Ran He

NaSr3Be3B3O9F4: a promising deep-ultraviolet nonlinear optical material resulting from the cooperative alignment of the [Be3B3O12F](10-) anionic group.

The demand for deep-ultraviolet (deep-UV) coherent light sources (l< 200 nm) has become increasingly urgent because they have important applications in semiconductor photolithography, laser micromachining, modern scientific instruments (super-high-resolution and angle-resolved photoemission spectrometer, for example) and so forth. To date, the most effective method to generate deep-UV coherent light with solid-state lasers is through cascaded frequency conversion, in particular multiharmonics, using deep-UV nonlinear optical (NLO) crystals. Therefore, the discovery of suitable deep-UV NLO crystals is of great importance. In the past decades, the anionic group theory, which reveals that the overall nonlinearity of a crystal is the geometrical superposition of the microscopic second-order susceptibility tensors of the NLO-active anionic groups, has been very successful in developing borate NLO crystals. Several important NLO crystals have been discovered, including b-BaB2O4 (BBO), [4] LiB3O5 (LBO), [5] CsB3O5 (CBO), CsLiB6O10 (CLBO), [7, 8] and YCa4O(BO3)3 (YCOB), which have been widely used in NLO optics. However, they cannot be used to generate deep-UV coherent light (l< 200 nm) by multiharmonic generation owing to some inherent shortcomings. Thus, the search for new NLO materials, particularly for deep-UVapplications, has attracted considerable attention. A deep-UV NLO material must have a very short absorption edge, and in this respect, beryllium borates are attractive as they are supposed to possess very large energy gap. It is also well known that the incorporation of fluorine can effectively cause the UV absorption edge of a crystal to blue-shift, so our group has made great efforts to search for new deep-UV NLO fluorine beryllium borate crystals. After more than ten years of intensive research in our group, the KBe2BO3F2 [16–18] (KBBF) crystal became the first practically usable deep-UV NLO crystal used to generate coherent 177.3 and 193 nm light. The excellent NLO properties of KBBF crystals are mainly determined by the (Be2BO3F2)1 layer made up of trigonal-planar [BO3] units and the tetrahedral [BeO3F] units. This deep-UV coherent light material has been used as a photon source in modern instruments and revealed many novel scientific phenomena which could not be observed by traditional techniques, as shown in the study of superconductor CeRu2 [19] and Bi2Sr2CaCu2O8+d. [20] Unfortunately, the KBBF crystal is very difficult to grow in thickness because of its strong layering tendency, which severely limits the coherent output power. Therefore, there is great demand for new types of fluorine beryllium borates which have deepUV transmission, moderate birefringence, and relatively large second harmonic generation (SHG) coefficients, and at the same time overcome the crystal-growth problems found in the KBBF crystal. Alkali-metal and alkaline-earth-metal cations are favorable for the transmission of UV light because there are no d–d electron or f–f electron transitions in this spectral region. As shown in numerous explorations, the size and charge of cations have great influence on the macroscopic packing of anions, which in turn determines the overall NLO properties in a crystal. 22] Herein, we utilize both alkali-metal and alkaline-earth-metal cations. Different charge/size combinations of mixed cations may have different influences on the packing of anions, so it is more likely to isolate new phases with interesting stoichiometries, structures, and properties. To date, no fluorine beryllium borates with mixed cations have been reported. Guided by this idea, we successfully obtained a new alkali-metal/alkaline-earth-metal fluorine beryllium borate NaSr3Be3B3O9F4, which contains the novel anionic group [Be3B3O12F] 10 as the basic building unit. Furthermore, the arrangement of these [Be3B3O12F] 10 groups is very favorable for generating large a NLO response and moderate birefringence and especially for avoiding the layering tendency during bulk crystal growth. Herein, we report the synthesis, crystal growth, structure, linear and nonlinear optical properties, thermal behavior, and electronic structure of NaSr3Be3B3O9F. These results indicate that the NaSr3Be3B3O9F4 crystal may be a promising NLO material in the deep-UV range. NaSr3Be3B3O9F4 [23] crystallizes in the noncentrosymmetric trigonal space group R3m. The crystal structure is depicted in Figure 1a. In the asymmetric unit, Sr, Na, Be, B each occupy one crystallographically unique position, and there are two unique F and O positions. The B atom is coordinated to three O atoms to form a planar BO3 unit with B O bond lengths [*] H. Huang, J. Yao, Z. Lin, X. Wang, R. He, W. Yao, N. Zhai, Prof. C. Chen Center for Crystal Research and Development Technical Institute of Physics and Chemistry Chinese Academy of Sciences, Beijing 100190 (China) E-mail: cct@mail.ipc.ac.cn

