4,479 research outputs found
When is there a multipartite maximum entangled state?
For a multipartite quantum system of the dimension , , is there an entangled state {\em maximum} in
the sense that all other states in the system can be obtained from the state
through local quantum operations and classical communications (LOCC)? When
, such state exists. We show that this condition is also
necessary. Our proof, somewhat surprisingly, uses results from algebraic
complexity theory.Comment: 10 pages, no figure. We know the answer is quite simple, but the
proof is somewhat involved. Comments are welcom
Sudden change in dynamics of genuine multipartite entanglement of cavity-reservoir qubits
We study the dynamics of genuine multipartite entanglement for a system of
four qubits. Using a computable entanglement monotone for multipartite systems,
we investigate the as yet unexplored aspects of a cavity-reservoir system of
qubits. For one specific initial state, we observe a sudden transition in the
dynamics of genuine entanglement for the four qubits. This sudden change occurs
only during a time window where neither cavity-cavity qubits nor
reservoir-reservoir qubits are entangled. We show that this sudden change in
dynamics of this specific state is extremely sensitive to white noise.Comment: 18 pages, 11 figure
Additivity and non-additivity of multipartite entanglement measures
We study the additivity property of three multipartite entanglement measures,
i.e. the geometric measure of entanglement (GM), the relative entropy of
entanglement and the logarithmic global robustness. First, we show the
additivity of GM of multipartite states with real and non-negative entries in
the computational basis. Many states of experimental and theoretical interests
have this property, e.g. Bell diagonal states, maximally correlated generalized
Bell diagonal states, generalized Dicke states, the Smolin state, and the
generalization of D\"{u}r's multipartite bound entangled states. We also prove
the additivity of other two measures for some of these examples. Second, we
show the non-additivity of GM of all antisymmetric states of three or more
parties, and provide a unified explanation of the non-additivity of the three
measures of the antisymmetric projector states. In particular, we derive
analytical formulae of the three measures of one copy and two copies of the
antisymmetric projector states respectively. Third, we show, with a statistical
approach, that almost all multipartite pure states with sufficiently large
number of parties are nearly maximally entangled with respect to GM and
relative entropy of entanglement. However, their GM is not strong additive;
what's more surprising, for generic pure states with real entries in the
computational basis, GM of one copy and two copies, respectively, are almost
equal. Hence, more states may be suitable for universal quantum computation, if
measurements can be performed on two copies of the resource states. We also
show that almost all multipartite pure states cannot be produced reversibly
with the combination multipartite GHZ states under asymptotic LOCC, unless
relative entropy of entanglement is non-additive for generic multipartite pure
states.Comment: 45 pages, 4 figures. Proposition 23 and Theorem 24 are revised by
correcting a minor error from Eq. (A.2), (A.3) and (A.4) in the published
version. The abstract, introduction, and summary are also revised. All other
conclusions are unchange
Generic local distinguishability and completely entangled subspaces
A subspace of a multipartite Hilbert space is completely entangled if it
contains no product states. Such subspaces can be large with a known maximum
size, S, approaching the full dimension of the system, D. We show that almost
all subspaces with dimension less than or equal to S are completely entangled,
and then use this fact to prove that n random pure quantum states are
unambiguously locally distinguishable if and only if n does not exceed D-S.
This condition holds for almost all sets of states of all multipartite systems,
and reveals something surprising. The criterion is identical for separable and
for nonseparable states: entanglement makes no difference.Comment: 12 page
Correlated multipartite quantum states
We investigate quantum states that possess both maximum entanglement and maximum discord between the pertinent parties. Since entanglement (discord) is defined only for bipartite (two-qubit) systems, we use an appropriate sum over all bipartitions as the associated measure. The ensuing definition - not new for entanglement - is thus extended here to quantum discord. Also, additional dimensions within the parties are considered (qudits). We also discuss quantum correlations that induce Mermin's Bell-inequality violation for all multiqubit systems. One finds some differences when quantum mechanics is defined over the field of real or of complex numbers. © 2013 American Physical Society.Fil: Batle, J.. Universitat de Les Illes Balears; EspañaFil: Casas, M.. Universitat de Les Illes Balears; España. Universitat de Les Illes Balears;Fil: Plastino, Ángel Luis. Universitat de Les Illes Balears; España. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto de Física La Plata. Universidad Nacional de La Plata. Facultad de Ciencias Exactas. Instituto de Física La Plata; Argentin
Geometric measure of entanglement for pure multipartite states
We provide methods for computing the geometric measure of entanglement for
two families of pure states with both experimental and theoretical interests:
symmetric multiqubit states with non-negative amplitudes in the Dicke basis and
symmetric three-qubit states. In addition, we study the geometric measure of
pure three-qubit states systematically in virtue of a canonical form of their
two-qubit reduced states, and derive analytical formulae for a three-parameter
family of three-qubit states. Based on this result, we further show that the W
state is the maximally entangled three-qubit state with respect to the
geometric measure.Comment: A minor error on the explanation of three-qubit GHZ state has been
corrected in the fourth paragraph of page 1. Thanks for Martin Aulbach
pointing out this erro
Maximally correlated multipartite quantum states
We investigate quantum states that posses both maximum entanglement and
maximum discord between the pertinent parties. Since entanglement (discord) is
defined only for bipartite (two qubit) systems, we shall introduce an
appropriate sum over of all bi-partitions as the associated measure. The
ensuing definition --not new for entanglement-- is thus extended here to
quantum discord. Also, additional dimensions within the parties are considered
({\it qudits}). We also discuss nonlocality (in the form of maximum violation
of a Bell inequality) for all multiqubit systems. The emergence of more
nonlocal states than local ones, all of them possessing maximum entanglement,
will be linked, surprisingly enough, to whether quantum mechanics is defined
over the fields of real or complex numbers.Comment: 13 pages, 5 figures, 2 table
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