![]() ![]() Here are a couple of things which are related to $\Gamma \tau = \hbar$, but which I don't want to discuss here because I'm not very prepared about them and also because I fear going off topic. paradoxical nature of reality palatable through the symbols and images of myth. I'll check better this point when I have some time. The Tao of Physics - Free download as Word Doc (.doc), PDF File (.pdf). I have never done backwards perturbation theory, but I'm assuming that the result (1) is also valid for $t<0$, with $-\Gamma t$ replaced by $-\Gamma \vert t\vert = +\Gamma t$. I start with the decay law of Rutherford and Soddy which states that the rate of decay $\dot N(t)$ of an unstable particle (or nucleus) at a given time $t$ is proportional to the number of those particles which are present $N$ at that time $t$. It becomes apparent at the atomic level and manifests itself more and more as one penetrates deeper into matter, down into the realm of subatomic particles. Like all elementary particles, taus have no known size. Nevertheless, just as the muon shares many of the properties with the electron, so too does the tau. For a proud Dane like Bohr, this was a very big deal, and Bohr is the only person to be awarded it who was not royalty and/or a famous general. The tau is a very heavy species of elementary particle that aren’t quite as common as the electron or the muon. In 1947 Bohr was awarded the Order of the Elephant from the Danish government. Like I found this a very good question but unlike him I am not a professional Physicist and so will try and answer the question on a simplistic level which may not suit as I do not know the level that he is working at but given that he is reading Thomson's book it must be quite advanced. From the Chinese Taoist text I Ching, as reported in Reference 2, pg. ![]()
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