Bi2(IO4)(IO3)3: A New Potential Infrared Nonlinear Optical Material Containing [IO4]3– Anion

A new potential infrared (IR) nonlinear optical (NLO) material Bi(2)(IO(4))(IO(3))(3) was synthesized by hydrothermal method. Bi(2)(IO(4))(IO(3))(3) crystallizes in the chiral orthorhombic space group P2(1)2(1)2(1) (No. 19) with a = 5.6831(11) Å, b = 12.394(3) Å, and c = 16.849(3) Å. It exhibits a three-dimensional framework through a combination of the IO(3), IO(4), BiO(8), and BiO(9) polyhedra and is the first noncentrosymmetric (NCS) structure containing [IO4](3-) anion. Bi(2)(IO(4))(IO(3))(3) has an IR cutoff wavelength of 12.3 μm and belongs to the type 1 phase-matchable class with a moderately large SHG response of 5 × KDP, which is in good agreement with the theoretical calculations.

Y(IO3)3 as a Novel Photocatalyst: Synthesis, Characterization, and Highly Efficient Photocatalytic Activity

Nonbonding layer-structured Y(IO3)3 was successfully prepared by a simple hydrothermal route and investigated as a novel photocatalyst for the first time. Its crystal structure was characterized by X-ray diffraction, high-resolution transmission electron microscopy, and scanning electron microscopy. The optical absorption edge and band gap of Y(IO3)3 have been determined by UV-vis diffuse reflectance spectra. Theoretical calculations of the electronic structure of Y(IO3)3 confirmed its direct optical transition property near the absorption edge region, and the orbital components of the conduction band and valence band (VB) were also analyzed. The photocatalytic performance of Y(IO3)3 was evaluated by photooxidative decomposition of rhodamine B under ultraviolet light irradiation. It demonstrated that Y(IO3)3 exhibits highly efficient photocatalytic activity, which is much better than those of commercial TiO2 (P25) and important UV photocatalysts BiOCl and BiIO4. The origin of the excellent photocatalytic performance of Y(IO3)3 was investigated by electron spin resonance and terephthalic acid photoluminescence techniques. The results revealed that the highly strong photooxidation ability that resulted from its very positive VB position should be responsible for the excellent photocatalytic performance.

Bandgaps in the deep ultraviolet borate crystals: Prediction and improvement

We identify the microscopic structural origins determining the bandgaps in the deep-ultraviolet borates, and propose an efficient method for the prediction of their bandgaps. This method considers only the chemical bond lengths around oxygen atoms and achieves the very high precision with the relative error <5% typically. Its validity is verified by the first-principles studies, which reveal the strong dependence of bandgaps on the coordination environment around oxygen atoms. Our studies have great implications on the search and design of optoelectronic functional materials with large bandgap.

ReBe2B5O11 (Re = Y, Gd): Rare-Earth Beryllium Borates as Deep-Ultraviolet Nonlinear-Optical Materials

Two novel rare-earth beryllium borates ReBe2B5O11 (Re = Y, Gd) have been discovered. These materials possess a unique structural feature with a platelike infinite ∞(2)[Be2B5O11]3– superlayer, which is first found in beryllium borates. The superlayer can be seen as sandwich-shaped with ∞(1)[B4O8]4– chains linking up with a ∞(2)[Be2BO5]3– sublayer above and below via the B–O–Be bond. Each ∞(2)[Be2B5O11]3– layer is further connected to the neighboring layer through Re3+ cations coordinating with O atoms. Both of these two crystals have very short cutoff wavelengths below 200 nm and exhibit relatively large nonlinear-optical (NLO) effects, indicating their promising applications as good deep-UV NLO crystals.

