Track-size distributions were measured for chemically etched CR-39 foils exposed to monoenergetic neutrons with energies ranging from 0.144 to 19 MeV and to various broad-spectrum neutron sources including spontaneous fission neutrons from (238)Pu. These tracks are due to energetic charged particles resulting from interactions of the neutrons with the CR-39. The tracks are visible with an optical microscope after chemical etching and vary in size and configuration depending on the particle, energy and angle of incidence. The foils were analysed using an automatic analysis system that scans the foils, identifies valid tracks and records the track-size parameters. The track-size distributions vary with neutron energy for the monoenergetic sources and with the hardness of the broad-spectrum sources. The distribution from the (238)Pu fission source is readily distinguishable from the other sources measured and from distributions owing to the background.
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http://dx.doi.org/10.1093/rpd/nci675 | DOI Listing |
J Radiol Prot
June 2021
Institute of Radiation Medicine, Fudan University, Shanghai 200032, People's Republic of China.
The motivation for this study was to explore a new method to test the particle spatial distribution for a therapeutic carbon beam. CR-39 plastic nuclear track detectors were irradiated to a 276.5 MeV umono-energy carbon beam at the heavy ion facility in the Shanghai Proton and Heavy Ion Center.
View Article and Find Full Text PDFRev Sci Instrum
February 2018
Instituto de Instrumentación para Imagen Molecular (I3M), CSIC-Universitat Politècnica de València, Camino de Vera s/n, Ed. 8B-N-1a, 46022 Valencia, Spain.
CR-39 nuclear track material is frequently used for the detection of protons accelerated in laser-plasma interactions. The measurement of track densities allows for determination of particle angular distributions, and information on the kinetic energy can be obtained by the use of passive absorbers. We present a precise method of measuring spectral distributions of laser-accelerated protons in a single etching and analysis process.
View Article and Find Full Text PDFPLoS One
March 2016
School of Geography, Earth and Environmental Sciences, University of Birmingham, Birmingham, United Kingdom.
We present a holistic approach to the study of early archosauriform evolution by integrating body and track records. The ichnological record supports a Late Permian-Early Triassic radiation of archosauriforms not well documented by skeletal material, and new footprints from the Upper Permian of the southern Alps (Italy) provide evidence for a diversity not yet sampled by body fossils. The integrative study of body fossil and footprint data supports the hypothesis that archosauriforms had already undergone substantial taxonomic diversification by the Late Permian and that by the Early Triassic archosauromorphs attained a broad geographical distribution over most parts of Pangea.
View Article and Find Full Text PDFRadiat Prot Dosimetry
October 2014
Division for Radiation Safety and Security, Paul Scherrer Institute (PSI), Villigen PSI, Switzerland.
Investigations on track density and track size distributions of different PADC (poly allyl diglycol carbonate) materials have been performed. The PADC used for the tests has been produced by Thermo Electron (USA), Track Analysis System Limited (UK), Chiyoda Technol Corporation (Japan) and Intercast srl (Italy). For each PADC material 120 detectors were randomly selected out of 2 sheets: 60 detectors from one sheet have been irradiated with a personal dose equivalent of 3 mSv in the field of a (241)Am-Be source at the calibration laboratory of PSI, whilst the other 60 detectors from the other sheet have been used as background samples.
View Article and Find Full Text PDFRadiat Prot Dosimetry
December 2006
Georgetown University, Radiation Medicine Department, 3970 Reservoir Road NW, Research Building Room E202A, Washington, DC 20057-1482, USA.
Track-size distributions were measured for chemically etched CR-39 foils exposed to monoenergetic neutrons with energies ranging from 0.144 to 19 MeV and to various broad-spectrum neutron sources including spontaneous fission neutrons from (238)Pu. These tracks are due to energetic charged particles resulting from interactions of the neutrons with the CR-39.
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