TY - JOUR
T1 - LET distributions from CR-39 plates on Space Shuttle missions STS-84 and STS-91 and a comparison of the results of the CR-39 plates with those of RRMD-II and RRMD-III telescopes
AU - Tawara, H.
AU - Doke, T.
AU - Hayashi, T.
AU - Kikuchi, J.
AU - Kyan, A.
AU - Nagaoka, S.
AU - Nakano, T.
AU - Takahashi, S.
AU - Terasawa, K.
AU - Yoshihira, E.
PY - 2002/1/1
Y1 - 2002/1/1
N2 - The LET distributions during the Space Shuttle missions STS-84 (altitude 270-412 km, average 375 km; inclination angle, 51.6°) and STS-91 (altitude 328-397 km, average 373 km; inclination angle, 51.6°) were measured using CR-39 plastic nuclear track detectors. A correction for the dip-angle dependence of the track-formation sensitivity of the CR-39 plates was applied to the data analysis. The absorbed doses and the dose equivalents around RRMD Detector Units, estimated from the LET distributions in the LET region of 4-200 keV/μm, fluctuated with standard deviations of ±21% to ±35% in both flight experiments. The LET distributions obtained from the CR-39 plates agreed well with that obtained from RRMD-II in STS-91. However, the particle fluxes obtained from RRMD-III in STS-84 and STS-91 were two or three times higher than those obtained from RRMD-II and the CR-39 plates. It was concluded that the LET distributions obtained from RRMD-II and the CR-39 plates in the present flight experiments did not include the contribution of target-fragmented secondary heavy particles produced by low-LET particles, such as relativistic or semi-relativistic protons and helium ions, whereas RRMD-III was able to detect these secondary particles because of its low triggering level.
AB - The LET distributions during the Space Shuttle missions STS-84 (altitude 270-412 km, average 375 km; inclination angle, 51.6°) and STS-91 (altitude 328-397 km, average 373 km; inclination angle, 51.6°) were measured using CR-39 plastic nuclear track detectors. A correction for the dip-angle dependence of the track-formation sensitivity of the CR-39 plates was applied to the data analysis. The absorbed doses and the dose equivalents around RRMD Detector Units, estimated from the LET distributions in the LET region of 4-200 keV/μm, fluctuated with standard deviations of ±21% to ±35% in both flight experiments. The LET distributions obtained from the CR-39 plates agreed well with that obtained from RRMD-II in STS-91. However, the particle fluxes obtained from RRMD-III in STS-84 and STS-91 were two or three times higher than those obtained from RRMD-II and the CR-39 plates. It was concluded that the LET distributions obtained from RRMD-II and the CR-39 plates in the present flight experiments did not include the contribution of target-fragmented secondary heavy particles produced by low-LET particles, such as relativistic or semi-relativistic protons and helium ions, whereas RRMD-III was able to detect these secondary particles because of its low triggering level.
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U2 - 10.1016/S1350-4487(01)00282-7
DO - 10.1016/S1350-4487(01)00282-7
M3 - Article
C2 - 11841106
AN - SCOPUS:0036008113
SN - 1350-4487
VL - 35
SP - 119
EP - 126
JO - Radiation Measurements
JF - Radiation Measurements
IS - 2
ER -