Difference between revisions of "Feynman Least Action Thesis"
(→Context) |
(→Context) |
||
| (4 intermediate revisions by the same user not shown) | |||
| Line 1: | Line 1: | ||
==Full Title== | ==Full Title== | ||
| − | The Principle of Least Action in Quantum Mechanics<ref>Richard P. Feynman, ''The Principle of Least Action in Quantum Mechanics'', Princeton University 1942, reprinted in ''Feynman's Thesis'', Ed Laurie M. Brown, 2005 ISBN 9789812563804</ref> was Feynman's 1942 PhD thesis. | + | The Principle of [[Least Action]] in Quantum Mechanics<ref>Richard P. Feynman, ''The Principle of Least Action in [[Quantum Mechanics]]'', Princeton University 1942, reprinted in ''Feynman's Thesis'', Ed Laurie M. Brown, 2005 ISBN 9789812563804</ref> was Feynman's 1942 PhD thesis. |
==Context== | ==Context== | ||
This thesis introduced the ideas that came to be known as the [https://en.m.wikipedia.org/wiki/Wheeler%E2%80%93Feynman_absorber_theory | This thesis introduced the ideas that came to be known as the [https://en.m.wikipedia.org/wiki/Wheeler%E2%80%93Feynman_absorber_theory | ||
Wheeler–Feynman absorber theory (also called the Wheeler–Feynman time-symmetric theory) | Wheeler–Feynman absorber theory (also called the Wheeler–Feynman time-symmetric theory) | ||
| − | ]derived from the assumption that the solutions of the electromagnetic | + | ]derived from the assumption that the solutions of the electromagnetic [[Field]] equations must be invariant under time-reversal transformation, as are the field equations themselves. Indeed, there is no apparent reason for the time-reversal symmetry breaking, |
| − | Maxwell's equations and the equations for electromagnetic waves have, in general, two possible solutions: a retarded (delayed) solution and an advanced one. | + | Maxwell's equations and the equations for electromagnetic waves have, in general, two possible solutions: a retarded (delayed) solution and an advanced one. This symmetry can be viewed as the primary distinction between the laws of physics versus the common sense laws or time as we experience it. |
==References== | ==References== | ||
Latest revision as of 00:05, 18 December 2023
Full Title
The Principle of Least Action in Quantum Mechanics[1] was Feynman's 1942 PhD thesis.
Context
This thesis introduced the ideas that came to be known as the [https://en.m.wikipedia.org/wiki/Wheeler%E2%80%93Feynman_absorber_theory Wheeler–Feynman absorber theory (also called the Wheeler–Feynman time-symmetric theory) ]derived from the assumption that the solutions of the electromagnetic Field equations must be invariant under time-reversal transformation, as are the field equations themselves. Indeed, there is no apparent reason for the time-reversal symmetry breaking, Maxwell's equations and the equations for electromagnetic waves have, in general, two possible solutions: a retarded (delayed) solution and an advanced one. This symmetry can be viewed as the primary distinction between the laws of physics versus the common sense laws or time as we experience it.
References
- ↑ Richard P. Feynman, The Principle of Least Action in Quantum Mechanics, Princeton University 1942, reprinted in Feynman's Thesis, Ed Laurie M. Brown, 2005 ISBN 9789812563804
Other Material
- See wiki page on the Eventful Universe
- You Tube Video for novices.
