Changes between Version 156 and Version 157 of DatabaseBasedAnalysis/Spectrum


Ignore:
Timestamp:
12/05/19 15:25:55 (6 years ago)
Author:
tbretz
Comment:

--

Legend:

Unmodified
Added
Removed
Modified
  • DatabaseBasedAnalysis/Spectrum

    v156 v157  
    117117\[\epsilon(\delta E) = \epsilon(\delta E, \Delta\Theta) = \frac{N'_\textrm{exc}(\delta E, \Delta\Theta)}{N'_\textrm{src}(\delta E,\Delta\Theta)}\]
    118118
    119 and \(N'_\textrm{exc}(\delta E,\Delta\Theta)\) and \(N'_\textrm{src}(\delta E,\Delta\Theta)\) are both expressed as the sum given above, the constants \(\rho_0\) and \(\tau_0\) cancel.
     119and \(N'_\textrm{exc}(\delta E,\Delta\Theta)\) and \(N'_\textrm{src}(\delta E,\Delta\Theta)\) are both expressed as the sum given above, the constants \(\rho_0\) and \(\tau_0\) cancel.
     120
     121The differential flux in an energy interval \(\delta E\) is then given as
     122
     123\[\phi(\delta E) = \phi(\delta E,\Delta\Theta) = \frac{1}{A_0\cdot \Delta T}\frac{M_\textrm{exc}(\delta E)}{\epsilon(\delta E)\cdot \delta E}\]
     124
     125Where \(A_0\) is total area of production and \(\Delta T\) the total observation time. The number of measured excess events is in that energy interval is \(M_\textrm{exc}(\delta E)=M_\textrm{exc}(\delta E, \Delta\Theta\).
     126
    120127
    121128