“…Similarly, these cross-section parameters are obtained for all FP glasses. It is evident that the emission cross-section is high in the lithium fluoro-phosphate glass with the value of 14.5x10 -21 cm 2 which is comparable to those obtained for Er 3+ doped phosphate glasses 6.43x10 -21 cm 2 [38]; germanium-silicate glasses 9.55x10 -21 cm 2 [39]; bismuth borate glasses 10.3x10 -21 cm 2 [40] and lower than that of tellurite glasses [27]; chalcogeneide glasses 15.73x10 -21 cm 2 [41]; The large value of emission cross section indicates that this glass is a promising material for lasing action. Besides, stimulated emission cross-section is low for the bismuth FP glass matrix (5.3x10 -21 cm 2 ).…”
Section: Absorption and Emission Cross-sectionssupporting
confidence: 68%
“…The obtained value of Ω 2 in lithium fluoro-phosphate glass is 9.91x10 -20 cm 2 which is higher than that in glasses such as bismuthate [25], phosphate [26], tellurite [27], borosilicate [28] and fluoro-phosphate [29] which indicates that higher asymmetry/covalency between erbium and oxygen ligand than the above glasses.…”
Section: Optical Absorption Spectra and Judd-ofelt Analysismentioning
confidence: 99%
“…In the case of sodium and bismuth glass matrices observed trend is found to be 2 > 4 > 6. [25][26][27][28][29]. The Ω 4 and Ω 6 parameters are related to the rigidity and viscosity of the medium in which the ions are situated and the Ω 4 parameter is affected by the factors causing the changes of Ω 2 and Ω 6 .…”
Section: Optical Absorption Spectra and Judd-ofelt Analysismentioning
“…Similarly, these cross-section parameters are obtained for all FP glasses. It is evident that the emission cross-section is high in the lithium fluoro-phosphate glass with the value of 14.5x10 -21 cm 2 which is comparable to those obtained for Er 3+ doped phosphate glasses 6.43x10 -21 cm 2 [38]; germanium-silicate glasses 9.55x10 -21 cm 2 [39]; bismuth borate glasses 10.3x10 -21 cm 2 [40] and lower than that of tellurite glasses [27]; chalcogeneide glasses 15.73x10 -21 cm 2 [41]; The large value of emission cross section indicates that this glass is a promising material for lasing action. Besides, stimulated emission cross-section is low for the bismuth FP glass matrix (5.3x10 -21 cm 2 ).…”
Section: Absorption and Emission Cross-sectionssupporting
confidence: 68%
“…The obtained value of Ω 2 in lithium fluoro-phosphate glass is 9.91x10 -20 cm 2 which is higher than that in glasses such as bismuthate [25], phosphate [26], tellurite [27], borosilicate [28] and fluoro-phosphate [29] which indicates that higher asymmetry/covalency between erbium and oxygen ligand than the above glasses.…”
Section: Optical Absorption Spectra and Judd-ofelt Analysismentioning
confidence: 99%
“…In the case of sodium and bismuth glass matrices observed trend is found to be 2 > 4 > 6. [25][26][27][28][29]. The Ω 4 and Ω 6 parameters are related to the rigidity and viscosity of the medium in which the ions are situated and the Ω 4 parameter is affected by the factors causing the changes of Ω 2 and Ω 6 .…”
Section: Optical Absorption Spectra and Judd-ofelt Analysismentioning
“…Three main loss components can be identified: propagation and coupling loss due light propagation in the polymer waveguide (polymer-only), scattering (Rayleigh) loss due to the presence of the NPs, and erbium absorption loss due to the presence of Er ions. The polymer-only loss is estimated using a non-doped polymer waveguide of the same dimensions and length, while the scattering loss is calculated using a Rayleigh model [29] and the fact that very low Er-induced absorption losses are expected at the longer wavelength of 1575 nm [30]. The analysis reveals a scattering loss in the range of 11 to 14 dB for wavelength range studied.…”
Optical interconnects have an important role to play in next-generation high-performance electronic systems by enabling power-efficient high-speed board-level communication links. Polymer-based optical waveguides is a leading technology for integrating optical links onto standard printed circuit boards as it is sufficiently low cost and enables cost-effective manufacturing and assembly. Various polymer-based optical backplanes have been reported in recent years enabling different on-board interconnection architectures. However, all currently demonstrated systems are purely passive, which limits therefore the reach, complexity and functionality of these on-board systems. Here, we present recent simulation and experimental studies towards the development of Erdoped polymer-based waveguide amplifiers. Two different approaches to integrate Er-doped materials in siloxane polymer are investigated: (i) ultrafast laser plasma implantation of Er-doped glasses and (ii) solutionbased dispersion of Er-doped nanoparticles. Experimental and simulation results on the achievable performance from such waveguide amplifiers are presented focusing on impact of the waveguide loss and upconversion on the gain figure.
“…the glass transition temperature them. More often, the difference T ∆ is a suitable measure for the thermal stability against crystallization and a large T ∆ represents strong inhibition of nucleation and crystallizing actions [26,27]. Therefore, it is desirable for the glass host to possess T ∆ as large as possible.…”
Section: Thermal Stability and Structural Behaviormentioning
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