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Assay and Acquisition of Radiopure Materials

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g4flukacomp [2011/11/12 11:52] – 134.84.75.248g4flukacomp [2011/11/12 13:43] (current) – 134.84.75.248
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 ==materails== ==materails==
 +
 +==plots==
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 +Several of the more important plots can be viewed below in separate sections and additional plots are available [[:G4FlukaComp:additionalplots|here]].
  
 ===muon primaries=== ===muon primaries===
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 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 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. 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   for 280 GeV muons the time to capture on hydrogen is plotted below
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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.  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 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. 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   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.}} {{:gfcompare:flux:nflux_myscintc9h12_mu_280gev.png?1000|Integrated flux for 280 GeV muons in scintillator.}}
- 
-  for 280 GeV muons and lead we plot the integrated flux as a function of energy 
-   
-{{:gfcompare:flux:nflux_mylead_mu_280gev.png?1000|Integrated flux for 280 GeV muons in Lead.}} 
  
   for 100 GeV muons and lead we plot the integrated flux as a function of energy   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.}} {{:gfcompare:flux:nflux_mylead_mu_100gev.png?1000|Integrated flux for 100 GeV muons in Lead.}}
g4flukacomp.1321120329.txt.gz · Last modified: 2011/11/12 11:52 (external edit)

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