2020
DOI: 10.1088/1742-6596/1612/1/012011
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New correlation relations in classical and quantum systems with different numbers of subsystems1

Abstract: We present a review of the general approach to the problem of correlations in classical statistics and quantum statistics of systems with different numbers of subsystems and demonstrate the information-entropic relations for systems without subsystems recently obtained for Shannon entropies. We present the example of a single-qudit state corresponding to the N-level atom, consider explicitly the qutrit state, and show that qutrit can be interpreted as a set of several qubits. For each of these qubits, there ex… Show more

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Cited by 6 publications
(4 citation statements)
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“…In this formalism, it is possible to use the probability representation of quantum states [16,20,[36][37][38][39] and expressions of quantum states in terms of the Jordan-Schwinger map [40,41], where the spin states are given in the form of two-mode oscillator wave functions. This so-called Hermite polynomial representation of spin states [42][43][44] is formulated as the probability distribution of oscillator quantum states.…”
Section: Discussionmentioning
confidence: 99%
“…In this formalism, it is possible to use the probability representation of quantum states [16,20,[36][37][38][39] and expressions of quantum states in terms of the Jordan-Schwinger map [40,41], where the spin states are given in the form of two-mode oscillator wave functions. This so-called Hermite polynomial representation of spin states [42][43][44] is formulated as the probability distribution of oscillator quantum states.…”
Section: Discussionmentioning
confidence: 99%
“…We can therefore consider the equality ( 53 ) as a realization of the inequality ( 54 ) for two identical qubits in state ( 46 ) at . Furthermore, the relation ( 53 ) can be treated as the Born rule for two qubits [ 66 , 67 , 68 ].…”
Section: Representation Of the Density Matrix In The Qutrit Subspacementioning
confidence: 99%
“…The coherent state tomogram at t = 0 is given by Eqs. ( 25)- (27). Employing the replacement μ → μ and ν → ν + μt in all formulas for the ground and coherent states of the oscillator and the Schrödinger cat state, we arrive at the results for tomograms of the corresponding free-particle states.…”
Section: The Evolution Of Free-particle Cat Statesmentioning
confidence: 99%
“…where tomograms w ±α 1 and w ±α 2 are probability distributions of two oscillators given by Eqs. ( 25)- (27). We can also consider the wave function of the form…”
Section: Cat States Of Two Oscillatorsmentioning
confidence: 99%