It is a pleasure and an honor for me to give this lecture in honor of Oscar
Klein who made major contributions to field theory, quantum electrodynamic
s and particle physics, including weak interactions. He was the first one t
o observe that the mu decay and the beta decay could be described by the sa
me interaction with the same coupling constant; this led to the discovery o
f the Universal Fermi Interaction.
Perhaps I should begin my discussion of the history of weak interactions by
separating it into three periods:
(1) Classical Period, 1898-1949.
(2) Transition Period, 1949-1956.
(3) Modern Period, 1956-.