The optical properties of Tm3+ doped Na5Lu9F32 single crystal
Tm(3+) doped Na5Lu9F(32) single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt(t=2, 4, 6) were calculated according to the measured absorption spectra and physical-chemical properties of the obtained Na5Lu9F(32) single crystal. The...
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Published in | Optoelectronics letters Vol. 13; no. 3; pp. 201 - 205 |
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Tianjin
Tianjin University of Technology
01.05.2017
Springer Nature B.V |
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Abstract | Tm(3+) doped Na5Lu9F(32) single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt(t=2, 4, 6) were calculated according to the measured absorption spectra and physical-chemical properties of the obtained Na5Lu9F(32) single crystal. The stimulated emission cross-section of the 3F4→3H6 transition(~1.8 μm) is 0.35×10(-20) cm2 for Tm(3+) doped Na5Lu9F(32) single crystal. The emission spectra under the excitation of 790 nm laser diode(LD) and fluorescence lifetime at 1.8 μm were measured to reveal the fluorescence properties of Tm(3+) doped Na5Lu9F(32) single crystal. The research results show that the Tm(3+) doped Na5Lu9F(32) single crystal has larger stimulated emission cross-section compared with other crystals. All these spectral properties suggest that this kind of Tm(3+)doped Na5Lu9F(32) crystal with high physical-chemical stability and high-efficiency emission at 1.8 μm may be used as potential laser materials for optical devices. |
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AbstractList | Tm3+ doped Na5Lu9F32 single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt (t=2, 4, 6) were calculated according to the measured absorption spectra and physical-chemical properties of the obtained Na5Lu9F32 single crystal. The stimulated emission cross-section of the 3F4→3H6 transition (~1.8 μm) is 0.35×10-20 cm2 for Tm3+ doped Na5Lu9F32 single crystal. The emission spectra under the excitation of 790 nm laser diode (LD) and fluorescence lifetime at 1.8 μm were measured to reveal the fluorescence properties of Tm3+ doped Na5Lu9F32 single crystal. The research results show that the Tm3+ doped Na5Lu9F32 single crystal has larger stimulated emission cross-section compared with other crystals. All these spectral properties suggest that this kind of Tm3+doped Na5Lu9F32 crystal with high physical-chemical stability and high-efficiency emission at 1.8 μm may be used as potential laser materials for optical devices. Tm 3+ doped Na 5 Lu 9 F 32 single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ω t ( t =2, 4, 6) were calculated according to the measured absorption spectra and physical-chemical properties of the obtained Na 5 Lu 9 F 32 single crystal. The stimulated emission cross-section of the 3 F 4 → 3 H 6 transition (~1.8 μm) is 0.35×10 -20 cm 2 for Tm 3+ doped Na 5 Lu 9 F 32 single crystal. The emission spectra under the excitation of 790 nm laser diode (LD) and fluorescence lifetime at 1.8 μm were measured to reveal the fluorescence properties of Tm 3+ doped Na 5 Lu 9 F 32 single crystal. The research results show that the Tm 3+ doped Na 5 Lu 9 F 32 single crystal has larger stimulated emission cross-section compared with other crystals. All these spectral properties suggest that this kind of Tm 3+ doped Na 5 Lu 9 F 32 crystal with high physical-chemical stability and high-efficiency emission at 1.8 μm may be used as potential laser materials for optical devices. Tm(3+) doped Na5Lu9F(32) single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt(t=2, 4, 6) were calculated according to the measured absorption spectra and physical-chemical properties of the obtained Na5Lu9F(32) single crystal. The stimulated emission cross-section of the 3F4→3H6 transition(~1.8 μm) is 0.35×10(-20) cm2 for Tm(3+) doped Na5Lu9F(32) single crystal. The emission spectra under the excitation of 790 nm laser diode(LD) and fluorescence lifetime at 1.8 μm were measured to reveal the fluorescence properties of Tm(3+) doped Na5Lu9F(32) single crystal. The research results show that the Tm(3+) doped Na5Lu9F(32) single crystal has larger stimulated emission cross-section compared with other crystals. All these spectral properties suggest that this kind of Tm(3+)doped Na5Lu9F(32) crystal with high physical-chemical stability and high-efficiency emission at 1.8 μm may be used as potential laser materials for optical devices. |
Author | 盛启国 夏海平 汤庆阳 何仕楠 章践立 陈宝玖 |
AuthorAffiliation | Key Laboratory of Photo-electronic Materials, Ningbo University, Ningbo 315211, China Department of Physics, Dalian Maritime University, Dalian 116026, China |
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CitedBy_id | crossref_primary_10_1016_j_optmat_2019_109294 crossref_primary_10_1007_s11801_018_8043_8 crossref_primary_10_1016_j_jlumin_2023_120237 crossref_primary_10_1016_j_jallcom_2018_06_286 crossref_primary_10_1016_j_jlumin_2019_116553 |
Cites_doi | 10.1016/j.matlet.2016.10.071 10.1007/s11801-016-6145-8 10.1134/S1063783409090236 10.1016/S0022-3093(87)80182-5 10.1016/j.jallcom.2015.04.112 10.1088/0022-3727/41/11/115409 10.1364/OL.33.001951 10.1007/s11801-016-5221-4 10.1007/s11801-015-5115-x 10.1016/S0022-3697(01)00129-9 |
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Notes | 12-1370/TN Bridgman lifetime excitation stimulated relaxation excited transparency spacing spectrometer termine Tm(3+) doped Na5Lu9F(32) single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt(t=2, 4, 6) were calculated according to the measured absorption spectra and physical-chemical properties of the obtained Na5Lu9F(32) single crystal. The stimulated emission cross-section of the 3F4→3H6 transition(~1.8 μm) is 0.35×10(-20) cm2 for Tm(3+) doped Na5Lu9F(32) single crystal. The emission spectra under the excitation of 790 nm laser diode(LD) and fluorescence lifetime at 1.8 μm were measured to reveal the fluorescence properties of Tm(3+) doped Na5Lu9F(32) single crystal. The research results show that the Tm(3+) doped Na5Lu9F(32) single crystal has larger stimulated emission cross-section compared with other crystals. All these spectral properties suggest that this kind of Tm(3+)doped Na5Lu9F(32) crystal with high physical-chemical stability and high-efficiency emission at 1.8 μm may be used as potential laser materials for optical devices. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
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Snippet | Tm(3+) doped Na5Lu9F(32) single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt(t=2, 4, 6)... Tm 3+ doped Na 5 Lu 9 F 32 single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ω t ( t =2,... Tm3+ doped Na5Lu9F32 single crystal with high optical quality was grown by an improved Bridgman method. The Judd-Ofelt intensity parameters Ωt (t=2, 4, 6) were... |
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SubjectTerms | Absorption spectra Bridgman method Chemical properties Cross-sections Crystal growth Emission spectra Excitation spectra Fluorescence Laser materials Lasers Optical Devices Optical properties Optics Photonics Physics Physics and Astronomy Semiconductor lasers Single crystals Stimulated emission 光学性质 化学稳定性 单晶体 受激发射截面 吸收光谱 布里奇曼法 掺杂晶体 激光二极管 |
Title | The optical properties of Tm3+ doped Na5Lu9F32 single crystal |
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