The use of a relational time in quantum mechanics is a framework in which one
promotes to quantum operators all variables in a system, and later chooses one
of the variables to operate like a clock''. Conditional probabilities are computed for variables of the system to take certain values when the clock’’
specifies a certain time. This framework is attractive in contexts where the
assumption of usual quantum mechanics of the existence of an external,
perfectly classical clock, appears unnatural, as in quantum cosmology. Until
recently, there were problems with such constructions in ordinary quantum
mechanics with additional difficulties in the context of constrained theories
like general relativity. A scheme we recently introduced to consistently
discretize general relativity removed such obstacles. Since the clock is now an
object subject to quantum fluctuations, the resulting evolution in the time is
not exactly unitary and pure states decohere into mixed states. Here we work
out in detail the type of decoherence generated, and we find it to be of
Lindblad type. This is attractive since it implies that one can have loss of
coherence without violating the conservation of energy. We apply the framework
to a simple cosmological model to illustrate how a quantitative estimate of the
effect could be computed. For most quantum systems it appears to be too small
to be observed, although certain macroscopic quantum systems could in the
future provide a testing ground for experimental observation.

生成讲解博客的中文版本

生成AI智能校验的中文版本