1971
DOI: 10.1364/josa.61.000143
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Loss Mechanisms and Measurements in Clad Glass Fibers and Bulk Glass

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Cited by 61 publications
(11 citation statements)
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“…It could also be due to different heat treatments of the two samples of glass since these are known to cause quite large changes in the loss coefficients. Results obtained for F2 at 633 nm with a rather simpler apparatus [12] using a helium/neon laser give 560 dB/km as compared with 390 dB/km from fig. 5a.…”
Section: /Zmmentioning
confidence: 91%
“…It could also be due to different heat treatments of the two samples of glass since these are known to cause quite large changes in the loss coefficients. Results obtained for F2 at 633 nm with a rather simpler apparatus [12] using a helium/neon laser give 560 dB/km as compared with 390 dB/km from fig. 5a.…”
Section: /Zmmentioning
confidence: 91%
“…In this work we improve and automate a well-known characterization approach for the study of locally out-scattered light [12,13] to provide accurate length-resolved measurements of the out-scattered fraction of light from a fiber under test (FUT). We name this technique (longitudinally resolved) Optical Side Scattering Radiometry (OSSR).…”
Section: Optical Side Scattering Radiometrymentioning
confidence: 99%
“…Furthermore, if the components of the scattered light in the optical fiber are all neglected, as was done in Vali and Shorthill (3,41, the peak S/N for a single detector reduces to j DP cw I 'l~c w (13) N peak 4 qB 0 4 hv B 0 'w hich is one-fourth of the SIN for a standard heterodyne technique with a synchronous detector , and one-half of that of the baseband direct-detection technique.…”
Section: Hi 'mentioning
confidence: 99%