I wrote the letter to The Physical Review about what I didn't yet call strangeness. I did call it that privately but I didn't call it that in the letter. But I did call the letter something like 'Isotopic Spin and Strange Particles.' Well, The Physical Review had a lot of problems with my letter. First of all they didn't like strange particles or curious particles or peculiar particles; they wanted new unstable particles because that was more pompous. Then their reviewer had terrible problems with the idea that a neutral meson, K⁰, could be different from its antiparticle, K⁰-bar, because everyone knew that a neutral meson like pi-zero was its own antiparticle. Well, I remembered vaguely reading Nick Kemmer's article in which he proposed the pi-zero, the isotopic spin one pion, or meson as they called it then. And I looked it up, and a huge part of the paper was devoted to showing that a neutral boson could be its own antiparticle, because the neutral - the spin zero formalism was the formalism of Pauli and Weisskopf. And Pauli and Weisskopf in their so-called anti-Dirac paper which gave the results of Weisskopf's one-year post-doc with Pauli. What they did was to write a theory of charged scalar particles showing that it could be made perfectly consistent and that charged particles didn't have to have spin 1/2; they could have spin zero. It was okay. Well, the way they constructed the neutral spin zero particle was to take the Pauli-Weisskopf theory and take away the charge, which left them with a particle and its antiparticle - distinct from each other. Like the plus and minus that Pauli and Weisskopf had, only now they were neutral. Then what Kemmer did was to take the sum and the difference of these - of these uncharged fields that were antiparticles of each other and show that the sum or the difference could be interpreted as a single meson field that was neutral and that was its own antiparticle. You could then throw away the other one and get pi-zero. Well, I pointed this out to The Physical Review, and they agreed that it was okay. Then they had another problem, which was that everybody knew that a particle obeying Fermi-Dirac statistics, because it had half-integral spin, had to have half-integral isotopic spin. And everybody knew that a particle obeying Bose Einstein statistics, because it had integral spin, had to have integral isotopic spin. Well, I went through the whole argument, showing that you could define, generalise statistics including isotopic spin. And it didn't matter: you could have fermions with either integral or half integral isotopic spin and mesons with either integral or half integral isotopic spin and you could still have generalised statistics including isotopic spin and it will all be okay. Then they printed it. By this time it was the fall of 1953. The secretary had sent in the notice, the draft board said it was okay, I didn't have to be drafted, but the paper was now in print.