15900 HVAC Instrumentation and Controls

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68] Razdobreev I, El Hamzaoui H, Ivanov VY, Kustov EF, Capoen B, Bouazaoui M. Optical spectroscopy of bismuth-doped pure silica fiber preform. Opt. Lett. 2010; 35: 1341–1343. [69] Bufetov IA, Semenov SL, Vel’miskin VV, Firstov SV, Bufetova GA, Dianov EM. Optical properties of active bismuth centres in silica fibres containing no other dopants. Quantum Electron. 2010; 40: 639–641. [70] Skuja LN, Trukhin AN, Plaudis AE. Luminescence in germanium-doped glassy SiO2. Phys. Status Solidi A. 1984; 84: K153–K157.

6] Ghosh S, Das S, Paul MC, Dasgupta K, Bohra D, Chaudhary HS, Panwar L, Bhatnagar PK, Vaijapurkar SG. Evaluation of the performance of high phosphorous with germa‐ nium codoped multimode optical fiber for use as a radiation sensor at low dose rates. Appl. Opt. 2011; 50: E80-E85. [7] Jones SC, Sweet JA, Braunlich P, Hoffman JM, Hegland JE. A remote fibre optic laser TLD system. Rad. Prot. Dos. 1993; 47: 525–528. [8] Houston AL, Justus BL, Falkenstein PL, Miller RW, Ning H, Altemus R. Remote optical fiber dosimetry.

The dynamics of the color centers formation under gamma irradiation was investigated by on-line measure‐ ments and by monitoring RIA change at several wavelengths (λ = 420, 525, and 750 nm). 5 kGy) dose, while the best linearity response of RIA vs. 5 kGy [55]. 5772/62547 optical transmission changes when exposed to ionizing radiation over a wide spectral range [56]. 8 MGy [57]. The optical attenuation in the sapphire fiber was measured on-line over the 500–2200 nm spectral range. The major RIA occurs below the 500 nm measuring limit.

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