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Absolutely maximally entangled state

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The absolutely maximally entangled (AME) state is a concept in quantum information science, which has many applications in quantum error-correcting code[1], discrete AdS/CFT correspondence[2], and AdS/CMT correspondence[2], etc.

Definition

The bipartite maximally entangled states is the one that the reduced density operators are maximally mixed, i.e., . Typical examples are Bell states.

A multipartite state of a system is called called absolutely maximally entangled if for any bipartition of , the reduced density operator is maximally mixed , where .

Property

The AME state does not always exit, in some give local dimension and number of party, there is no AME state. For a table of AME state in low dimensions, see table of AME states.

References

  1. ^ Goyeneche, Dardo; Alsina, Daniel; Latorre, José I.; Riera, Arnau; Życzkowski, Karol (2015-09-15). "Absolutely maximally entangled states, combinatorial designs, and multiunitary matrices". Physical Review A. 92 (3): 032316. doi:10.1103/PhysRevA.92.032316.
  2. ^ a b Pastawski, Fernando; Yoshida, Beni; Harlow, Daniel; Preskill, John (2015-06-23). "Holographic quantum error-correcting codes: toy models for the bulk/boundary correspondence". Journal of High Energy Physics. 2015 (6): 149. doi:10.1007/JHEP06(2015)149. ISSN 1029-8479.