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Finite no-jump propagator and survival identity
Statement
Assume AC (hence Countable Choice for integration). In the finite GKSL interface set , , , and . A density matrix means a positive matrix of trace one. For a density matrix , let . Then for every , is invertible, , is completely positive, and . If with , then .
Facts & Assumptions
Use finite matrices, density matrices and the finite GKSL conventions. Finite GKSL evolution and the QEC channel interface
Bounded matrix exponentials are differentiable groups, with derivative given by multiplication by their generator. The exponential series of a bounded operator
Integrate continuous scalar or finite-dimensional matrix derivatives on compact intervals; Countable Choice is sufficient. Fundamental theorem of calculus for Banach-valued continuous curves
Adopt AC, including its Countable Choice consequence for the stated integration interface. The Axiom of Choice The Axiom of Countable Choice (AC_ω)
Proof
Given: The matrices and density matrix in the statement, and .
Goal: Establish positivity, the trace derivative, and the survival bounds.
The matrix exponential supplier gives , and . For every positive matrix and every ancilla dimension, conjugation by tensored with the ancilla identity preserves positivity, so is completely positive. In particular is positive and nonzero, since is invertible; its trace is positive.
Differentiate the two finite matrix factors and use cyclicity of trace: . Thus . If , positivity gives , so the derivative of is nonnegative. Integrating this derivative gives . This includes and the empty jump family.
Source notes
Plenio–Knight, Section IV.C, Eqs. (122), (124)–(128), motivates the no-jump/jump split in a cavity example. This item supplies its own finite-matrix argument; no general existence theorem is imported from that example.
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Sources
- M. B. Plenio and P. L. Knight, The quantum-jump approach to dissipative dynamics in quantum optics · Section IV.C, PDF pp. 46–49, Eqs. (120)–(133), especially (122), (124)–(128)