1983
DOI: 10.1364/ao.22.003073
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Attenuation at 106μm in loaded and unloaded polycrystalline KRS-5 fibers

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Cited by 16 publications
(2 citation statements)
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“…The Ϫ2 dependence suggests that the scattering is dominated by Rayleigh-Gans or Mie mechanisms rather than by Rayleigh scattering. 32,33 Rayleigh-Gans scattering has been shown to occur in some polycrystalline IR fibers when the bulk defects are large in the transverse dimension compared to the wavelength of light but small in optical path difference. A further strong indication that the main scattering mechanism is Rayleigh-Gans is the large degree of forward scattering that we observed.…”
Section: Fiber Lossmentioning
confidence: 99%
“…The Ϫ2 dependence suggests that the scattering is dominated by Rayleigh-Gans or Mie mechanisms rather than by Rayleigh scattering. 32,33 Rayleigh-Gans scattering has been shown to occur in some polycrystalline IR fibers when the bulk defects are large in the transverse dimension compared to the wavelength of light but small in optical path difference. A further strong indication that the main scattering mechanism is Rayleigh-Gans is the large degree of forward scattering that we observed.…”
Section: Fiber Lossmentioning
confidence: 99%
“…The temperature change of the refractive index due to electronic absorption, dn~/dT, of KRS-6 (68 mol % T1C1) was determined by Takahei and Kobayashi [9] to be -160 x 10-6/K over the interval 40 to 300 K. Afanas'ev and Nosov [29] give dn/dT = -254 • 10-6/K for KRS-5 and dn/dT = -234 • 10-6/K for KRS-6 at 0.633/zm. Available data includes the laser-calorimetry measurements of Harrington et al [30] on crystalline KRS-5 at HF and DF laser wavelengths; transmission measurements on long polycrystalline KRS-5 fibers at 10.6 ~m by Harrington and Standlee [31]; laser calorimetry at 1, 5, and 10/xm by Belousov et al [32] on crystalline KRS-5 and KRS-6; carbon-monoxide laser calorimetry measurements of Nosov et al [33] on crystalline KRS-5 and KRS-6; and differentialspectrophotometry measurements of Hidaka et aL [12] on crystalline KRS-5. Available data includes the laser-calorimetry measurements of Harrington et al [30] on crystalline KRS-5 at HF and DF laser wavelengths; transmission measurements on long polycrystalline KRS-5 fibers at 10.6 ~m by Harrington and Standlee [31]; laser calorimetry at 1, 5, and 10/xm by Belousov et al [32] on crystalline KRS-5 and KRS-6; carbon-monoxide laser calorimetry measurements of Nosov et al [33] on crystalline KRS-5 and KRS-6; and differentialspectrophotometry measurements of Hidaka et aL [12] on crystalline KRS-5.…”
Section: Mixed Thallous Halides Krs-5 and Krs-6mentioning
confidence: 99%