Difference between revisions of "Least fission fragment K.E needed for ionization"
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===Projectiles=== | ===Projectiles=== | ||
| − | From the mass distribution spectrum below, a peak exists for A=103 and another for A=83. | + | From the mass distribution spectrum below, a peak exists for A=103 and another for A=83 for Th-232 fission reaction. |
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| + | [[File:Energy_7.5_a_biggerthan1.jpg|100px]] | ||
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| + | The same fragments are used as projectiles toward the absorber. | ||
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| + | ===Results and Conclusions=== | ||
Revision as of 20:24, 23 December 2010
Simulation Conditions and constraints
Detector Construction
The detector is designed based on example N03, a Ar/CO2 (90-10) layer absorber of thickness 10 cm, and has 1 atmospheric pressure and 300 K temperature.
Physics List
G4hIonization is the process under the generic ion, electrons are expected to scatter in all directions, but the only process under study is Bremsstrahlung.
Projectiles
From the mass distribution spectrum below, a peak exists for A=103 and another for A=83 for Th-232 fission reaction.
The same fragments are used as projectiles toward the absorber.