That guy who made his own reactor

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using tin foil and fissile material from 1950s glow in the dark stuff. does anyone have a link/ know anything about this? i vaguely remember reading about it a while back but maybe i just dreamt it or something...?
 
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I read the book, here it is:

https://www.amazon.com/dp/037550351X/?tag=pfamazon01-20

If you read it carefully, you will find that all the actual evidence that he got the reactor to run is due to the boy scout himself. My guess on this is that nothing significant actually happened, but that the author of the book was a little too easily convinced.
 
yeah, i was a bit sceptical about how he could have made it work when i thought about it. I'm glad i didnt just make the whole thing up though.
 
Anybody knows why Xe135 captures neutrons at such huge cross section at thermal energies? Is it something related with the nuclear structure of the final nucleus Xe136?
Thanks
 
There also exists a tv documentary:
http://www.imdb.com/title/tt0378468/

Quite interesting. If there really was in increase of the thorium activity, it must be attributed to the growing amounts of radioactive thorium progeny after Hahn had isolated the material from lantern mantles.
 
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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