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Communication in Statistics- Theory and Methods

Quantum mutual entropy in terms of local quantum Bernoulli noises

Qi Han, Yanan Han, Yaxin Kou, Ziqiang Lu

Published May 2, 2021• 13 citations
Publisher

Abstract

Localization of quantum Bernoulli noises(LQBNs) are the family of local annihilation and local creation operator acting on Bernoulli functionals. In this paper, we give the local quantum mutual entropy I(ρk;Λ*) based on the local quantum entropy S(ρk). Furthermore, we demonstrate that this quantum mutual entropy I(ρk;Λ*) also has the basic properties.

DOI
10.1080/03610926.2021.1916532

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Localization of quantum Bernoulli noises(LQBNs) are the family of local annihilation and local creation operator acting on Bernoulli functionals. In this paper, we give the local quantum mutual entropy I(ρk;Λ*) based on the local quantum entropy S(ρk). Furthermore, we demonstrate that this quantum mutual entropy I(ρk;Λ*) also has the basic properties.
Localization of quantum Bernoulli noises (LQBNs) are the family of local annihilation and local creation operators acting on Bernoulli functionals. In this paper, we construct a density operator ρk represented by LQBNs, and define a new quantum entropy S(ρk) based on LQBNs. Furthermore, we demonstrate that this quantum entropy S(ρk) also has the basic properties of von Neumann entropy, such as concavity, subadditivity, and nonnegativity. In particular, we obtain the necessary and sufficient condition for S(ρk)=k.
Local Quantum Bernoulli Noises (LQBNs) is the localization of Quantum Bernoulli Noises (QBNs), which has high research value in the field of quantum information and has received widespread attention in recent years. In this paper, a new entropy exchange and coherent information with localization characteristics are studied. According to the quantum channel constructed by LQBNs, the relationship between coherent information and coherent mutual entropy with localization characteristics is proved. Finally, we also prove that the coherent information based on LQBNs may disappear.
Abstract In the era of rapid development of quantum mechanics, some issues in the field of quantum information have become increasingly important. Local quantum Bernoulli noises (LQBNs) is a localized Bernoulli functional, and it is the localization of quantum Bernoulli noises (QBNs). The distinctive feature of LQBNs lies in its localization properties, which make it highly valuable in the field of quantum information. In this paper, we study three new types of quantum conditional entropy with localization characteristics from three dimensions: local quantum conditional entropy, local quantum conditional entropy at the same position, and classical-quantum conditional entropy. Based on the locality of LQBNs, we prove that the local quantum conditional entropy is concave and unitary invariant. Surprisingly, we find that the local quantum mutual information (entropy) corresponding to the same position is 0. The local quantum conditional entropy defined based on the local quantum state at a specific position, proposed in this paper, provides new insights into understanding the impact of local quantum noise on the information transmission in quantum channels. This discovery not only deepens our understanding of the internal structure of local quantum entropy, but also reveals its influence on the performance of quantum communication.
Quantum noise has always been an important issue in the field of quantum information transmission. As the localization of quantum noise, local quantum Bernoulli noises (LQBNs) have attracted extensive attention in recent years. In this paper, the quantum conditional entropy based on LQBNs is deeply discussed, and a new definition of quantum conditional entropy is given. Then we find that this quantum conditional entropy has some basic properties such as concavity, conditional reduced entropy and unitary invariance. This research is of great significance to the field of quantum information, which can help us to understand the influence of local quantum noises on quantum information transmission.
In this paper we show that annihilation and creation operators on the space of Bernoulli functionals in discrete time can be naturally interpreted as discrete-time quantum Bernoulli noises (QBNs). We first examine their algebraic properties and prove among other things that the family of annihilation-creation sum operators generates a commutative group of unitary operators. Additionally, then by using QBN we prove an operator version of the discrete-time Clark formula. We also obtain a QBN-based necessary and sufficient condition for an operator process to be adapted. We define integrals of adapted operator processes with respect to QBN and show their operator martingale property. Finally, we give a representation formula for operators on the space of Bernoulli functionals.
Quantum Bernoulli noises (QBNs) are the family of annihilation and creation operators acting on Bernoulli functionals, which can describe a two-level quantum system with infinitely many sites. In this paper, we consider the problem to construct quantum Markov semigroups (QMSs) directly from QBNs. We first establish several new theorems concerning QBNs. In particular, we define the number operator acting on Bernoulli functionals by using the canonical orthonormal basis, prove its self-adjoint property, and describe precisely its connections with QBN in a mathematically rigorous way. We then show the possibility to construct QMS directly from QBN. This is done by combining the general results on QMS with our new results on QBN obtained here. Finally, we examine some properties of QMS constructed from QBN.