We report on micro-Raman spectra of several mixed laser ceramics, i.e., 5at.%Tm: at.% Tm: (ScxY1-xO2)(3) with x = 0.121, 0.252, 0.489 and 5at.%Tm:Y2O3 ceramic. The samples were fabricated by solid-state pressureless consolidation of nanopowders produced by laser ablation of solid target in airflow. In particular, we studied the influence of Sc3+ content on the active vibration modes in terms of peak positions and shifts, linewidths and shapes: these parameters are relevant for the emission bandwidth of the laser medium. A shift towards higher frequencies is measured with the increase of the Sc3+ content in all samples in particular in (Tm 0.048 Y 0.463 Sc 0.489 O 2 ) 3 where the main Raman peaks are placed at 395, 494, 635 cm(-1) while their shifts with Tm:Y2O3 are 22.6, 25.1, 40.1 cm(-1), respectively. The assignment of the vibrational spectrum was obtained by density functional theory (DFT) with the Perdew-Burke-Enzerhof (PBE) exchange-correlation functional within the harmonic approximation framework. (c) 2024 Optica Publishing Group under the terms of the Optica Open Access Publishing Agreement
Dependence of the Raman vibration modes on structural properties of Tm:(ScxY1 −x)2O3 laser ceramics with 0 ≤ x < 1 / Pirri A.; Santonocito A.; Maksimov R.N.; Shitov V.A.; Becucci M.; Patrizi B.; Vannini M.; Toci G.. - In: OPTICS EXPRESS. - ISSN 1094-4087. - STAMPA. - 32:(2024), pp. 23932-23944. [10.1364/OE.518356]
Dependence of the Raman vibration modes on structural properties of Tm:(ScxY1 −x)2O3 laser ceramics with 0 ≤ x < 1
Becucci M.;
2024
Abstract
We report on micro-Raman spectra of several mixed laser ceramics, i.e., 5at.%Tm: at.% Tm: (ScxY1-xO2)(3) with x = 0.121, 0.252, 0.489 and 5at.%Tm:Y2O3 ceramic. The samples were fabricated by solid-state pressureless consolidation of nanopowders produced by laser ablation of solid target in airflow. In particular, we studied the influence of Sc3+ content on the active vibration modes in terms of peak positions and shifts, linewidths and shapes: these parameters are relevant for the emission bandwidth of the laser medium. A shift towards higher frequencies is measured with the increase of the Sc3+ content in all samples in particular in (Tm 0.048 Y 0.463 Sc 0.489 O 2 ) 3 where the main Raman peaks are placed at 395, 494, 635 cm(-1) while their shifts with Tm:Y2O3 are 22.6, 25.1, 40.1 cm(-1), respectively. The assignment of the vibrational spectrum was obtained by density functional theory (DFT) with the Perdew-Burke-Enzerhof (PBE) exchange-correlation functional within the harmonic approximation framework. (c) 2024 Optica Publishing Group under the terms of the Optica Open Access Publishing AgreementFile | Dimensione | Formato | |
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