Neutron flux calculation using FFT in a nuclear reactor

praharmitra
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well, that's the heading of a project i am doing...i need some help on neutron detectors...

how they are dectected and what is the probable graph of count rate vs, pulse height that i might get for a nuclar fission reaction of U-235...

can anyone help?
 
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i am doing similar project
 
Is one doing a fission detector or a neutron detector, and is one doing detections of neutrons ex-reactor, or for a power reactor (in-core or ex-core) detector?

The application determines the type of detector.

For example there are fission detectors that use the fission reaction. There are detectors which use the (n,p) scattering.

And there are detectors that use Rh or V (n-capture).

See - http://www.tpub.com/content/doe/h1013v2/css/h1013v2_76.htm
 
There are several detectors of thermal neutrons. A boron-10 proportional counter uses BF3 gas. See
http://www.orau.org/PTP/collection/proportional counters/bf3info.htm
Helium-3 is also used in gas proportional chambers. When it absorbs a neutron, it fissions to a proton plus tritium, plus about 763 KeV of kinetic energy. In both cases, the pulse height is taken off the anode wire using capacitor coupling, and is independent of the neutron energy. Lithium-6 is also used.
 
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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