Article(id=1319726555752935932, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319726426404803327, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20250102, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1739721600000, receivedDateStr=2025-02-17, revisedDate=1741708800000, revisedDateStr=2025-03-12, acceptedDate=null, acceptedDateStr=null, onlineDate=1792576930224, onlineDateStr=2026-10-21, pubDate=1766160000000, pubDateStr=2025-12-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792576930224, onlineIssueDateStr=2026-10-21, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792576930224, creator=13701087609, updateTime=1792576930224, updator=13701087609, issue=Issue{id=1319726426404803327, tenantId=1146029695717560320, journalId=1263187385517883426, year='2025', volume='53', issue='12', pageStart='3433', pageEnd='3832', issueExtLink='null', onlineDate='null', pubDate='1766160000000', pubDateStr='2025-12-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792576899386, creator='13701087609', updateTime=1792577516933, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1319729016953749818, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319726426404803327, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1319729016953749819, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319726426404803327, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=3446, endPage=3460, ext={EN=ArticleExt(id=1319726555987816957, articleId=1319726555752935932, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Growth, Spectra, and Laser Performance of Er3+-Activated Gd3Ga5O12 and Lu3Ga5O12 Mid-Infrared Laser Crystals, columnId=1321945006265450712, journalTitle=Journal of the Chinese Ceramic Society, columnName=Special Issue on Synthesis and Application of Large-Size High-Quality Artificial Crystals—Research Article, runingTitle=null, highlight=null, articleAbstract=
Introduction

Mid-infrared (MIR) lasers operating within a spectral region of 2.7-3.0 μm have a significant importance in applications such as laser surgery and remote sensing. Trivalent erbium (Er3+) ions are among the most efficient activators for MIR lasers, leveraging the 4I11/2→4I13/2 transition. Nevertheless, the realization of high-power and efficient laser output is often hindered due to the self-terminating effect and substantial thermal loading in Er3+-doped gain medium. This study was to investigate the high-performance Er3+-doped Gd3Ga5O12 (GGG) and Lu3Ga5O12 (LuGG) laser crystals with the low phonon energy and high thermal conductivity.

Methods

High-quality single crystals of Er: GGG, Er/Pr: GGG, and Er: LuGG were grown by the Czochralski method in an optimized atmosphere (i.e., 98% N2 + 2% O2) with iridium crucibles and (111)-oriented seeds. Raw materials underwent multi-step sintering to guarantee the phase purity. Comprehensive spectroscopic analysis was conducted on the polished samples. The room-temperature absorption spectra were determined by a model Lambda 900 spectrophotometer. The fluorescence spectra at the mid-infrared (MIR: 2500-3000 nm), near-infrared (NIR: 950-1750 nm) and upconversion (UC: 500-700 nm) bands were measured under 965/967 nm excitation by an optical parametric oscillator (OPO) or a xenon lamp using models FLS920 and FSP920 fluorescence spectrometers. The fluorescence decay curves for the 4I11/2 and 4I13/2 energy levels were recorded to determine the fluorescence lifetime. The laser performance was assessed under two pumping schemes (i.e., a xenon lamp and a 965 nm fiber-coupled laser diode (LD)). The crystals were fabricated into laser gain media of various sizes and doping profiles, including a bonded configuration (undoped GGG/56% Er: GGG) to alleviate thermal lensing. The continuous-wave (CW) performance was evaluated via input-output power curves, slope efficiency, laser threshold, and beam quality factor (M2). The passive Q-switching was implemented with two-dimensional materials (i.e., graphene and a Bi2Te3/graphene heterostructure) as saturable absorbers. The main pulsed laser metrics (i.e., pulse train profile, average output power, pulse width, repetition rate, and peak power) were systematically determined.

Results and Discussion

The as-grown crystals display a high optical quality with intense and broad absorption bands centered at 965 nm. The 30% Er, 0.5% Pr: GGG composition has a notably high absorption cross-section of 5.13×10-21 cm2 and a full width at half maximum (FWHM) of 15 nm, indicating a superior spectral overlap with commercial 980 nm InGaAs laser diodes and enabling efficient pump coupling. The incorporation of Pr3+ ions can enhance the MIR fluorescence emission based on a cross-relaxation energy transfer mechanism, i.e., 4I13/2 (Er3+) + 3H4 (Pr3+) → 4I15/2 (Er3+) + 3F4 (Pr3+). This process effectively depopulates the lower laser level (4I13/2), leading to a reversal of the intrinsic lifetime ratio between metastable states. Specifically, a ratio of τ(4I11/2)/τ(4I13/2) of 2.348 appears in the sample 30% Er, 0.5% Pr:GGG, which is critical for overcoming the self-termination barrier in Er3+ -based~3 μm lasers.

