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1.
X-ray diffraction (XRD), electron paramagnetic resonance (EPR), and magnetic susceptibility measurements have been employed to investigate the samples from the (Gd2O3) x ·(B2O3)(60−x)·(ZnO)40 (0 ≤ x ≤ 20 mol%) system. The XRD pattern for the prepared samples shows that the vitreous phase is present only for x ≤ 15 mol%. For the samples containing 20 mol% Gd2O3 the presence of a unique crystalline phase, GdBO3, embedded in a vitreous matrix was evidenced. In this case the XRD patterns show the presence of nanometer sized crystals (64 nm) in a glassy matrix. The EPR spectra of the studied samples exhibit three important features with effective g-values of ≈6, 2.8, 2.0 and a weaker feature at g ≈ 4.8. For low Gd2O3 contents (x < 3 mol%), the EPR spectra have the typical ‘‘U’’-type shape. For higher contents of Gd2O3 (x ≥ 3 mol%), the spectral features are broadened and finally are dominated by a single broad absorption line located at g ≈ 2.0. This broad EPR line is associated to the Gd3+ ions present predominantly as clustered species. Magnetic susceptibility data show that for x > 1 mol% the Gd3+ ions are present not only as isolated species but also as species coupled through antiferromagnetic exchange interactions.  相似文献   

2.
Glasses of the xFe2O3·(100−x)[B2O3·SrO] system, with 0 ≤ x ≤ 30 mol% were studied by X-ray diffraction, density, optical microscopy and FT-IR spectroscopy measurements. The X-ray patterns for the prepared system show that vitreous phase is present only in the sample with x < 40 mol%. For x ≥ 40 mol% in the studied samples is evidenced crystalline phase of Fe2O3. SEM measurements for the sample with x = 40 mol% shows that there are formed Fe2O3 microcrystallites with 10–20 μm dimension. FT-IR spectroscopy measurements shown that BO3 and BO4 are the main structural units of the glass system and the iron ions are located in the glass network.  相似文献   

3.
X-ray diffraction and FTIR spectroscopy measurements have been employed to investigate the xGd2O3 · (100 − x)[2Bi2O3 · B2O3] glass ceramics system, with 0  ≤ x ≤ 20 mol%. Heat treatment of glass samples at 625 °C for 24 h led to the formation of two crystalline phases. One crystalline phase is for the sample without gadolinium ions which belongs to the cubic system and another one is for the sample containing 20 mol% Gd2O3 which is orthorhombic with two unit cell parameters very close to each other. Between x = 0 mol% and x = 20 mol% there is a mixture of these crystalline phases. FTIR spectroscopy data suggest that the gadolinium ions play the network modifier role in the studied glasses. These data show that the glass structure consists of the BiO3, BiO6, BO3, and BO4 structural units, and the conversion among these units mainly depends on the Gd2O3 content.  相似文献   

4.
X-ray diffraction (XRD), Fourier transform infrared (FTIR) and electron paramagnetic resonance (EPR) spectroscopies have been employed to investigate the xGd2O3 · (95 − x)[2Bi2O3 · B2O3] · 5V2O5 glass system, with 0 ≤ x ≤ 25 mol%. The glass samples have been prepared by melting at 1,100 °C for 10 min followed by rapid cooling at room temperature. The structure of samples was analyzed by means of XRD. The pattern obtained did not reveal any crystalline phase in the samples up to 25 mol%. FTIR spectroscopy data suggest that the gadolinium ions play the network modifier role in the studied glasses. These data show that the glass network consists of BiO3, BiO6, BO3, BO4, and VO4 structural units. The FTIR data show that a conversion among these units takes place and this process mainly depends on the Gd2O3 content. The EPR spectra of the studied glasses exhibit three important features with effective g-values of ≈5.9, 2.85, 2.0 and a weaker feature at g eff ≈ 4.8. For low Gd2O3 contents (x ≤ 10 mol%), the EPR spectra have the typical ‘‘U’’-type shape. For higher contents of Gd2O3 (x > 10 mol%), the spectral features are broadened and finally are dominated by a single broad absorption line located at g eff ≈ 2.0. This broad EPR line is associated to the Gd3+ ions present predominantly as clustered species.  相似文献   

5.
Solid solution series, (Bi2O3)1−x (Y2O3)x and (Bi2O3)1−x (Gd2O3)x, forx = 0.10, 0.20, 0.30 and 0.40 were synthesized by standard ceramic technique. The structural phase characterization was carried out using X-ray powder diffraction technique. It was found that the solid solution containing 20–40 mole% of Y2O3 had face-centred cubic structure. All samples of the solid solution series, (Bi2O3)1−x (Gd2O3)x, had rhombohedral single phase in the concentration range 0.10 ≤x ≤ 0.40. Lattice parameters offcc phase of Y2O3 doped samples were calculated from the X-ray diffraction data. The lattice constant ‘a’ gradually decreases with increasing content of dopant concentration (x) for the Y2O3 doped system and obeys Vegard’s rule. The unit cell parameters for the (Bi2O3)1−x (Gd2O3)x doped samples showing rhombohedral phase were obtained on hexagonal setting.  相似文献   

