On the novel double perovskites A2Fe(Mn0.5W0.5)O6 (A= Ca,Sr, Ba). Structural evolution and magnetism from neutron diffraction data

New A₂Fe(Mn_0.5W_0.5)O₆ (A = Ca, Sr, Ba) double perovskite oxides have been prepared by ceramic techniques. X-ray diffraction (XRD) complemented with neutron powder diffraction (NPD) indicate a structural evolution from monoclinic (space group P2₁/n) for A = Ca to cubic (Fm-3m) for A = Sr and finally to hexagonal (P6₃/mmc) for A = Ba as the perovskite tolerance factor increases with the A²⁺ ionic size. The three oxides present different tilting schemes of the FeO₆ and (Mn,W)O₆ octahedra. NPD data also show evidence in all cases of a considerable anti-site disordering, involving the partial occupancy of Fe positions by Mn atoms, and vice-versa. Magnetic susceptibility data show magnetic transitions below 50 K characterized by a strong irreversibility between ZFC and FC susceptibility curves. The A = Ca perovskite shows a G-type magnetic structure, with weak ordered magnetic moments due to the mentioned antisite disordering. Interesting magnetostrictive effects are observed for the Sr perovskite below 10 K.     

运用Nd:YAG激光器的InGaAsP超晶格激光诱导无序

对与ＩｎＰ晶格匹配的ＩｎＧａＡｓＰ四元系量子阱材料进行了热稳定性能的研究,通过光荧光谱（ＰＬ）的测量发现：量子阱材料在６５０ ℃以上的常规退火条件下,有最大可达１５５ ｍ ｅＶ 的ＰＬ峰值蓝移,表明禁带宽度有明显增大．运用１．０６４ μｍ 连续输出的Ｎｄ：ＹＡＧ激光器进行光子吸收诱导无序（ＰＡＩＤ）技术的研究,比较量子阱材料被辐照前后荧光谱的峰值位置和谱宽,发现量子阱结构的禁带宽度在激光辐照后有明显增大,证明有量子阱混合现象产生．衬底预加热结果表明,提高衬底温度可减少ＰＡＩＤ中的激光辐照时间和平均功率密度．     

Raman spectra and thermal disordering of the crystalline structure of benzene

Disordering of rotational degrees of freedom of molecules in a benzene crystal is investigated from Raman spectra. Nonuniform smearing of the spectrum of librational vibrations to the wing of the Rayleigh line is established. The changes observed are interpreted on the basis of calculations of frequencies, intensities, vibration modes, and barriers to molecular reorientations in the crystal by the method of atom-atom potentials. The line broadening in the spectrum of external vibrations by reorientations of molecules in the crystal as a function of their mode is analyzed. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 66, No. 3, pp. 394–400, May–June, 1999.     

Thermal analysis of paraffins as model compounds for polyethylene

The n‐paraffins C₅₀H₁₀₂, C₄₄H₉₀, and C₂₆H₅₄ were analyzed with standard and temperature‐modulated differential scanning calorimetry. Crystallization and ordering from the melt to the condis phase showed practically no supercooling. These observations were confirmed with hot‐stage microscopy and a melting‐point apparatus. Only the organization of the C₂₆H₅₄ condis crystals to fully ordered crystals showed a supercooling of 4.0 K. The measurement of the apparent reversing heat capacity with a 0.05‐K modulation amplitude revealed that the melting of C₅₀H₁₀₂ was completed within 1.0 K and the isotropization of C₂₆H₅₄ was completed within less than 0.6 K, but 62–78% of the total transitions occurred over a much narrower temperature range of 0.1 K or less. The link to polyethylene was made with fractions of the masses 15,520, 2150, and 560 Da. The 560‐Da sample corresponded to C₄₀H₈₂ and showed also almost no supercooling, whereas the others, with folded and extended‐chain crystals, supercooled by about 10 K. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 2810–2822, 2000     

Effects of fields and anchoring on biaxial nematic ordering

Symmetry of a nematic liquid crystal phase is broken by an anchoring wall and also by an external field. Nematic system sandwiched between biaxial anchoring walls is introduced as a correspondent to a bulk nematic system exposed to a couple of fields, an electric field and a magnetic one in directions perpendicular to each other, and thermal behaviours of the system are studied. The crossover between a homeotropic structure and homogeneous one occurs, similarly to the bulk system in the fields, in which the anchoring condition of coexistence is shown to have the same expression as the one at the bulk. As to a characteristic phenomenon at the sandwiched system, it is proved that an appearance of a biaxial nematic order suppresses a uniaxial nematic order. A surface transition, i.e., a wetting phenomenon is shown to occur also in the biaxial nematics, even though the uniaxial order is suppressed therein.     

Defects in crystals studied by Raman scattering

Raman studies of crystal defects are reviewed. Raman spectroscopy is a powerful technique and has been used widely for investigating disordered structures. The degree of disorder in a crystal is quantitatively evaluated in terms of the phonon correlation length. The asymmetric Raman line shapes in defective crystals such as microcrystals, ion-implanted semiconductors are well reproduced by the spatial correlation (SC) model. The effect of alloying induced-potential fluctuations on Raman scattering is also explained within the framework of the SC model. In disordered graphite, the in-plane phonon correlation length is obtained from the relative intensity ratio of the disorder induced peak. The initial lattice disordering rates and the relaxation rates of disorder are determined, using real-time Raman measurements during ion irradiation in a scale of seconds. In this way, the phonon confinement due to the local defects is observed in the kinetic manner. Localized vibrational modes of defects in crystals are also described. In particular, Raman observation of the hydrogen molecule in crystalline semiconductors is discussed in detail.     

