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arXiv · 1407.2146

Device independent Schmidt rank witness by using Hardy paradox

Amit Mukherjee·Arup Roy·Some Sankar Bhattacharya·Subhadipa Das·Md. Rajjak Gazi·Manik Banik
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Abstract

Schmidt rank of bipartite pure state serves as a testimony of entanglement. It is a monotone under local operation + classical communications (LOCC) and puts restrictions in LOCC convertibility of quantum states. Identifying the Schmidt rank of an unknown quantum state therefore seek importance from information theoretic perspective. In this work it is shown that a modified version of Hardy's argument, which reveals the contradiction of quantum theory with local realism, turns out to be useful for inspecting the minimal Schmidt rank of the unknown state and hence also the minimal dimension of the system. Use of Hardy's test in such task provides a practical advantage: the Schmidt rank can be determined without knowing the detailed functioning of the experimental devices i.e., Hardy's test suffices to be a device independent Schmidt rank witness.

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Amit Mukherjee, Arup Roy, Some Sankar Bhattacharya, Subhadipa Das, Md. Rajjak Gazi, Manik Banik. 2014-07-08. Device independent Schmidt rank witness by using Hardy paradox. https://arxiv.org/abs/1407.2146

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