2004
DOI: 10.1016/j.matlet.2004.05.083
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Characterization of broadband amplified spontaneous emission of erbium-doped tellurite fiber with D-shape cladding

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Cited by 4 publications
(3 citation statements)
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“…In order to cover the above wavelength range, it is crucial to extract optical gain in EDF for the wavelengths shorter than the 1480 nm. Usually, the optical gain ranging from 1450 nm to 1480 nm for fiber lasers can be obtained by photon absorption method through the laser transition between 3 H 4 → 3 F 4 multiplet in thulium-doped fiber [5][6][7], the 4 I 13/2 → 4 I 15/2 multiplet in erbium-doped tellurite fiber [8,9] or by photon inelastic scattering method through the transition between the virtual excited states to ground state in silica Raman fiber [10]. Conventionally, the 4 I 13/2 → 4 I 15/2 multiplet of silica-based EDF at room temperature can only emit fluorescence at the wavelengths longer than 1490 nm [11].…”
Section: Introductionmentioning
confidence: 99%
“…In order to cover the above wavelength range, it is crucial to extract optical gain in EDF for the wavelengths shorter than the 1480 nm. Usually, the optical gain ranging from 1450 nm to 1480 nm for fiber lasers can be obtained by photon absorption method through the laser transition between 3 H 4 → 3 F 4 multiplet in thulium-doped fiber [5][6][7], the 4 I 13/2 → 4 I 15/2 multiplet in erbium-doped tellurite fiber [8,9] or by photon inelastic scattering method through the transition between the virtual excited states to ground state in silica Raman fiber [10]. Conventionally, the 4 I 13/2 → 4 I 15/2 multiplet of silica-based EDF at room temperature can only emit fluorescence at the wavelengths longer than 1490 nm [11].…”
Section: Introductionmentioning
confidence: 99%
“…Peak wavelength instability is shown in figure 4(b). This effect may be explained by approaching the lasing threshold due to back reflections from the splice of rare-earth-doped fiber with silica fiber similar to [13]. It may be clearly observed at a fiber length of 34 cm.…”
Section: Resultsmentioning
confidence: 89%
“…For multi-channel WDM transmission, it is essential to have a flat-gain broadband spectrum to minimize channel-to-channel crosstalk and gain excursion [8,9,10]. However, the bandwidths of the conventional erbium-doped fiber amplifier (EDFA) for the C-band (1530–1565 nm) and the thulium-doped fiber amplifier (TDFA) for the S-band (1460–1530 nm) are limited [11,12]. A logical approach to achieving broadband gain covering the S + C band is to dope with both Er 3+ and Tm 3+ [13,14,15,16].…”
Section: Introductionmentioning
confidence: 99%