Returning to Cornell, he gave a lecture on the subject, which I attended. Now, there is no unique way to make a quantum theory from classical mechanics, although all the textbooks make believe there is. The next day at the meeting, I saw Slotnick and said, “Slotnick, I worked it out last night, I wanted to see if I got the same answers you do. The Nobel Prize in Physics 1965, Born: 11 May 1918, New York, NY, USA, Died: 15 February 1988, Los Angeles, CA, USA, Affiliation at the time of the award: California Institute of Technology (Caltech), Pasadena, CA, USA, Prize motivation: "for their fundamental work in quantum electrodynamics, with deep-ploughing consequences for the physics of elementary particles.".
I just changed the delta to an f, just as I would for the classical case.
Do you have one too?”.
Feynman didn’t even know what Dirac meant. Now, this has the attractive feature that it solves both problems at once. His calculation concerned the coefficient of spontaneous emission of an atom. For he then went on to give a lecture as though he had worked this all out before and was completely prepared, but he had not, he worked it out as he went along. and just calculated things out by Taylor series expansion, out came the Schrödinger equation. I don’t know, let’s assume they come back without an index – then, there will be a gradual shifting in phase between the return and the original signal so that we would only have to figure that the contributions act as if they come from only a finite thickness, that of the first wave zone. He had the courage to simply guess at the form of an equation, the equation we now call the Dirac equation, and to try to interpret it afterwards. I said, “that’s the momentum transferred by the electron, the electron deflected by different angles.” “Oh”, he said, “no, I only have the limiting value as Q approaches zero; the forward scattering.” Well, it was easy enough to just substitute Q equals zero in my form and I then got the same answers as he did. “It struck Feynman that everyone had a favorite principle or theory and he was violating them all” — Gleick (1992). That is, if you took the probability that this would happen and that would happen – everything you could think of would happen, it would not add up to one. Perhaps a thing is simple if you can describe it fully in several different ways without immediately knowing that you are describing the same thing. But that inertia-like term was infinite for a point-charge. You have no clue of precisely what function to put in for f, but it was an interesting possibility to keep in mind when developing quantum electrodynamics.
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