6.
In order to further elucidate the local structure of ternary xGd2O3(100 − x)[0.7TeO2 · 0.3V2O5] glasses with x = 0, 5, 10, 15, 20 mol%, FTIR spectroscopy, XRD diffraction and density measurement were performed. FTIR and density data show that by increasing the gadolinium ions content of the samples the excess of oxygen may be accommodated by the inter-conversion of some [VO4] into [VO5] structural units and of [TeO3] into [TeO4] units. The composition of the heat-treated glasses was found to consist mainly of the Te2V2O9 crystalline phase. Varying x between 15 and 20 mol% Gd2O3 produces structural modification having as result an increase of the glass network polymerization degree. Accordingly, the gadolinium ions play a particular role related to the improvement of the homogeneity of the glasses and in accommodating the glass network with the excess of oxygen.  相似文献   

7.
A range of phospho-tellurite glasses containing gadolinium was prepared and infrared absorption spectra were measured. Structural changes, as recognized by analyzing band shapes of IR spectra, revealed that Gd2O3 causes a higher extent of network polymerization as far as x ≤ 15 mol% because the conversion of [TeO4] to [TeO3] structural units is supported by the increase of metaphosphate structural groups. While for x between 20 and 30 mol% Gd2O3 show some drastic structural modifications which lead to the increase in the glass fragility. Thus the addition of V2O5 resulted in gradual depolymerization of the phosphate chains and formation of short phosphate units, which are linked to vanadium through P–O–V bonds. The formation of P–O–V bonds increases the cross-link between the phosphate chains and the bending mode of Te–O–Te or O–Te–O linkages.  相似文献   

8.
xV2O5·(100 − x)[0.7P2O5·0.3CaO] glass system was obtained for 0 ≤ x ≤ 35 mol% V2O5. In order to obtain information regarding their structure, several techniques such as X-Ray diffraction, FT-IR, and EPR spectroscopies were used. X-Ray diffraction patterns of investigated samples are characteristic of vitreous solids. FT-IR spectra of 0.7P2O5·0.3CaO glass matrix and its deconvolution show the presence in the glass structure of all structural units characteristic to P2O5. Their number are increasing for x ≤ 3 mol% V2O5 then, for higher content of vanadium ions, the number of phosphate structural units are decreasing leading to a depolymerization of the structure. The structural units characteristic to V2O5 were not evidenced but their contribution to the glass structure can be clearly observed. EPR revealed a well resolved hyperfine structure (hfs) typical for vanadyl ions in a C4v symmetry for x ≤ 3 mol% V2O5. For 5 < x < 20 mol% V2O5 the spectra show a superposition of two EPR signals one due to a hfs structure and another consisting of a broad line typical for associated V4+–V4+ ions. For x ≥ 20 mol% V2O5 only the broad line can be observed. The composition dependence of the line-width suggests the presence of dipole–dipole interaction between vanadium ions up to x ≤ 5 mol% V2O5 and superexchange interactions between vanadium ions for x > 5 mol% V2O5.  相似文献   

9.
Structural investigation of xFe2O3·(100 − x)[3B2O3·SrO] glass system, with 0 ≤ x ≤ 40 mol%, was performed by means of X-Ray diffraction (XRD), Fourier transform infrared (FTIR) and Raman spectroscopies. The purpose of this work was to investigate the structural changes that appear in the 3B2O3·SrO glass matrix with the addition and increasing of iron ions content. The XRD pattern for the prepared samples shows that vitreous phase is present only for x ≤ 40 mol%. For sample containing 50 mol% Fe2O3 was evidenced the presence of a unique crystalline phase, Fe2O3, embedded in an amorphous matrix. FTIR data show that BO3 and BO4 are the main structural units of the glass system and the iron ions are located in the network. The Raman spectrum of glass matrix indicates a structure with several borate groups (di-, meta-, pyro-borate, etc.). In higher concentrations the iron ions break the regulate glass network and determines the appearance of BO4 isolated units.  相似文献   

