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1.
The system CoIn2S4xSe4(1−x) has been investigated by X-ray powder methods on samples quenched at 700 °C. The spinel type phase has a phase width of 1≥x>0.9. A new layered compound is formed for 0.9>x>0.45 which crystallizes with the α-FeGa2S4-type with a=392.6 pm and c=1270.3 pm (x=0.5) for the hexagonal cell. Platelike crystals of the layered phase are obtained by transport reactions with iodine in a temperature gradient 750→700 °C. The band gaps of these crystals measured by optical absorption vary from 1.2 to 1.4 eV. The electrical conductivities of the crystals are found in the order of 10−5 Ω−1 cm−1.  相似文献   

2.
The Bi1−xLnxO1.5 solid solutions (Ln=La, Pr, Nd), of the β21/ε (Bi-Sr-O) structural type, have been investigated in their Ln-rich domains. For Ln=La, Pr, and Nd, the upper limits are 0.35, 0.35 and 0.33, respectively. The Bi4Ln2O9 ε phase (x=0.33) appears to be the single definite compound. For Bi4La2O9, Bi4Pr2O9 and Bi4Nd2O9, the ε-type cells are respectively: a=9.484(4) Å, b=3.982(2) Å, c=7.030(3) Å, β=104.75(3)°; a=9.470(5) Å, b=3.945(2) Å, c=6.968(4) Å, β=104.73(3)° and a=9.439(3) Å, b=3.944(2) Å, c=6.923(2) Å, β=105.03(3)°. Upon heating, each monoclinic (ε) compound transforms successively into rhombohedral phases (β21) and finally into a cubic fluorite-type phase. For La- and Pr-based compounds, all transitions are reversible; for Nd, depending on the thermal treatment, the reversibility of ε→β2 can be incomplete. These transformations are characterized using X-ray thermodiffractometry, differential thermal analysis, dilatometry and impedance spectroscopy versus temperature. Examination of Bi4(Ln, Ln′)2O9 samples allows to correlate the evolution of the thermal behavior and of the unit cell parameters, to the lanthanide size. A partial plot of the (Bi2O3)1−x-(La2O3)x phase diagram (0≤x≤0.40) is proposed.  相似文献   

3.
The Er2+xTi2−xO7−δ (x = 0.096; 35.5 mol% Er2O3) solid solution and the stoichiometric pyrochlore-structured compound Er2Ti2O7 (x = 0; 33.3 mol% Er2O3) are characterized by X-ray diffraction (phase analysis and Rietveld method), thermal analysis and optical spectroscopy. Both oxides were synthesized by thermal sintering of co-precipitated powders. The synthesis study was performed in the temperature range 650-1690 °C. The amorphous phase exists below 700 °C. The crystallization of the ordered pyrochlore phase (P) in the range 800-1000 °C is accompanied by oxygen release. The ordered pyrochlore phase (P) exists in the range 1000−1200 °C. Heat-treatment at T ≥ 1600 °C leads to the formation of an oxide ion-conducting phase with a distorted pyrochlore structure (P2) and an ionic conductivity of about 10−3 S/cm at 740 °C. Complex impedance spectra are used to separately assess the bulk and grain-boundary conductivity of the samples. At 700 °C and oxygen pressures above 10−10 Pa, the Er2+xTi2−xO7−δ (x = 0, 0.096) samples are purely ionic conductors.  相似文献   

4.
We investigated isomorphous substitution of several metal atoms in the Aurivillius structures, Bi5TiNbWO15 and Bi4Ti3O12, in an effort to understand structure-property correlations. Our investigations have led to the synthesis of new derivatives, Bi4LnTiMWO15 (Ln = La, Pr; M = Nb, Ta), as well as Bi4PbNb2WO15 and Bi3LaPbNb2WO15, that largely retain the Aurivillius (n = 1) + (n = 2) intergrowth structure of the parent oxide Bi5TiNbWO15, but characteristically tend toward a centrosymmetric/tetragonal structure for the Ln-substituted derivatives. On the other hand, coupled substitution, 2TiIV → MV + FeIII in Bi4Ti3O12, yields new Aurivillius phases, Bi4Ti3−2xNbxFexO12 (x = 0.25, 0.50) and Bi4Ti3−2xTaxFexO12 (x = 0.25) that retain the orthorhombic noncentrosymmetric structure of the parent Bi4Ti3O12. Two new members of this family, Bi2Sr2Nb2RuO12 and Bi2SrNaNb2RuO12 that are analogous to Bi2Sr2Nb2TiO12, possessing tetragonal (I4/mmm) Aurivillius structure have also been synthesized.  相似文献   

