2013
DOI: 10.1103/physreva.87.012122
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Selective and efficient quantum state tomography and its application to quantum process tomography

Abstract: We present a method for quantum state tomography that enables the efficient estimation, with fixed precision, of any of the matrix elements of the density matrix of a state, provided that the states from the basis in which the matrix is written can be efficiently prepared in a controlled manner. Furthermore, we show how this algorithm is well suited for quantum process tomography, enabling to perform selective and efficient quantum process tomography.

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Cited by 9 publications
(6 citation statements)
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“…From measurements on these probes, intensive parameters, like temperature, chemical potential, or couplings of Hamiltonians or of dissipators, are infered with a sensitivity given by the inverse of the quantum Fisher Information. Thermal probes are crucial for both fundamental issues and technological applications (Benedict, 1984;Childs, 2001;Giazotto et al, 2006). Estimations with dissipative dynamics (Alipour et al, 2014;Bellomo et al, 2009Bellomo et al, , 2010aZhang and Sarovar, 2015) are also instances of process tomography (Baldwin et al, 2014;Bendersky and Paz, 2013;Merkel et al, 2013;Mohseni et al, 2008) with partial prior knowledge.…”
Section: Thermodynamical and Non-equilibrium Steady Statesmentioning
confidence: 99%
“…From measurements on these probes, intensive parameters, like temperature, chemical potential, or couplings of Hamiltonians or of dissipators, are infered with a sensitivity given by the inverse of the quantum Fisher Information. Thermal probes are crucial for both fundamental issues and technological applications (Benedict, 1984;Childs, 2001;Giazotto et al, 2006). Estimations with dissipative dynamics (Alipour et al, 2014;Bellomo et al, 2009Bellomo et al, , 2010aZhang and Sarovar, 2015) are also instances of process tomography (Baldwin et al, 2014;Bendersky and Paz, 2013;Merkel et al, 2013;Mohseni et al, 2008) with partial prior knowledge.…”
Section: Thermodynamical and Non-equilibrium Steady Statesmentioning
confidence: 99%
“…A Chernoff bound 37,38 can be applied to estimate the number of experimental runs needed to realize a desired precision. 39,40 The possible outcomes of one experimental run are 0 for no projection and 1 if a (0,2) charge state is measured, the expectation value is tr(P j ρ). Repeating this experiment N run times thus leads to a binomial distribution.…”
Section: Estimating the Errormentioning
confidence: 99%
“…Toolkits developed in quantum tomography [22][23][24][25][26][27][28][29][30][31][32][33] have concomitantly evolved into modern schemes appropriate for characterizing those components efficiently. A notable branch of schemes attempt to cope with a large number of qubits by directly estimating quantum properties [34][35][36][37][38][39][40][41][42].…”
Section: Introductionmentioning
confidence: 99%