TY - JOUR
T1 - Charge resolution of CR-39 plastic nuclear track detectors for intermediate energy heavy ions
AU - Ota, S.
AU - Yasuda, N.
AU - Sihver, L.
AU - Kodaira, S.
AU - Kurano, M.
AU - Naka, S.
AU - Ideguchi, Y.
AU - Benton, E. R.
AU - Hasebe, Nobuyuki
PY - 2011/6/15
Y1 - 2011/6/15
N2 - The charge resolution (δZ) for heavy ions (nuclear charge: Z < 40) of 0.1-1 GeV/n energy in CR-39 plastic nuclear track detector (PNTD) and its dependence on etching time, and on projectile Z and energy were investigated and optimized as part of an effort to make precise measurements of projectile charge-changing cross sections. Two types of CR-39 PNTD, HARZLAS TD-1 and BARYOTRAK, were exposed to heavy ion beams with seven values of Z behind thick targets to produce projectile fragments. Following chemical etching (7 N NaOH at 70 °C) for varying etch times, δZ of the projectiles was determined for each detector type. A strong dependence of δZ on the amount of bulk etch (B) was seen. It was also observed that δZ can be remarkably improved with longer etching time as a function of B-1/2, in accordance with the trend seen in other types of track detector such as glass nuclear track detector. However, for B ≥ 60 μm (30 h etching), saturation occurs and there is no further improvement in δZ. Analysis of the correlations between projectile Z, energy, detector response, and fluctuation of the response make it possible to develop a model to predict the δZ for projectiles of given Z and energy. The predicted and measured values of δZ show good agreement within 10%. We conclude that 4 ≤ Z ≤ 30 at intermediate energy can be identified with good δZ in these detectors. The predictive model will be used in designing future cross section measurement experiments.
AB - The charge resolution (δZ) for heavy ions (nuclear charge: Z < 40) of 0.1-1 GeV/n energy in CR-39 plastic nuclear track detector (PNTD) and its dependence on etching time, and on projectile Z and energy were investigated and optimized as part of an effort to make precise measurements of projectile charge-changing cross sections. Two types of CR-39 PNTD, HARZLAS TD-1 and BARYOTRAK, were exposed to heavy ion beams with seven values of Z behind thick targets to produce projectile fragments. Following chemical etching (7 N NaOH at 70 °C) for varying etch times, δZ of the projectiles was determined for each detector type. A strong dependence of δZ on the amount of bulk etch (B) was seen. It was also observed that δZ can be remarkably improved with longer etching time as a function of B-1/2, in accordance with the trend seen in other types of track detector such as glass nuclear track detector. However, for B ≥ 60 μm (30 h etching), saturation occurs and there is no further improvement in δZ. Analysis of the correlations between projectile Z, energy, detector response, and fluctuation of the response make it possible to develop a model to predict the δZ for projectiles of given Z and energy. The predicted and measured values of δZ show good agreement within 10%. We conclude that 4 ≤ Z ≤ 30 at intermediate energy can be identified with good δZ in these detectors. The predictive model will be used in designing future cross section measurement experiments.
KW - Charge resolution
KW - Charge-changing cross section
KW - CR-39 nuclear track detector
KW - Galactic cosmic ray
KW - Heavy ion
KW - Nuclear fragmentation
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U2 - 10.1016/j.nimb.2011.03.018
DO - 10.1016/j.nimb.2011.03.018
M3 - Article
AN - SCOPUS:79955504214
SN - 0168-583X
VL - 269
SP - 1382
EP - 1388
JO - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
JF - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
IS - 12
ER -