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1.
张泽  吴玉琨  郭可信 《物理学报》1984,33(5):696-700
本文利用电子衍射及高分辨点阵象实验方法证实了Ni3(Tix,V1-x)合金系在铸态下存在有9R,10H,16H,20H,21H,44H等长周期结构以及2H结构。它们与体心四方基体相(结构与Ni3V相同)及六角基体相(结构与Ni3Ti相同)有固定取向关系:{001}长周期∥{001}(Ni3Ti)∥{112}Ni3V);〈100〉长周期∥〈100〉(Ni3Ti)∥〈110〉(Ni3V)。样品经长期高温退火处理后其它长周期结构均向9R结构转变。 关键词:  相似文献   

2.
Pratibha L Gai  C N R Rao 《Pramana》1975,5(5):274-283
Lattice imaging technique of high resolution electron microscopy has been employed to examine 4H, 6H and 9R ABO3 perovskite polytypes. The lattice images can be correlated with the lattice periodicity and the stacking sequence of AO3 layers and BO6 octahedra. The study shows the utility and validity of the lattice imaging technique for the study of relatively close-packed systems. Commonwealth Visiting Professor, University of Oxford (1974–75).  相似文献   

3.
Extreme room temperature conductivity enhancements have been reported for nanocrystalline AgI of up to ×?10(4) relative to bulk β-AgI (Guo et?al 2005 Adv.?Mater. 17 2815-9). These samples were identified as possessing 7H and 9R polytype structures, which can be considered as heterostructures composed of thin, commensurate layers in the β (wurtzite) and γ (zincblende) phases. It has been proposed that space-charge layer formation at β|γ-interfaces causes near complete disordering of the Ag(+)?sublattice in these polytypes, resulting in a massive intrinsic enhancement of ionic conductivity. We have performed molecular dynamics simulations of β- and γ-AgI and mixed β|γ?superlattices, to study the effect of heterostructuring on intrinsic defect populations and Ag(+) transport. The ionic conductivities and Ag(+)?diffusion coefficients vary as β?>?7H?≈?9R?≈?10L?>?γ. The β|γ-heterostructured polytypes show no enhancement in defect populations or Ag(+)?mobilities relative to the β-AgI phase, and instead behave as simple composites of β- and γ-AgI. This contradicts the proposal that the extreme conductivity enhancement observed for 7H and 9R polytypes is explained by extensive space-charge formation.  相似文献   

4.
The 773 K isothermal section of the Dy–Ni–Si ternary system was investigated and constructed by X-ray powder diffraction in this paper. Eighteen ternary phases (DyNiSi, DyNi2Si2, DyNiSi2, Dy2Ni3Si5, DyNiSi3, Dy2NiSi3, Dy3Ni6Si2, DyNi10Si2, Dy4NiSi7, DyNi2Si, DyNi5Si3, DyNi4Si, Dy3NiSi2, DyNi6Si6, Dy8Ni31Si11, Dy3Ni2Si4, Dy4Ni5Si and Dy9Ni2Si14) were confirmed to exist in this work. In those ternary phases, Dy9Ni2Si14 is a new phase, Dy2NiSi3 and Dy4NiSi7 have solid solution phenomena and the solid solution ranges are Dy33.3Ni14.7–18.7Si52–48 and Dy4Ni0.3–1.2Si7.7–6.8, respectively. We constructed 14 two phase regions and 52 three phase regions in the Dy–Ni–Si ternary phase diagram at 773 K. Because the phase relation is not very clear between 66.7 and 50 Si at.% in the Dy–Si binary system, we use dot lines to estimate tentative phase regions in this region.  相似文献   

5.
本文用X射线衍射、差热分析及金相分析方法测定了Sm-Ni二元系合金相图。在此二元系中观察到8个金属间化合物:Sm3Ni(664℃分解),SmNi(熔点为1079℃),SmNi2(1034℃分解),SmNi3(1135℃分解),Sm2Ni7(1220℃分解),SmNi4(1282℃分解),SmNi5(熔点为1430℃)和Sm2Ni17(1288℃分解)。发生三个共晶反应:Sm3Ni-SmNi(570℃,~32at%Ni),SmNi-SmNi2(809℃,53.5at%Ni)和Sm2Ni17-Ni(1280℃,94at%Ni)。无论是Sm在Ni中或是Ni在Sm中,均未观察到明显的固溶度。 关键词:  相似文献   

