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Er3+基于其~4I11/2→~4I13/2在2.7~3.0μm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Gd_3Ga_5O12(GGG)和Lu_3Ga_5O12(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2.75μm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 m W以及372 mW的中红外连续激光输出。最后,采用石墨烯和Bi_2Te3二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 m W的中红外脉冲激光,最短脉冲宽度为243 ns。
Abstract: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 Gd_3Ga_5O12(GGG) and Lu_3Ga_5O12(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 Bi_2Te3/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 m W 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 Bi_2Te3/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 m W, 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 Bi_2Te3/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.
[1] YASUHIRO, MOTOSHI S, KENJIRO W, et al. Infrared laser-mediated gene induction in targeted single cells in vivo[J]. Nat Methods, 2009, 6(1):79–81.
[2] Dong X, Jochmann M A, Elsner M, et al. Monitoring Microbial Mineralization Using Reverse Stable Isotope Labeling Analysis by Mid-Infrared Laser Spectroscopy[J]. Environ Sci Technol, 2017(20):51.
[3] Rangel G F, Lorena Diaz de León Martínez, Walter L S, et al. Recent advances and trends in mid-infrared chem/bio sensors[J]. Trends Anal Chem, 2024, 180.
[4] LIU Z L, WANG X M, HU Q L, et al. Jamming effectiveness of mid-infrared lasers on the quaternary cross–shaped detector[J]. Phys Conf Ser, 2023, 2464(1).
[5]刘永岩,杨雪莹,田颖,等.基于石墨烯/WS2可饱和吸收体的中红外Er3+:ZBLAN锁模激光器及其波长可调谐性能[J].发光学报,2024, 45(8):1354–1363.LIU Yongyan, YANG Xueying, TIAN Ying, et al. Chin J Lumin, 2024,45(8):1354–1363.
[6]叶传香,李珺子,王金涛.基于WTe2可饱和吸收体的超快掺铒光纤激光器[J].光学学报, 2024, 44(20):2014004.YE Chuanxiang, LI Junzi, WANG Jintao. Acta Opt Sin, 2024, 44(20):2014004.
[7]陈言,张沛雄,权聪,等.基于石墨烯可饱和吸收体的Er:YAG被动调Q激光器[J].人工晶体学报, 2024, 53(7):1127–1135.CHEN Yan, ZHANG Peixiong, QUAN Cong, et al. J Synth Cryst,2024, 53(7):1127–1135.
[8]翟学君,高露露,闵欢欢,等.钙钛矿可饱和吸收体红外激光器研究进展[J].激光与红外, 2023, 53(8):1139–1147.ZHAI Xuejun, GAO Lulu, MIN Huanhuan, et al. Laser Infrared, 2023,53(8):1139–1147.
[9]叶珊珊,黄海波,陈颂元,等. Ti CN作为可饱和吸收体的2.8μm被动调Q锁模光纤激光器[J].光电工程, 2023, 50(7):89–97.YE Shanshan, HUANG Haibo, CHEN Songyuan, et al. Opto Electron Eng, 2023, 50(7):89–97.
[10] SOROKINA I T, VODOPYANOV K L. Solid-State Mid-Infrared Laser Sources[M]. Berlin, Heidelberg:Springer Berlin Heidelberg,2003.
[11] Mills D P, Liddle S T. Ligand design in modern lanthanide chemistry:Reactivity and catalysis[M]. Alberta:John Wiley&Sons, Ltd, 2016.
[12]?VEJKAR R,?ULC J, JELíNKOVáH, et al. Diode-pumped Er:SrF2laser tunable at 2.7μm[J]. Opt Mater Express, 2018, 8(4):1025.
[13] ZHANG H L, SUN D L, LUO J Q, et al. 28.02 W LD side-pumped CW laser operated at 2.8μm in YSGG/Er:YSGG/YSGG crystal[J].Opt Express, 2024, 32(7):11665–11672.
[14] BAE J E, LOIKO P, NORMANI S, et al. Er:LiYF4 planar waveguide laser at 2.8μm[J]. Appl Phys Lett, 2024, 125(8):081101.
[15] QUAN C, SUN D L, ZHANG H L, et al. Growth, spectroscopy and high-power laser operation of Er:YAP crystal with different Er3+concentrations[J]. J Lumin, 2022, 251:119122.
[16] ZHANG H L, BIAN J T, SUN D L, et al. Improvement of 2.8μm laser performance on LD side-pumped Lu YSGG/Er:LuYSGG/LuYSGG bonding crystal[J]. Opt Laser Technol, 2023, 158:108840.