10.
Glasses in the system (Gd2O3)x·(B2O3)(60−x)·(ZnO)40 (0 ≤ × ≤ 15 mol%) have been prepared by the melt-quenching technique. The local structure and the thermal behaviour of the obtained glasses were investigated using X-ray diffraction (XRD), differential thermal analysis (DTA) and Fourier transform infrared (FTIR) spectroscopy. The XRD pattern of the glasses confirmed their amorphous nature. Compositional dependence of the glass transition (Tg), fragility index (F), activation energy of the glass transition (Eg), activation energy for the crystallization process (Ep) were determined by DTA investigations. FTIR data revealed that the short-range order of glasses is affected by the addition of the Gd2O3 to the host glass matrix. The compositional dependence of the different structural units which appear in the investigated glasses was followed. FTIR data suggest that the gadolinium ions play the network modifier role in the studied glasses.  相似文献   

11.
The compounds Gd1−x Nd x BaSrCu3O7−δ (where x=0, 0.1 and 0.2) and Gd1−x Dy x BaSrCu3O y (where x=0, 0.1 and 0.3) were synthesized using the solid state reaction technique. The tetragonal crystallization of the compounds was identified by powder X-ray diffraction. The microrange crystallite formation and the substitution elements present in the compounds were observed by SEM and EDX analyses. The suppression of superconducting transition temperature and the variation of magnetization parameters for the substitution of rare-earth magnetic elements Nd and Dy ions were observed by low-temperature electrical resistance and magnetization measurements.  相似文献   

12.
Ceramic powders of (Nd x Gd1−x )2Zr2O7 (x = 0, 0.1, 0.3, 0.5, 0.7, 0.9, 1.0) were synthesized by chemical-coprecipitation followed by calcination method, and were then pressureless-sintered at 1,600 °C for 10 h in air. Phase constituents and morphologies of the synthesized powders and sintered ceramics were identified by X-ray diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscopy (TEM). A high-temperature dilatometer and a laser-flash method were used to analyze the thermal expansion coefficient and thermal diffusion coefficient of different ceramics from room temperature up to 1,400 °C. Thermal conductivity was calculated from thermal diffusivity, density, and specific heat. (Nd x Gd1−x )2Zr2O7 (0.1 ≤ x ≤ 1.0) ceramics are with a pyrochlore-type structure; however, pure Gd2Zr2O7 exhibits a defective fluorite-type structure. The average linear thermal expansion coefficients of different (Nd x Gd1−x )2Zr2O7 ceramics decrease with increasing the value of x from 0 to 1.0 in the temperature range of 25–1,400 °C. The thermal conductivities of (Nd x Gd1−x )2Zr2O7 ceramics are located within the range of 1.33 to 2.04 W m−1 K−1 from room temperature to 1,400 °C.  相似文献   

13.
Glasses from xFe2O3 · (100 − x)[P2O5 · TeO2] system, with 0 ≤ x ≤ 50 mol%, were investigated by X-ray diffraction, FT-IR and EPR spectroscopies. The XRD patterns show a vitreous state of studied samples for x ≤ 35 mol% Fe2O3. The FT-IR spectrum of the P2O5 · TeO2 glass matrix reveals a structure formed from PO4, TeO4 and TeO3 units. The addition and the increasing of Fe2O3 content modify progressively the structure of the glass matrix. The local structure in the investigated glasses was revealed by means of EPR using Fe3+ (3d5; 6S5/2) ions as paramagnetic probes. The EPR spectra present two resonance absorption lines characteristic to Fe3+ ions centred at geff ≈ 2.0, for 0.5 ≤ x ≤ 35 mol% and geff ≈ 4.3, for 0.5 ≤ x ≤ 5 mol%. The variation of the EPR parameters, the intensity and line-width of these absorption lines, with iron ions composition has been followed.  相似文献   

14.
Glasses in the system xGd2O3·(100 − x)[TeO2·GeO2] with 0 ≤ x ≤ 50 mol% have been prepared from melt quenching method. In this paper, we investigated changes of the coordination numbers of germanium, tellurium, and gadolinium ions by investigations of FTIR, EPR, and UV–VIS spectroscopy. By analyzing the structural changes resulted from the IR spectra we found that the bending modes of [GeO4] structural units and the deformed modes of the Te–O–Te linkages produce intercalation of the [GdO n ] entities in the germanate–tellurate chain network and densification of the glasses by increasing the number of [GeO6] structural units. EPR spectra of the studied samples reveal that the gadolinium ions play a role of network former. The UV–VIS spectra show broad UV absorption bands located in the 250–350 nm region. Their intensity increase with the increasing of Gd2O3 content showing that these stronger transitions can be due to the presence of the O=Ge bonds (n–π* excitations) of [GeO5] structural units. The [GeO5] structural units are more stable thermodynamically than their analogues and the [GeO6] structural units produce the improvement of the amorphous character of these glasses.  相似文献   

