General Particle Source in GEANT4

Jehan Jayanetti
Messages
1
Reaction score
0
I have created a macro file that should produce a Gaussian (Normal) distribution of gamma particles ranging in energy from 0 to 250 keV as follows:

/control/verbose 0
/run/verbose 0
/tracking/verbose 0
/gps/particle gamma
/gps/ene/type Gauss
/gps/ene/min 0 keV
/gps/ene/max 250 keV
/run/beamOn 10000000

I have used the gps (General Particle Source) command to generate this distribution.
However, when I examine the distribution in Matlab it appears as a mono-energetic distribution. I thought the macro commands executed at the Idle> prompt should override the underlying C++ code, but it appears that they do not.
 
Physics news on Phys.org
Jehan Jayanetti said:
I thought the macro commands executed at the Idle> prompt should override the underlying C++ code, but it appears that they do not.

How could it? Suppose you have something hard coded in the C++. How could the macro possibly override that?
 
Hi
i have a problem related Geant4 source,i wana creat a gamma source of conic shape..any one help or guide me..
kind regards
 
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}...
Back
Top