Yelisseyev Alexander P, Jiang Xingxing, Isaenko Ludmila I, Kang Lei, Bai Lei, Lin Zheshuai, Goloshumova Alina A, Lobanov Sergei I, Naumov Dmitry Y
Institute of Geology and Mineralogy, Siberian Branch of the Russian Academy of Sciences, 3 Ac. Koptyug ave, Novosibirsk 630090, Russia.
Phys Chem Chem Phys. 2015 Jan 7;17(1):500-8. doi: 10.1039/c4cp04689g.
SrMgF4 has an extremely large bandgap Eg of 12.50 eV as obtained from reflection dispersion. The symmetry of this crystal is monoclinic P21 at room temperature and transforms to the orthorhombic Cmc21 phase near 478 K as the temperature increases. The acentric character of the low-temperature (LT) phase is confirmed by pyroelectric luminescence at T < 440 K. The fundamental absorption edge of the LT phase is located at 122 nm (10.15 eV). A considerable difference between the absorption edge and bandgap Eg is due to the strong exciton absorption. The first-principles electronic structure, refractive indices, nonlinear susceptibility and polarizability were calculated for both LT and high-temperature (HT) phases. Band-to-band transitions are direct for the LT phase but indirect for HT. In spite of relatively low birefringence (∼0.017) and nonlinear susceptibility (∼0.044 pm V(-1), an order lower than that in KDP), SrMgF4 crystals are considered promising for nonlinear optics thanks to their transparency far in the vacuum ultraviolet spectral region.
通过反射色散得到,SrMgF₄具有12.50 eV的极大带隙E₉。该晶体在室温下的对称性为单斜P2₁,随着温度升高,在接近478 K时转变为正交Cmc2₁相。低温(LT)相的非中心特性在T < 440 K时通过热释电发光得到证实。LT相的基本吸收边位于122 nm(10.15 eV)处。吸收边与带隙E₉之间存在相当大的差异是由于强激子吸收。对LT相和高温(HT)相都计算了第一性原理电子结构、折射率、非线性极化率和极化率。带间跃迁对于LT相是直接的,但对于HT相是间接的。尽管双折射相对较低(约0.017)且非线性极化率较低(约0.044 pm V⁻¹,比KDP中的低一个数量级),但由于SrMgF₄晶体在真空紫外光谱区域具有远高于其他材料的透明度,因此被认为在非线性光学方面具有潜力。