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Note
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By complete set of observables one means the maximal set of linearly independent observables (where the trivial observable represented by identity operator is excluded). A set which does not fulfil the above conditions is called incomplete one.
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14
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0040571625
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Throughout this paper we will use the base-2 logarithm rather than natural one
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Throughout this paper we will use the base-2 logarithm rather than natural one.
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0000847290
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See e.g. V. Bužek, G. Drobný, G. Adam, R. Derka, P. L. Knight: J. Mod. Opt. 44 (1997) 2607; for an extensive presentation of the use of Jaynes principle see W. T. Grandy, Am. J. Phys 65 (1997) 466
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0000847290
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See e.g. V. Bužek, G. Drobný, G. Adam, R. Derka, P. L. Knight: J. Mod. Opt. 44 (1997) 2607; for an extensive presentation of the use of Jaynes principle see W. T. Grandy, Am. J. Phys 65 (1997) 466
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R. Jozsa (unpublished); Hoi-Kwong Lo: Opt. Commun. 119 (1995) 552; A. E. Allahverdyan, D. B. Saakian: Los Alamos e-print quant-ph/9702034
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Note
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⊗N. However, to prove the lemma one does not need to make such an assumption.
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private communication
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R. Jozsa: private communication.
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Jozsa, R.1
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