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1.
An absorption band at 3644 cm−1 is caused by isolated OH ions. O ions cause an absorption band at 213 nm the oscillator strength of which is 0.020. Charge-compensation of O ions is effected by F ion vacancies (F). As for CaF2 crystals there occur monomers and dimers of [O – F] complexes. The mass action constants of association of F with oxygen centres are KAD = ⅓ exp (4.28 – 0.82 eV/kT) for [O – F], KAT = 4 exp (17.4 – 1.25 eV/kT) for [2 O – F] and KAQ = exp (4.2 – 0.89 eV/kT) for [2 O – 2 F].  相似文献   

2.
Following the chemical reaction method pure and doped lead hydrogen phosphate single crystals were grown in silica gel using different gel density, various concentrations of phosphoric acid, and lead nitrate solutions. As the gel pH plays an important role in the formation of different H3PO4 species in the phosphoric acid system, the pH range in which HPO ions dominate, was considered which in turn in necessary for the growth of lead hydrogen phosphate crystals. Characteristics of these crystals were carried out by infrared spectral analysis and microhardness study.  相似文献   

3.
The hyperfine structure has been investigated in the EPR spectra of X-irradiated KCl: CrO, Ca2+ and KBr: CrO, Ca2+ crystals. Preliminarily spectra were simplified by means of heating the crystals up to 400 K for KCl and 440 K for KBr, that destroys the less stable CrO · V centers. It is ascertained, that principal directions of g- and A-tensors do not coincide, and principal A-values are determined. Calculations, making use of the experimental meanings of g- and A-tensor components, showed, that the degree of distortion of oxygen tetrahedra in CrO · Ca2+ · V centers is almost the same in both KCl and KBr crystals; besides, these calculations suggest the existence of a strong covalent bonding between the central Cr5+ ion and four oxygen ligands in CrO ions.  相似文献   

4.
Optical quality calcite single crystals, CaCO3, have been grown under hydrothermal conditions in the of CaCO3 - NH4Br - H2O system doped with Li ions. 24- liter autoclaves including titanium inserts were used in these experiments. Optical properties of calcite crystals were studied. The light absorption index of the crystals grown is similar to rhombohedron materials, but pinacoidai calcite have no V-shaped defects.  相似文献   

5.
BaVTiO3 single crystals can be grown from a basic BaCl2 flux. The electric conductivity was measured at a- and c-domain crystals and optical absorption as well as photoconductivity were ascertained at a-domain crystals using plane polarized light in dependence on direction. Properties and their anisotropy are discussed on the basis of their local relations in the ferroelectric host lattice and compared with the properties of BaNbTiTiO3 single crystals described in the preceding communication.  相似文献   

6.
The UHV surface preparation of AB materials (crystals and thin films) has been monitored with XPS and AES. Clean and stoichiometric surfaces of AB crystals were prepared by means of low energy ion bombardment and subsequent low temperature annealing. Stoichiometric Cd3As2 and Zn3P2 thin films with very low amounts of C and O were deposited by the evaporation of bulk material in the UHV. The quality of prepared AB crystal and thin film surfaces was sufficient to carry out density of states investigations (UPS, RELS) with success.  相似文献   

7.
Investigations of the OH ion incorporation into LiNbO3 crystals and the comparison of calculated and measured densities show that undoped congruent lithium niobate crystals contain Li+ and O− − ion vavancies O and Li+. If really present, stacking faults are of inferior importance. The good agreement of the absorption edges of stoichiometric and of 2.7 mol% MgO containing congruent lithium niobate crystals is explained by the occupance of all oxygen sites within these crystals.  相似文献   

8.
Experimental results for various states of buoyancy driven flow in vertical (Bi0.23Sb0.75)2Te3 molten zones with covered surface are presented. Critical thermal wall Rayleigh numbers Ra for the onset of time-dependent convection have been determined by means of temperature measurements. The stability diagram obtained for the existing buoyancy driven convection shows the increase of Ra with increasing aspect ratio. This relation is also known from other crystal growth configurations and is due to the damping influence of container walls. At the beginning in the oscillatory region of convection extremely long periods of oscillation (maximum 850 s) were observed, which are caused by another mechanism than periods (25 … 37 s) registered at increasing melt heights. Furthermore, Bi0.5Sb1.5Te3 crystals were grown by using the vertical zone melting technique. The microscopic striations observed in the grown crystals correlate exactly with the temperature signals caused by time dependent convection. However, the fluctuations of the tellurium distribution in axial direction measured by scanning the Seebeck coefficient are presumably generated by unsteady solutal convection during growth.  相似文献   

9.
Single crystals of La2(SO4)3 · 9 D2O were grown from saturated D2O solutions. According to X-ray diffraction measurements, the crystals have a hexagonal structure with unit cell parameters a = 10.996 Å and c = 8.077 Å (space group C–P63/m). Several physical properties were also determined (density, refractive indices, dielectric constants, specific heat, coefficient of linear expansion, microhardness).  相似文献   

10.
Precipitates of the metastable -phase grown in an Al-(6.8 at.%)Zn alloy are investigated by means of a technique of high resolution electron microscopy, namely by two-beam lattice fringe imaging with tilted illumination. It is demonstrated by this direct method that the -precipitates are in fact semicoherent. The transition of fully coherent Guinier-Preston zones into semicoherent precipitates of the -phase takes place by formation of additional (III)rh and { III }rh planes inside the zones.  相似文献   