6.
Magnetic and structural behaviour and phase relationships of materials of composition R3Ni7B2 (R = Nd-Lu) were investigated. Detailed X-ray analysis yields that two hexagonal structures are encountered. For the heavy rare earth (Gd-Lu) the compounds crystallize in the CeNi3 structure. The space group is P63/mmc and each unit cell contains two formula units. The R3Ni7B2 where R = Nd-Sm (including Yb3Ni7B2) crystallize in the CeCo4B structure. The space group is P6/mmm and each unit cell contains one formula unit. The detailed crystal structures are discussed. The magnetic measurements show that Yb3Ni7B2 and Lu3Ni7B2 are Pauli paramagnetic. Sm3Ni7B2 is ferromagnetically ordered with a huge intrinsic magnetic hardness. The magnetization at the coercive field at low temperatures is extremely time dependent. The R3Ni7B2 which crystallize in CeNi3 structure are antiferromagnetic at low temperatures. All Mossbauer and magnetization experimental results can be explained assuming an antiferromagnetic exchange interaction in both 2(c) and 4(f) crystallographic sites and a ferromagnetic interaction between these sites.  相似文献   

7.
In this work, the luminescence properties of samarium ions-doped titanium dioxide prepared by the sol-gel process were studied. A strong orange red emission (4G5/26H7/2 (orange) and 4G5/2-6H9/2 (red)) ascribed to the electron transitions in 4f5 configuration of Sm3+ ions was observed upon excitation into TiO2 host. The energy transfer from TiO2 to Sm3+ was verified and the relevant mechanism was discussed. In addition, the impacts of metal ion codopants upon the TiO2:Sm3+ luminescence properties were studied. The results indicated that the central excitation band shifted to blue in the bismuth-codoped materials (0.5-4% in molar ratio), while it shifted to red in the zirconium-codoped materials. Such materials may find applications in white light-emission diode (LED) and tunable solid lasers.  相似文献   

8.
The Sm3+-doped CaWO4 nanoparticles were synthesized by hydrothermal method. The room temperature photoluminescence (PL) spectra of Sm3+-doped CaWO4 nanoparticles doped with different Sm3+ concentrations under 405 nm excitation have been investigated. The PL spectra showed four strong emission peaks at 460, 571, 609, and 653 nm. The first emission peak at 460 nm could be due to a structural defect of the lattice, an oxygen-deficient WO3 complex. The other three emissions at 571, 609, and 653 nm were due to the f-f forbidden transitions of the 4f electrons of Sm3+, corresponding to 4G5/26H5/2 (571 nm), 6H7/2 (609 nm), and 6H9/2 (653 nm), respectively. In addition, the optimum Sm3+ concentration in CaWO4 nanoparticles for optical emission was determined to be 1.0%. The Sm3+4G5/26H7/2 (609 nm) emission intensity of Sm3+-doped CaWO4 nanoparticles significantly increased with the increase of Sm3+ concentration, and showed a maximum when Sm3+ doping content was 1.0%. If Sm3+ concentration continued to increase, namely more than 1.0%, the Sm3+4G5/26H7/2 emission intensity would decrease. The present materials might be a promising phosphor for white-light LED applications.  相似文献   

9.
郭常霖 《物理学报》1982,31(10):1369-1379
碳化硅(SiC)是典型的层状结构化合物。到目前为止,已发现了150种以上的多型体。作者曾发展了一种特殊的劳厄法可有效地鉴定碳化硅多型体。这种方法,我们发现了85种碳化硅新多型体。为了测定其中一些多型体的结构,拍摄了回摆和魏森堡照相作结构分析,但没有成功。因为这些照相中只有一些基本类型6H,15R和8H的衍射斑点而没有高层多型体的斑点,这是由于新多型体在晶体中含量很少且这些薄晶体多型体处于基本类型6H,8H,15R中间的缘故。本文提出了一种测定碳化硅多型体晶体结构的劳厄法。提出了计算劳厄斑点衍射强度的方法。对结构系列[(33)m32]3,[(33)m34]3,[(22)m23]3和[(44)m43]3多型体的结构因子Fhkl的计算方法作了简化。利用这种方法对9种碳化硅新多型体的晶体结构作了测定,其结构用z字形堆垛(Жданов符号)表示时为231R:[(33)1232]3,249R:[(33)1332]3,321R:[(33)1732]3, 339R:[(33)1832]3,237R:[(33)1234]3,417R:[(33)2234]3, 453R:[(33)2434]3,93R:[(44)343]3,261R:[(44)1043]3关键词:  相似文献   

