Campuses:
This shows you the differences between two versions of the page.
| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| g4flukacomp [2011/11/12 09:28] – 134.84.75.248 | g4flukacomp [2011/11/12 13:43] (current) – 134.84.75.248 | ||
|---|---|---|---|
| Line 14: | Line 14: | ||
| ==materails== | ==materails== | ||
| + | |||
| + | ==plots== | ||
| + | |||
| + | Several of the more important plots can be viewed below in separate sections and additional plots are available [[: | ||
| ===muon primaries=== | ===muon primaries=== | ||
| ==capture plots== | ==capture plots== | ||
| - | | + | |
| + | For the scintillator material composed of C< | ||
| + | Borexino scintillator, | ||
| + | |||
| + | Several of the more important plots can be viewed below and additional plots are available [[: | ||
| + | |||
| + | for 280 GeV muons the time to capture on hydrogen is plotted below | ||
| + | |||
| + | {{: | ||
| + | |||
| + | for 280 GeV muons the radius at which the hydrogen capture takes place is plotted below, the distance is computed from the axis of the cylinder | ||
| + | |||
| + | {{: | ||
| + | |||
| + | for 280 GeV muons the multiplicity within each event of hydrogen captures is plotted below | ||
| + | |||
| + | {{: | ||
| + | |||
| + | ==energy flux== | ||
| + | |||
| + | 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. | ||
| + | |||
| + | Several of the more important plots can be viewed below and additional plots are available [[: | ||
| + | |||
| + | for 280 GeV muons and Borexino scintillator 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 | ||
| + | |||
| + | {{: | ||