2014
DOI: 10.1364/oe.22.031473
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Investigation of UV optical fibers under synchrotron irradiation

Abstract: Abstract:The focus of the present paper deals, for the first time, with commercial UV optical fibers, characterizing their behaviour as they are subjected to very high flux wiggler generated synchrotron radiation. Five distinct types of UV optical fibers, produced by three manufactures, were exposed to total doses between 5 Gy and 2000 Gy. The exposure to synchrotron radiation was performed in two campaigns. The tests were run off-line and considered the dependence of the radiation induced attenuation (RIA) as… Show more

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Cited by 9 publications
(9 citation statements)
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“…Figure a shows the UV–vis spectrum of 1 – 900 , which exhibits two distinct maxima at 220 and 248 nm, consistent with π–π* or n−π* transitions (details in Figure b). Exposure to air for 15 s decreases: (a) the intensity of the two peaks likely due to the reaction of the respective centers with oxygen and water and (b) the signal intensity in the region between 400 and 600 nm. The first site with an absorption maximum at 251 nm resembles oxygen-deficient centers of the second type (ODC II), which are typically associated with silylene sites. , The second peak has parameters with values between those typical of E’ sites and ODC­(II), and can, therefore, be associated either with paramagnetic silicon defects or with distorted silylenes. ,, Part of the broad shoulder might originate from another transition belonging to ODC­(II), expected at 393 nm; however, the formation of a similar shoulder is also observed in the spectra of irradiated silicas. , The spectrum of 1 – 700 looks very similar to 1 – 900 , suggesting the presence of similar defects, while spectra of 1 – 150 and 1 – 500 do not show any absorption bands (Figure S5).…”
Section: Resultsmentioning
confidence: 99%
“…Figure a shows the UV–vis spectrum of 1 – 900 , which exhibits two distinct maxima at 220 and 248 nm, consistent with π–π* or n−π* transitions (details in Figure b). Exposure to air for 15 s decreases: (a) the intensity of the two peaks likely due to the reaction of the respective centers with oxygen and water and (b) the signal intensity in the region between 400 and 600 nm. The first site with an absorption maximum at 251 nm resembles oxygen-deficient centers of the second type (ODC II), which are typically associated with silylene sites. , The second peak has parameters with values between those typical of E’ sites and ODC­(II), and can, therefore, be associated either with paramagnetic silicon defects or with distorted silylenes. ,, Part of the broad shoulder might originate from another transition belonging to ODC­(II), expected at 393 nm; however, the formation of a similar shoulder is also observed in the spectra of irradiated silicas. , The spectrum of 1 – 700 looks very similar to 1 – 900 , suggesting the presence of similar defects, while spectra of 1 – 150 and 1 – 500 do not show any absorption bands (Figure S5).…”
Section: Resultsmentioning
confidence: 99%
“…Under these conditions, three of the optical fibers proved to be radiation hardened, while two of them were sensitive to synchrotron radiation exposure. All the optical fibers showed a recovery of the optical absorption after storage for 10 days at room temperature [46]. A special setup was developed to monitor the dynamics of the color centers in the UV spectral range (Fig.…”
Section: Experimental Dosimetrymentioning
confidence: 99%
“…[4,5] The RIA in optical fibers has been extensively studied. [6][7][8][9][10][11] During the past decades and a number of papers have treated the modeling of RIA with the irradiation dose at a single wavelength during irradiation and recovery after irradiation. The power-law model, the stretched saturating exponential model, and the saturating exponentials model have been proposed by different authors.…”
Section: Introductionmentioning
confidence: 99%