无机材料学报 ›› 2024, Vol. 39 ›› Issue (3): 330-336.DOI: 10.15541/jim20230462 CSTR: 32189.14.10.15541/jim20230462
所属专题: 【AI4材料】Al4材料(202512)
TAM YU Puy Mang1,2(
), 徐愉3, 高泉浩1,2, 周海琼1,2, 张振4, 尹浩1,5, 李真1,2,5(
), 吕启涛5, 陈振强1,2,5, 马凤凯1,2(
), 苏良碧4
收稿日期:2023-10-09
修回日期:2023-11-20
出版日期:2024-03-20
网络出版日期:2023-11-28
通讯作者:
李真, 教授. E-mail: ailz268@126.com;作者简介:TAM YU Puy Mang (1997-), 女, 硕士研究生. E-mail: pmtamyu@outlook.com
TAM YU Puy Mang1,2(
), XU Yu3, GAO Quanhao1,2, ZHOU Haiqiong1,2, ZHANG Zhen4, YIN Hao1,5, LI Zhen1,2,5(
), LÜ Qitao5, CHEN Zhenqiang1,2,5, MA Fengkai1,2(
), SU Liangbi4
Received:2023-10-09
Revised:2023-11-20
Published:2024-03-20
Online:2023-11-28
Contact:
LI Zhen, professor. E-mail: ailz268@126.com;About author:TAM YU Puy Mang (1997-), female, Master candidate. E-mail: pmtamyu@outlook.com
Supported by:摘要:
3 μm波段中红外激光处于大气传输窗口, 又可以作为基础光源, 是激光技术研究的前沿。目前, 铒离子激活的激光晶体材料是产生3 μm中红外激光的重要途径之一。然而, Er3+离子4I11/2激光上能级荧光寿命较短, 下能级4I13/2的寿命较长, 难以实现粒子数反转, 导致自终止现象。为了解决这一难题, 往往需要高浓度掺杂, 通过能量传递降低4I13/2能级的寿命。然而高浓度掺杂又会造成晶体热性能变差, 限制了掺Er3+激光晶体效率和功率。三阶铒离子容易在氟化物晶体中形成团簇, 导致稀土离子间距缩短, 即使在低掺杂浓度下稀土离子之间的能量传递作用仍较为显著。同时, 低浓度掺杂还可以减轻激光运转下晶体的热堆积效应。掺铒氟化物晶体已成为一类重要的高功率、高效率中红外激光材料。然而, 掺铒氟化物晶体的光谱性能与铒离子团簇结构之间的相互联系尚不明确, 制约了掺铒氟化物晶体光谱和激光性能的进一步发展。本文采用第一性原理计算模拟了铒离子在CaF2、SrF2和PbF2晶体中的团簇结构。结果显示, 铒离子团簇结构随基质晶体变化逐渐演变。结合模拟计算和实验表征定性揭示了不同晶体离子团簇与光谱性能的联系, 为掺铒氟化物中红外激光晶体材料的调控与设计提供参考。
中图分类号:
TAM YU Puy Mang, 徐愉, 高泉浩, 周海琼, 张振, 尹浩, 李真, 吕启涛, 陈振强, 马凤凯, 苏良碧. 掺铒CaF2、SrF2、PbF2晶体的光谱性能与团簇结构研究[J]. 无机材料学报, 2024, 39(3): 330-336.
TAM YU Puy Mang, XU Yu, GAO Quanhao, ZHOU Haiqiong, ZHANG Zhen, YIN Hao, LI Zhen, LÜ Qitao, CHEN Zhenqiang, MA Fengkai, SU Liangbi. Spectroscopic Properties and Optical Clusters in Erbium-doped CaF2, SrF2 and PbF2 Crystals[J]. Journal of Inorganic Materials, 2024, 39(3): 330-336.
