Empirical assessment of the detection efficiency of CR-39 at high proton fluence and a compact, proton detector for high-fluence applications
Author(s) -
M. J. Rosenberg,
F. H. Séguin,
C. Waugh,
H. G. Rinderknecht,
D. Orozco,
J. A. Frenje,
M. Gatu Johnson,
H. Sio,
A. B. Zylstra,
N. Sinenian,
C. K. Li,
R. D. Petrasso,
V. Yu. Glebov,
C. Stöeckl,
M. Hohenberger,
T. C. Sangster,
S. Le Pape,
A. J. Mackin,
R. M. Bionta,
O. L. Landen,
R. Zacharias,
Y. Kim,
H. W. Herrmann,
J. D. Kilkenny
Publication year - 2014
Publication title -
review of scientific instruments
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.605
H-Index - 165
eISSN - 1089-7623
pISSN - 0034-6748
DOI - 10.1063/1.4870898
Subject(s) - fluence , proton , detector , pinhole (optics) , nuclear physics , physics , materials science , inertial confinement fusion , scattering , optics , irradiation , atomic physics , plasma
CR-39 solid-state nuclear track detectors are widely used in physics and in many inertial confinement fusion (ICF) experiments, and under ideal conditions these detectors have 100% detection efficiency for ∼0.5-8 MeV protons. When the fluence of incident particles becomes too high, overlap of particle tracks leads to under-counting at typical processing conditions (5 h etch in 6N NaOH at 80 °C). Short etch times required to avoid overlap can cause under-counting as well, as tracks are not fully developed. Experiments have determined the minimum etch times for 100% detection of 1.7-4.3-MeV protons and established that for 2.4-MeV protons, relevant for detection of DD protons, the maximum fluence that can be detected using normal processing techniques is ≲3 × 10(6) cm(-2). A CR-39-based proton detector has been developed to mitigate issues related to high particle fluences on ICF facilities. Using a pinhole and scattering foil several mm in front of the CR-39, proton fluences at the CR-39 are reduced by more than a factor of ∼50, increasing the operating yield upper limit by a comparable amount.
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