Campuses:
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==materails== | ==materails== | ||
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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 [[: | ||
===muon primaries=== | ===muon primaries=== | ||
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==capture plots== | ==capture plots== | ||
- | | + | For the scintillator material composed of C< |
+ | Borexino scintillator, | ||
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+ | Several of the more important plots can be viewed below and additional plots are available [[: | ||
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+ | for 280 GeV muons the time to capture on hydrogen is plotted below | ||
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+ | {{: | ||
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+ | 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 | ||
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+ | {{: | ||
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+ | for 280 GeV muons the multiplicity within each event of hydrogen captures is plotted below | ||
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+ | {{: | ||
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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. | ||
+ | |||
+ | 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 | ||
+ | |||
+ | {{: | ||
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+ | for 100 GeV muons and lead we plot the integrated flux as a function of energy | ||
+ | |||
+ | {{: |