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Classical shadow tomography provides an efficient method for predicting functions of an unknown quantum state from a few measurements of the state.
1904
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1904
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1912
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N. Linden, S. Popescu, and W. K. Wootters, “Almost every pure state of three qubits is completely determined by its two-particle reduced density matrices,” Phys. Rev. Lett. 89
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N. Linden and W. K. Wootters, “The parts determine the whole in a generic pure quantum state,” Phys. Rev. Lett. 89
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Matteo Paris and Jaroslav Rehacek, Quantum state estimation , Vol. 649 (Springer Science & Business Media, 2004)
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Lajos Diósi, “Three-party pure quantum states are determined by two two-party reduced states,” Phys. Rev. A 70
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Benoît Collins and Piotr Śniady, “Integration with Respect to the Haar Measure on Unitary, Orthogonal and Symplectic Group,” Communications in Mathematical Physics 264
2006
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2007
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2007
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2010
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Giacomo Torlai, Guglielmo Mazzola, Juan Carrasquilla, Matthias Troyer, Roger Melko, and Giuseppe Carleo, “Neural-network quantum state tomography,” Nature Physics 14
2018
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2018
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2018
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2018
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2010
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2011
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2011
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2016
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J. Haah, A. W. Harrow, Z. Ji, X. Wu, and N. Yu, “Sample-optimal tomography of quantum states,” IEEE Transactions on Information Theory 63
2017
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2017
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2017
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2017
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2018
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2018
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2018
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2018
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2019
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Jordan Cotler and Frank Wilczek, “Quantum overlapping tomography,” Phys. Rev. Lett. 124
2020
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G.I. Struchalin, Ya. A. Zagorovskii, E.V. Kovlakov, S.S. Straupe, and S.P. Kulik, “Experimental estimation of quantum state properties from classical shadows,” PRX Quantum 2
2021
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2021
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2021
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2021
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