100 research outputs found
Entanglement of three-qubit Greenberger-Horne-Zeilinger-symmetric states
The first characterization of mixed-state entanglement was achieved for
two-qubit states in Werner's seminal work [Phys. Rev. A 40, 4277 (1989)]. A
physically important extension of this result concerns mixtures of a pure
entangled state (such as the Greenberger-Horne-Zeilinger [GHZ] state) and the
completely unpolarized state. These mixed states serve as benchmark for the
robustness of entanglement. They share the same symmetries as the GHZ state. We
call such states GHZ-symmetric. Despite significant progress their multipartite
entanglement properties have remained an open problem. Here we give a complete
description of the entanglement in the family of three-qubit GHZ-symmetric
states and, in particular, of the three-qubit generalized Werner states. Our
method relies on the appropriate parameterization of the states and on the
invariance of entanglement properties under general local operations. An
immediate application of our results is the definition of a symmetrization
witness for the entanglement class of arbitrary three-qubit states.Comment: 4 pages, 2 figure
Implementation of the Deutsch-Jozsa algorithm with Josephson charge qubits
We investigate the realization of a simple solid-state quantum computer by
implementing the Deutsch-Jozsa algorithm in a system of Josephson charge
qubits. Starting from a procedure to carry out the one-qubit Deutsch-Jozsa
algorithm we show how the N-qubit version of the Bernstein-Vazirani algorithm
can be realized. For the implementation of the three-qubit Deutsch-Jozsa
algorithm we study in detail a setup which allows to produce entangled states.Comment: accepted for publication in Journal of Modern Optic
Monogamy equalities for qubit entanglement from Lorentz invariance
A striking result from nonrelativistic quantum mechanics is the monogamy of
entanglement, which states that a particle can be maximally entangled only with
one other party, not with several ones. While there is the exact quantitative
relation for three qubits and also several inequalities describing monogamy
properties it is not clear to what extent exact monogamy relations are a
general feature of quantum mechanics. We prove that in all many-qubit systems
there exist strict monogamy laws for quantum correlations. They come about
through the curious relation between the nonrelativistic quantum mechanics of
qubits and Minkowski space. We elucidate the origin of entanglement monogamy
from this symmetry perspective and provide recipes to construct new families of
such equalities.Comment: 4 pages, 3 figure
Partial transpose as a direct link between concurrence and negativity
Detection of entanglement in bipartite states is a fundamental task in
quantum information. The first method to verify entanglement in mixed states
was the partial-transpose criterion. Subsequently, numerous quantifiers for
bipartite entanglement were introduced, among them concurrence and negativity.
Surprisingly, these quantities are often treated as distinct or independent of
each other. The aim of this contribution is to highlight the close relations
between these concepts, to show the connections between seemingly independent
results, and to present various estimates for the mixed-state concurrence
within the same framework.Comment: 10 pages, 3 figure
Advanced control with a Cooper-pair box: stimulated Raman adiabatic passage and Fock-state generation in a nanomechanical resonator
The rapid experimental progress in the field of superconducting nanocircuits
gives rise to an increasing quest for advanced quantum-control techniques for
these macroscopically coherent systems. Here we demonstrate theoretically that
stimulated Raman adiabatic passage (STIRAP) should be possible with the
quantronium setup of a Cooper-pair box. The scheme appears to be robust against
decoherence and should be realizable even with the existing technology. As an
application we present a method to generate single-phonon states of a
nanomechnical resonator by vacuum-stimulated adiabatic passage with the
superconducting nanocircuit coupled to the resonator
Maximum N-body correlations do not in general imply genuine multipartite entanglement
The existence of correlations between the parts of a quantum system on the one hand, and entanglement between them on the other, are different properties. Yet, one intuitively would identify strong N-party correlations with N-party entanglement in an N-partite quantum state. If the local systems are qubits, this intuition is confirmed: The state with the strongest N-party correlations is the Greenberger-Horne-Zeilinger (GHZ) state, which does have genuine multipartite entanglement. However, for high-dimensional local systems the state with strongest N-party correlations may be a tensor product of Bell states, that is, partially separable. We show this by introducing several novel tools for handling the Bloch representation
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