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1.
该文通过1 400℃固相烧结制备出Zn2+和Sn4+共取代的Y3Fe5-2xZnxSnxO12(x=0~0.35)铁氧体材料,详细研究了离子取代量对钇铁石榴石铁氧体微观结构及磁性能的影响。研究表明,Zn2+、Sn4+都进入了钇铁石榴石铁氧体的晶格中。随着离子取代量的增加,钇铁石榴石铁氧体的密度与饱和磁化强度先增大后减小;其磁损耗则先减小后增大,在x=0.25时磁损耗取得最小值。该研究进一步说明了Zn2+和Sn4+取代在一定范围内可有效降低材料的磁损耗及控制材料的饱和磁化强度。  相似文献   

2.
用固相法制备Li0.45Zn0.3Ti0.2Mn0.03Mn0.03Fe1.99O4铁氧体,研究了CaO-ZnO-B2O3(CZB)玻璃助烧剂对磁性能和结构的影响。结果表明,适量的CZB玻璃相可促进固相反应,显著降低烧结温度。通过X线衍射(XRD)和扫描电镜(SEM)分析表明,CZB玻璃没有影响LiZn铁氧体的尖晶石相结构,且其可促进晶粒生长。磁性能变化规律表明,CZB的质量分数为0.25%时,饱和磁感应强度(Bs)达最大,矫顽力(Hc)降低。Hc在质量分数为2.5%时达到最小,随后有所上升。微掺杂时,毛细管力起主导作用,少量掺杂时,液相中的扩散起主导作用,两者都促进了固相反应。过量掺杂时,玻璃相阻碍晶粒生长,各项异性场增大,导致Bs下降、Hc和铁磁共振线宽(ΔH)增大。添加CZB的LiZn铁氧体在910℃时具有较好的磁性能,可兼容低温共烧技术应用于移相器的设计。  相似文献   

3.
采用溶胶-凝胶燃烧合成法制备了Mg2+掺杂的Li-Zn铁氧体Li0.1Zn0.8MgxFe2.1-xO4(x=0,0.02,0.04,0.06,0.08).借助于TG-DSC、XRD、FT-IR、SEM和Agilent8722ET网络分析仪等表征手段,研究了样品的形成过程、晶体结构、微观形貌和电磁损耗性能.结果表明,当x≤0.06时,粉体为单一的尖晶石型锂锌铁氧体;随着掺镁量的增加,样品的晶格常数先增大后减小.掺入适量镁离子能有效调整铁氧体的微波电磁参数,当x=0.06时,在6.5 GHz 和15 GHz附近损耗角正切(tan δ)峰值达到最大(分别为0.11和0.54),此时微波电磁损耗最佳.利用微波电磁理论分析了电磁参数的变化机理.  相似文献   

4.
采用传统固相法制备Nd2O3掺杂富钛型(Ba0.75Sr0.25) Ti1+xO3(x为摩尔比)陶瓷,通过扫描电镜及LCR测试系统,研究不同x值、Nd2O3掺杂量及烧结工艺对钛酸锶钡基陶瓷微观结构与介电性能的影响。结果表明,随着x值及Nd2O3掺杂量增大,陶瓷试样均出现柱状第二相。当x=0.01且w(Nd2O3)=0.4%时,陶瓷试样经1 250 ℃烧结2 h后,其室温相对介电常数(εr)高达8.67×103,介电损耗(tan δ)仅为7.87×10-3。随着x值及Nd2O3掺杂量增大,陶瓷的居里峰显著移动。  相似文献   

5.
采用传统固相反应法制备Li2+xZnTi3O8+0.5x微波介质陶瓷,研究了A位Li的非化学计量比对Li2+xZnTi3O8+0.5x陶瓷的烧结特性、相结构及微波介电性能的影响。结果表明:随着Li2+xZnTi3O8+0.5x(x=–0.2~+0.2)陶瓷中Li含量的逐渐增加,TiO2相逐渐消失,陶瓷的致密度逐渐升高,介电常数逐渐降低,Q.f值先上升再下降,谐振频率温度系数逐渐降低,然后保持不变。当x=–0.05时,Li1.95ZnTi3O7.975陶瓷取得最佳的综合微波介电性能:εr=26.41,Q.f=65 200 GHz,τf=–4.16×10–6/℃。  相似文献   

