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Cell simulation in Geant4 Phase 1

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Presentation on theme: "Cell simulation in Geant4 Phase 1"— Presentation transcript:

1 Cell simulation in Geant4 Phase 1
S. Chauvie INFN - Turin CERN, December 6th, 2004

2 Simple cell-like simulation
Water Our conclusion are not so innovative but since we deal with a not so used MC are not trivial 100 m

3 Photons, 10 keV Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

4 Energy deposition Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

5 Range Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

6 e-, 50 keV Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

7 Energy deposition Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

8 Range Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

9 e+, 50 keV Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

10 Energy deposition Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

11 Range Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

12 p, 2 MeV Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

13 Energy deposition Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

14 Range Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

15 12C, 25 MeV/u Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

16 Energy deposition Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

17 Range Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

18 Soyland-Hassfjel experiment
Energy spectrum & Track diameter Cells 1,5 mm Water Our conclusion are not so innovative but since we deal with a not so used MC are not trivial Po source , 5,3 MeV

19 Kinetic energy distribution in 1,5 mm water
Soyland-Hassfjel experiment:4,5 MeV peak Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

20 Nanodosimetry experiments
Particle Energy (MeV/u) Target Ref Br 0,4 tissue eq. gas Varma Med Biol 25/ (1980) O 2,57 tissue eq. gas Varma Radiat. Res (1977) Ge 17,2 propane Paretske Proc VI Symp Micro U331 1,4 propane Toburem Radiat Prot Dos 31 No1/ U331 5,9 water “ Alpha 72 Varma Proc V Symp Micro 75-95 p 1 tissue eq gas Wingate Radiat Res (1976) Alpha 1 “ “ Alpha “ “ Ne Varma Radiat Res Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

21 Kramer, Katz, Chatterje, Cuncinotta, Zaider, Wingate
Tracks model Kramer, Katz, Chatterje, Cuncinotta, Zaider, Wingate Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

22 16O, 2,57 MeV/u, Water Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

23 16O, 2,57 MeV/u, Water Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

24 2,57 MeV 12C water Our conclusion are not so innovative but since we deal with a not so used MC are not trivial

25 1 MeV/u p water Our conclusion are not so innovative but since we deal with a not so used MC are not trivial


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