Abstract

In this research, for the first time, the polycarbonate/bismuth oxide (PC–Bi2O3) composite was studied as a beta-ray sensor using a pure beta-emitter 90Sr source. Firstly, the range and stopping power of the electrons in the composite at various loadings of 0, 10, 20, 30, 40, and 50 wt% were calculated using the ESTAR program. Results of simulation demonstrated that the concentration of the heavy metal oxide particles into the polymer matrix played an important role in evaluating the range and stopping power of the electrons in the composite. Secondly, at the experimental phase, the pure Polycarbonate and 50 wt% PC–Bi2O3 nanocomposite with dimensions of 4 × 4 × 0.1 cm3 were prepared and irradiated by 90Sr. Also, current–voltage (I–V) plot exhibited linear response ranging from 100 to 1000 V at the fixed source‐to‐surface distance (SSD). Then the amount of electric current as the sensor response was measured in various dose rates at the fixed voltage of 400 V for the pure Polycarbonate and 50 wt% PC–Bi2O3 nanocomposite using an electrometer, in which results showed that the sensitivities were found as 20.3, and 33.3 nC mSv−1 cm−3, respectively. This study showed that this composite could serve as a novel beta-ray sensor.

Highlights

  • In this research, for the first time, the polycarbonate/bismuth oxide (PC–Bi2O3) composite was studied as a beta-ray sensor using a pure beta-emitter 90Sr source

  • The surface morphology of the prepared 50 wt% PC–Bi2O3 nanocomposite was analyzed by Field Emission Scanning Electron Microscopy (FESEM) and Energy-Dispersive X-ray Spectroscopy (EDS)

  • It can be mentioned that increasing the weight fraction of the ­Bi2O3 particles into the Polycarbonate matrix lead to a linear decrease of the range of beta particles in the composite material

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Summary

Introduction

For the first time, the polycarbonate/bismuth oxide (PC–Bi2O3) composite was studied as a beta-ray sensor using a pure beta-emitter 90Sr source. The interaction mechanisms of beta particles with matter are categorized in two sections, electron excitation and ionization, in which electrons interact with the particles traversing the material via the Coulomb electric ­field[16,17,18]. Electrons lose their energies by friction attributed to the CSDA or continuous slowing-down a­ pproximation[19,20,21]. Polycarbonate is essentially an amorphous polymer expected to have more suitable

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