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A(0)(1 + k2/mA)~2. 06 GeV given in the quasielastic scattering vM + n —> fi~ + p experiment of Baker et al. (1981), and also in reasonable agreement with values of m ^ obtained from single pion electroproduction at threshold using the low energy theorem of Nambu and Shrauner (1962) (for which experimental references are given in both the Joos et al. and Baker et al. articles). At the 1968 Nobel Symposium on Elementary Particle Theory, I gave a brief talk (Adler, 1968a) reviewing various methods that had been proposed to measure the nucleon axial-vector form factor: quasielastic neutrino scattering, neutrino production of the A(1232), electroproduction of a single soft pion (the Nambu-Shrauner proposal), and electroproduction of the A(1232) plus an additional soft pion (the proposal of my paper R14 with Weisberger).
1968). Current Algebra at Small Distances, in Proceedings of the International School of Physics "Enrico Fermi" Course XLI, J. , Academic Press, New York, pp. 55-81. See p. 56 of this proceedings. [19] Bjorken, J. D. (1969). Asymptotic Sum Rules at Infinite Momentum. Phys. Rev. 179, 15471553. [20] Broadhurst, D. , A. L. Kataev, and C. J. Maxwell (2004). Comparison of the Gottfried and Adler Sum Rules Within the Large-iVc Expansion. Phys. Lett. B 590, 76-85. [19] Bugg, D. V. (2003). Comments on the a and K.
The intent behind our appointments was that we would reinvigorate high energy theory at the Institute, which had fallen into a decline with the departures of Lee, Yang, and Pais to professorships elsewhere, and with a turn of Dyson's research interests towards astrophysics. Before going to Princeton, as mentioned above, I spent the spring term of 1966 as a postdoc in Murray Gell-Mann's group at Cal Tech. By this time the successes of PCAC and current algebra had attracted a lot of attention and stimulated an outpouring of papers, the more important ones of which appear in the volume which Dashen and I put together a year later.