We study the number of measurements required for quantum process tomography under prior information, such as a promise that the unknown channel is unitary. We introduce the notion of an interactive observable and we show that any unitary channel acting on a d-level quantum system can be uniquely identified among all other channels (unitary or otherwise) with only O(d2) interactive observables, as opposed to the O(d4) required for tomography of arbitrary channels. This result generalizes to the problem of identifying channels with at most q Kraus operators, and slight improvements can be obtained if we wish to identify such a channel only among unital channels or among other channels with q Kraus operators. These results are proven via explicit construction of large subspaces of Hermitian matrices with various conditions on rank, eigenvalues, and partial trace. Our constructions are built upon various forms of totally nonsingular matrices.
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March 2014
Research Article|
March 13 2014
Process tomography for unitary quantum channels
Gus Gutoski;
Gus Gutoski
1
Perimeter Institute for Theoretical Physics
, Waterloo, Ontario N2L 2Y5, Canada
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Nathaniel Johnston
Nathaniel Johnston
2Institute for Quantum Computing,
University of Waterloo
, Waterloo, Ontario N2L 3G1, Canada
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J. Math. Phys. 55, 032201 (2014)
Article history
Received:
October 23 2013
Accepted:
February 17 2014
Citation
Gus Gutoski, Nathaniel Johnston; Process tomography for unitary quantum channels. J. Math. Phys. 1 March 2014; 55 (3): 032201. https://doi.org/10.1063/1.4867625
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