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Springer proceedings in mathematics

A Dynamical Point of View of Quantum Information: Entropy and Pressure

Alexandre Baraviera, Carlos F. Lardizabal, Artur Oscar Lopes, Marcelo Terra Cunha

Published Jan 1, 2011• 2 citations
Publisher
DOI
10.1007/978-3-642-11456-4_7

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Quantum Information is a new area of research which has been growing rapidly since the last decade. This topic is very close to potential applications to the so called Quantum Computer. In our point of view it makes sense to develop a more "dynamical point of view" of this theory. We want to consider the concepts of entropy and pressure for "stationary systems" acting on density matrices which generalize the usual ones in Ergodic Theory (in the sense of the Thermodynamic Formalism of R. Bowen, Y. Sinai and D. Ruelle). We consider the operator $\mathcal{L}$ acting on density matrices $ρ\in \mathcal{M}_N$ over a finite $N$-dimensional complex Hilbert space $\mathcal{L}(ρ):=\sum_{i=1}^k tr(W_iρW_i^*)V_iρV_i^*,$ where $W_i$ and $V_i$, $i=1,2,... k$ are operators in this Hilbert space. $\mathcal{L}$ is not a linear operator. In some sense this operator is a version of an Iterated Function System (IFS). Namely, the $V_i (.) V_i^*=:F_i(.)$, $i=1,2,...,k$, play the role of the inverse branches (acting on the configuration space of density matrices $ρ$) and the $W_i$ play the role of the weights one can consider on the IFS. We also analyze the discrete Wigner function. We suppose that for all $ρ$ we have that $\sum_{i=1}^k tr(W_iρW_i^*)=1$. A family $W:=\{W_i\}_{i=1,..., k}$ determines a Quantum Iterated Function System (QIFS) $\mathcal{F}_{W}$, $\mathcal{F}_W=\{\mathcal{M}_N,F_i,W_i\}_{i=1,..., k}.$

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Quantum Information is a new area of research which has been growing rapidly since the last decade. This topic is very close to potential applications to the so called Quantum Computer. In our point of view it makes sense to develop a more "dynamical point of view" of this theory. We want to consider the concepts of entropy and pressure for "stationary systems" acting on density matrices which generalize the usual ones in Ergodic Theory (in the sense of the Thermodynamic Formalism of R. Bowen, Y. Sinai and D. Ruelle). We consider the operator L\mathcal{L}L acting on density matrices ρ∈MNρ\in \mathcal{M}_Nρ∈MN​ over a finite NNN-dimensional complex Hilbert space L(ρ):=∑i=1ktr(WiρWi∗)ViρVi∗,\mathcal{L}(ρ):=\sum_{i=1}^k tr(W_iρW_i^*)V_iρV_i^*,L(ρ):=∑i=1k​tr(Wi​ρWi∗​)Vi​ρVi∗​, where WiW_iWi​ and ViV_iVi​, i=1,2,...ki=1,2,... ki=1,2,...k are operators in this Hilbert space. L\mathcal{L}L is not a linear operator. In some sense this operator is a version of an Iterated Function System (IFS). Namely, the Vi(.)Vi∗=:Fi(.)V_i (.) V_i^*=:F_i(.)Vi​(.)Vi∗​=:Fi​(.), i=1,2,...,ki=1,2,...,ki=1,2,...,k, play the role of the inverse branches (acting on the configuration space of density matrices ρρρ) and the WiW_iWi​ play the role of the weights one can consider on the IFS. We also analyze the discrete Wigner function. We suppose that for all ρρρ we have that ∑i=1ktr(WiρWi∗)=1\sum_{i=1}^k tr(W_iρW_i^*)=1∑i=1k​tr(Wi​ρWi∗​)=1. A family W:={Wi}i=1,...,kW:=\{W_i\}_{i=1,..., k}W:={Wi​}i=1,...,k​ determines a Quantum Iterated Function System (QIFS) FW\mathcal{F}_{W}FW​, FW={MN,Fi,Wi}i=1,...,k.\mathcal{F}_W=\{\mathcal{M}_N,F_i,W_i\}_{i=1,..., k}.FW​={MN​,Fi​,Wi​}i=1,...,k​.
The notion of information in quantum mechanics has traditionally been viewed through the lens of entropy, mutual information, and measurement back‑action. In this work we introduce a new concept, Quantum Measurement Information Pressure (QMIP), which quantifies the effective mechanical or energetic pressure exerted by the informational change that occurs during a quantum measurement. QMIP is defined as the derivative of the measurement‑induced informational entropy with respect to an effective measurement volume or a parameter that governs the coupling between the system and the measuring apparatus. We present a detailed mathematical formulation of QMIP, discuss its physical interpretation in terms of work extraction and feedback control, and outline potential experimental realizations in quantum feedback systems. By bridging the gap between information theory and physical forces at the quantum scale, QMIP offers a fresh perspective on the thermodynamic cost of quantum measurement and suggests pathways towards high‑impact applications, possibly deserving recognition at the Nobel level.
The theories of noncommutative dynamical entropy and quantum symbolic dynamics for quantum-dynamical systems are analyzed from the point of view of quantum information theory. Using a general quantum-dynamical system as a communication channel, one can define different classical capacities depending on the character of resources applied for encoding and decoding procedures and on the type of information sources. It is shown that for Bernoulli sources, the entanglement-assisted classical capacity, which is the largest one, is bounded from above by the quantum-dynamical entropy defined in terms of operational partitions of unity. Stronger results are proved for the particular class of quantum-dynamical systems---quantum Bernoulli shifts. Different classical capacities are exactly computed and the entanglement-assisted one is equal to the dynamical entropy in this case.