Author
Listed:
- Rizal Kurniadi
(Department of Physics, Institut Teknologi Bandung, Jalan Ganesha 10, Bandung, Indonesia)
- Abdul Waris
(Department of Physics, Institut Teknologi Bandung, Jalan Ganesha 10, Bandung, Indonesia)
- Sparisoma Viridi
(Department of Physics, Institut Teknologi Bandung, Jalan Ganesha 10, Bandung, Indonesia)
Abstract
Nuclear fission has been modeled notoriously using two approaches method, macroscopic and microscopic. This work will propose another approach, where the nucleus is treated as a toy model. The aim is to see the usefulness of particle distribution in fission yield calculation. Inasmuch nucleus is a toy, then the Fission Toy Model (FTM) does not represent real process in nature completely. The fission event in FTM is represented by one random number. The number is assumed as width of distribution probability of nucleon position in compound nuclei when fission process is started. By adopting the nucleon density approximation, the Gaussian distribution is chosen as particle distribution. This distribution function generates random number that randomizes distance between particles and a central point. The scission process is started by smashing compound nucleus central point into two parts that are left central and right central points. The yield is determined from portion of nuclei distribution which is proportional with portion of mass numbers. By using modified FTM, characteristic of particle distribution in each fission event could be formed before fission process. These characteristics could be used to make prediction about real nucleons interaction in fission process. The results of FTM calculation give information that the γ value seems as energy.
Suggested Citation
Rizal Kurniadi & Abdul Waris & Sparisoma Viridi, 2016.
"Monte Carlo simulation based toy model for fission process,"
International Journal of Modern Physics C (IJMPC), World Scientific Publishing Co. Pte. Ltd., vol. 27(03), pages 1-12, March.
Handle:
RePEc:wsi:ijmpcx:v:27:y:2016:i:03:n:s0129183116500303
DOI: 10.1142/S0129183116500303
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