Under 965 nm LD pumping, a CW laser emission at 2.75 μm is attained. The 56% Er: GGG crystal has a maximum output power of 325 mW with a slope efficiency of 16.15%. The bonded GGG/56% Er: GGG structure improves the thermal management, increasing the maximum power to 453 mW and the slope efficiency to 17.1%, while also improving beam quality (i.e., M2 reduces from 1.68 to 1.48). The Er/Pr: GGG crystal (11% Er, 0.4% Pr) shows a superior thermal performance, reaching 372 mW output and a higher damage threshold, due to the lower Er3+ concentration and efficient energy transfer.

The passive Q-switching with graphene and Bi2Te3/graphene absorbers produce impressive pulsed outcomes. The graphene-based Q-switched bonded GGG/Er, Pr: GGG/GGG crystal has a maximum average power of 186 mW, a pulse width of 360 ns, and a repetition rate of 120.5 kHz, corresponding to a pulse energy of 1.54 μJ and a peak power exceeding 4.28 W. The Bi2Te3/graphene Q-switched Er: LuGG laser can deliver a higher average power of 274 mW with a shorter pulse width of 340 ns at 135 kHz, yielding a pulse energy of 2.03 μJ and a peak power of > 5.97 W. These findings affirm a potential of these materials in high-performance pulsed MIR lasers.

Conclusions

This work established Er3+-doped GGG and LuGG crystals as highly promising gain media for efficient ~2.75 μm mid-infrared lasers. The strategies of Pr3+ co-doping and crystal bonding proved effective in mitigating the self-terminating effect and thermal load, leading to the improvement of substantial performance. The effective operation in both continuous-wave and passively Q-switched regimes could underscore the applicability of these crystals in practical high-power MIR laser systems.

, authors=Longxing ZHENG1, 2, Zhaojie ZHU1, Zhenyu YOU3, Yan WANG1, Chaoyang TU1, authorsList=Longxing ZHENG, Zhaojie ZHU, Zhenyu YOU, Yan WANG, Chaoyang TU, authorCompany=null, correspAuthors=Yan WANG, Chaoyang TU, authorNote=

ZHENG Longxing (1997-), male, Doctoral candidate. E-mail:

, correspAuthorsNote=
TU Chaoyang (1963-), male, Ph.D., Professor; E-mail: ;
WANG Yan (1975-), female, Ph.D., Professor.
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Er3+基于其4I11/2→4I13/2在2.7~3.0 μm的特征发射,常作为中红外固态激光器增益介质的激活离子。采用提拉法生长了一系列Er3+掺杂的Gd3Ga5O12(GGG)和Lu3Ga5O12(LuGG)晶体,计算了吸收截面、发射截面以及能级寿命等光谱参数,研究了Er3+掺杂浓度、Pr3+共掺对Er:GGG晶体中红外波段荧光发射的影响。对生长的晶体进行了激光实验,采用氙灯泵浦Er/Pr:GGG晶体实现了平均功率为297 mW的2.75 μm中红外脉冲激光输出,通过965 nm的半导体LD激光泵浦Er:GGG、GGG/Er:GGG以及Er/Pr:GGG晶体分别实现了最大输出功率为325、453 mW以及372 mW的中红外连续激光输出。最后,采用石墨烯和Bi2Te3二维材料作为可饱和吸收体,对GGG/Er,Pr:GGG/GGG键合晶体和Er:LuGG晶体实现的中红外激光进行了调Q实验(激光调谐品质因数实验),实现了最大平均输出功率分别为186 mW和274 mW的中红外脉冲激光,最短脉冲宽度为243 ns。

, authors=郑龙兴1, 2, 朱昭捷1, 游振宇3, 王燕1, 涂朝阳1, authorsList=郑龙兴, 朱昭捷, 游振宇, 王燕, 涂朝阳, authorCompany=null, correspAuthors=王燕, 涂朝阳, authorNote=

郑龙兴(1997—),男,博士研究生。

, correspAuthorsNote=
涂朝阳(1963—),男,博士,研究员;
王燕(1975—),女,博士,研究员。
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Er3+激活的Gd3Ga5O12和Lu3Ga5O12中红外激光晶体的生长、光谱与激光性能
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郑龙兴 1, 2 , 朱昭捷 1 , 游振宇 3 , 王燕 1 , 涂朝阳 1
硅酸盐学报 | 大尺寸高品质人工晶体制备与应用专题—研究论文 2025,53(12): 3446-3460
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硅酸盐学报 |大尺寸高品质人工晶体制备与应用专题—研究论文 2025 , 53 (12) : 3446 -3460
Er3+激活的Gd3Ga5O12和Lu3Ga5O12中红外激光晶体的生长、光谱与激光性能
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郑龙兴(1997—),男,博士研究生。

