| 248 | 0 | 142 |
| 下载次数 | 被引频次 | 阅读次数 |
铌酸镓镧晶体(La_3Ga5.5Nb0.5O14,LGN)作为重要的中红外(2~20μm)非线性光学材料,具有宽的光谱透过范围(0.28~7.40μm)、大的二阶非线性系数(d11=(3.0±0.1) pm/V)及高的激光损伤阈值(>1.41 GW/cm2@1064 nm),成为高功率中红外激光系统急需的优异晶体材料。本文总结了LGN晶体的结构特性、大尺寸生长技术、性能表征以及激光应用的研究进展。针对晶体生长过程中的热应力开裂与组分挥发难题,通过优化温场梯度、改善生长参数,成功制备直径80 mm大尺寸高质量单晶,为目前国际上尺寸最大的光学级LGN单晶。首次提出通过组分调控实现双折射色散与非线性系数的协同优化策略,开发出La3(Nb1–xTax)0.5Ga5.5O14(LGNTx)系列固溶体单晶,极大提升了有效非线性系数。利用LGN晶体差频产生技术实现了4.4~5.7μm中红外输出,而LGNTx混晶则将差频输出波长进一步扩展至6.84μm,这是目前氧化物晶体连续调谐输出的最长差频产生波长。上述研究结果为未来新型中红外非线性光学材料设计以及LGN晶体的规模化使用提供了重要的理论依据和应用前景。
Abstract:As an important mid-infrared(at 2-20 μm) nonlinear optical material, La3 Ga5.5Nb0.5O14(LGN) crystal has a wide spectral transmission range(at 0.28-7.40 μm), large second-order nonlinear coefficients(d11 = 3.0±0.1 pm/V), and high laser damage thresholds(>1.41 GW/cm2@1064 nm), which makes it an excellent crystal material for high-power mid-infrared laser systems. In this review, we systematically summarize the structural properties of the LGN crystal, the large-size growth technology, the performance characterization, and the research progress of laser applications. To solve some problems of thermal stress cracking and volatilization of components during the growth process, a large-size and high-quality single crystal with a diameter of 80 mm is prepared via optimizing the temperature gradient and improving the growth parameters. Also we propose a synergistic optimization strategy of birefringent dispersion and nonlinear coefficient through component modulation, and develop La3(Nb1-xTax)0.5Ga5.5O14(LGNTx) series of solid-solution single crystals, greatly improving the effective nonlinear coefficient. The LGN crystal has 4.4-5.7 μm mid-infrared output using the difference frequency generation technique, and the LGNTx hybrid crystals can extend the difference frequency output wavelength to 6.84 μm, which is the longest wavelength for the continuous tuning output of oxide crystals. The results above provide an important theoretical basis and application prospect for designing new mid-infrared nonlinear optical materials and the large-scale use of LGN crystal in the future. Summary and prospects This review represents a comprehensive and in-depth summary of the La3 Ga5.5Nb0.5O14(LGN) crystal, covering important achievements in various key aspects, such as crystal structure and basic properties, large-size growth technology, nonlinear optical properties, mid-infrared nonlinear optical properties, and applications. In terms of large-size crystal growth, some technical problems of thermal stress cracking and component segregation during the growth of LGN are solved, and the preparation of large-size single crystals with the diameters of 60-80 mm is stablized. Meanwhile, the LGN crystal has nonlinear optical properties and applications, which provides a support for the development of high-power mid-infrared laser systems. In the future, we need to optimize the crystal growth to obtain more accurate temperature regulation, further shorten the growth cycle, improve the growth efficiency, reduce the internal defects, and improve the annealing process, to obtain larger size(≥4 inches) high-quality LGN crystal, providing a better material base for high-performance mid-infrared laser. In addition, it is also necessary to investigate the performance regulation mechanism of LGN hybrid crystals in depth, and further optimize their nonlinear optical properties via utilizing elemental doping and structural fine-tuning, such as improving the nonlinear coefficient and broadening the gain bandwidth, to provide nonlinear optics crystals with excellent performances for the realization of high-power OPCPA applications. Developing mid-infrared laser sources and optoelectronic devices can meet a demand for mid-infrared wavelength lasers in biomedicine, environmental monitoring, national defense, security, and etc..
[1] FRANKEN P A, HILL A E, PETERS C W, et al. Generation of optical harmonics[J]. Phys Rev Lett, 1961, 7(4):118–119.
[2] BLOEMBERGEN N. Nonlinear optics[M]. New York:W. A.Benjamin, Inc., 1965:1–18.