[17] LIU J J, ZONG M Y, WANG D Z, et al. Acousto-optic Q-switched Er:Ca F2–SrF2 laser at 2.73μm[J]. Infrared Phys Technol, 2021, 116:103758.
[18]赵呈春,李善明,徐民,等.激光晶体研究进展[J].中国激光, 2024,51(11):387–412.ZHAO Chengchun, LI Shangming, XU Min, et al. Chin J Lasers, 2024,51(11):387–412.
[19]任永春,李健达,曹笑,等.高熔点稀土氧化物激光晶体的研究进展[J].人工晶体学报, 2024, 53(11):1829–1839.REN Yongchun, LI Jianda, CAO Xiao, et al. J Synth Cryst, 2024,53(11):1829–1839.
[20]赵呈春,张沛雄,李善明,等.稀土离子掺杂氟化物激光晶体研究进展[J].人工晶体学报, 2022, 51(Z1):1573–1587.ZHAO Chengchun, ZHANG Peixiong, LI Shangming, et al. J Synth Cryst, 2022, 51(Z1):1573–1587.
[21]程艳玲,于浩海,张怀金,等.自倍频晶体的研究和激光应用进展[J].应用技术学报, 2021, 21(2):95–108.CHENG Yanling, YU Haohai, ZHANG Huaijin, et al. J Appl Technol,2021, 21(2):95–108.
[22]李江,田丰,刘子玉.中红外激光陶瓷的研究进展与展望[J].人工晶体学报, 2020, 49(8):1467–1487.LI Jiang, TIAN Feng, LIU Ziyu. J Synth Cryst, 2020, 49(8):1467–1487.
[23]罗永治,余盛全,阴明,等.过渡金属离子掺杂Ⅱ–Ⅵ族中红外激光陶瓷研究进展[J].人工晶体学报, 2021, 50(5):947–958.LUO Yongzhi, YU Shengquan, YING Ming, et al. J Synth Cryst, 2021,50(5):947–958.
[24]余盛全,敬畏,胥涛,等.稀土离子掺杂Ca F2透明激光陶瓷的研究进展[J].中国陶瓷, 2016, 52(7):1–4.YU Shengquan, JING Wei, XU Tao, et al. China Ceram, 2016, 52(7):1–4.
[25]李晴,王俊,马杰,等.倍半氧化物激光陶瓷的研究进展[J].硅酸盐学报, 2024, 52(3):1006–1022.LI Qing, WANG Jun, MA Jie, et al. J Chin Ceram Soc, 2024, 52(3):1006–1022.
[26]李剑峰,雷浩,王森宇,等. 2~5μm全固态中红外高功率光纤激光源研究进展(特邀)[J].中国激光, 2024, 51(1):105–131.LI Jianfeng, LEI Hao, WANG Yusen, et al. Chin J Lasers, 2024, 51(1):105–131.
[27]罗正钱,宋鲁明,阮秋君.可见光掺稀土光纤激光器研究进展:从连续波至飞秒脉冲(特邀)[J].中国激光, 2024, 51(1):33–51.LUO Zhengqian, SONG Luming, RUAN Qiujun. Chin J Lasers, 2024,51(1):33–51.
[28]战泽宇,陈吉祥,刘萌,等. 1.7μm超快光纤激光器研究进展(特邀)[J].红外与激光工程, 2022, 51(1):223–237.ZHANG Zeyu, CHEN Jixiang, LIU Meng, et al. Infrared Laser Eng,2022, 51(1):223–237.
[29]侯绍冬,闫培光,阮双琛.中红外超快光纤激光器研究进展[J].强激光与粒子束, 2021, 33(11):37–51.HOU Shaodong, YAN Peiguang, QUAN Shuangchen. High Power Laser and Particle Beams, 2021, 33(11):37–51.
[30]张会丽. 2.8–3.1微米Ho3+掺杂激光晶体的生长与性能研究[D].合肥:中国科学技术大学, 2017.ZHANG Huili. Growth and properties of 2.8–3.1μm Ho3+doped laser crystals[D]. Hefei:University of Science and Technology of China,2017.
[31] GALAZKA Z, UECKER R, IRMSCHER K, et al. Czochralski growth and characterization of β-Ga2O3 single crystals[J]. Cryst Res Technol,2010, 45(12):1229–1236.
