Selective and efficient quantum process tomography in arbitrary finite dimension

The characterization of quantum processes is a key tool in quantum information processing tasks for several reasons: on one hand, it allows one to acknowledge errors in the implementations of quantum algorithms; on the other, it allows one to characterize unknown processes occurring in nature. Bende...

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Publicado: 2018
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Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_24699926_v98_n6_p_Perito
http://hdl.handle.net/20.500.12110/paper_24699926_v98_n6_p_Perito
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spelling paper:paper_24699926_v98_n6_p_Perito2023-06-08T16:36:10Z Selective and efficient quantum process tomography in arbitrary finite dimension Quantum optics Set theory Finite dimensions Mutually unbiased basis Quantum algorithms Quantum channel Quantum process Quantum process tomography Quantum-information processing Tensor products Quantum efficiency The characterization of quantum processes is a key tool in quantum information processing tasks for several reasons: on one hand, it allows one to acknowledge errors in the implementations of quantum algorithms; on the other, it allows one to characterize unknown processes occurring in nature. Bendersky, Pastawski, and Paz [A. Bendersky, F. Pastawski, and J. P. Paz, Phys. Rev. Lett. 100, 190403 (2008)PRLTAO0031-900710.1103/PhysRevLett.100.190403; Phys. Rev. A 80, 032116 (2009)PLRAAN1050-294710.1103/PhysRevA.80.032116] introduced a method to selectively and efficiently measure any given coefficient from the matrix description of a quantum channel. However, this method heavily relies on the construction of maximal sets of mutually unbiased bases (MUBs), which are known to exist only when the dimension of the Hilbert space is the power of a prime number. In this article, we lift the requirement on the dimension by presenting two variations of the method that work on arbitrary finite dimensions: one uses tensor products of maximal sets of MUBs, and the other uses a dimensional cutoff of a higher prime power dimension. © 2018 American Physical Society. 2018 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_24699926_v98_n6_p_Perito http://hdl.handle.net/20.500.12110/paper_24699926_v98_n6_p_Perito
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Quantum optics
Set theory
Finite dimensions
Mutually unbiased basis
Quantum algorithms
Quantum channel
Quantum process
Quantum process tomography
Quantum-information processing
Tensor products
Quantum efficiency
spellingShingle Quantum optics
Set theory
Finite dimensions
Mutually unbiased basis
Quantum algorithms
Quantum channel
Quantum process
Quantum process tomography
Quantum-information processing
Tensor products
Quantum efficiency
Selective and efficient quantum process tomography in arbitrary finite dimension
topic_facet Quantum optics
Set theory
Finite dimensions
Mutually unbiased basis
Quantum algorithms
Quantum channel
Quantum process
Quantum process tomography
Quantum-information processing
Tensor products
Quantum efficiency
description The characterization of quantum processes is a key tool in quantum information processing tasks for several reasons: on one hand, it allows one to acknowledge errors in the implementations of quantum algorithms; on the other, it allows one to characterize unknown processes occurring in nature. Bendersky, Pastawski, and Paz [A. Bendersky, F. Pastawski, and J. P. Paz, Phys. Rev. Lett. 100, 190403 (2008)PRLTAO0031-900710.1103/PhysRevLett.100.190403; Phys. Rev. A 80, 032116 (2009)PLRAAN1050-294710.1103/PhysRevA.80.032116] introduced a method to selectively and efficiently measure any given coefficient from the matrix description of a quantum channel. However, this method heavily relies on the construction of maximal sets of mutually unbiased bases (MUBs), which are known to exist only when the dimension of the Hilbert space is the power of a prime number. In this article, we lift the requirement on the dimension by presenting two variations of the method that work on arbitrary finite dimensions: one uses tensor products of maximal sets of MUBs, and the other uses a dimensional cutoff of a higher prime power dimension. © 2018 American Physical Society.
title Selective and efficient quantum process tomography in arbitrary finite dimension
title_short Selective and efficient quantum process tomography in arbitrary finite dimension
title_full Selective and efficient quantum process tomography in arbitrary finite dimension
title_fullStr Selective and efficient quantum process tomography in arbitrary finite dimension
title_full_unstemmed Selective and efficient quantum process tomography in arbitrary finite dimension
title_sort selective and efficient quantum process tomography in arbitrary finite dimension
publishDate 2018
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_24699926_v98_n6_p_Perito
http://hdl.handle.net/20.500.12110/paper_24699926_v98_n6_p_Perito
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