5.
The semiconducting system Bi2−xFexTe3 (x = 0.0, 0.02, 0.04 and 0.08) was synthesized at 1000 °C for 30 h. The scanning electron microscope (SEM) image reveals the tendency of the Bi2−xFexTe3 system to form a sheet structure with more pronounced alignment and to enhance the formation of some microstructure tubes. The structure of the system under study was refined on the basis of X-ray powder diffraction data using the Rietveld method. The analysis revealed the complete miscibility of Fe in the Bi2Te3 matrix and hence the formation of single phase. The system crystallizes in the space group R-3m [1 6 6]. The lattice parameters and the unit cell size slightly change by the incorporation of Fe. The refinement of instrumental and structural parameters led to reliable values for the RB, RF and Chi2.  相似文献   

6.
Rahana Yoosuf 《Thin solid films》2007,515(15):6188-6191
An insurmountable disadvantage of CuInSe2 is the low band gap, which limits the open-circuit voltage to value well below 500 mV in solar cells. The incorporation of sulfur into CuInSe2 thin film was investigated to establish a scientific basis for the graded band gap CuIn(Se1 − x,Sx)2 thin films. CuIn(Se1 − x,Sx)2 thin films were obtained by reactive annealing of Cu11In9 precursors in a mixture of sulfur and selenium atmosphere while post-sulfurization of single phase CuInSe2 did not result in CuIn(Se1 − x,Sx)2 thin films. A band gap of 1.36 eV, was obtained for the prepared CuIn(Se1 − x,Sx)2.  相似文献   

7.
Undoped and doped either by Eu3+ or Tb3+ bismuth borate Ba3BiB9O18 was structurally characterized and analyzed by fluorescence spectroscopy. Belonging to synthetic borate member of the family Ba3XB9O18, layers of planar triangular B3O6 groups connecting with deformed BaO6 hexagons are interleaved by 9-coordinate Ba atoms, and 6-coordinate Bi atoms. Its crystal structure was determined and refined from powder X-ray diffraction data by the Rietveld method and the results showed that Ba3BiB9O18 belongs to space group P63/m with unit cell dimensions of a = 7.1999(2) Å, c = 17.3567(6) Å, and z = 2. Curves of differential thermal analysis and thermogravimetric analysis showed that Ba3BiB9O18 is a congruent melting compound and chemically stable above 728 °C. Ba3Bi1−xEuxB9O18 and Ba3Bi1−xTbxB9O18 form a continuous solid solution from x = 0.01 to x = 0.9. The ultraviolet excited photoluminescence intensity increased with both Eu3+ and Tb3+ concentration in the matrix of Ba3BiB9O18. There may be an interesting correlation between spectroscopic properties and lattice structural features of doped Ba3BiB9O18.  相似文献   

8.
This paper presents an increase to x = 0.67 of the zirconium content in the conductive Bi2−xZrxO3+δ solid solution. Complete incorporation of Zr in the βIII-Bi2O3 structure, confirmed by X-ray powder diffraction, has produced a phase with a lower volume and superior conductivity than those predicted by an earlier study. The observed βIII-δ Bi2−xZrxO3+δ phase transition around 730 °C has been characterised for the first time and shows a segregation of a mixture of predominantly γ-Bi2O3 and approximately 30% of the ZrO2, before total reincorporation of the Zr in the high temperature δ-phase.  相似文献   

9.
The La1−xBix(Mg0.5Sn0.5)O3 ceramics were prepared by the conventional solid-state method with various sintering temperatures. The X-ray diffraction patterns of the La0.97Bi0.03(Mg0.5Sn0.5)O3 ceramics revealed no significant variation of phase with sintering temperatures. An apparent density of 6.50 g cm−3, a dielectric constant (?r) of 20.2, a quality factor (Q × f) of 58,100 GHz and a temperature coefficient of resonant frequency (τf) of −84.2 ppm °C−1 were obtained for La0.97Bi0.03(Mg0.5Sn0.5)O3 ceramics that were sintered at 1550 °C for 4 h.  相似文献   

10.
Bi2YVO8 was prepared by solid-state reaction for the first time. The structural and photocatalytic properties of Bi2YVO8 were studied. The results showed that this compound has the tetragonal crystal system with space group I4/mmm. The band gap of Bi2YVO8 was estimated to be about 2.09 eV by plotting (αhν)2 versus and obtaining the axis intercept value according to Tauc's equation. For the photocatalytic water splitting reaction, H2 or O2 evolution was observed from pure water with Bi2YVO8 as the photocatalyst under ultraviolet light irradiation (wavelength = 390 nm). Degradation of aqueous methylene blue photocatalyzed by this compound was investigated under visible light irradiation. Bi2YVO8 showed higher photocatalytic activity compared to Bi2YTaO7, Bi2InTaO7 or TiO2 (P-25). Complete removal of aqueous methylene blue was achieved after visible light irradiation for 170 min. The decrease of the total organic carbon and the formation of inorganic products such as SO42− and NO3 revealed the continuous mineralization of aqueous methylene blue during photocatalytic reaction.  相似文献   

