Magnitude of Fissile Element at the Order of a Neutron.

nucerl
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Consider a fissile element whose magnitude is at the order of a neutron. In this situation, how can we derive the point kinetic equations?

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nucerl said:
Consider a fissile element whose magnitude is at the order of a neutron. In this situation, how can we derive the point kinetic equations?
Please clarify what one means by "Magnitude of Fissile Element at the Order of a Neutron".

There are 'fissile' nuclides which readily fission upon absorption of a neutron, as opposed to 'fertile' nuclides which require interaction with high energy (MeV) neutrons in order to fission but otherwise absorb neutrons and subsequently decay, possibly into fissile species.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...

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