Statistical mechanics of multipartite entanglement
Giuseppe Florio
Abstract
Entanglement is one of the most intriguing features of quantum
mechanics. It is widely used in quantum communication and
information processing and plays a key role in quantum computation.
At the same time, entanglement is not fully understood. It is deeply
rooted into the linearity of quantum theory and in the superposition
principle and (for pure states) is essentially and intuitively
related to the impossibility of factorizing the state of the total
system in terms of states of its constituents.
The characterization and quantification of entanglement is an open
and challenging problem. It is possible to give a good definition of
bipartite entanglement [1] in terms of the von Neumann entropy and
the entanglement of formation. The problem of defining multipartite
entanglement is more difficult and no unique definition exists [2].
I introduce the notion of maximally multipartite entangled states
(MMES) [3] of $n$ qubits as a generalization of the bipartite case.
Their bipartite entanglement does not depend on the bipartition and
is maximal for all possible bipartitions. Some examples of MMES for
small $n$ are investigated, both analytically and numerically. These
states are the solutions of an optimization problem, that can be
recast in terms of statistical mechanics [4].
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[3] P. Facchi, G. Florio, G. Parisi and S. Pascazio, ``Maximally\
multipartite entangled states" arXiv\:0710.2868 [quant-ph].\
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[4] P. Facchi, G. Florio, U. Marzolino, G. Parisi and S. Pascazio,\
``Statistical mechanics of multipartite entanglement"\
arXiv\:0803.4498 [quant-ph].\
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