2008
DOI: 10.1016/j.jlumin.2007.05.010
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Tm and Tm–Tb-doped germanate glasses for S-band amplifiers

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Cited by 16 publications
(9 citation statements)
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“…A population inversion density of 1.6 Â 10 18 Tm 3+ ions cm À3 was obtained for a pump intensity of 2.7 kW cm À2 , which is $5.3 times bigger that one verified in Tm(0.1%):Ho(0.15%):Ge-Ga-As-S-CsBr [7] ($3 Â 10 17 cm À3 ). This population inversion density is also higher than that one estimated for Tm(0.1%):Tb(0.2%):GLKZ [4] ($2 Â 10 17 cm À3 ) and for Tm(0.1%):Tb(0.15%):Ge-Ga-As-S-CsBr [7] ($2.5 Â 10 17 cm À3 ) glasses for similar pumping conditions. This result points that Tm:Ho:ZBLAN doped with 0.5 mol% of Tm 3+ and codoped with 1 mol% of Ho 3+ maximizes its amplification potential gain based on the Tm 3+ -stimulated emission near 1.5 mm, so making this material very promising system for light signal amplification in S-band of telecommunication.…”
Section: Discussioncontrasting
confidence: 45%
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“…A population inversion density of 1.6 Â 10 18 Tm 3+ ions cm À3 was obtained for a pump intensity of 2.7 kW cm À2 , which is $5.3 times bigger that one verified in Tm(0.1%):Ho(0.15%):Ge-Ga-As-S-CsBr [7] ($3 Â 10 17 cm À3 ). This population inversion density is also higher than that one estimated for Tm(0.1%):Tb(0.2%):GLKZ [4] ($2 Â 10 17 cm À3 ) and for Tm(0.1%):Tb(0.15%):Ge-Ga-As-S-CsBr [7] ($2.5 Â 10 17 cm À3 ) glasses for similar pumping conditions. This result points that Tm:Ho:ZBLAN doped with 0.5 mol% of Tm 3+ and codoped with 1 mol% of Ho 3+ maximizes its amplification potential gain based on the Tm 3+ -stimulated emission near 1.5 mm, so making this material very promising system for light signal amplification in S-band of telecommunication.…”
Section: Discussioncontrasting
confidence: 45%
“…In addition, this reminiscence luminescence of 3 F 4 state exhibits an exponential decay with a lifetime similar to that one observed for single Tm-doped ZBLAN ($7 ms). On the other hand, residual 3 F 4 luminescence was not observed in the case of Tm:Ho in tellurite [10], chalcogenide [7] and Tm:Tb in germanate (GLKZ) [4] glasses. This luminescence effect (residual) evidences that the fast energy migration through 3 F 4 excited states leads to two distinct types of Tm 3+ excited ions in ZBLAN glass (or classes): (i) class 1-excited Tm 3+ ions close by Ho 3+ that has a K 1 transfer rate resultant from Tm( 3 F 4 )-Ho( 5 I 7 ) transfer minus Ho( 5 I 7 )-Tm( 3 F 4 ) back-transfer rates and (ii) class 2-excited Tm 3+ ions ( 3 F 4 ) far from Ho 3+ ions (or isolated) having an intrinsic lifetime of $7 ms.…”
Section: Rate Equations For Optical Excitation Of the 3 H 4 Levelmentioning
confidence: 96%
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“…The luminescent 3 F 4 level of Tm 3+ , for example, can be efficiently depopulated by Ho 3+ and Tb 3+ ions in fluorozirconate ͑ZBLAN͒, tellurite, Ge-Ga-As-S-CsBr and GeO 2 -Li 2 O-K 2 O -ZnO codoped glasses, making these materials suitable for use as optical amplifiers operating in 1.4-1.5 m region of the spectrum. [1][2][3][4][5] For applications requiring laser operation at 2.9 m, Ho 3+ -doped LiYF 4 ͑YLF͒ crystal 6 operating on the 5 I 6 → 5 I 7 transition has the potential for pulsed laser operation despite the longer ϳ16 ms lifetime of the lower laser ͑ 5 I 7 ͒ level when compared to the lifetime of the upper laser ͑ 5 I 6 ͒ level which is ϳ3 ms. 7 Many applications, however, require continuous wave ͑cw͒ operation in this spectral range. To achieve this end, a deactivator ion must be introduced in order to quench the excited state population in the 5 I 7 level.…”
Section: Introductionmentioning
confidence: 99%