Fig. 3 Selective excited and height normalized emission spectra of 4S3/2→4I15/2 transition in Er3+-doped fluoride (a) CaF2; (b) SrF2; (c) PbF2; Colorful figures are available on website
| Symbol | Formation energy/eV | ||
|---|---|---|---|
| CaF2 | SrF2 | PbF2 | |
| 11|0|0|11 | -0.637 | - | - |
| 11|0|0|12 | -0.624 | -0.725 | -0.371 |
| 11|0|1|21 | -1.272 | - | - |
| 11|0|4|21 | - | - | -1.109 |
| 21|0|2|21 | -2.305 | -1.700 | -1.145* |
| 21|0|3|31 | -3.214 | -2.308 | - |
| 21|0|6|31 | - | - | -1.825 |
| 31|0|1|31 | -3.909 | -2.722* | -1.662* |
| 31|0|5|41 | -4.729 | - | - |
| 31|0|8|41 | -4.555 | -4.200 | -3.350 |
| 31|0|8|41-C | -4.628 | -4.220 | - |
| 41|1|0|41 | -4.328* | -2.865* | -1.511* |
| 41|0|8|41-O | -5.749 | -5.651 | -3.754 |
| 41|0|8|41-A1 | -5.781 | -5.655 | -3.807 |
| 41|0|8|51-O | -6.407 | - | - |
| 41|0|8|51-A | -6.564 | - | -4.280 |
| 51|0|8|51 | -7.860 | -7.233 | -4.760 |
| 61|0|8|51 | -8.568 | -8.134 | -5.360 |
| 61|0|8|61 | -9.042 | - | - |
Table S1 Formation energy of Er3+ clusters in CaF2, SrF2 and PbF2
| Symbol | Formation energy/eV | ||
|---|---|---|---|
| CaF2 | SrF2 | PbF2 | |
| 11|0|0|11 | -0.637 | - | - |
| 11|0|0|12 | -0.624 | -0.725 | -0.371 |
| 11|0|1|21 | -1.272 | - | - |
| 11|0|4|21 | - | - | -1.109 |
| 21|0|2|21 | -2.305 | -1.700 | -1.145* |
| 21|0|3|31 | -3.214 | -2.308 | - |
| 21|0|6|31 | - | - | -1.825 |
| 31|0|1|31 | -3.909 | -2.722* | -1.662* |
| 31|0|5|41 | -4.729 | - | - |
| 31|0|8|41 | -4.555 | -4.200 | -3.350 |
| 31|0|8|41-C | -4.628 | -4.220 | - |
| 41|1|0|41 | -4.328* | -2.865* | -1.511* |
| 41|0|8|41-O | -5.749 | -5.651 | -3.754 |
| 41|0|8|41-A1 | -5.781 | -5.655 | -3.807 |
| 41|0|8|51-O | -6.407 | - | - |
| 41|0|8|51-A | -6.564 | - | -4.280 |
| 51|0|8|51 | -7.860 | -7.233 | -4.760 |
| 61|0|8|51 | -8.568 | -8.134 | -5.360 |
| 61|0|8|61 | -9.042 | - | - |
| Symbol | Formation energy/eV | ||
|---|---|---|---|
| La3+ | Tb3+ | Y3+ | |
| 11|0|0|11 | -0.107 | - | - |
| 11|0|0|12 | -0.204 | -0.346 | -0.355 |
| 11|0|1|21 | -0.653 | -0.791 | - |
| 11|0|2|21 | - | - | -0.785 |
| 21|0|1|21 | -0.914 | - | - |
| 21|0|2|21 | - | -1.040 | -1.123 |
| 21|0|5|31 | - | -1.530 | -1.523 |
| 21|0|1|31 | -1.580 | - | - |
| 31|0|1|31 | -1.911 | -1.622* | -1.590* |
| 31|0|2|41 | -2.215 | - | - |
| 31|0|8|41 | -1.511* | -3.172 | -3.203 |
| 41|1|0|41 | -2.319 | -1.690* | -1.488* |
| 41|0|8|41-O | - | -3.452 | -3.542 |
| 41|0|8|41-A1 | - | -3.504 | -3.575 |
| 41|0|8|41-A2 | -2.132* | -3.383 | -3.417 |
| 41|0|8|51-A | -2.605 | -3.984 | -4.108 |
| 51|0|8|51 | -3.196 | -4.585 | -4.627 |
| 61|0|8|51 | -3.811 | -5.153 | -5.169 |
| 61|0|8|61 | -4.075 | - | - |
Table S2 Formation energy of the clusters in La3+:PbF2, Tb3+:PbF2 and Y3+:PbF2
| Symbol | Formation energy/eV | ||
|---|---|---|---|
| La3+ | Tb3+ | Y3+ | |
| 11|0|0|11 | -0.107 | - | - |
| 11|0|0|12 | -0.204 | -0.346 | -0.355 |
| 11|0|1|21 | -0.653 | -0.791 | - |
| 11|0|2|21 | - | - | -0.785 |
| 21|0|1|21 | -0.914 | - | - |
| 21|0|2|21 | - | -1.040 | -1.123 |
| 21|0|5|31 | - | -1.530 | -1.523 |
| 21|0|1|31 | -1.580 | - | - |
| 31|0|1|31 | -1.911 | -1.622* | -1.590* |
| 31|0|2|41 | -2.215 | - | - |
| 31|0|8|41 | -1.511* | -3.172 | -3.203 |
| 41|1|0|41 | -2.319 | -1.690* | -1.488* |
| 41|0|8|41-O | - | -3.452 | -3.542 |
| 41|0|8|41-A1 | - | -3.504 | -3.575 |
| 41|0|8|41-A2 | -2.132* | -3.383 | -3.417 |
| 41|0|8|51-A | -2.605 | -3.984 | -4.108 |
| 51|0|8|51 | -3.196 | -4.585 | -4.627 |
| 61|0|8|51 | -3.811 | -5.153 | -5.169 |
| 61|0|8|61 | -4.075 | - | - |
Fig. S1 Salculated thermodynamic stable centers of Er3+ in fluoride (C) CaF2; (S) SrF2; (P) PbF2 Centers are divided into three groups, the monomers, cubic sublattice clusters and square antiprism structure clusters which are denoted as “1”, “2” and “3”, respectively
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