The strange equation of quantum gravity
... T1 (t), T2 (t), where t is an arbitrary parameter, which can be chosen freely. The coordinates (t, ~x) in the argument of the gravitational field gµν (~x, t) are arbitrary parameters of this sort. This manner of describing evolution is more general than giving the evolution in a preferred time param ...
... T1 (t), T2 (t), where t is an arbitrary parameter, which can be chosen freely. The coordinates (t, ~x) in the argument of the gravitational field gµν (~x, t) are arbitrary parameters of this sort. This manner of describing evolution is more general than giving the evolution in a preferred time param ...
Abstracts
... ABSTRACT: In this talk we address two questions related to repeated measurements performed in unstable systems in the limit of infinite frequency limit. The first one concerns the Zeno dynamics discussed in several contributions to this conference. Given an unstable system we have two ways to achiev ...
... ABSTRACT: In this talk we address two questions related to repeated measurements performed in unstable systems in the limit of infinite frequency limit. The first one concerns the Zeno dynamics discussed in several contributions to this conference. Given an unstable system we have two ways to achiev ...
Chapter 1 Introduction to Recursive Methods
... c0 (k) = f (k)−k hence describes the curve along which capital is time constant. Moreover notice, that given kt next period capital kt+1 is decreasing in ct . For consumption values above the curve c0 , capital must decrease, while when the chosen c is below this curve, one has kt+1 > kt . If f (0) ...
... c0 (k) = f (k)−k hence describes the curve along which capital is time constant. Moreover notice, that given kt next period capital kt+1 is decreasing in ct . For consumption values above the curve c0 , capital must decrease, while when the chosen c is below this curve, one has kt+1 > kt . If f (0) ...