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郑龙兴1, 2 , 朱昭捷1, 游振宇3, 王燕1 , 涂朝阳1
作者信息
  • 1.中国科学院福建物质结构研究所,功能晶体与器件全国重点实验室,福州 350002
  • 2.中国科学院大学,北京 100039
  • 3.泉州师范学院光子技术研究院,福建 泉州 362000
通讯作者:
涂朝阳(1963—),男,博士,研究员;
王燕(1975—),女,博士,研究员。
作者简介:

郑龙兴(1997—),男,博士研究生。

Growth, Spectra, and Laser Performance of Er3+-Activated Gd3Ga5O12 and Lu3Ga5O12 Mid-Infrared Laser Crystals
Longxing ZHENG1, 2 , Zhaojie ZHU1, Zhenyu YOU3, Yan WANG1 , Chaoyang TU1
Affiliations
  • 1.State Key Laboratory of Functional Crystals and Devices, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou 350002, China
  • 2.University of Chinese Academy of Sciences, Beijing 100039, China
  • 3.Institute of Photonic Technology, Quanzhou Normal University, Quanzhou 362000, Fujian, China
  • Corresponding Author:
    TU Chaoyang (1963-), male, Ph.D., Professor; E-mail: ;
    WANG Yan (1975-), female, Ph.D., Professor.

    ZHENG Longxing (1997-), male, Doctoral candidate. E-mail:

出版时间: 2025-12-20 doi: 10.14062/j.issn.0454-5648.20250102
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Er3+基于其4I11/2→4I13/2在2.7~3.0 μm的特征发射,常作为中红外固态激光器增益介质的激活离子。采用提拉法生长了一系列Er3+掺杂的Gd3Ga5O12(GGG)和Lu3Ga5O12(LuGG)晶体,计算了吸收截面、发射截面以及能级寿命等光谱参数,研究了Er3+掺杂浓度、Pr3+共掺对Er:GGG晶体中红外波段荧光发射的影响。对生长的晶体进行了激光实验,采用氙灯泵浦Er/Pr:GGG晶体实现了平均功率为297 mW的2.75 μm中红外脉冲激光输出,通过965 nm的半导体LD激光泵浦Er:GGG、GGG/Er:GGG以及Er/Pr:GGG晶体分别实现了最大输出功率为325、453 mW以及372 mW的中红外连续激光输出。最后,采用石墨烯和Bi2Te3二维材料作为可饱和吸收体,对GGG/Er,Pr:GGG/GGG键合晶体和Er:LuGG晶体实现的中红外激光进行了调Q实验(激光调谐品质因数实验),实现了最大平均输出功率分别为186 mW和274 mW的中红外脉冲激光,最短脉冲宽度为243 ns。

铒掺杂钆镓榴石晶体  /  激光晶体  /  提拉法生长晶体
Introduction

Mid-infrared (MIR) lasers operating within a spectral region of 2.7-3.0 μm have a significant importance in applications such as laser surgery and remote sensing. Trivalent erbium (Er3+) ions are among the most efficient activators for MIR lasers, leveraging the 4I11/2→4I13/2 transition. Nevertheless, the realization of high-power and efficient laser output is often hindered due to the self-terminating effect and substantial thermal loading in Er3+-doped gain medium. This study was to investigate the high-performance Er3+-doped Gd3Ga5O12 (GGG) and Lu3Ga5O12 (LuGG) laser crystals with the low phonon energy and high thermal conductivity.

Methods

High-quality single crystals of Er: GGG, Er/Pr: GGG, and Er: LuGG were grown by the Czochralski method in an optimized atmosphere (i.e., 98% N2 + 2% O2) with iridium crucibles and (111)-oriented seeds. Raw materials underwent multi-step sintering to guarantee the phase purity. Comprehensive spectroscopic analysis was conducted on the polished samples. The room-temperature absorption spectra were determined by a model Lambda 900 spectrophotometer. The fluorescence spectra at the mid-infrared (MIR: 2500-3000 nm), near-infrared (NIR: 950-1750 nm) and upconversion (UC: 500-700 nm) bands were measured under 965/967 nm excitation by an optical parametric oscillator (OPO) or a xenon lamp using models FLS920 and FSP920 fluorescence spectrometers. The fluorescence decay curves for the 4I11/2 and 4I13/2 energy levels were recorded to determine the fluorescence lifetime. The laser performance was assessed under two pumping schemes (i.e., a xenon lamp and a 965 nm fiber-coupled laser diode (LD)). The crystals were fabricated into laser gain media of various sizes and doping profiles, including a bonded configuration (undoped GGG/56% Er: GGG) to alleviate thermal lensing. The continuous-wave (CW) performance was evaluated via input-output power curves, slope efficiency, laser threshold, and beam quality factor (M2). The passive Q-switching was implemented with two-dimensional materials (i.e., graphene and a Bi2Te3/graphene heterostructure) as saturable absorbers. The main pulsed laser metrics (i.e., pulse train profile, average output power, pulse width, repetition rate, and peak power) were systematically determined.

