HgSO4: An excellent mid-infrared sulfate nonlinear optical crystal with wide band gap and strong second harmonic generation response

被引:13
作者
Han, Yinglei [1 ,2 ]
Zhao, Xin [1 ]
Xu, Feng [1 ]
Li, Bingxuan [1 ]
Ye, Ning [3 ]
Luo, Min [1 ]
机构
[1] Chinese Acad Sci, Fujian Inst Res Struct Matter, Key Lab Optoelect Mat Chem & Phys, Fuzhou 350002, Fujian, Peoples R China
[2] ShanghaiTech Univ, Sch Phys Sci & Technol, Shanghai 201210, Peoples R China
[3] Tianjin Univ Technol, Inst Funct Crystal, Tianjin Key Lab Funct Crystal Mat, Tianjin 300384, Peoples R China
基金
中国国家自然科学基金;
关键词
Nonlinear optics; Sulfates; Mid-infrared; Second harmonic generation; Crystal growth; DAMAGE; POLAR; PRINCIPLES; FLUORIDE; ZNGEP2; RB; CS;
D O I
10.1016/j.jallcom.2022.163727
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
A mercury-based sulfate nonlinear optical (NLO) material, HgSO4, was successfully grown using a hydro-thermal method. It crystallizes in the polar space group Pmn2(1) and forms a three-dimensional spatial network structure consisting of [HgO8] polyhedras and [SO4] polyhedras. The powder second harmonic generation (SHG) measurement showed that HgSO4 is a phase-matching material and has a very strong SHG efficiency of 11 times that of KDP. Such a remarkable SHG response is due to the well-ordered arrangement of the distorted [HgO8] and [SO4] polyhedras. In parallel, large bandgap (4.13 eV) and laser damage threshold (26.5 x AgGaS2) are exhibited. Further characterizations showed that this compound possesses a large birefringence and a wide transmission window from the near-UV to mid-IR, suggesting that HgSO4 may be an excellent mid-IR NLO crystal. (C) 2022 Elsevier B.V. All rights reserved.
引用
收藏
页数:8
相关论文
共 63 条
[1]   Toward reliable density functional methods without adjustable parameters: The PBE0 model [J].
Adamo, C ;
Barone, V .
JOURNAL OF CHEMICAL PHYSICS, 1999, 110 (13) :6158-6170
[2]  
[Anonymous], 2008, 2008 C LASERS ELECTR
[3]  
Bonefacic A., 1963, CROAT CHEM ACTA, V35, P195
[4]   LINEAR AND NONLINEAR OPTICAL PROPERTIES OF ZNGEP2 AND CDSE [J].
BOYD, GD ;
BUEHLER, E ;
STORZ, FG .
APPLIED PHYSICS LETTERS, 1971, 18 (07) :301-&
[5]   Efficient mid-infrared laser using 1.9-μm-pumped Ho:YAG and ZnGeP2 optical parametric oscillators [J].
Budni, PA ;
Pomeranz, LA ;
Lemons, ML ;
Miller, CA ;
Mosto, JR ;
Chicklis, EP .
JOURNAL OF THE OPTICAL SOCIETY OF AMERICA B-OPTICAL PHYSICS, 2000, 17 (05) :723-728
[6]   A microcrystal method for the measurement of birefringence [J].
Cao, Liling ;
Peng, Guang ;
Liao, Wenbin ;
Yan, Tao ;
Long, Xifa ;
Ye, Ning .
CRYSTENGCOMM, 2020, 22 (11) :1956-1961
[7]   Polar or Nonpolar? A+ Cation Polarity Control in A2Ti(IO3)6 (A = Li, Na, K, Rb, Cs, Tl) [J].
Chang, Hong-Young ;
Kim, Sang-Hwan ;
Ok, Kang Min ;
Halasyamani, P. Shiv .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 2009, 131 (19) :6865-6873
[8]  
Chemla D. S., 1971, Optics Communications, V3, P29, DOI 10.1016/0030-4018(71)90207-0
[9]   Deep-UV nonlinear optical crystal KBe2BO3F2-discovery, growth, optical properties and applications [J].
Chen, C. T. ;
Wang, G. L. ;
Wang, X. Y. ;
Xu, Z. Y. .
APPLIED PHYSICS B-LASERS AND OPTICS, 2009, 97 (01) :9-25
[10]  
CHEN CT, 1985, SCI SIN B-CHEM B A M, V28, P235