... p.154
In those early Chicago days, Frank (C.N.) Yang and I became close friends. Yang was extremely bright. Both of us were very young, and had an enormous curiosity towards
practically all subjects rational. Often we would have different ideas and opinions and occasionally our discussions would become quite animated. That added a great
deal of life to our student days.
...
...p. 160
During that period, I had several discussions with Steinberger. One day around the beginning of May he came to see me and said that he had just given a seminar at Brookhaven on his experiment. Yang had been in the audience and had strongly objected to my idea that there could be asymmetry in Steinberger's hyperon experiment due to parity violation. I then called Yang and told him that since we last saw each other, at the Rochester Conference, there had been a theoretical breakthrough. I asked him not to express his objections further in public until he could talk it over with me.
...p.161
The next morning Yang drove from Brookhaven to Columbia and we had a very intensive session. I told him my idea and analysis in detail. He was quickly convinced of its importance and wanted to work on it with me.
Yang is endowed with a highly critical mind. It always made me feel more confident if I could overcome his objections with substantive arguments. Furthermore, he is an excellent physicist. The implications of parity nonconservation extended over all facets of physics. I thought Yang's participation would undoubtedly enrich the final product. Therefore I expressed my welcome.
On that day, we covered an enormous variety of physical processes, arguing, debating, sometimes even shouting; occasionally we would switch our points of view, just to make sure. The tremendous intensity of our working together in opposition and in harmony, the immense open feeling that the whole world was lying in front of us, the fearlessness of youth, these are what made life meaningful!
p.162
Both of us, of course, knew there existed very good experimental evidence for parity conservation in the strong reaction. But how solid was it? By the end of the day, we were convinced that for strong interactions it was indeed very good (even for strange particles). In addition, there was also excellent proof for parity conservation in the electromagnetic interaction.
My original idea, that all weak decays of strange particles could be parity violating, stood firm. However, for the weak interaction of non-strange particles further investigation was needed, and both of us agreed we should look into that.
Before Yang joined me on that day, I had been thinking of writing up the work I had already done on parity nonconservation in strange particle decays. However, Yang convinced me to hold off on this since it was a better idea to enlarge the scope to encompass the whole weak interaction. We separated and each of us continued the examination of parity questions in beta decay.
Beta decay is a field with a long history. A very large body of knowledge was available at that time. Since parity conservation had been an implicit assumption in all analyses, and the notion of parity was commonly used, it required a very careful examination of all the available experimental facts to see whether parity nonconservation could also be extended to beta decay. One of the world's great experts on beta decay is C.S. Wu, whose office was a few floors above mine at Columbia. I visited her and told her of these ideas. She was extremely interested in them and kindly lent me the authoritative book on beta decay edited by K. Siegbahn.
At that time, because of parity conservation, beta decay was described by an interaction consisting of five coupling constants, C_i (i = S, P, V, A, T). For our purpose, we introduced five additional parity-violating constants C_i'. Yang and I started a systematic investigation of all known beta decay phenomena by using the general parity nonconserving interaction. We raced through the Siegbahn book and kept in touch often by telephone. It took us about two weeks to finish the entire beta-decay analysis. (In computational skill, Yang and I were evenly matched. This race was extremely intense, but in the best spirit of collaboration and competition, with both of us as Winners. Any attempt to try to place which one was ahead in such intensive and extensive calculations is meaningless.)
...p.163
From then on, the theoretical analysis could be made independently of any detailed calculations. We then expanded our scope to other processes, such as \pi-\mu decay. It took another month of intensive work for us to complete the analysis and to write the theoretical paper. The next scene of the parity drama was set, with many more participants.
There remained the experimental question of how to detect possible parity violation in beta decay. Again I discussed with C.S. Wu the best way to measure asymmetry in spin-momentum correlation in beta decay. She suggested the possible use of a strongly polarized {}^{60}Co \beta-source, for which however a low-temperature set-up was needed. Subsequently, she approached the Bureau of Standards in Washington. This led to the decisive experiment by Wu, Ambler, Hayward, Hoppes and Hudson, which was followed within a few days by the detection of parity violation in \pi-\mu decay, by Garwin, Lederman and Weinrich, and by Friedman and Telegdi. Because of the practical difficulty in accumulating data on strange particles, parity violation in ##\Lambda##-decay was established half a year later by the Steinberger group.
p.163
Reflections on a Collaboration
In recounting these happy days of thirty and forty years ago, I re-read the account given by Yang in 1983. Once again, I was distressed and amazed by what he wrote.
p.164
For instance, take his version of the breakthrough on parity violation. According to Yang, one day in late April or early May of 1956 he came from Brookhaven to visit me at Columbia, and during our conversation in a restaurant he suddenly had the idea of detecting parity nonconservation in ##\Lambda##-decay. He further said that when he told that idea to me, I resisted.
It is a matter of record that, weeks before Yang visited me on that day, I already had the idea. I explained it to Jack Steinberger shortly after the Rochester Conference which took place in early April. In fact, the first experimental attempt to detect parity violation in ##\beta##-decay had already been carried out at Columbia by Budde, Chrétien, Leitner, Samios, Schwartz and Steinberger before Yang joined me on that day. Their result was published in Physical Review (with an acknowledgment to me), before the theoretical paper by Yang and myself.
In his version of our collaboration, Yang has made a systematic effort to paint a picture of himself as leader, from beginning to end, with me as subordinate. Any physicist who knew us in those days would know this to be untrue. Our collaboration had always been one of equal partnership. Our talents were different, but complementary. That is why the collaboration was successful.
Yang's effort to present such an image extends even to our early days in Chicago. According to his account, although I was Fermi's student, Yang was in effect my teacher. This is indeed extremely strange, considering that Fermi was one of the great teachers of all time. At Chicago, Yang and I were both graduate students. We had many discussions, with lots of give and take, and we enlarged each other's horizons. But how could Yang ever mistake these exchanges between novices for the quality of guidance and instruction that I received from Fermi?
From May 1948 to December 1949, Fermi directed my research over a wide range of subjects, which included, besides particle and nuclear physics, heat conductivity of dense matter, white dwarfs, stellar stability, hydrodynamics and magneto-hydrodynamics. These led to several papers which, except for the Lee-Rosenbluth-Yang article, had nothing to do with Yang.
The collaboration between Yang and myself ended about twenty-five years ago. Its merit, as represented by our joint papers, has withstood the test of time. Both of us have made many other independent contributions to physics. The world has rewarded us with recognition and success. Shouldn't that be sufficient?