91 | | \(N(\Delta E, \Delta\theta)\) is the number of produced events in the energy interval \(E\in\Delta E=[E_\textrm{min};E_\textrm{max}]\) and the zenith angle interval \(\theta\in\Delta\theta=[\theta_\textrm{min};\theta_\textrm{max}]\). The weighted number of events \(N'(\Delta E, \Delta\theta)\) in that interval is then |
92 | | |
93 | | \[N'(\Delta E, \Delta\theta) = \sum_{i=0...N}^{E\in\Delta E}\sum_{j=0...N}^{\theta\in\Delta\theta} \omega(E_i, \theta_j)\] |
| 91 | \(n(\delta E, \delta\theta)\) is the number of produced events in the energy interval \(E\in\delta E=[e_\textrm{min};e_\textrm{max}]\) and the zenith angle interval \(\theta\in\delta\theta=[\theta_\textrm{min};\theta_\textrm{max}]\). The weighted number of events \(n'(\delta E, \delta\theta)\) in that interval is then |
| 92 | |
| 93 | \[n'(\delta E, \delta\theta) = \sum_{i=0...n}^{E\in\delta E}\sum_{j=0...n}^{\theta\in\delta\theta} \omega(E_i, \theta_j)\] |
97 | | \[N'(\Delta E, \Delta\theta) = \sum_{i=0...N}^{E\in\Delta}\sum_{j=0...N}^{\theta\in\Delta\theta} \rho(E_i)\cdot\tau(\theta_j) = \sum_{i=0...N}^{E\in\Delta E}\rho(E_i)\cdot\sum_{j=0...N}^{\theta\in\Delta\theta} \tau(\theta_j)\] |
| 97 | \[n'(\delta E, \delta\theta) = \sum_{i=0...n}^{E\in\Delta}\sum_{j=0...N}^{\theta\in\Delta\theta} \rho(E_i)\cdot\tau(\theta_j) = \sum_{i=0...n}^{E\in\Delta E}\rho(E_i)\cdot\sum_{j=0...N}^{\theta\in\Delta\theta} \tau(\theta_j)\] |
| 98 | |
| 99 | The weighted number of produced events \(N'(\Delta E, \Delta\Theta)\) in the total energy interval \(E\in\Delta E=[E_\textrm{min};E_\textrm{max}]\) and the total zenith angle interval \(\theta\in\Delta\Theta=[\Theta_\textrm{min};\Theta_\textrm{max}]\) is then |
| 100 | |
| 101 | \[N'(\Delta E, \Delta\Theta) = \sum_{i=0...N}^{E\in\Delta}\sum_{j=0...N}^{\theta\in\Delta\Theta} \rho(E_i)\cdot\tau(\theta_j) = \sum_{i=0...N}^{E\in\Delta E}\rho(E_i)\cdot\sum_{j=0...N}^{\theta\in\Delta\Theta} \tau(\theta_j)\] |
| 102 | |
| 103 | with \(N\) being the total number of produced events; |
| 104 | |
| 105 | |
| 106 | |
| 107 | |