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Work at Chicago. Pseudo-scalar meson theory
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Work at Chicago. Pseudo-scalar meson theory
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35. The atmosphere at Princeton. Getting a job in Chicago | 1834 | 03:03 | |
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37. Fermi | 2933 | 04:16 | |
38. Work at Chicago. Pseudo-scalar meson theory | 1408 | 03:56 | |
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40. Discussions with Enrico Fermi; resonance and symmetry | 2196 | 01:55 |
He kept a little notebook with useful formulae, which were all exact–perfect. Every factor of two correct, every sign correct, every dimension correct, everything was right. He never put anything into his little notebook that he carried around with him without making sure it was perfectly correct. And that made it possible for him to do a lot of practical problems just on being asked because he had worked them out before and some of the critical formulae were in his little book. Most things he had thought about before in some form or other, most questions in physics were questions… were… were new forms of questions that he had already answered. And so if you asked him something he would begin at the top left of the blackboard and write line after line and then later on, perhaps at the bottom right or else before that, he would get the answer and put a box around it. And the answer was always correct; he never made any mistakes. A greater contrast with Viki Weisskopf could not be imagined. Everything Viki wrote was modular powers of two, powers of pi, powers of i–the numerator and denominator could well be interchanged. I remember when in a nuclear theory class he tried to derive the resonance formula…
[Q] The Breit-Wigner? The Breit-Wigner formula?
The Breit-Wigner formula, which in atomic theory was called the Weisskopf-Wigner formula. Breit and Wigner sort of generalized it to nuclear theory, but it was exactly the same formula as the Weisskopf-Wigner formula in atomic theory. Well, he got it all wrong, just completely wrong. The… the numerator was in the denominator, the denominator was in the numerator, the sign was wrong, the values, there were factors of two and pi floating around. So he said ‘Well’, he said,’ this time I haven't prepared, I have to admit, I haven't prepared this lecture, so… but next time I'll come in prepared and I'll derive it correctly’. Well he came in next time and again he tried to derive it and failed again. Now of course every student in that class learnt how to derive the formula. So it was much more effective than Julian Schwinger's smooth presentation, which really didn't leave you learning anything because he glossed over all the difficulties and presented only a very smooth picture of what was happening. Really didn't leave you with much of an idea of how to do it yourself, whereas Viki's mistakes were very educational. Now Fermi got everything right, but he wasn't a formalism person at all. He just calculated things usually with arithmetic, and got the answer by some trick that was very, very simple. However, it was a trick, and it was based on the fact that he had solved the problem several times before in different guises and put the… put the answers in his little notebook. So that it was a little hard to learn from him also because you would–if you were to do the problem yourself— you would have to invent that trick, which was not necessarily so easy. He didn't do it in, he didn't do a problem in a general way so that you would immediately recognize that that was the same way that you would do the problem. He had his own little twist, which you would have had to invent if you were to do it yourself. Anyway, it was all fine. But if you asked him a question to which he didn't know the answer, then things got much more difficult. He was not so happy about that and the discussion became difficult, and very interesting, but difficult. And of course I asked him fairly often things that he didn't, questions to which he didn't really know the answer, and we had some very interesting discussions as a result.
New York-born physicist Murray Gell-Mann (1929-2019) was known for his creation of the eightfold way, an ordering system for subatomic particles, comparable to the periodic table. His discovery of the omega-minus particle filled a gap in the system, brought the theory wide acceptance and led to Gell-Mann's winning the Nobel Prize in Physics in 1969.
Title: Fermi
Listeners: Geoffrey West
Geoffrey West is a Staff Member, Fellow, and Program Manager for High Energy Physics at Los Alamos National Laboratory. He is also a member of The Santa Fe Institute. He is a native of England and was educated at Cambridge University (B.A. 1961). He received his Ph.D. from Stanford University in 1966 followed by post-doctoral appointments at Cornell and Harvard Universities. He returned to Stanford as a faculty member in 1970. He left to build and lead the Theoretical High Energy Physics Group at Los Alamos. He has numerous scientific publications including the editing of three books. His primary interest has been in fundamental questions in Physics, especially those concerning the elementary particles and their interactions. His long-term fascination in general scaling phenomena grew out of his work on scaling in quantum chromodynamics and the unification of all forces of nature. In 1996 this evolved into the highly productive collaboration with James Brown and Brian Enquist on the origin of allometric scaling laws in biology and the development of realistic quantitative models that analyse the influence of size on the structural and functional design of organisms.
Tags: University of Chicago, Institute of Nuclear Studies, Enrico Fermi, Victor Weisskopf, Julian Schwinger
Duration: 4 minutes, 16 seconds
Date story recorded: October 1997
Date story went live: 24 January 2008