nu and 1/nu separately. We find that alpha and nu vary along the critical line of the theory, which however exhibits a remarkable resilience of Z_2 criticality. We propose this novel universality class to be that of the quantum phase transition from a Mott-Hubbard insulator to a charge-fractionalized insulator in two spatial dimensions.Comment: 4 pages, 3 figures, submitted to Phys. Rev. Let

    O estresse no manejo pré-abate e na qualidade da carne suína.

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    O estresse no manejo prĂ©-abate e na qualidade da carne suĂ­na; Caracterização do estresse; Avaliação da resposta fisiolĂłgica dio estresse; Formas de avaliaçÔes; Determinação do cortisol; Determinação de lactato; Mecanismos atravĂ©s dos quais podem afetar a qualidade da carne; InfluĂȘncia da genĂ©tica na qualidade da carne; Gene rendimento napole (RN); gene Halotano; SituaçÔes de estresse no manejo prĂ©-abate.bitstream/item/58222/1/publicacao-i7n63h7v1.pd

    Metal-Insulator Transition in the Two-Dimensional Hubbard Model at Half-Filling with Lifetime Effects within the Moment Approach

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    We explore the effect of the imaginary part of the self-energy, ImÎŁ(k⃗,ω)Im\Sigma(\vec{k},\omega), having a single pole, Ω(k⃗,ω)\Omega(\vec{k},\omega), with spectral weight, α(k⃗)\alpha(\vec{k}), and quasi-particle lifetime, Γ(k⃗)\Gamma(\vec{k}), on the density of states. We solve the set of parameters, Ω(k⃗,ω\Omega(\vec{k},\omega), α(k⃗)\alpha(\vec{k}), and Γ(k⃗)\Gamma(\vec{k}) by means of the moment approach (exact sum rules) of Nolting. Our choice for ÎŁ(k,ω)\Sigma(k,\omega), satisfies the Kramers - Kronig relationship automatically. Due to our choice of the self - energy, the system is not a Fermi liquid for any value of the interaction, a result which is also true in the moment approach of Nolting without lifetime effects. By increasing the value of the local interaction, U/WU/W, at half-filling (ρ=1/2\rho = 1/2), we go from a paramagnetic metal to a paramagnetic insulator, (Mott metal - insulator transition (MMITMMIT)) for values of U/WU/W of the order of U/W≄1U/W \geq 1 (WW is the band width) which is in agreement with numerical results for finite lattices and for infinity dimensions (D=∞D = \infty). These results settle down the main weakness of the spherical approximation of Nolting: a finite gap for any finite value of the interaction, i.e., an insulator for any finite value of U/WU/W. Lifetime effects are absolutely indispensable. Our scheme works better than the one of improving the narrowing band factor, B(k⃗)B(\vec{k}), beyond the spherical approximation of Nolting.Comment: 5 pages and 5 ps figures (included

    Resummation scheme for 3d Yang-Mills and the two-loop magnetic mass for hot gauge theories

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    Perturbation theory for non-Abelian gauge theories at finite temperature is plagued by infrared divergences caused by magnetic soft modes ∌g2T\sim g^2T, which correspond to the fields of a 3d Yang-Mills theory. We revisit a gauge invariant resummation scheme to solve this problem by self-consistent mass generation using an auxiliary scalar field, improving over previous attempts in two respects. First, we generalise earlier SU(2) treatments to SU(N). Second, we obtain a gauge independent two-loop gap equation, correcting an error in the literature. The resulting two-loop approximation to the magnetic mass represents a ∌15\sim 15% correction to the leading one-loop value, indicating a reasonable convergence of the resummation.Comment: 16 pages, 3 figure
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