[3] BIERLEIN J D, VANHERZEELE H. Potassium titanyl phosphate:Properties and new applications[J]. J Opt Soc Am B, 1989, 6(4):622.
[4] CHEN C T, WU B C, JIANG A D, et al. A new-type ultraviolet SHG crystal-beta-BaB2O4[J]. Sci. Sin. B, 1985, 28(3):235–43.
[5] CHEN C T, WU Y C, JIANG A D, et al. New nonlinear–optical crystal:Li B3O5[J]. J Opt Soc Am B, 1989, 6(4):616.
[6] CHEN C T, LU J H, TOGASHI T, et al. Second-harmonic generation from a KBe2BO3F2 crystal in the deep ultraviolet[J]. Opt Lett, 2002,27(8):637.
[7] PETROV V, GHOTBI M, KOKABEE O, et al. Femtosecond nonlinear frequency conversion based on BiB3O6[J]. Laser Photonics Rev, 2010,4(1):53–98.
[8] ROTHMAN L S, GORDON I E, BABIKOV Y, et al. The HITRAN2012 molecular spectroscopic database[J]. J Quant Spectrosc Radiat Transf, 2013, 130:4–50.
[9] PHAM–DUC B. Satellite remote sensing of the variability of the continental hydrology cycle in the lower Mekong basin over the last two decades[D]. Paris:Sorbonne Université, 2018.
[10] ZHENG C, YE X Y, CAI S G, et al. Observation of nonlinear saturable and reverse–saturable absorption in silver nanowires and their silica gel glass composite[J]. Appl Phys B, 2010, 101(4):835–840.
[11] NAKAMURA R, INAGAKI Y, HATA H, et al. Wide-bandgap nonlinear crystal LiGaS2 for femtosecond mid-infrared spectroscopy with chirped-pulse upconversion[J]. Appl Opt, 2016, 55(33):9365–9369.
[12] GUPTA A K, MISHRA A, FAROOQUI M, et al. Generation of mid-infrared and terahertz radiation for defence applications[M]//MOHAN M, MAINI A K, BHATTACHERJEE A B, et al. Advances in laser physics and technology. Foundation Books. 2014:225–241.
[13] DAS S, BHAR G C, GANGOPADHYAY S, et al. Linear and nonlinear optical properties of ZnGeP2 crystal for infrared laser device applications:Revisited[J]. Appl Opt, 2003, 42(21):4335–4340.
[14] DMITRIEV V G, GURZADYAN G G, NIKOGOSYAN D N.Handbook of nonlinear optical crystals[M]. Berlin Heidelberg:Springer, 2013.
[15] BADIKOV V, MITIN K, NOACK F, et al. Orthorhombic nonlinear crystals of AgxGaxGe1-x Se2 for the mid-infrared spectral range[J]. Opt Mater, 2009, 31(4):590–597.
[16] WANG J Y, LU D Z, YU H H, et al. Langasite family nonlinear optical crystals[J]. Acta Phys Chim Sin, 2020, 36(1):1907009.
[17]陈创天,叶宁,林峧,等.运用晶体非线性光学效应的阴离子基团理论探索新型紫外非线性光学材料[J].自然科学进展, 2000, 10(8):673–683.CHEN Chuangtian, YE Ning, LIN Jiao, et al. Prog Nat Sci, 2000,10(8):673–683.
[18] DUDKA A P, MILL B V, PISAREVSKY Y V. Refinement of the crystal structures of the La3Ta0.5Ga5.5O14 and La3Nb0.5Ga5.5O14compounds[J]. Crystallogr Rep, 2009, 54(4):558–567.
[19]王玉周.硅酸镓镧族中红外非线性光学晶体生长及其性能优化研究[D].济南:山东大学, 2023.WANG Yuzhou. Study on growth and performance optimization of mid-infrared nonlinear optical crystals of gallium lanthanum silicate family[D]. Jinan:Shandong University, 2023.
[20] TAUC J, GRIGOROVICI R, VANCU A. Optical properties and electronic structure of amorphous germanium[J]. Phys Status Solidi B,1966, 15(2):627–637.
[21] THOMAS M E, JOSEPH R I, TROPF W J. Infrared transmission properties of sapphire, spinel, yttria, and ALON as a function of temperature and frequency[J]. Appl Opt, 1988, 27(2):239–245.
[22] ZHANG Y T, WANG B, JIA X H, et al. The effect of co–substitution of heterovalent ions Ga3+and Sb5+on nonlinear optical properties of phosphate crystals[J]. Mater Adv, 2024, 5(10):4286–4292.
