Bounds on probability of transformations between multipartite pure states

W Cui, W Helwig, HK Lo - Physical Review A—Atomic, Molecular, and Optical …, 2010 - APS
W Cui, W Helwig, HK Lo
Physical Review A—Atomic, Molecular, and Optical Physics, 2010APS
For a tripartite pure state of three qubits, it is well known that there are two inequivalent
classes of genuine tripartite entanglement, namely the Greenberger-Horne-Zeilinger (GHZ)
class and the W class. Any two states within the same class can be transformed into each
other with stochastic local operations and classical communication with a nonzero
probability. The optimal conversion probability, however, is only known for special cases.
Here, lower and upper bounds are derived for the optimal probability of transformation from …
For a tripartite pure state of three qubits, it is well known that there are two inequivalent classes of genuine tripartite entanglement, namely the Greenberger-Horne-Zeilinger (GHZ) class and the W class. Any two states within the same class can be transformed into each other with stochastic local operations and classical communication with a nonzero probability. The optimal conversion probability, however, is only known for special cases. Here, lower and upper bounds are derived for the optimal probability of transformation from a GHZ state to other states of the GHZ class. A key idea in the derivation of the upper bounds is to consider the action of the local operations and classical communications (LOCC) protocol on a different input state, namely , and to demand that the probability of an outcome remains bounded by 1. We also find an upper bound for more general cases by using the constraints of the so-called interference term and 3-tangle. Moreover, some of the results are generalized to the case in which each party holds a higher dimensional system. In particular, the GHZ state generalized to three qutrits; that is, shared among three parties can be transformed to any tripartite three-qubit pure state with probability 1 via LOCC. Some of our results can also be generalized to the case of a multipartite state shared by more than three parties.
American Physical Society
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