TY - JOUR
T1 - Comparison between theoretical model and experimental calibrations and its inference for track formation in bubble detectors
AU - Guo, S. L.
AU - Doke, T.
AU - Li, L.
AU - Chen, B. L.
AU - Zhang, D. H.
AU - Kikuchi, J.
AU - Terasawa, K.
AU - Komiyama, M.
AU - Hara, K.
AU - Fuse, T.
AU - Yasuda, N.
AU - Murakami, T.
N1 - Funding Information:
The authors wish to thank the National Institute of Radiological Science, Chiba, Japan for providing the heavy ion beam. The authors are grateful to Chen Wang for his help in many aspects and two anonymous referees for constructive reviews. This work was supported by the National Natural Science Foundation of China (NNSFC) (No. 19975071) and China Nuclear Science Foundation (No. Y1797F0122).
PY - 2005/11
Y1 - 2005/11
N2 - Calculations on the formation of a linear track of a heavy ion in bubble detector have been carried out based on a theoretical model considering the minimum energy (including bubble surface energy, internal energy, evaporation energy, expansion energy, kinetic energy and viscous energy) required during the formation of a critical bubble at the cost of the ionization energy of the heavy ion. The calculated minimum energy is 8.99 keV for dichlorodifluoromethane (R-12) at 25 °C. The results of calculations have been combined with those of calibrations of bubble detectors with heavy ions at accelerator. The threshold (1.51±0.04) MeV mg-1 cm2 is obtained in the calibration with heavy ions for the above liquid and temperature. It shows that the distance over which the heavy ion traverses and transfers energy to the superheated liquid to produce a critical bubble is 4.67 times the radius of the seed bubble. The radius of the cylinder along which the heavy ion deposits energy to form a seed bubble is about 5.2 nm. This dimension indicates that the process of track formation in bubble detectors is consistent with the model of thermal spike.
AB - Calculations on the formation of a linear track of a heavy ion in bubble detector have been carried out based on a theoretical model considering the minimum energy (including bubble surface energy, internal energy, evaporation energy, expansion energy, kinetic energy and viscous energy) required during the formation of a critical bubble at the cost of the ionization energy of the heavy ion. The calculated minimum energy is 8.99 keV for dichlorodifluoromethane (R-12) at 25 °C. The results of calculations have been combined with those of calibrations of bubble detectors with heavy ions at accelerator. The threshold (1.51±0.04) MeV mg-1 cm2 is obtained in the calibration with heavy ions for the above liquid and temperature. It shows that the distance over which the heavy ion traverses and transfers energy to the superheated liquid to produce a critical bubble is 4.67 times the radius of the seed bubble. The radius of the cylinder along which the heavy ion deposits energy to form a seed bubble is about 5.2 nm. This dimension indicates that the process of track formation in bubble detectors is consistent with the model of thermal spike.
KW - Bubble detector
KW - Heavy ion calibration
KW - Superheated drop detector
KW - Theoretical model for track formation
KW - Thermal spike model
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U2 - 10.1016/j.radmeas.2005.06.009
DO - 10.1016/j.radmeas.2005.06.009
M3 - Conference article
AN - SCOPUS:27744438827
SN - 1350-4487
VL - 40
SP - 229
EP - 233
JO - Radiation Measurements
JF - Radiation Measurements
IS - 2-6
T2 - Proceedings of the 22nd International Conference on Nuclear Tracks in Soils
Y2 - 23 August 2004 through 27 August 2004
ER -