[32]张庆礼,殷绍唐,王爱华,等. GGG系列激光晶体研究进展[J].量子电子学报, 2002, 19(6):481–484.ZHANG Qingli, YIN Shaotang, WANG Aihua, et al. Chin J Quantum Electron, 2002, 19(6):481–484.
[33]侯立群,祖继锋,董玥,等.钕玻璃、Nd:YAG和Nd:GGG热容激光特性比较[J].强激光与粒子束, 2006, 18(6):881–885.HOU Liqun, ZU Jifeng, DONG Yue, et al. High Power Laser Part Beams, 2006, 18(6):881–885.
[34] SUN G H, ZHANG Q L, YANG H J, et al. Crystal growth and characterization of Ho-doped Lu3Ga5O12 for 2μm laser[J]. Mater Chem Phys, 2013, 138(1):162–166.
[35] BONACCORSO F, SUN Z, HASAN T, et al. Graphene photonics and optoelectronics[J]. Nat Photonics, 2010, 4:611–622.
[36] QI X L, ZHANG S C. Topological insulators and superconductors[J].Rev Mod Phys, 2011, 83(4):1057–1110.
[37] ZHANG H, LU S B, ZHENG J, et al. Molybdenum disulfide(MoS)as a broadband saturable absorber for ultra–fast photonics[J]. Opt Express, 2014, 22(6):7249–7260.
[38] CHEN B H, ZHANG X Y, WU K, et al. Q-switched fiber laser based on transition metal dichalcogenides MoS2, MoSe2, WS2, and WSe2[J].Opt Express, 2015, 23(20):26723.
[39] LI X L, XU J L, WU Y Z, et al. Large energy laser pulses with high repetition rate by graphene Q-switched solid–state laser[J]. Opt Express, 2011, 19(10):9950–9955.
[40] YAO B Q, LI L J, ZHENG L L, et al. Diode–pumped continuous wave and Q-switched operation of a c–cut Tm, Ho:YAlO(3)laser[J]. Opt Express, 2008, 16(7):5075–5081.
[41] POPA D, SUN Z, HASAN T, et al. Graphene Q-switched, tunable fiber laser[J]. Appl Phys Lett, 2011, 98(7):073106.
[42] ZHANG H J, LIU C X, QI X L, et al. Topological insulators in Bi2Se3,Bi2Te3 and Sb2Te3 with a single dirac cone on the surface[J]. Nat Phys,2009, 5:438–442.
[43] CHEN Y L, ANALYTIS J G, CHU J H, et al. Experimental realization of a three-dimensional topological insulator, Bi2Te3[J]. Science, 2009,325(5937):178–181.
[44] ZHAO X Y, SUN D L, LUO J Q, et al. Spectroscopic and laser properties of Er:LuSGG crystal for high-power~2.8μm mid-infrared laser[J]. Opt Express, 2020, 28(6):8843–8852.
[45] LI H Y, SUN D L, ZHANG H L, et al. Structure, spectroscopy and laser operation at~2.8μm of a novel Er:SGGG crystal[J]. Opt Laser Technol, 2025, 181:111797.
[46] LIU Y Y, WANG Y, YOU Z Y, et al. Growth, structure and spectroscopic properties of melilite Er:Ca LaGa3O7 crystal for use in mid-infrared laser[J]. J Alloys Compd, 2017, 706:387–394.
[47] WU J L, WANG J J, ZHANG X Y, et al. Exploration of the crystal growth, spectroscopy, and LD-pumped 2.7μm laser operation of Er:LuScO3 sesquioxide crystals[J]. Infrared Phys Technol, 2023, 135:104976.
[48] HOU W T, ZHAO H Y, QIN Z P, et al. Spectroscopic and continuous-wave laser properties of Er:GdScO3 crystal at 2.7μm[J].Opt Mater Express, 2020, 10(11):2730.
[49] HOU W T, XU Z A, ZHAO H Y, et al. Spectroscopic analysis of Er:Y2O3 crystal at 2.7μm mid-IR laser[J]. Opt Mater, 2020, 107:110017.
[50] HOU W T, ZHAO H Y, LI N, et al. Spectroscopic properties of Er:Lu2O3 crystal in mid-infrared emission[J]. Opt Mater, 2019, 98:109508.
[51] HOU W T, XU Z A, ZHAO H Y, et al. Enhanced 2.7μm continuous-wave emission of Er, Pr:Lu2O3 crystal[J]. J Lumin, 2020,224:117094.