Novel perovskite-related barium tungstate Ba11W4O23

Ba₁₁W₄O₂₃ was synthesized at 1300 °C, followed by quenching with liquid nitrogen. The crystal structure, which was known to be cryolite-related but has remained unclear, was initially determined by single-crystal X-ray diffraction for the isostructural Ru-substituted compound Ba₁₁(W_3.1Ru_0.9)O_22.5, which was discovered during exploratory synthesis in the Ba-Ru-O system. The structure of Ba₁₁W₄O₂₃ was refined by a combined powder X-ray and neutron Rietveld method (Fd-3m, a=17.1823(1) Å, Z=8, R_p=3.09%, R_wp=4.25%, χ²=2.8, 23 °C). The structure is an example of A-site vacancy-ordered 4×4×4 superstructure of a simple perovskite ABO₃, and it may be written as (Ba_1.75□_0.25)BaWO_5.75□_0.25, emphasizing vacancies on both metal and anion sites. The local structure of one of two asymmetric tungsten ions is the WO₆ octahedron, typical of perovskite. The other tungsten, however, is surrounded by oxygen and anionic vacancies statistically distributed over three divided sites to form 18 partially occupied oxygen atoms (∼30% on average), represented as WO_18/3. The A-site cation-vacancies are ordered at the 8a (, , ) site in between adjoining WO_18/3 polyhedra which form 1-D arrangements along [110] and equivalent directions. In situ high-temperature XRD data have shown that the quenched Ba₁₁W₄O₂₃ at room temperature is isostructural to the high-temperature phase at 1100 °C.     

Structural Aspects of Lithium Transfer in Solid Electrolytes Li2x Zn2-3xTi1+xO4 (0.33≤ x≤ 0.67)

Solid solutions Li_{2x Zn2-3x}Ti_1+xO₄, where x =1/3, 1/2, 3/5, 2/3, were studied by powder X-ray diffractometry and differential thermal analysis. Conductivity measurements have been performed in the gas phase at different temperatures and oxygen pressures. Distribution of cations over the sites of the spinel structure has been determined. Conductivity increases substantially with lithium concentration. The high lithium conductivity of Li₃Zn_0.5Ti₄O₁₀ (x=3/5) and Li₄Ti₅O₁₂ (x=2/3) is the result of two sequential phase transitions associated with different lithium distributions in high-temperature phases with defective NaCl type structures. Possible routes of lithium ion transport are discussed and rationalized based on the conductivity and crystal data.     

Order-disorder in In perovskites: The example of A(In2/3B″1/3)O3 (A=Ba, Sr; B″=W, U)

We describe the preparation and structural characterization of four In-containing perovskites from neutron powder diffraction (NPD) and X-ray powder diffraction (XRPD) data. Sr₃In₂B″O₉ and Ba(In_2/3B″_1/3)O₃ (B″=W, U) were synthesized by standard ceramic procedures. The crystal structure of the W-containing perovskites and Ba(In_2/3U_1/3)O₃ have been revisited based on our high-resolution NPD and XRPD data, while for the new U-containing perovskite Sr₃In₂UO₉ the structural refinement was carried out from high-resolution XRPD data. At room temperature, the crystal structure for the two Sr phases is monoclinic, space group P2₁/n, where the In atoms occupy two different sites Sr₂[In]_2d[In_1/3B″_2/3]_2cO₆, with a=5.7548(2) Å, b=5.7706(2) Å, c=8.1432(3) Å, β=90.01(1)° for B″=W and a=5.861(1) Å, b=5.908(1) Å, c=8.315(2) Å, β=89.98(1)° for B″=U. The two phases with A=Ba should be described in a simple cubic perovskite unit cell (S.G. Pm3¯m) with In and B″ distributed at random at the octahedral sites, with a=4.16111(1) Å and 4.24941(1) Å for W and U compounds, respectively.     

无杂质空位扩散法造成InGaAsP/InP多量子阱结构带隙蓝移规律的研究

采用光荧光谱(PL)和光调制反射谱(PR)的方法,研究了由Si₃N₄、SiO₂电介质盖层引起的无杂质空位(IFVD)诱导的InGaAsP四元化合物半导体多量子阱(MQWs)结构的带隙蓝移。实验中Si₃N₄、SiO₂作为电介质盖层,用来产生空位,再经过快速热退火处理(RTA)。实验结果表明:多量子阱结构带隙蓝移和退火温度、复合盖层的组合有关。带隙蓝移随退火温度的升高而加大。InP、Si₃N₄复合盖层产生的带隙蓝移量大于InP、SiO₂复合盖层。而InGaAs、SiO₂复合盖层产生的带隙蓝移量则大于InGaAs、Si₃N₄复合盖层。同时,光调制反射谱的测试结果与光荧光测试的结果基本一致,因此,PR谱是用于测试带隙变化的另一种方法。