The most important result would seem to be that the techniques which have suc ceeded so well in electrodynamics will be equally successful in obtaining sensible answers from meson theories.This was all pretty speculative since the pion was only identified experi mentally the same year that Case finished his dissertation, and not much was known about its properties yet. In his work the meson was assumed to be a pseudo-scalar boson (known today to be true-the only scalar boson is the pu tative Higgs boson). The coupling between meson and nucleon was taken as a pseudovector, but it turns out that pseudoscalar coupling, the only other pos sibility, would lead to the same results for the magnetic moments (Luttinger, 1948).This scenario raises several interesting questions, the answers to which are the subject of speculation by the authors of this article, as described next. Why did Case publish his dissertation in such abbreviated form? The answer seems to be that J. M. Luttinger had already obtained the same results before Case did. Later Case did in fact present the details of his calculations (Case, 1949a) with an acknowledgment, in a footnote, that he received a preprint of Luttinger's work (1948) prior to publication. He also pointed out that his results agree with those of Luttinger. The rationale for publishing is that it included the electron-neutron interaction, not considered by Luttinger, and that Case's and Luttinger's calculational models were different (Case, 1949a). Case used the Schwinger-Tomonaga formalism while Luttinger used secondquantization in Fock space. (Roughly speaking, this difference in calculational methods is analogous, in a nonrelativistic theory, to the difference between Schrodinger wave mechanics and Heisenberg matrix mechanics. The equiva lence in the nonrelativistic case had been proved much earlier, using the fact that Schrodinger's Hilbert space L2 is isometrically isomorphic to the Fock space, I2 . In fact, all Hilbert spaces of the same dimension are isometrically isomorphic.) So our guess is that Case's showing that Schwinger's methods yielded the same results as second-quantization was an important result at the time, along with his previous observation that the methods already known to be applicable to quantum electrodynamics (i.e., renormalization) could be extended to problems involving mesons.One last point: The fact that pseudoscalar and pseudovector couplings of the meson and nucleon fields are equivalent is literally true only for the calcu lation of the magnetic moment. Other quantities of interest require the intro duction of "equivalent hamiltonians." It was exactly this approximate equiv alence that led to the "Case's theorem" debacle described in Section 3 of this article.