15.
16.
Multiferroic ceramic samples of Bi1−x Gd x FeO3 (x=0, 0.05, 0.1 and 0.15) have been prepared by rapid liquid-phase sintering technique. The effect of Gd substitution on ferroelectric and magnetic properties of Bi1−x Gd x FeO3 ceramics has been investigated. The results of X-ray diffraction (XRD) patterns show that the single-phase BiFeO3 sample has a rhombohedral structure and Gd3+ substitution for Bi3+ has not affected its structure. Experimental results suggest that for Bi1−x Gd x FeO3 system, the ferroelectric and magnetic properties of BiFeO3 are improved by Gd doping and the loop area increases with the Gd content. When x=0.15, saturated ferroelectric hysteresis loop is observed at room temperature with the maximal 2Pr=1.62 μC/cm2, which is about 578.6% higher than that of BiFeO3.  相似文献   

17.
Mixed lithium–zinc borophosphate glasses were prepared and studied in three compositional series xLi2O–(50−x)ZnO–50P2O5, xLi2O–(50−x)ZnO–10B2O3–40P2O5 and xLi2O–(50−x)ZnO–20B2O3–30P2O5 with x = 0, 10, 20, 30, 40 and 50 mol% Li2O. The obtained glasses were characterized by the measurements of the density (ρ), molar volume (V M), glass transition temperature (T g) and thermal expansion coefficient (α). For the investigation of structural changes 11B and 31P MAS NMR and Raman spectroscopy were applied. The replacement of zinc by lithium in borophosphate glasses slightly decreases V M and T g, while α increases. In Li–Zn metaphosphate glasses the compositional dependence of T g reveals a minimum, while at the borophosphate series T g decreases monotonously with increasing Li2O content. Chemical stability of Li–Zn borophosphate glasses is very good for glasses with x = 030 mol% Li2O. Spectral studies showed in the glass series with 10 mol% B2O3 only the presence of BO4 sites. In the glasses with 20 mol% B2O3 the presence of BO3 and two BO4 sites was revealed in ZnO-rich glasses and only one BO4 site in Li2O-rich glasses; the number of BO3 groups decreases with increasing Li2O content which is ascribed to the formation of P–O–Zn covalent bonds in ZnO-rich glasses.  相似文献   

18.
    
The effect of Ca doping in EuBaSrCu3O7−δ has been investigated by X-ray diffraction, ac susceptibility, and electrical resistivity measurements. X-Ray diffraction analyses of the samples showed that up to 30 at.% Ca can be substituted for Sr in EuBaSrCu3O7−δ, which has orthorhombic symmetry. The orthorhombicity decreases with increase inx, in EuBaSr1−xCax Cu3O7−δ, the material becoming tetragonal atx=0.2. Ac susceptibility and dc electrical resistivity measurements as function of temperature from 10 to 300 K showed that the superconducting transition temperatureT c decreases monotonically from 84 to 75K as the Ca concentrationx increases from 0.0 to 0.3 The decrease inT c can be attributed to the structural change taking place in EuBaSrCu3O7 as a consequence of replacement of Sr by Ca.  相似文献   

19.
Since infrared spectroscopy and density are advantageous tools for the investigations of glasses, we have used them to obtain information concerning the local structure of xGd2O3·(100 − x)[4Bi2O3·GeO2] glass system, with 0 ≤ x ≤ 30 mol%. Gd2O3 play the network modifier role in the studied glasses and determines, by progressive addition, the increase of structural volume difference between the hypothetical crystalline compounds and the quenched samples. FTIR spectroscopy data show that the glass structure consists on the BiO6, GeO4 and GeO6 structural units, and the conversion among these units mainly depends on the Gd2O3 content.  相似文献   

20.
The degradation behaviour of phosphate glass with nominal composition, 40Na2O-10BaO-xB2O3-(50-x)P2O5, where 0 ≤ x ≤ 20 mol%, was studied in water, HCl and NaOH solutions at room temperature to 60°C for different periods extending up to 300 h. These glasses were synthesized by conventional melt-quench technique. Dissolution rates were found to increase with B2O3 content in the glass. The dissolution rates for the glass having 10 mol% B2O3 were found to be 0·002 g/cm2 and 0·015 g/cm2 in distilled water and 5% NaOH solution, respectively, at room temperature after 225 h of total immersion period, whereas it increased considerably to 0·32 g/cm2 in 5% NaOH at 60°C after 225 h. However, glass samples with x = 15 and 20 mol% B2O3 were dissolved in 5% HCl solution after 5 h immersion. The degradation behaviour has been correlated with the structural features present in the glass. The optical microscopy of the corroded surface revealed that the corrosion mechanism were different in acid and alkali media.  相似文献   

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