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Lectures on Quantum Mechanics (1)

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Lectures on Quantum Mechanics (1)

0Lectures OH Quantum MechanicsPAUL A. M. DIRACAll rights reserved under Pan American and International Copyright ( onvemions.p ibl io graph if. a I No

Lectures on Quantum Mechanics (1) oteThis Dover edition, first published in 2001. is an unabridged reprint of I he work originally published by the Belter Graduate School of Science. Y

eshiva University, New York, in 1964.Library oj Congress Cataloging-in-Publication DataDirac, p. A. M. (Paul Adrien Maurice). 1902-Lectures on quantum Lectures on Quantum Mechanics (1)

mechanics / by Paul A M. Dirac.p. cm.Originally published: New York : Beller Graduate School of Science.Yeshiva University. 1964.ISBN 0-486-41713-1 (

Lectures on Quantum Mechanics (1)

pbk.)I. Quantum theory. I. Title.QC174.125 .D55 2001530.12 —dc2100-065608Manufactured in the United States of AmericaDover Publications. Inc.. 31 East

0Lectures OH Quantum MechanicsPAUL A. M. DIRACAll rights reserved under Pan American and International Copyright ( onvemions.p ibl io graph if. a I No

Lectures on Quantum Mechanics (1) d Surfaces444. Quantization on Flat Surfaces67www.pdfgrip.comDR. DIRACLecture No. 1THE HAMILTONIAN METHODI’m very happy to be here at Yeshiva and to h

ave this chance to talk to yon about some mathematical methods that I have been working on for a number of years. I would like first to describe in a Lectures on Quantum Mechanics (1)

few words the general object of these methods.In atomic theory we have to deal with various fields. There are some fields which are very familiar, lik

Lectures on Quantum Mechanics (1)

e the electromagnetic and the gravitational fields; but in recent times we have a number of other fields also to concern ourselves with, because accor

0Lectures OH Quantum MechanicsPAUL A. M. DIRACAll rights reserved under Pan American and International Copyright ( onvemions.p ibl io graph if. a I No

Lectures on Quantum Mechanics (1) ve in atomic physics the general problem of setting up a theory of various fields in interaction with each other. We need a theory conforming to the p

rinciples of quantum mechanics, but it is quite a difficult matter to get such a theory.One can get a much simpler theory if one goes over to the corr Lectures on Quantum Mechanics (1)

esponding classical mechanics, which is the form which quantum mechanics takes when one makes Planck’s constant h tend to zero. It is very much easier

Lectures on Quantum Mechanics (1)

to visualize what one is doing in terms of classical______[I]www.pdfgrip.com

0Lectures OH Quantum MechanicsPAUL A. M. DIRACAll rights reserved under Pan American and International Copyright ( onvemions.p ibl io graph if. a I No

0Lectures OH Quantum MechanicsPAUL A. M. DIRACAll rights reserved under Pan American and International Copyright ( onvemions.p ibl io graph if. a I No

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