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Damage Effects of Ionizing Radiation in Polymer Film Electrets

Published online by Cambridge University Press:  01 February 2011

Marco Aurélio Parada
Affiliation:
[email protected], Universidade de São Paulo, Departamento de Física e Matemática, Avenida Bandeirantes 3900, Ribeirão Preto, São Paulo, 14040-901, Brazil
Renato Amaral Minamisawa
Affiliation:
[email protected], Universidade de São Paulo, Departamento de Física e Matemática, Avenida Bandeirantes 3900, Ribeirão Preto, São Paulo, 14040-901, Brazil
Marcos Vasques Moreira
Affiliation:
[email protected], Instituto de Radioterapia e Megavoltagem de Ribeirão Preto (IRMEV), Rua Sete de Setembro 1150, Ribeirão Preto, São Paulo, 14010-180, Brazil
Adelaide de Almeida
Affiliation:
[email protected], Universidade de São Paulo, Departamento de Física e Matemática, Avenida Bandeirantes 3900, Ribeirão Preto, São Paulo, 14040-901, Brazil
Iulia Muntele
Affiliation:
[email protected], Alabama A&M University, Physics, 4900 Meridian Stre et, Normal, AL, 35762, United States
Daryush Ila
Affiliation:
[email protected], Alabama A&M University, 2Center for Irradiation of Materials, P.O. Box 1447, Normal AL, Hunstsville, Alabama, 35762-1447, United States
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Abstract

Electret sensors or dosimeters can be used to quantify the ionizing radiation dose from charged particles or waves beams (α, β, -e, p etc… γ, X), and with appropriate converters, from fast and slow neutrons. The electret state is reached, by some insulating materials (electrical conductivity lower than 10−8 (Ω m)−1), when once charged, the incorporated charge is quasi-permanent ≈ 109 s. The charge densities are read (before and after the irradiations) and the radiation dose inferred from the difference between them. PFA (Tetrafluoroethylene-per-fluoromethoxyethylene) and FEP (Tetrafluoroethylene-hexa-fluoropropylene) damage mechanisms were studied bombarding these fluoropolymers with: 1 MeV protons at constant current and fluences from 1×1011 tower 1×1016 ions/cm2, 60Co gamma and X-rays, respectively of 1.25 and 0.106 MeV for absorbed doses of 0.5, 1.0, 8,0 and 100 Gy. The emission of chemical species was monitored with a Residual Gas Analyzer (RGA), during proton bombardment and techniques of Optical Absorption Photospectrometry (OAP), Fourier Transform Infrared (FTIR) and Micro-Raman spectroscopy were used to analyze the virgin, exposed and irradiated films.

Type
Research Article
Copyright
Copyright © Materials Research Society 2006

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