2020
DOI: 10.1111/jace.17311
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Effect of Yb concentration on the microstructures, spectra, and laser performance of Yb: CaF2 transparent ceramics

Abstract: Ytterbium‐doped calcium fluoride transparent ceramics is considered as a promising laser gain medium. How to prepare low scattering loss ceramics is the main challenge at present. In this study, a simple route of hot‐pressing method was introduced to fabricate high optical quality of Yb: CaF2 laser ceramics with different concentration of Yb ions. The influence of Yb concentration on the particle sizes of the powders, microstructure, fluorescence spectra, output power, and laser emitting spectra of Yb: CaF2 tr… Show more

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Cited by 19 publications
(5 citation statements)
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“…Normally, the ceramics prepared by CSP contain a significant amount of residual pores and amorphous grain boundaries (GBs) after the reaction involved grain growth, which is highly detrimental to the transmittance of ceramics. [ 11 ] Therefore, the transparent ceramic in visible‐light spectra has never been realized by CSP except for the one with an extremely low melting point of LiF. [ 12 ] Generally, the transmittance (T) of polycrystalline ceramic is expressed by the following equation, [ 13 ] T badbreak= (1 badbreak− Rs) exp(badbreak−γd)\[ \begin{array}{*{20}{c}}{T\; = \;\left( {1\; - \;{R_s}} \right)\;{\rm{exp}}\left( { - \gamma d} \right)}\end{array} \] where R s describes the reflection losses at the two sample surfaces, γ is the total absorption coefficient, and d is the sample thickness.…”
Section: Resultsmentioning
confidence: 99%
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“…Normally, the ceramics prepared by CSP contain a significant amount of residual pores and amorphous grain boundaries (GBs) after the reaction involved grain growth, which is highly detrimental to the transmittance of ceramics. [ 11 ] Therefore, the transparent ceramic in visible‐light spectra has never been realized by CSP except for the one with an extremely low melting point of LiF. [ 12 ] Generally, the transmittance (T) of polycrystalline ceramic is expressed by the following equation, [ 13 ] T badbreak= (1 badbreak− Rs) exp(badbreak−γd)\[ \begin{array}{*{20}{c}}{T\; = \;\left( {1\; - \;{R_s}} \right)\;{\rm{exp}}\left( { - \gamma d} \right)}\end{array} \] where R s describes the reflection losses at the two sample surfaces, γ is the total absorption coefficient, and d is the sample thickness.…”
Section: Resultsmentioning
confidence: 99%
“…d) TEM image of the microstructure on the CaF 2 ‐HCl nanoceramic, and HRTEM images of a clean and coherent GB. e) In‐line transmittance spectra for CaF 2 ‐HCl, UD‐CaF 2 ‐HCl, Deox‐CaF 2 ‐HCl and HP‐CaF 2 (dot line), [ 11 ] respectively. f) Digital image of CaF 2 ‐HCl, UD‐CaF 2 ‐HCl, and Deox‐CaF 2 ‐HCl ceramics on a printed paper (left), and photographs showing the view with and without CaF 2 ‐HCl nanoceramic under sunlight (right).…”
Section: Resultsmentioning
confidence: 99%
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