[52] MA W W, QIAN X B, WANG J Y, et al. Highly efficient dual-wavelength mid-infrared CW Laser in diode end-pumped Er:SrF2single crystals[J]. Sci Rep, 2016, 6:36635.
[53] MA W W, SU L B, XU X D, et al. Effect of erbium concentration on spectroscopic properties and 2.79μm laser performance of Er:Ca F2crystals[J]. Opt Mater Express, 2016, 6(2):409.
[54] MA W W, SU L B, XU X D, et al. Improved 2.79μm continuous-wave laser performance from a diode-end pumped Er, Pr:CaF2 crystal[J]. J Alloys Compd, 2017, 695:3370–3375.
[55] SHEN B J, KANG H X, CHEN P, et al. Performance of continuous-wave laser-diode side-pumped Er:YSGG slab lasers at2.79μm[J]. Appl Phys B, 2015, 121(4):511–515.
[56] QUAN C, SUN D L, ZHANG H L, et al. 7.25 W LD side-pumped Er:YGG CW laser operated at 2.8μm[J]. Appl Phys B, 2023, 129(11):184.
[57] WANG Z T, SUN D L, ZHANG H L, et al. Temperature distribution and the laser performance of LD end-pumped LuYSGG/Er:LuYSGG composite crystal[J]. CrystEngComm, 2023, 25(35):5012–5020.
[58] QUAN C, SUN D L, LUO J Q, et al. 2.7μm dual-wavelength laser performance of LD end-pumped Er:YAP crystal[J]. Opt Express, 2018,26(22):28421–28428.
[59] CHEN Y W, et al. 2.8μm laser realized on a novel Er:LuYAP crystal end-pumped by a 969 nm LD[J]. Cryst Growth Des, 2024, 24(21):8803–8810.
[60] WANG Z T, SUN D L, ZHANG H L, et al. 45.7 W high power MIR laser operation and electro-optical Q-switched performance of Er:GYAP crystal[J]. Opt Laser Technol, 2025, 183:112392.
[61] YANG Z H, ZHANG Z, CONG Z H, et al. Continuous-wave and Fe2+:ZnSe passively Q-switched mid-infrared lasers based on 2 at.%Er3+:Ca F2 crystal[J]. Results Opt, 2024, 15:100650.
[62] WANG S Z, TANG F, LIU J J, et al. Growth and highly efficient mid-infrared continuous-wave laser of lightly-doped Er:SrF2single-crystal fibers[J]. Opt Mater, 2019, 95:109255.
[63] UEHARA H, YASUHARA R, TOKITA S, et al. Efficient continuous wave and quasi-continuous wave operation of a 2.8μm Er:Lu2O3ceramic laser[J]. Opt Express, 2017, 25(16):18677–18684.
[64] SANAMYAN T, KANSKAR M, XIAO Y, et al. High power diode-pumped 2.7μm Er3+:Y2O3 laser with nearly quantum defect-limited efficiency[J]. Opt Express, 2011, 19(Suppl 5):A1082–A1087.
[65] FAN M Q, LI T, ZHAO S Z, et al. Watt-level passively Q-switched Er:Lu2O3 laser at 2.84μm using MoS2[J]. Opt Lett, 2016, 41(3):540–543.
[66] KONG L C, QIN Z P, XIE G Q, et al. Black phosphorus as broadband saturable absorber for pulsed lasers from 1μm to 2.7μm wavelength[J].Laser Phys Lett, 2016, 13(4):045801.
[67] FAN M Q, LI T, ZHAO S Z, et al. Multilayer black phosphorus as saturable absorber for an Er:Lu2O3 laser at~3μm[J]. Photon Res,2016, 4(5):181.
[68] LI C, LIU J, JIANG S Z, et al. 28μm passively Q-switched Er:CaF2diode-pumped laser[J]. Opt Mater Express, 2016, 6(5):1570.
[69] FAN M Q, LI T, ZHAO J, et al. Continuous wave and ReS2 passively Q-switched Er:SrF2 laser at~3μm[J]. Opt Lett, 2018, 43(8):1726.
基本信息:
DOI:10.14062/j.issn.0454-5648.20250102
中图分类号:O734;O782
引用信息:
[1]郑龙兴,朱昭捷,游振宇,等.Er~(3+)激活的Gd_3Ga_5O_(12)和Lu_3Ga_5O_(12)中红外激光晶体的生长、光谱与激光性能[J].硅酸盐学报,2025,53(12):3446-3460.DOI:10.14062/j.issn.0454-5648.20250102.
基金信息:
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)