[23] TAKEDA H, SHIMAMURA K, KOHNO T, et al. Growth and characterization of La3Nb0.5Ga5.5O14 single crystals[J]. J Cryst Growth,1996, 169(3):503–508.
[24] TAKEDA H, SHIMAMURA K, CHANI V I, et al. Effect of starting melt composition on crystal growth of La3Ga5SiO14[J]. J Cryst Growth,1999, 197(1–2):204–209.
[25] KONG H K, WANG J Y, ZHANG H J, et al. Growth and characterization of La3Ga5.5Nb0.5O14 crystal[J]. J Cryst Growth, 2006,292(2):408–411.
[26] YU F P, YUAN D R, YIN X, et al. Czochralski growth and characterization of the piezoelectric single crystal La3Ga5.5Nb0.5O14[J].Solid State Commun, 2009, 149(31/32):1278–1281.
[27] LU D Z, XU T X, YU H H, et al. Acentric langanite La3Ga5.5Nb0.5O14crystal:A new nonlinear crystal for the generation of mid-infrared parametric light[J]. Opt Express, 2016, 24(16):17603–17615.
[28] WANG Y Z, LIANG F, WANG J Y, et al. Growth of a large-aperture mid-infrared nonlinear optical La3Nb0.5Ga5.5O14 crystal for optical parametric chirped–pulse amplification[J]. CrystEngComm, 2021,23(41):7212–7218.
[29] BRICE J C. The cracking of czochralski-grown crystals[J]. J Cryst Growth, 1977, 42:427–430.
[30] CUI C, LIANG F, LU D Z, et al. Phase-matching condition in rotatory nonlinear optics[J]. Phys Rev A, 2022, 105(2):023512.
[31] GUO F, LU D Z, SEGONDS P, et al. Phase-matching properties and refined Sellmeier equations of La3Ga55Nb05O14[J]. Opt Mater Express,2018, 8(4):858.
[32] WANG Y Z, LIANG F, LU D Z, et al. Birefringence dispersion management of langasite nonlinear crystals for the improvement of mid-infrared amplification[J]. Cryst Growth Des, 2023, 23(1):620–628.
[33] CUI C, LU D Z, LIANG F, et al. Mid-Infrared pulsed nanosecond difference frequency generation of oxide LGN crystal up to 5.7μm[J].Opt Lett, 2021, 46(4):785–788.
[34] GU H X, LU D Z, CUI C, et al. Extending mid-infrared wavelength to6.84μm in oxide nonlinear optical crystal via birefringence dispersion management[J]. Opt Lett, 2024, 49(19):5643–5646.
[35] NIU S J, WANG S T, ABABAIKE M, et al. Tunable near-and mid-infrared(1.36–1.63μm and 3.07–4.81μm)optical vortex laser source[J]. Laser Phys Lett, 2020, 17(4):045402.
[36] BOURSIER E, ARCHIPOVAITE G M, DELAGNES J C, et al. Study of middle infrared difference frequency generation using a femtosecond laser source in LGT[J]. Opt Lett, 2017, 42(18):3698–3701.
[37] YIN F Y, LIU L, ZHU M H, et al. Transparent lead–free ferroelectric(K, Na)NbO3 single crystal with giant second harmonic generation and wide mid-infrared transparency window[J]. Adv Opt Mater, 2022,10(23):2201721.
[38] CUSSAT–BLANC S, IVANOV A, LUPINSKI D, et al. KTi OPO4,KTi OAs O4, and KNbO3 crystals for mid-infrared femtosecond optical parametric amplifiers:Analysis and comparison[J]. Appl Phys B, 2000,70(1):S247–S252.
[39] ARCHIPOVAITE G M, PETIT S, DELAGNES J C, et al. 100 kHz Yb-fiber laser pumped 3μm optical parametric amplifier for probing solid-state systems in the strong field regime[J]. Opt Lett, 2017, 42(5):891–894.
[40] CHATTERJEE U, RUDRA A M, BHAR G C. Widely tunable difference frequency generation(2.6–7.7μm)in lithium iodate[J]. Opt Commun, 1995, 118(3/4):367–374.
基本信息:
DOI:10.14062/j.issn.0454-5648.20250371
中图分类号:O734;O782
引用信息:
[1]顾洪旭,韩金锋,路大治,等.La_3Ga_(5.5)Nb_(0.5)O_(14)晶体生长及非线性光学性能研究进展[J].硅酸盐学报,2025,53(12):3484-3493.DOI:10.14062/j.issn.0454-5648.20250371.
基金信息:
国家重点研发计划(2023YFB3610603); 国家自然科学基金(52272004)