Abstract
We prove upper bounds on the rate, called "mixing rate", at which the von Neumann entropy of the expected density operator of a given ensemble of states changes under non-local unitary evolution. For an ensemble consisting of two states, with probabil- ities of p and 1 - p, we prove that the mixing rate is bounded above by for any Hamiltonian of norm 1. For a general ensemble of states with probabilities dis- tributed according to a random variable X and individually evolving according to any set of bounded Hamiltonians, we conjecture that the mixing rate is bounded above by a Shannon entropy of a random variable X. For this general case we prove an upper bound that is independent of the dimension of the Hilbert space on which states in the ensemble act.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 986-994 |
| Number of pages | 9 |
| Journal | Quantum Information and Computation |
| Volume | 13 |
| Issue number | 11-12 |
| DOIs | |
| State | Published - 2013 |
All Science Journal Classification (ASJC) codes
- Theoretical Computer Science
- Statistical and Nonlinear Physics
- Nuclear and High Energy Physics
- Mathematical Physics
- General Physics and Astronomy
- Computational Theory and Mathematics
Keywords
- Convex
- Entanglement rate
- Mixing rate
- Von Neumann entropy