id	author	title	date	pages	extension	mime	words	sentences	flesch	summary	cache	txt
work_visjxrhh6bf4jjlalvcchkeiui	W. C. Myrvold	Relativistic Quantum Becoming	2003	44	.pdf	application/pdf	12232	752	64	account of the world unfolding in time, I am accepting, with Albert, that the quantummechanical state description is, or ought to be, a representation of the state of a system, and not operator), we cannot give a quantum-mechanical account of the state of the system.6 condition in a quantum context, what we will require is that differences in states on distinct We will demand that state transitions satisfy the local evolution condition: obtainable from the state ρ(σ) via an operation local to the region Γ between the two quantum field theories exhibit what Albert calls dynamical compatibility with special relativity, and this state transition is a selective operation local to the region in which the measurement state transitions from one hypersurface to another are solely the result of local operations. With or without collapse, relativizing quantum states to spacelike hypersurfaces is not a merely	./cache/work_visjxrhh6bf4jjlalvcchkeiui.pdf	./txt/work_visjxrhh6bf4jjlalvcchkeiui.txt