10.
Magnetic and heat capacity measurements have been carried out on the polycrystalline Gd1−xScxNi2 solid solutions (0≤x≤1), which crystallize in the cubic C15 Laves phases superstructure (space group F4?3m). These solid solutions are ferromagnetic with a Curie temperature below 76 K. Their Curie temperature decreases from 75.4 K for GdNi2 to 13.6 K for Gd0.2Sc0.8Ni2. At high temperatures, all solid solutions, except ScNi2, are Curie-Weiss paramagnets. The Debye temperature as well as phonon, conduction electron and magnetic contributions to the heat capacity have been determined from heat capacity measurements. The magnetocaloric effect has been estimated both in terms of isothermal magnetic entropy change and adiabatic temperature change for selected solid solutions in magnetic fields up to 3 T.  相似文献   

11.
CaNb2O6:Sm3+ films were prepared on quartz glass and α-Al2O3(001) substrates by pulsed laser deposition. The structural, morphological, and optical properties of the CaNb2O6:Sm3+ films were characterized by X-ray diffraction (XRD), atomic force microscopy (AFM), emission-scan electron microscopy (SEM), Raman spectroscopy, X-ray photoelectron spectroscopy (XPS) and photoluminescence spectroscopy (PL) measurements. The results show that the structure and properties of CaNb2O6:Sm3+ films were dependent on substrates. The CaNb2O6:Sm3+ films on Al2O3(0001) substrate have better crystallinity. The full-width at half-maximum (FWHM) of (131) peak are 0.45 and 0.32 for the CaNb2O6:Sm3+ film on glass and Al2O3(001), respectively. The crystallite size of CaNb2O6:Sm3+ films grown on glass and Al2O3(001) was about 8.22 and 9.98 nm, respectively. The oxidation state of the Sm element on the films was Sm3+ state. The photoluminescence (PL) spectra were measured at room temperature, the CaNb2O6:Sm3+ films on Al2O3(001) substrate have a better PL intensity, the identified emission bands were by the intra 4f transitions of Sm3+ from the excited level to the lower levels at 567 nm for 4G5/26H5/2 transition, at 609 nm for 4G5/26H7/2 transition, and at 657 nm for 4G5/26H9/2 transition.  相似文献   

12.
The crystalline structures of martensite phases in Ni2MnGa-based ternary alloys have been studied in a wide range of temperatures and compositions transmission and scanning electron microscopy, X-ray diffraction, and electron diffraction. It is found that long-period nanostructural phases with thin-plate morphology are formed as a result of martensitic transformation in Ni2MnGa-based alloys.  相似文献   

13.
Gd2O3:Sm3+ and Gd2O3:Sm3+,Bi3+ powders were prepared by a combustion method. Their structures were determined using X-ray diffraction. UV-visible absorption and photoluminescence spectra were investigated for Gd2O3:Sm3+ and Gd2O3:Sm3+,Bi3+ at different annealing temperatures and different doping concentrations. The emission spectra of all samples presented the characteristic emission narrow lines arising from the 4G5/26HJ transitions (J=5/2, 7/2, and 9/2) of Sm3+ ions upon excitation with UV irradiation. The emission intensity of Sm3+ ions was largely enhanced with introducing Bi3+ ions into Gd2O3:Sm3+ and the maximum occurred at a Bi3+ concentration of 0.5 mol%. The relevant mechanisms were discussed with the sensitization theory by Dexter and the aggregation behavior of Bi3+ ions.  相似文献   

14.
Dy3+ and Sm3+ doped Sr5SiO4Cl6 phosphors were prepared by the modified solid state method and their luminescent properties were studied. From a powder X-ray diffraction (XRD) analysis the formation of Sr5SiO4Cl6 was confirmed. In the photoluminescence emission spectra, the Sr5SiO4Cl6:Dy3+ phosphors show efficient blue and yellow band emissions, which originates from the 4F9/26H15/2 and 4F9/26H13/2 transitions of Dy3+ ion, respectively. Photoluminescence properties of Sm3+ doped Sr5SiO4Cl6 phosphor exhibited characteristic orange-red emission coming from the intra-4f-shell 4G5/26HJ electron transitions.  相似文献   

15.
The method for carbothermal reduction of spherical particles of amorphous silicon dioxide is developed, and hexagonal α-SiC polytype nanocrystals are synthesized. The prepared samples are characterized by X-ray diffraction, Raman spectroscopy, photoluminescence spectroscopy, and electron microscopy. The silicon carbide nanocrystals prepared have sizes in the range 5–50 nm depending on the diameter of initial silicon dioxide particles. A detailed analysis of the positions of the lines in the Raman spectra, their broadening, and shift makes it possible to reliably establish that the samples under investigation predominantly contain the 6H and 4H silicon carbide polytypes and insignificant amounts of the 2H and 3C phases. The 15R and 21R polytypes in the samples are absent. It is noted that the samples are characterized by a substantial size effect: the luminescence intensity of small silicon carbide nanocrystals is more than three times higher than that of large SiC nanocrystals.  相似文献   

