Broadband 2.9 μm mid-infrared fluorescence behavior of Dy3+/Tm3+ co-doped zirconium fluoride glasses
•With the introduction of Tm3+, Dy3+ can achieve broadband emission between 2600 and 3400 nm.•The mid-infrared fluorescence intensity enhanced with the increase of Tm3+ due to the energy transfer process between Dy3+ and Tm3+.•Larger absorption and emission cross-sections the glass owned, the gain c...
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Veröffentlicht in: | Infrared physics & technology 2022-11, Vol.126, p.104330, Article 104330 |
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Sprache: | eng |
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Zusammenfassung: | •With the introduction of Tm3+, Dy3+ can achieve broadband emission between 2600 and 3400 nm.•The mid-infrared fluorescence intensity enhanced with the increase of Tm3+ due to the energy transfer process between Dy3+ and Tm3+.•Larger absorption and emission cross-sections the glass owned, the gain coefficient was also greatly improved.•The fluorescence lifetime at 2.9 μm were prolonged with the addition of Tm3+.
We report the 2600–3400 nm strong mid-infrared (MIR) fluorescence emission with the full width at half maximum (FWHM) of 355 nm in the zirconium fluoride glass incorporated with Dy3+, Tm3+ ions. In this paper, Dy3+, Tm3+ ions co-doped ZrF4-BaF2-LaF3-AlF3-YF3 zirconium fluoride glasses are synthesized by high temperature melting method. Structure information is obtained by raman spectroscopy, and the maximum phonon energy of the synthesized glass is 575 cm−1. Optical performance is mainly characterized by transmission spectrum, absorption spectrum and emission spectrum, theoretical analysis is described by Judd-Ofelt (J-O) theory, cross sections and gain coefficient. Under the 808 nm Laser Diode (LD), the 2.9 μm mid-infrared emission intensity is significantly enhanced with the introduction of Tm3+, and the fluorescence lifetime is prolonged 1.85 ms, the relevant energy transfer mechanism has been further analyzed. All results show that the new glass material may be a potential medium for mid-infrared broadband fiber amplifiers and lasers. |
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ISSN: | 1350-4495 1879-0275 |
DOI: | 10.1016/j.infrared.2022.104330 |