منابع مشابه
Upgrade of the Monte Carlo code FIDO
During rf heating on minority ions and current drive the velocity distribution is determined by the balance between the wave-particle interaction and the relaxation through Coulomb collision. This is simulated by the Monte Carlo code fido [1–3], which solves the Fokker-Planck equation in the low collisionality banana-transport regime, including finite orbit width and rf induced transport. The f...
متن کاملUnfolding X-ray spectrum in the diagnostic range using the Monte Carlo Code MCNP5
Introduction: Unfolding X-ray spectrum is a powerful tool for quality control of X-ray tubes. Generally, the acquisition of the X-ray spectrum in diagnostic radiology departments is complicated and difficult due to high photon flux. Measurement of x ray spectra using radiation detectors could not be performed accurately, because of the pulse pile up. Therefore, indirect methods...
متن کاملNew Features of the Monte-Carlo Code MOCADI
MOCADI, the Monte-Carlo code for tracking of ions in ion-optical systems with non-Liouvillian elements, has been extended. New event generators for targets were added besides projectile fragmentation. General twobody kinematics with possible excitation energy of target and projectile nucleus and nuclear fission with different parametrizations of the total kinetic energy distribution of the frag...
متن کاملLimitations in the PHOTON Monte Carlo gamma transport code
Three Monte Carlo gamma transport codes, MCNP, EGS, PHOTON, differ in the degree of difficulty in implementing them for calculation and in the requirements for the input file. Differences in the results were discovered when evaluating the same case using these three transport codes. These differences that are energy dependent are presented here. r 2002 Published by Elsevier Science B.V. PHOTON ...
متن کاملElectron Reflection in Monte Carlo Simulations with the code GEANT
Target preheat is a significant concern in inertial confinement fusion experiments because, when the temperature of the target becomes too large, the areal density (density times radius) required for ignition cannot be attained. The majority of preheat comes from fast electrons produced when the laser interacts with the target. When these energetic electrons are slowed by collisions, they relea...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
ژورنال
عنوان ژورنال: Nuclear Science and Engineering
سال: 1971
ISSN: 0029-5639,1943-748X
DOI: 10.13182/nse71-a21258