Campuses:
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g4flukacomp_v1 [2013/04/15 12:07] – villaa | g4flukacomp_v1 [2013/05/13 23:07] (current) – villaa | ||
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* Geant4.9.5 | * Geant4.9.5 | ||
* FLUKA 2011.2 patch level 17 (Dec 2012) | * FLUKA 2011.2 patch level 17 (Dec 2012) | ||
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+ | ==plots== | ||
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+ | Several of the more important plots can be viewed below in separate sections and additional plots are available [[: | ||
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+ | ==energy flux== | ||
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+ | As muons propagate through a cylindrical volume they begin creating neutrons and eventually the flux through the cylindrical area comes to constant. | ||
+ | flux (over the whole 10m sensitive cylinder) as a function of energy. | ||
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+ | for Borexino scintillator (C9H12 at 0.887 g/cm^2) we plot the integrated flux as a function of neutron energy for several muon primary energies | ||
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+ | {{: | ||
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+ | for water we plot the integrated flux as a function of neutron energy for several muon primary energies | ||
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+ | {{: | ||
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+ | for calcium carbonate (CaCO_3) we plot the integrated flux as a function of neutron energy for several muon primary energies **NOTE: Anthony found an error he made in material definition wherin Ca was being basically replaced by Na, working out new plots now...** | ||
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+ | {{: | ||
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+ | **__UPDATE__**: | ||
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+ | {{: | ||
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+ | for natural iron we plot the integrated flux as a function of neutron energy for several muon primary energies | ||
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+ | {{: | ||
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+ | for natural lead we plot the integrated flux as a function of neutron energy for several muon primary energies | ||
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+ | {{: | ||
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+ | **__UPDATE__**: | ||
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+ | {{: |