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In
quantum information theory Quantum information is the information of the quantum state, state of a quantum system. It is the basic entity of study in quantum information theory, and can be manipulated using quantum information processing techniques. Quantum information re ...
and
operator theory In mathematics, operator theory is the study of linear operators on function spaces, beginning with differential operators and integral operators. The operators may be presented abstractly by their characteristics, such as bounded linear operat ...
, the Choi–Jamiołkowski isomorphism refers to the correspondence between
quantum channel In quantum information theory, a quantum channel is a communication channel which can transmit quantum information, as well as classical information. An example of quantum information is the state of a qubit. An example of classical information i ...
s (described by
completely positive map In mathematics a positive map is a map between C*-algebras that sends positive elements to positive elements. A completely positive map is one which satisfies a stronger, more robust condition. Definition Let A and B be C*-algebras. A linear m ...
s) and quantum states (described by
density matrices In quantum mechanics, a density matrix (or density operator) is a matrix that describes the quantum state of a physical system. It allows for the calculation of the probabilities of the outcomes of any Measurement in quantum mechanics, measurement ...
), this is introduced by Man-Duen Choi and Andrzej Jamiołkowski. It is also called
channel-state duality In quantum information theory, the channel-state duality refers to the correspondence between quantum channels and quantum states (described by density matrices). Phrased differently, the duality is the isomorphism between completely positive map ...
by some authors in the quantum information area, but mathematically, this is a more general correspondence between positive operators and the complete positive superoperators.


Definition

To study a quantum channel \mathcal from system S to S', which is a trace-preserving completely positive map from operator spaces \mathcal(\mathcal_S) to \mathcal(\mathcal_), we introduce an auxiliary system A with the same dimension as system S. Consider the
maximally entangled state Quantum entanglement is the phenomenon that occurs when a group of particles are generated, interact, or share spatial proximity in a way such that the quantum state of each particle of the group cannot be described independently of the state of ...
: , \Phi^+\rangle=\frac\sum_^, i\rangle\otimes, i\rangle=\frac(, 0\rangle\otimes, 0\rangle+\cdots+, d-1\rangle\otimes, d-1\rangle) in the space of \mathcal_A\otimes\mathcal_S. Since \mathcal is completely positive, (I_A\otimes \mathcal)(, \Phi^+\rangle\langle\Phi^+, ) is a nonnegative operator. Conversely, for any nonnegative operator on \mathcal_A\otimes\mathcal_, we can associate a completely positive map from \mathcal(\mathcal_S)to \mathcal(\mathcal_). This kind of correspondence is called Choi-Jamiołkowski isomorphism.


References

{{DEFAULTSORT:Choi-Jamiolkowski isomorphism Quantum information theory