6533b851fe1ef96bd12a8e3f

RESEARCH PRODUCT

Continuous variable tangle, monogamy inequality, and entanglement sharing in Gaussian states of continuous variable systems

Fabrizio IlluminatiGerardo Adesso

subject

Quantum PhysicsLOCCLogarithmGaussianFOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)Quantum PhysicsQuantum entanglementMeasure (mathematics)Condensed Matter - Other Condensed Mattersymbols.namesakeMultipartiteMonotone polygonQUANTUM TELEPORTATION NETWORKQubitsymbolsStatistical physicsQuantum Physics (quant-ph)Mathematical PhysicsOther Condensed Matter (cond-mat.other)Optics (physics.optics)Physics - OpticsMathematics

description

For continuous-variable systems, we introduce a measure of entanglement, the continuous variable tangle ({\em contangle}), with the purpose of quantifying the distributed (shared) entanglement in multimode, multipartite Gaussian states. This is achieved by a proper convex roof extension of the squared logarithmic negativity. We prove that the contangle satisfies the Coffman-Kundu-Wootters monogamy inequality in all three--mode Gaussian states, and in all fully symmetric $N$--mode Gaussian states, for arbitrary $N$. For three--mode pure states we prove that the residual entanglement is a genuine tripartite entanglement monotone under Gaussian local operations and classical communication. We show that pure, symmetric three--mode Gaussian states allow a promiscuous entanglement sharing, having both maximum tripartite residual entanglement and maximum couplewise entanglement between any pair of modes. These states are thus simultaneous continuous-variable analogs of both the GHZ and the $W$ states of three qubits: in continuous-variable systems monogamy does not prevent promiscuity, and the inequivalence between different classes of maximally entangled states, holding for systems of three or more qubits, is removed.

https://doi.org/10.1088/1367-2630/8/1/015