2008
DOI: 10.1016/j.yofte.2008.01.004
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Superfluorescence from Yb- and Yb–Er-doped phosphotellurite glass fibres

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Cited by 13 publications
(4 citation statements)
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“…One can also notice that the shape of the emission bands changes due to changes in the fiber length: for long fibers (3 and 7 cm), the bands are not anymore flat and uniform, the emission bands exhibit pronounced peaks and dips, the number of which consistently increases with fiber length. These changes in the emission spectra induced by the changes in the fiber lengths are a clear sign of spectral hole burning effect as reported in [31]. These changes are due to strong reabsorption of the peak wavelength at 974 nm by Yb 3+ ions and at 1534 nm by Er 3+ ions originated from high concentration of the rare-earth ions (1.58·10 20 cm −3 for Er and 4.75·10 20 cm −3 for Yb) and insufficient pump level to stimulate luminescence.…”
Section: Resultssupporting
confidence: 58%
“…One can also notice that the shape of the emission bands changes due to changes in the fiber length: for long fibers (3 and 7 cm), the bands are not anymore flat and uniform, the emission bands exhibit pronounced peaks and dips, the number of which consistently increases with fiber length. These changes in the emission spectra induced by the changes in the fiber lengths are a clear sign of spectral hole burning effect as reported in [31]. These changes are due to strong reabsorption of the peak wavelength at 974 nm by Yb 3+ ions and at 1534 nm by Er 3+ ions originated from high concentration of the rare-earth ions (1.58·10 20 cm −3 for Er and 4.75·10 20 cm −3 for Yb) and insufficient pump level to stimulate luminescence.…”
Section: Resultssupporting
confidence: 58%
“…In such a configuration, neodymium ions function as donors, supplying a portion of their excitation energy in the course of Nd 3+ →Yb 3+ resonant energy transfer. Spectral adjustment of the doping ions results in a broad luminescence spectrum, which allows to manufacture fibre lasers working as sources of amplified spontaneous emission (ASE) [17,18]. Excitation of neodymium ions with 808 nm wavelength leads to the population of 4 F 3/2 energy state, from which the emission in the band of 890 nm proceeds corresponding to the transition of photons to the ground state 4 I 9/2 , with simultaneous energy transfer to the excited state 2 F 5/2 in Yb 3+ ions.…”
Section: Broadband Luminescence At 1µm Wavelength In Ndmentioning
confidence: 99%
“…Фосфатные волокна успешно зарекомендовали себя в качестве усиливающей среды в волоконных лазерах [9,[12][13][14] и усилителях [15][16][17], в то же время исследованию широкополосных источников из-лучения на основе фосфатных волокон посвящено незначительное ко-личество работ [18,19].…”
Section: Introductionunclassified