11.
La2O3 and Nd2O3 were used to substitute Bi2O3 and the effects of complex substitution on the sintering behavior and the microwave dielectric properties of BiNbO4 ceramics were studied. With 0.5 wt.% CuO-V2O5 mixtures addition, all of the Bi1−x(La0.38Nd0.62)xNbO4 ceramics could be densified below 920 °C. The triclinic phases are identified in Bi1−x(La0.38Nd0.62)xNbO4 ceramics with x=0.01 sintered at 820 °C and the triclinic intensities increase with increasing the x value and sintering temperature. The saturated bulk density slightly decreases from 7.17 to 7.13 g/cm3 and the εr value from 44.24 to 42.76 with increasing x from 0 to 0.07 for Bi1−x(La0.38Nd0.62)xNbO4 ceramics. The saturated Q×f value is between 10,300 and 12,400 GHz depending on the x value. The τf values of dense Bi1−x(La0.38Nd0.62)xNbO4 ceramics decrease from 28.32 to 12.79 ppm/°C with x varying from 0 to 0.01 and remain almost unchanged with further increasing x.  相似文献   

12.
Sr2−xCaxBi4Ti5O18(x = 0, 0.05) powders synthesized by solid state route were uniaxially pressed and sintered at 1225 °C for 2 h. The obtained dense ceramics exhibited crystallographic anisotropy with a dominant c axis parallel to the uniaxial pressing direction which was quantified in terms of the Lotgering factor. Microstructure anisotropy of both compositions (x = 0, 0.05) consisted of plate like grains exhibiting their larger surfaces mostly perpendicular to the uniaxial pressing direction. Dielectric and ferroelectric properties of Sr2−xCaxBi4Ti5O18 ceramics were measured under an electric field (E) applied parallel and perpendicularly to uniaxial pressing direction. The obtained dielectric ?R(T) and polarization (P-E) curves depended strongly on E direction thus denoting a significant effect from microstructure and crystallographic texture. Sr2−xCaxBi4Ti5O18 properties were also significantly affected by Ca content (x): Curie temperature increased from 280 °C (x = 0) to 310 °C (x = 0.05) while ?R and remnant polarization decreased for x = 0.05. The present results are discussed within the framework of the processing and crystal structure-properties relationships of Aurivillius oxides ceramics.  相似文献   

13.
We describe the synthesis and characterization of new intergrowth Aurivillius related phases, Bi4LnNb3O15 (Ln = La, Pr, Nd) and Bi4LaTa3O15. Both powder X-ray diffraction and electron microscopy investigations show that the compounds adopt orthorhombic structures with the cell parameters a ∼ 5.5 Å, b ∼ 5.5 Å and c ∼ 20.9 Å, suggesting an ordered intergrowth structure that consists of n = 1 [Bi2NbO6] and n = 2 [Bi2LnNb2O9]+ Aurivillius fragments which are stacked alternately along the c-axis. The oxides do not show a second harmonic generation (SHG) response toward 1064 nm laser radiation; they do not show a ferroelectric-paraelectric transition either between 30 and 900 °C in dielectric measurements, indicating a centrosymmetric structure. Optical absorption studies show that the intergrowth phases possess considerably smaller band gaps than the parent Nb2O5 and Ta2O5.  相似文献   

14.
New quenched-in fluorite-type materials with composition (BiO1.5)0.94−x(LaO1.5)0.06(PbO)x, x = 0.02, 0.03, 0.04 and 0.05, were synthesised by solid state reaction. The new materials undergo a number of phase transformations during heating between room temperature and 750 °C, as indicated by differential thermal analysis. Variable temperature X-ray diffraction performed on the material (BiO1.5)0.92(LaO1.5)0.06(PbO)0.02 revealed that the quenched-in fcc fluorite-type material first undergoes a transformation to a β-Bi2O3-type tetragonal phase around 400 °C. In the range 450-700 °C, α-Bi2O3-type monoclinic, Bi12PbO19-type bcc and β12-type rhombohedral phases, and what appeared to be a ?-type monoclinic phase, were observed, before a single-phase fluorite-type material was regained at 750 °C.  相似文献   

