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| | Quantum information in base $n$ defined by state partitions |
 | | In this particular case, the F's can be identified with certain projection operators from the set of all possible mutually orthogonal ones, whose two eigenvalues can be identified with the two states. |
 | | Measurement of the propositions, ``the particle is in state {1,2,3}'' and, ``the particle is in state {3,6,9}'' can be evaluated by taking the set theoretic intersection of the respective sets; i.e., by the proposition, ``the particle is in state {1,2,3} |
 | | We obtain k partitions of the product states with n elements per partition in such a way that every single product state is obtained by the set theoretic intersection of k elements of all the different partitions. |
| tph.tuwien.ac.at /~svozil/publ/2002-statepart-prl.htm (1748 words) |
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