1993
DOI: 10.1103/physrevd.48.748
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Sum-over-histories origin of the composition laws of relativistic quantum mechanics and quantum cosmology

Abstract: This paper is concerned with the question of the existence of composition laws in the sum-overhistories approach to relativistic quantum mechanics and quantum cosmology, and its connection with the existence of a canonical formulation. In nonrelativistic quantum mechanics, the propagator is represented by a sum over histories in which the paths move forward in time. The composition law of the propagator then follows from the fact that the paths intersect an intermediate surface of constant time once and only o… Show more

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Cited by 65 publications
(147 citation statements)
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“…the fact that one of their arguments is in the causal future of the other, or in other words the order between these arguments. This order-dependence can be imposed in each of the histories summed over in a clear way using a proper time formulation [3,4]: starting from the same proper time dependent expression g(x 1 , x 2 , T ), the Hadamard function is obtained by integrating over both positive and negative values of the proper time; the resulting amplitude is then a-causal, and does not register any ordering between its arguments; the Feynman propagator is instead obtained restricting this integration to positive proper times only, and this ordering is precisely what makes it causal. What about quantum gravity?…”
Section: Introductionmentioning
confidence: 99%
“…the fact that one of their arguments is in the causal future of the other, or in other words the order between these arguments. This order-dependence can be imposed in each of the histories summed over in a clear way using a proper time formulation [3,4]: starting from the same proper time dependent expression g(x 1 , x 2 , T ), the Hadamard function is obtained by integrating over both positive and negative values of the proper time; the resulting amplitude is then a-causal, and does not register any ordering between its arguments; the Feynman propagator is instead obtained restricting this integration to positive proper times only, and this ordering is precisely what makes it causal. What about quantum gravity?…”
Section: Introductionmentioning
confidence: 99%
“…We discuss first the path integral or sumover-histories realization of Green functions for the relativistic particle, and then how the same idea can be implemented at least at a formal level in the case of quantum gravity in the traditional metric (second order) formalism (most of this section is from [13], but see also [14] for an account of the sum-oev-histories realization of several Green's functions for the relativistic particle). Finally, we outline the analogy with the Barrett-Crane spin foam model, that furnishes the conceptual starting point for our analysis.…”
Section: B Flashback On the Path Integral Realization Of The Projectmentioning
confidence: 99%
“…(2.10)], and all histories contribute to the total transition amplitude, setting the integration range in (2.24) to -∞, +∞ yields the total propagator from x' to x'' and vice versa. 23,24 The classical trajectory emerges through destructive interference between all paths except those for which the phase of the integrand is stationary. 40 We may write eq.…”
Section: B Quantum Description Of the Free Particle As A Constrainedmentioning
confidence: 99%