15.
Solar cells with a short-circuit current density (Jsc) of 6 mA/cm2, an open circuit voltage (Voc) of 280 mV and a conversion efficiency of 0.5% under a 1000 W/m2 solar radiation were prepared by sequential chemical deposition of Bi2S2 (160 nm) and PbS (400 nm) thin films. The optical band gap (Eg) of Bi2S3 (160 nm) decreased from 1.67 to 1.61 eV upon heating the as-deposited film at 250 °C in air for 15 min to make it crystalline, but also reduced its thickness to 100 nm. Photoconductivity of this film is 0.003 (Ω cm)− 1. The Eg of PbS film (200 nm) deposited at 25 °C (24 h) is 0.57 eV, and is 0.49 eV for the film deposited at 40 °C. The electrical conductivity of the latter is 0.48 (Ω cm)− 1. The photo-generated current density for a Bi2S3(100 nm)/PbS(300 nm) absorber stack is above 40 mA/cm2 under AM 1.5 G (1000 W/m2) solar radiation. However, the optical losses in the cell structure reduces the Jsc. Spectral sensitivity of the external quantum efficiency of the cell establishes the contribution of Bi2S3 and PbS to Jsc. The energy level diagram of the cell structure suggests a built-in potential of 470 mV for the present case. Six series-connected cells gave the Voc of 1.4 V and Jsc of 5 mA/cm2.  相似文献   

16.
Mass density, glass transition temperature and ionic conductivity are measured in xLi2O-(40 − x)Na2O-50B2O3-10Bi2O3 and xK2O-(40 − x)Na2O-50B2O3-10Bi2O3 glass systems with 0 ≤ x ≤ 40 mol%. The strength of the mixed alkali effect in Tg, dc electrical conductivity and activation energy has been determined in each glass system. The magnitudes of the mixed alkali effect in Tg for the mixed Li/Na glass system are much smaller than those in the mixed K/Na glasses. The impact of mixed alkali effect on dc electrical conductivity in mixed Li/Na glass system is more pronounced than in the K/Na glass system. The results are explained based on dynamic structure model.  相似文献   

17.
Lead-free (K0.5Na0.5)(Nb1−xTax)O3 ceramics with x = 0.00-0.30 were prepared by the solid-state reaction technique. The effects of Ta on microstructure, crystallographic structure, phase transition and piezoelectric properties have been investigated. It has been shown that the substitution of Ta decreases Curie temperature TC and orthorhombic-tetragonal phase transition temperature TO-T, while increasing the rhombohedral-orthorhombic phase transition temperature TR-O. In addition, piezoelectric activity is enhanced with the increase of Ta content. The ceramics with x = 0.30 have the high value of piezoelectric coefficient d33 = 205 pC/N. Moreover, kp shows little temperature dependence between −75° C and 75 °C, and d33 exhibits very good thermal stability over the range from −196 °C to 75 °C in the aging test.  相似文献   

18.
19.
Amorphous composite films, composed of a Ti1 − xVxO2 solid-solution phase and a V2O5 phase, were produced by chemical bath deposition and subsequently air-annealed at various temperatures up to 550 °C. The microstructure and chemical composition of the as-prepared and annealed films were investigated by a combinatorial experimental approach using Scanning electron microscopy, X-ray powder diffraction and X-ray photoelectron spectroscopy. Ultraviolet-Visible Spectrometry was applied to determine the optical band gap of the as-prepared and annealed films. It followed that the incorporation of vanadium in the as-deposited films reduces the optical band gap of TiO2 from about 3.8 eV to 3.2 eV. Annealing of the films up to 350 °C leads to slight increase of band gap, as attributed to a reduction of the defect density in the initially amorphous oxide films due to the gradual development of long-range order and a concurrent reduction of the V4+-dopant concentration in the Ti1 − xVxO2 solid-solution phase. The films crystallized upon annealing in air at 550 °C, which resulted in drastic changes of the phase constitution, optical absorbance and surface morphology. Due to the lower solubility of V4+ in crystalline TiO2, V4+ segregates out of the crystallizing Ti1 − xVxO2 solid-solution phase, forming crystalline V2O5 at the film surface.  相似文献   

20.
A new series of solid solutions of the type, AxBa1−xBi2Mo4O16 (A = Ca, Sr, Pb) have been isolated. The domain of the solid solutions is very narrow and is in the range (0.01 ≤ x ≤ 0.10). All the phases were synthesized by the solid-state technique. The crystal structure is similar to that of the monoclinic scheelite type BaBi2Mo4O16. The structure consists of layers of [Bi2O2] units separated by (Ba/AO)10 units and isolated MoO4 tetrahedra. Their semiconductor band gaps render them as potential materials for photocatalysis.  相似文献   

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