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--- g4flukacomp [2011/11/12 10:53] – 134.84.75.248
+++ g4flukacomp [2011/11/12 13:43] (current) – 134.84.75.248
@@ Line 14: / Line 14: @@
 ==materails==
+==plots==
+Several of the more important plots can be viewed below in separate sections and additional plots are available [[:G4FlukaComp:additionalplots|here]].
 ===muon primaries===
@@ Line 21: / Line 25: @@
 For the scintillator material composed of C<sub>9</sub>H<sub>12</sub> which has density 0.887 g/cm<sup>3</sup> which is similar to the
 Borexino scintillator, several plots have been produced.
+Several of the more important plots can be viewed below and additional plots are available [[:G4FlukaComp:additionalplots|here]].
   for 280 GeV muons the time to capture on hydrogen is plotted below
@@ Line 33: / Line 39: @@
 {{:gfcompare:capture:gfn3mult.png?500|Multiplicity of neutron captures on hydrogen. Muons start at 280 GeV.}}
+==energy flux==
+As muons propagate through a cylindrical volume they begin creating neutrons and eventually the flux through the cylindrical area comes to constant.  This means in the first small percentage of the cylinder the flux is increasing and after that one can reliably extract the flux.  Below we plot the integrated
+flux (over the whole 10m sensitive cylinder) as a function of energy.
+Several of the more important plots can be viewed below and additional plots are available [[:G4FlukaComp:additionalplots|here]]
+  for 280 GeV muons and Borexino scintillator we plot the integrated flux as a function of energy
+{{:gfcompare:flux:nflux_myscintc9h12_mu_280gev.png?1000|Integrated flux for 280 GeV muons in scintillator.}}
+  for 100 GeV muons and lead we plot the integrated flux as a function of energy
+{{:gfcompare:flux:nflux_mylead_mu_100gev.png?1000|Integrated flux for 100 GeV muons in Lead.}}

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