Results and Discussion

The as-grown crystals display a high optical quality with intense and broad absorption bands centered at 965 nm. The 30% Er, 0.5% Pr: GGG composition has a notably high absorption cross-section of 5.13×10-21 cm2 and a full width at half maximum (FWHM) of 15 nm, indicating a superior spectral overlap with commercial 980 nm InGaAs laser diodes and enabling efficient pump coupling. The incorporation of Pr3+ ions can enhance the MIR fluorescence emission based on a cross-relaxation energy transfer mechanism, i.e., 4I13/2 (Er3+) + 3H4 (Pr3+) → 4I15/2 (Er3+) + 3F4 (Pr3+). This process effectively depopulates the lower laser level (4I13/2), leading to a reversal of the intrinsic lifetime ratio between metastable states. Specifically, a ratio of τ(4I11/2)/τ(4I13/2) of 2.348 appears in the sample 30% Er, 0.5% Pr:GGG, which is critical for overcoming the self-termination barrier in Er3+ -based~3 μm lasers.

Under 965 nm LD pumping, a CW laser emission at 2.75 μm is attained. The 56% Er: GGG crystal has a maximum output power of 325 mW with a slope efficiency of 16.15%. The bonded GGG/56% Er: GGG structure improves the thermal management, increasing the maximum power to 453 mW and the slope efficiency to 17.1%, while also improving beam quality (i.e., M2 reduces from 1.68 to 1.48). The Er/Pr: GGG crystal (11% Er, 0.4% Pr) shows a superior thermal performance, reaching 372 mW output and a higher damage threshold, due to the lower Er3+ concentration and efficient energy transfer.

The passive Q-switching with graphene and Bi2Te3/graphene absorbers produce impressive pulsed outcomes. The graphene-based Q-switched bonded GGG/Er, Pr: GGG/GGG crystal has a maximum average power of 186 mW, a pulse width of 360 ns, and a repetition rate of 120.5 kHz, corresponding to a pulse energy of 1.54 μJ and a peak power exceeding 4.28 W. The Bi2Te3/graphene Q-switched Er: LuGG laser can deliver a higher average power of 274 mW with a shorter pulse width of 340 ns at 135 kHz, yielding a pulse energy of 2.03 μJ and a peak power of > 5.97 W. These findings affirm a potential of these materials in high-performance pulsed MIR lasers.

Conclusions

This work established Er3+-doped GGG and LuGG crystals as highly promising gain media for efficient ~2.75 μm mid-infrared lasers. The strategies of Pr3+ co-doping and crystal bonding proved effective in mitigating the self-terminating effect and thermal load, leading to the improvement of substantial performance. The effective operation in both continuous-wave and passively Q-switched regimes could underscore the applicability of these crystals in practical high-power MIR laser systems.

erbium-doped gadolinium gallium garnet crystal  /  laser crystal  /  Crystal growth by Czochralski method
郑龙兴, 朱昭捷, 游振宇, 王燕, 涂朝阳. Er3+激活的Gd3Ga5O12和Lu3Ga5O12中红外激光晶体的生长、光谱与激光性能. 硅酸盐学报, 2025 , 53 (12) : 3446 -3460 . DOI: 10.14062/j.issn.0454-5648.20250102
Longxing ZHENG, Zhaojie ZHU, Zhenyu YOU, Yan WANG, Chaoyang TU. Growth, Spectra, and Laser Performance of Er3+-Activated Gd3Ga5O12 and Lu3Ga5O12 Mid-Infrared Laser Crystals[J]. Journal of the Chinese Ceramic Society, 2025 , 53 (12) : 3446 -3460 . DOI: 10.14062/j.issn.0454-5648.20250102
  • 国家重点研发计划(2022YFB3605700)
  • 国家自然科学基金区域创新与发展联合基金(U21A20508)
  • 福建省科技计划引导性项目(2024H0033; 2022H0043)
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doi: 10.14062/j.issn.0454-5648.20250102
  • 接收时间:2025-02-17
  • 首发时间:2026-10-21
  • 出版时间:2025-12-20
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  • 收稿日期:2025-02-17
  • 修回日期:2025-03-12
基金
国家重点研发计划(2022YFB3605700)
国家自然科学基金区域创新与发展联合基金(U21A20508)
福建省科技计划引导性项目(2024H0033; 2022H0043)
作者信息
    1.中国科学院福建物质结构研究所,功能晶体与器件全国重点实验室,福州 350002
    2.中国科学院大学,北京 100039
    3.泉州师范学院光子技术研究院,福建 泉州 362000

通讯作者:

涂朝阳(1963—),男,博士,研究员;
王燕(1975—),女,博士,研究员。
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