“Twentieth century physics already has undergone two breathtaking revolutions—in relativity and in quantum mechanics. We may be standing on the threshold of a third.” Thus spoke Geoffrey F. Chew on the occasion of the Rouse Ball Lecture which he delivered at the University of Cambridge on March 12, 1963. The title of this lecture is “The Dubious Role of the Space‐Time Continuum in Subatomic Physics”.

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M. L. Goldberger, La Théorie quantique des Champs. Douzième Conseil de Physique, October 1961, p. 179.
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Proceedings of the 1962 International Conference on High Energy Physics at CERN, p. 529. (In response to a question by Heisenberg asking, “What are the implications of the assumption that Regge poles exist and no other kind of poles to field theory?”, Professor Chew replied, “I really do not understand field theory well enough to have a reliable opinion on this question.” The Regge‐pole concept is embodied in the formalism of the S‐matrix of the strong interactions. It is a mathematical concept that represents a single‐particle state of a non‐elementary particle. Regge poles are important because they are assumed to determine the asymptotic behavior of the S‐matrix).
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A. W. Stern, Physics Today, May 1949, p. 5.
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