"The idea behind the Feynman path integral goes back to a paper by P. A. M. Dirac published in 1933 in Physikalische Zeitschrift der Sowjetunion. It formed the core of Richard Feynman’s space–time approach to quantum mechanics and quantum electrodynamics. Although the path integral was not mathematically well defined, it was widely used in quantum field theory, statistical mechanics, and string theory. Recently, path integrals have been the guide to spectacular developments in pure mathematics."
Quote Details
Added by wikiquote-import-bot
Unverified quote
0 likes
Original Language: English
Available Languages (1)
Sources
Meinhard E. Mayer:
https://en.wikiquote.org/wiki/Statistical_mechanics
Revision History
No revisions have been submitted for this quote.
Categories
Statistical mechanics
27 quotes on TrueQuotesView all quotes by Statistical mechanics →
Related Quotes
"With the growing importance of models in statistical mechanics and in field theory, the path integral method of Feynm…"
"You should call it entropy, for two reasons. In the first place your uncertainty function has been used in statistica…"
"There is an interesting analogy... with the philosophy of the natural sciences, which has flourished under the combin…"
"Another crucial point is that MOND as we know it now is arguably only an approximate 'effective field theory' that ap…"
"The need for a fundamentally different approach to the study of physical processes at the molecular level motivated t…"
"The kinetic theory of gases is a small branch of physics which has passed from the stage of excitement and novelty in…"
"As the natural sciences have developed to encompass increasingly s, scientific rationality has become ever more stati…"
"The rapid development of quantum mechanics stimulated research in and theory. Initiated during the mid-twenties, inte…"
"The path integral is a formulation of quantum mechanics equivalent to the standard formulations, offering a new way o…"
"Carnot's Principle. ...If physical phenomena were due exclusively to the movements of atoms whose mutual attraction d…"