codes:en_brems

# Differences

This shows you the differences between two versions of the page.

 codes:en_brems [2014/10/02 17:47]ute codes:en_brems [2014/10/02 17:49] (current)ute Both sides previous revision Previous revision 2014/10/02 17:49 ute 2014/10/02 17:47 ute 2014/07/07 16:33 christoph 2014/07/07 16:31 christoph 2014/07/07 16:31 christoph 2014/07/07 16:27 jannis 2014/07/07 16:25 christoph 2014/07/07 16:24 christoph 2014/07/07 16:22 christoph 2014/07/07 16:21 christoph 2014/07/07 16:12 christoph created 2014/10/02 17:49 ute 2014/10/02 17:47 ute 2014/07/07 16:33 christoph 2014/07/07 16:31 christoph 2014/07/07 16:31 christoph 2014/07/07 16:27 jannis 2014/07/07 16:25 christoph 2014/07/07 16:24 christoph 2014/07/07 16:22 christoph 2014/07/07 16:21 christoph 2014/07/07 16:12 christoph created Line 10: Line 10: ​ where E_kin denotes the kinetic energy of the incident electron in Joule, omega is the where E_kin denotes the kinetic energy of the incident electron in Joule, omega is the - frequency of the emitted photon in s$^{−1}$ and Theta_i is the scattering angle. The function + frequency of the emitted photon in 1/s and Theta_i is the scattering angle. The function to calculate the doubly differential cross section for pair production can be called by\\ to calculate the doubly differential cross section for pair production can be called by\\ <​code>​ <​code>​ Line 16: Line 16: ​ where E_kin denotes the kinetic energy of the created positron in Joule, omega the frequency where E_kin denotes the kinetic energy of the created positron in Joule, omega the frequency - of the incident photon in s$^{−1}$ and Theta_p the angle between both.\\ + of the incident photon in 1/s and Theta_p the angle between both.\\ The code can be downloaded {{en_brems.cpp|here}}. The code can be downloaded {{en_brems.cpp|here}}. If you use this code, please cite {{bremsstrahlung_koehn_ebert_final_pagenumber.pdf|this article}}. If you use this code, please cite {{bremsstrahlung_koehn_ebert_final_pagenumber.pdf|this article}}.