16.
The luminescence spectra and decay curves for the 4G5/2 level of Sm3+ ions in 55.95P2O5+14K2O+6KF+14.95BaO+9Al2O3+0.1Sm2O3 glass, referred to as PKFBASm01, have been studied as a function of pressure up to 40.5 GPa at room temperature. With the increase in pressure, a continuous red shift of the 4G5/26H9/2, 7/2, 5/2 transitions and a progressive increase in the magnitude of the crystal-field splittings for these transitions are observed. The decay curves for the 4G5/2 level of the Sm3+ ions in PKFBASm01 glass are found to exhibit single exponential behavior at ambient pressure and become non-exponential at higher pressures, accompanied by shortening of lifetimes. A generalized Yokoto–Tanimoto model has been used to explain the pressure-induced non-exponential nature of the decay curves.  相似文献   

17.
The magnetic properties and microstructure of cast and annealed Sm2Fe17−xTax (0 ≤ x ≤ 2) alloys were investigated by means of microstructural, X-ray diffraction and thermomagnetic analysis. A process for obtaining the Sm2Fe17 phase nearly free of iron in the as-cast state is described. The method consists of adding 5 at% of Ta to the melt. By this addition of Ta to the basic alloy, a two phase structure of the as-cast ingots consisting of Sm2Fe17 phase and a Pauli paramagnetic hexagonal Laves phase - TaFe2, can be obtained. X-ray diffraction showed an increase of the lattice spacing dependent upon the tantalum concentration in the alloy, which indicated some solid solubility of Ta in the Sm2Fe17 phase. Quantitative electron probe microanalysis confirmed the solid solubility of tantalum in the Sm2Fe17 phase of up to 2.3 (± 0.5) at%. This resulted in an increase of the Curie temperature of the Sm2Fe17−x phase, which was determined by means of thermomagnetic analysis.  相似文献   

18.
19.
A series of Eu2+ and Sm3+ co-doped Li2SrSiO4 phosphors are prepared by the high temperature solid-state reaction. The morphology, structure and spectroscopic properties of the prepared samples are characterized by scanning electron microscopy, X-ray diffraction, diffuse reflection spectra, photoluminescence spectra and electron paramagnetic resonance spectra, respectively. The effect of Sm3+ doping concentration on the photoluminescence intensity of the prepared samples is also investigated. The results indicate that the crystal structure of Li2SrSiO4 is not changed with the Eu2+, Sm3+ co-doping. The spherical-like particle size of the obtained product is about 20–30 nm in diameter. When the Sm3+ concentration is 0.3 mol% and the Eu2+ concentration is 0.7 mol%, the phosphors show the maximum emission intensity, which is 50% higher than that of Eu2+ doped Li2SrSiO4. Excited at 420 nm, the phosphor presents a single broad emission band peaking at 558 nm, which is ascribed to the 4f65d1 → 4f7 transitions of Eu2+ and 4G5/2 → 6H5/2 and 4G5/2 → 6H7/2 transitions of Sm3+. The Commission International de I′Eclairage chromaticity coordinates of Li2SrSiO4:0.7 mol% Eu2+, 0.3 mol% Sm3+ are x = 0.28, y = 0.28.  相似文献   

20.
A novel trivalent samarium doped SrZnV2O7 nanophosphors was developed via urea assisted solution combustion method using metal nitrates as initial raw materials. The qualitative and quantitative phase analysis was carried out using Rietveld refinement technique. It was found to crystallize in monoclinic lattice with the P121/n1 (14) space group. The photoluminescent spectral study of SrZnV2O7:Sm3+ revealed that the excitation of 405 nm yields the characteristic emission peaks at 569, 599, 640 and 702 nm due to 4G5/26H5/2, 4G5/26H7/2, 4G5/26H9/2 and 4G5/26H11/2 respectively. The optimum concentration of Sm3+ ion in SrZnV2O7 for best luminescence was found to be 2 mol%. The luminescence intensity was further enhanced by incorporating compensator charge R+ (R=Li, Na, and K) into the SrZnV2O7:0.02Sm3+ nanophosphor. The critical distance for non-radiative energy transfer was calculated to be 26.64 Å. Dipole–dipole (d–d) interactions were ascribed as the major factor responsible for concentration quenching arising from the over-doping of the activator ions. The results indicate that these nanophosphors are suitable candidate for PC-WLEDs using near UV excitation.  相似文献   

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