11.
The EPR and optical absorption spectra of paramagnetic centers produced by X-irradiation in LiNaSO4 single crystals were investigated. 7 EPR lines are observed at room temperature and 6 more lines – at LNT. The angular dependences of line positions at LNT are studied and the principal g-factor values are defined. The comparison with published data permitted to assign six the most anisotropic lines to ion-radical SO with different orientations in the lattice; two lines to ion-radical SO; slightly anisotropic doublet line – to O ozonide ion; isotropic line with g = 2. 0045 – to ion radical SO.  相似文献   

12.
By fitting the theoretically calculated temperature-dependent conductivity σ to the measured dependencies log σT ÷ 1/T the following parameters have been determined: free formation enthalpy of anti-Frenkel defects gAF = 2.05 eV – 6.35 kT; mobilities of Fion vacancies F and interstitials F: vνT = 600 exp (-0.70 eV/kT) cm2 K/Vs, viT = 1.1 · 104 exp (-0.93 eV/kT) cm2 K/Vs. — The free association enthalpies of complexes consisting of single foreign ions (Sc3+, Y3+, La3+, Sm3+, Li+, K+, Na+, O) and the charge-compensating defect were obtained. The vibration frequency of F ions in the neighbourhood of F and F is changed by a factor of 2.6 and 0.6, respectively.  相似文献   

13.
The second harmonics generation of Nd-laser radiation (λ = 1.06 microns) of the isomorphic family of crystals with yttrium-aluminium borate (YAB) structure — RAl3(BO3)4 (R = Y, Sm, Eu, Gd, Dy, Er, Ho, Tu) — investigated using the powder method and the theoretical calculation of SHG–coefficients — are reported. The refraction indices (for λ = 5481 Å) and optical sign for all studied YAB-type crystals are determined with the help of the immersion method. All studied crystals possess PM direction and oee-interaction. The SH-intensity is of KDP order of magnitude, with reasonable correlation of experimental and theoretical data. Theoretical analysis of the contributions of different ions to the integral d magnitude has shown identical signs for all ion species in YAB structure type.  相似文献   

14.
Based on simple approximations the backscattering minimum yield is estimated for axial ion channeling in perfect crystals of six CuBIIIC chalcopyrite compounds. The results obtained for CuInSe2 are compared with experimental channeling spectra. Point defect concentrations up to about 1021 cm−3 are estimated for CuInSe2 single crystals grown by the vertical Bridgman method. A simple power law is found for the fluence dependence of the damage density in oxygen implanted CuInSe2 single crystals.  相似文献   

15.
The formulae for absolute Rdisap and relative R velocities of disappearance and lifetime τ of faces of growing crystals have been derived for stationary growth. It was shown that the quantities are determined by the relative growth velocity RA/RcritA of the vanishing face A with respect to the critical growth velocity RcritA and by the geometry of a crystal expressed by the trigonometric functions of interfacial angles β and γ formed between face A and the adjacent faces. R increases and τ decreases with the increase in RA/RcritA to certain limiting values. The calculations have been verified and illustrated by the experimental results for triclinic potassium bichromate (KBC) crystals. Results enable ones to predict values of velocities of disappearance and lifetimes of undesirable, supplementary faces of any real crystal.  相似文献   

16.
The conditions of growth, monodomenization, and detwinning are considered in order to obtain optically perfect barium–sodium niobate crystals (BSN). Optical homogeneity and that of chemical composition are investigated. It is shown that possible variations of composition in a crystal's volume are below 1%. Thermal E and optical Eg° widths of the forbidden zone are determined in the absorption spectra.  相似文献   

17.
The decomposition behaviour of an Al-2.0 at.% Zn-1.0 at.% Mg alloy after direct quench (DQ) and indirect quench (IQ:T = 23 °C, t) to the ageing temperature T = 160 °C (above the temperature of the rapid homogeneous nucleation, Th) was investigated by means of TEM and isothermal resistivity measurements. The precipitation density of the η-particles yields a maximum value at pre-ageing times about 10 min at T = 23 °C. To clear up the reason for that phenomenon a loop-formation and clustering model was introduced.  相似文献   

18.
The resistivity, the dielectric constant, and the positron lifetimes in La-doped SrTiO3 have been measured for La content x of 0—10 at.%. It was found that with increasing x, the variations of the resistivity and the dielectric constant and the positron lifetime parameters are nonmonotonic. The positron experiments have shown that the La-doping induces mainly formation of Sr vacancies and variation of Sr vacancy configuration; the most probable configuration is the isolated Sr vacancies (V) as x < 0.5 at.%, the associated defects (La V) for 0.5 < x < 1 at.%, and the associated defects (2 La V) above x = 1 at.%. The results suggest that the variation of the resistivity can be regarded as variation of electron density, and the variation of the dielectric constant results mainly from variations of the space-charge polarizaion and Sr-vacancy concentration and configuration.  相似文献   

19.
In order to establish reproducible conditions for chemical lap polishing of GaAs with NaOCl solutions, containing also OH- and CO -ions, the mechanism of dissolution was investigated using the rotating disk arrangement. In solutions with excess OCl concentrations likewise diffusion and a reaction of the first order with respect to OH and CO, complexing agents for Ga-ions, control the dissolution rate, and the surfaces of the wafers are polished. OH and CO32– concentrations in excess with respect to OCl lead to rate determining OCl diffusion and to irregularly polished or film covered surfaces. Diffusion constants for OH, CO and OCl are given.  相似文献   

20.
GaP layers were grown by liquid phase epitaxy from tin solution on semi-insulating GaAs substrates with various amounts of Te added to the melt (xTe = 10−4 …︁ 3 · 10−2). The Sn and Te concentrations in the layers were determined by chemical analysis as function of x. An analysis of the electrical measurements shows that the carrier transport in the layers is essentially determined by impurity band conduction effects.  相似文献   

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