1995
DOI: 10.1049/el:19950428
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Characterisation of Bragg gratings in fibreswith the heat-scan technique

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Cited by 21 publications
(6 citation statements)
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“…This spectral response is generated by the optical beating between the spectra of the unperturbed grating regions, modulated by the phase shift induced by the loading. The main difference, here, with previously reported works on phase-shifted FBG [11][12][13], is when the birefringence axes are rotated, which may happen if the loading is along a direction different to the fast or slow axis of the fiber, and then there is coupling between polarization modes as shown in Fig. 3(b).…”
Section: Response Of Fbg Written In Specialty Single-mode Fibersmentioning
confidence: 70%
“…This spectral response is generated by the optical beating between the spectra of the unperturbed grating regions, modulated by the phase shift induced by the loading. The main difference, here, with previously reported works on phase-shifted FBG [11][12][13], is when the birefringence axes are rotated, which may happen if the loading is along a direction different to the fast or slow axis of the fiber, and then there is coupling between polarization modes as shown in Fig. 3(b).…”
Section: Response Of Fbg Written In Specialty Single-mode Fibersmentioning
confidence: 70%
“…The relatively short length of the FBGs and the separation between the fiber and the hot wire means that the hot wire is effectively heating up the entire FBG, causing the grating to shift up in wavelength by approximately 0.3 nm. The localized heat source does not create any spectral separation of the peak such as that seen in the previous heat scanning techniques, [8][9][10] and allows fast continuous scanning with only peak wavelength detection algorithms. The low temperature and short exposure time do not create any annealing-induced changes in the grating profile or reflected peak wavelength.…”
Section: Characterizationmentioning
confidence: 99%
“…Heat scanning techniques have also been used to characterize FBGs that induce a phase change in the FBG spectra. [8][9][10] Limitations include slow scanning times to allow for thermal stabilization, requiring up to 20 min for FBG characterization. These combined limitations of scanning time, setup complexity, stripping coating, and resolution meant they were not directly suitable for the basis for the automated marking of long DTG arrays as part of a device manufacturing process.…”
Section: Introductionmentioning
confidence: 99%
“…The fiber's refractive index in this small heated region will be perturbed when the fiber is heated at this point due to the thermo-optical effect. When heating the fiber at a certain point, the change in the fiber's length can be neglected compared with the thermallyinduced phase shift because the thermal expansion coefficient is much smaller than the thermal-optical coefficient of the fiber [126]. Due to the thermo-optical effect, the refractive index of the fiber will change when a phase shift is introduced at this heating point.…”
Section: Chapter 6 Tunable Comb Filter and Tunable Multi-wave Length mentioning
confidence: 99%
“…As a result, broad spectral perturbations will be introduced into the short-wavelength side of the main spectral peaks [126]. By placing heat sinks on the two sides of each resistance wire, the broad spectral perturbations of the spectral peak in the shortwavelength range can be reduced (as shown in Fig.…”
Section: Tunable and Switchable Multiwavelength Optical Sourcementioning
confidence: 99%