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Fixed Points of Completely Positive Trace-Preserving Maps in Infinite Dimension

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abstract

Completely positive trace-preserving maps $S$, also known as quantum channels, arise in quantum physics as a description of how the density operator $\rho$ of a system changes in a given time interval, allowing not only for unitary evolution but arbitrary operations including measurements or other interaction with an environment. It is known that if the Hilbert space $\mathscr{H}$ that $\rho$ acts on is finite-dimensional, then every $S$ must have a fixed point, i.e., a density operator $\rho_0$ with $S(\rho_0)=\rho_0$. In infinite dimension, $S$ need not have a fixed point in general. However, we prove here the existence of a fixed point under a certain additional assumption which is, roughly speaking, that $S$ leaves invariant a certain set of density operators with bounded ``cost'' of preparation. The proof is an application of the Schauder-Tychonoff fixed point theorem. Our motivation for this question comes from a proposal of Deutsch for how to define quantum theory in a space-time with closed timelike curves; our result supports the viability of Deutsch's proposal.

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representative citing papers

A hierarchy of thermodynamically consistent quantum operations

quant-ph · 2025-05-29 · accept · novelty 7.0

Quantum operations consistent with the weak third law are exactly the strictly positive ones; for the strong third law, channels are exactly the rank non-decreasing ones; fully consistent channels must have a strictly positive fixed state.

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  • A hierarchy of thermodynamically consistent quantum operations quant-ph · 2025-05-29 · accept · none · ref 42 · internal anchor

    Quantum operations consistent with the weak third law are exactly the strictly positive ones; for the strong third law, channels are exactly the rank non-decreasing ones; fully consistent channels must have a strictly positive fixed state.