Ab initio studies on the mechanism for linear and nonlinear optical effects in YAl3(BO3)4

First-principles studies of the linear and nonlinear optical properties for YAl3(BO3)4 (YAB) are presented. Based upon the electronic band structure, the optical refractive indices, birefringence, and second harmonic generation (SHG) coefficients of YAB are calculated, which are in good agreement with experimental values. In addition, the SHG-weighted electron density analysis and the real-space atom-cutting method are adopted to elucidate the origin of the linear and nonlinear optical effects in YAB. The results show that the anionic (BO3) groups have dominant contributions to the birefringence. The contribution of the Al cations to the optical effects is negligibly small. However, the Y cations bond to the neighbor O anions and form the deformed (YO6) octahedra, which results in the large SHG effects in YAB.

Hydrothermal growths, optical features and first-principles calculations of sillenite-type crystals comprising discrete MO4 tetrahedra

Highly crystalline single crystals of sillenite-type Bi10Cd3O20 and Bi12(BixM1−x)O20 (M = B, Si, P, V, Mn, Fe, Ga, Ge) were successfully grown under mild hydrothermal conditions. Bulk crystals with smallest average size of 100 μm and preferable shapes can be obtained by optimizing respective growth conditions. The morphologies for Bi25FeO40 show regular evolutions along with different synthesis routes. Characterizations were performed by means of powder X-ray diffraction analyses, chemical analyses, optical spectra and first-principles calculations. It is found that all of the crystals possess certain transparency along with distinct absorptions in the visible region, corresponding to the discrete MO4 tetrahedra in the crystal lattices. Band gap energies of the fabricated sillenite crystals vary from approximately 1.66 eV for Bi12(Bi0.375Mn0.625)O20 to 2.85 eV for Bi12GeO20, as estimated from the absorption data. The impacts of tetrahedrally coordinated transition-metal cations on their electronic structures were investigated by first-principles computational approaches.

Energy band gap engineering in borate ultraviolet nonlinear optical crystals: ab?initio studies

The development of ultraviolet (UV) nonlinear optical (NLO) crystals demands optical materials with wide energy band gaps. Here we report first-principles studies on the electronic structures in several UV NLO borates with representative structures. Combined with model analysis, we find that the oxygen non-bonding 2p orbitals play an important role on the top of valence bands. The energy band gap can be adjusted by modifying the coordination environment around the oxygen atoms. Under ideal conditions the energy band gaps achieve 9xa0eV if the non-bonding orbitals are totally eliminated, despite the original values varying from 6.6 to 8.3xa0eV.

K2FeGe3Se8: a new antiferromagnetic iron selenide.

A new iron selenide, K2FeGe3Se8, has been obtained by spontaneous crystallization. It adopts a new structure type in the noncentrosymmetric monoclinic space group P2(1). In the structure, FeSe4 and GeSe4 tetrahedra are connected alternately via corner-sharing to form one-dimensional (1D) (∞)(1)[FeGeSe6]6– chains along the a-direction. These chains are further linked by sharing Ge2Se6 units to generate two-dimensional (2D) (∞)(2)[FeGe3Se8]2– layers stacked parallel to the ac-plane and separated by K+ cations. Deduced from temperature-dependent susceptibility measurement and specific heat measurement under different magnetic fields, K2FeGe3Se8 exhibits an antiferromagnetic transition at 10 K. Furthermore, the magnetic property shows anisotropy between directions parallel and perpendicular to the plane of (∞)(2)[FeGe3Se8]2– layer. The diffuse reflectance spectra measurement indicates that the band gap of K2FeGe3Se8 is 1.95(2) eV, consistent with the calculated values of 1.80 and 1.53 eV in the spin-up and spin-down directions, respectively. Based on electronic structure calculation, the spin of the Fe2+ cation is 1.85, which is comparable to the experimental value.