In general, the fiber-optic radiation sensors (FORSs) have many advantages such as good flexibility and no interferences from pressure, humidity, and electromagnetic field -. In addition, the FORSs can be used in narrow spaces with high spatial resolution due to their small sizes. Owing to these advantages, the FORSs have been developed to detect some ionizing radiations in hazardous radiation fields  . Meanwhile, the radiation induced luminescence (RIL) such as Cerenkov radiation and fluorescence can be frequently observed in a spent fuel storage pit. Since the luminescence is generated by interactions between the ionizing radiations and transparent media, this type of light signal can be a significant signal in some cases  .
The purpose of this study is to detect ionizing radiations in the hazardous conditions by measuring the RIL. The RIL can be generated in various fiber-optic materials. In previous research, a FORS using the RIL was fabricated to verify spent fuel in a nuclear power plant; here, the silica optical fiber was employed as a sensor probe . To enhance signal to noise ratio (SNR) of the FORS, in this study, we fabricated a sapphire based FORS. To evaluate the sensor, we measured the spectrum and intensity of the luminescence generated from the fiber-optic radiation sensor according to the thickness of the PMMA block by irradiation of gamma rays emitted from a Co-60 source. And the result was compared with the value calculated from the formula of Lambert-Beer .
2. Materials and Methods
In the study, a cylindrical sapphire crystal (Al2O3, COMA technology) was used as a sensing material. The diameter and length of the sapphire crystal are 1 mm and 3 cm, respectively. Also, the refractive index is 1.75 and the density is 3.97 g/cm3.
A plastic optical fiber (POF, SH6001, Mitsubishi Rayon) was used to transmit the luminescence signal generated from the sapphire crystal to a spectrometer. The core and cladding of transmitting POF are composed of the polymethylmethacrylate (PMMA) and the fluorinated polymer, respectively. The outer diameter of this fiber is 1.5 mm and the refractive index of the core is 1.49. The numerical aperture (NA) is 0.5 and the length is 20 m.
To measure the luminescence of the FORS, the spectrometer (QE65000, Ocean Optics) was employed. The range of measurable spectrum is from 200 nm to 1100 nm and the SNR is 1000:1. In our experiments, the acquisition time of the RIL signal was fixed at 5000 ms.
Figure 1 shows experimental setup to measure the gamma ray using the sapphire based FORS. The FORS was fabricated with the sapphire crystal, plastic optical fiber and a band pass filter (47B film, Kodak); here, the filter was used to separate the luminescence of the sapphire from the noise signals generated in the plastic optical fibers for transmission. The gamma ray source used in this study is the Co-60 source in the Kyoto University Critical Assembly (KUCA) and its activity is 1047 TBq. The distance between theCo-60 source and the FORS was 14 cm. The PMMA blocks having geometrical dimensions of 20 cm × 20 cm × 1 cm were used to detect the gamma rays as a function of the PMMA thickness. The luminescence generated in the FORS by irradiation of gamma rays is transmitted via 20 m-length plastic optical fiber to the spectrometer.
Figure 2 shows the spectra of the luminescence generated from the FORS. The luminescence ranged from 400 nm to 480 nm with the emission peak at about 420 nm was observed; this result is caused by the use of the filter. The plastic optical fiber used to transmit the light signals from the sensor probe (sapphire) also produce the RIL by interaction of the gamma rays. In these experiments, the luminescence generated from the sensor probe and the noise signal from the plastic optical fiber are not measured simultaneously but are measured separately at the same position with the Co-60 source. As a result, only the luminescence signals generated from the sapphire were measured using a modified subtraction method .
Figure 3 shows the repeatability of the FORS. The luminescence signals were measured 10 times at the same position with the same experimental setup. The measured counts of luminescence were within ±0.065% line, and the relative standard deviation (%RSD) of 0.03% was obtained.
Measured luminescence spectra of the FORS according to the thickness of PMMA block can be found in Figure 4. In this experiment, the count of the luminescence peak decreased with the thickness of PMMA block, because the number of primary or secondary electrons due to gamma interactions are reduced. Figure 5 presents
Figure 1. Experimental setup for measuring the luminescence generated in the FORS by irradiation of gamma rays.
Figure 2. Spectra of the luminescence signals generated in the FORS.
Figure 3. Repeatability of luminescence signals of the FORS.
Figure 4. Measured luminescence spectra of the FORS according to the thickness of PMMA block.
Figure 5. Measured luminescence intensities of the FORS and value calculated using the formula of Lambert-Beer.
measured luminescence intensities of the FORS according to the thickness of PMMA block and the value calculated from the formula of Lambert-Beer. The measured luminescence intensities of the FORS were in good agreements with the value calculated from the formula of Lambert-Beer.
In harmful radiation environments, the FORSs have a number of advantages, such as availability in narrow spaces and real-time measurement. In this study, we have fabricated a FORS by using a sapphire, filter, and plastic optical fiber. We measured only the luminescence light generated from the sapphire by using the modified subtraction method. Then, the wavelength range and the peak of the luminescence were measured according to the thickness of PMMA block. Also, the repeatability of the FORS outputs was evaluated. At last, the measured relative intensities of the luminescence according to the thickness of PMMA block were compared with the value calculated using the formula of Lambert-Beer.
This research was supported by National Nuclear R & D Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Science, ICT and future Planning (2014M2B2A9031841) and this research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Science, ICT and future Planning (2014R1A2A2A04002620 and 2013R1A1A1061647).
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