Let and introduce an isomorphic reference system . Choose a basis and the maximally entangled stateComplete positivity makesa positive density operator. This is the normalized Choi matrix, with the reference placed first. Its spectral decomposition can be writtenThe number is at most .
Here an index state is a chosen basis vector in the reference. The corresponding relative state of is the generally unnormalized vectorThus . Define a linear map by its columns:Then , soExpand both sides in reference matrix units. The block with reference indices on the left is ; on the right it is . Since matrix units span all operators and is linear,This constructs the Kraus representation explicitly from the relative states, rather than assuming it.
Finally, trace preservation implies for every density operator thatTaking every rank-one orthogonal projection as forces the Hermitian operator in brackets to have the same quadratic form as the identity. ThereforeThe argument is finite-dimensional, as appropriate to the quantum-information setting; a channel with a different output dimension has the same construction with rectangular Kraus operators.
Fix a basis for the transposition map . If , write . ThenThus transposition is a positive linear map and also preserves the trace.
For dimension , apply it to one subsystem of the maximally entangled state from part (a):where is the swap operator, . It satisfies and , so its eigenvalues are on symmetric vectors and on antisymmetric vectors. In particular,A positive input has therefore acquired a negative expectation value after adjoining an identity channel. Transposition is positive but not completely positive in dimension at least two. The one-dimensional case is the identity map and is completely positive; the dimension qualification is necessary.
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