6.
采用固相反应烧结法制备了铁氧体材料Y_(3-x)Nd_xFe_5O_(12)(0≤x≤2),研究了不同烧结温度和Nd~(3+)掺杂量对样品微观结构和磁性能的影响。发现在Nd~(3+)掺杂量相同的情况下,样品密度随烧结温度的升高而升高,最终在1340℃接近饱和;晶格常数随着Nd~(3+)掺杂量的增加而增大,当x>1.5时,样品出现杂相;饱和磁化强度随着Nd~(3+)掺杂量的增加先增大后减小,x=1时,样品的饱和磁化强度达到最大值31.9 A·m~2·kg~(–1)。  相似文献   

7.
通过固相烧结法结合半化学法制备了ZnO-(1-x)TiO2-xSnO2(x=0.04~0.20)陶瓷,掺杂1.0%3V2O5(质量分数)-B2O3降低陶瓷的烧结温度,研究了B位取代对ZnTiO3相结构及介电性能的影响。结果表明,Sn的加入促进了六方相分解,形成了立方尖晶石结构的固溶相Zn2(Ti1-xSnx)O4;随烧结温度升高,Sn的固溶量增加,900℃时,最大固溶量为0.08 mol。900℃烧结试样,随x增加,其介电常数ε先增大后减小,而介电损耗tanδ恰好相反,先减小后增大,当x=0.12时,得到ε的最大值(ε=29)和tanδ的最小值(tanδ=9.86×10-5)。900℃烧结的具有优良介电性能的ZnO-(1-x)TiO2-xSnO2(x=0.04~0.20)陶瓷有很好的实际应用前景。  相似文献   

8.
为研制适用于915 MHz RFID天线小型化应用需要的磁介基板材料,采用固相反应烧结法研究了H3BO3掺杂对(Ba0.5Sr0.5)3Co2Fe24O41铁氧体微观形貌和磁介性能的影响。通过研究发现,H3BO3掺杂能很好地促进Co2Z铁氧体的低温烧结成相。同时,H3BO3掺杂也有利于抑制Co2Z铁氧体晶粒生长。随着H3BO3掺杂量的增多,材料体系的磁导率持续下降,而介电常数先上升后下降。当掺杂H3BO3的质量分数为4%,材料体系在915MHz时可获得磁导率为2.45,介电常数为10.41,磁损耗正切为0.057,介电损耗正切为0.005的综合磁介性能。  相似文献   

9.
采用固相法制备了(Ba0.85Ca0.15)(Ti0.92Zr0.08)O3-x%Co2O3(BCTZ-xCo,x=01.4)无铅压电陶瓷。研究了不同Co掺杂量对该陶瓷的显微结构、介电性能及压电性能的影响。结果表明,所有样品均具有单一的钙钛矿结构,随Co2O3含量的增加,晶粒尺寸逐渐细化减小,介电常数εr、压电常数d33、平面机电耦合系数kp均呈下降趋势。机械品质因数Qm显著增大,当x=0.7时,具有最佳的综合电性能,其中d33=392pC/N,kp=46.0%,Qm=435,介电损耗tanδ=0.62%,表明BCTZ-xCo陶瓷材料是一种具有应用前景的无铅压电材料。  相似文献   

10.
采用传统固相法制备了Ca1-xBaxCu3Ti4O12(x=0, 0.005, 0.010, 0.020, 0.030, 0.040, 0.050, 0100,摩尔分数) 陶瓷。用X线衍射仪、扫描电子显微镜、介电温谱测试系统及阻抗测试仪研究了Ba2+掺杂量的变化对Ca1-xBaxCu3Ti4O12陶瓷的相结构、微观形貌及电性能影响。研究结果表明,随着Ba2+掺杂量的增加,陶瓷试样产生了第二相CuO,同时Ba2+掺杂使CaCu3Ti4O12的晶格常数增大。Ca1-xBaxCu3Ti4O12陶瓷的晶粒尺寸随Ba2+掺杂量的增加而减小,气孔率随之降低。掺杂适量的Ba2+可有效降低CaCu3Ti4O12陶瓷的介电损耗,也可降低相对介电常数随温度的变化率。一定量的Ba2+掺杂还能增加CaCu3Ti4O12的晶界电阻。  相似文献   

11.
A detailed theoretical study of the electronic structure, optical, elastic and thermodynamics properties of jadeite have been performed by means of the first principles based on the state-of-the-art of density functional theory within the generalized gradient approximation. The optimized lattice constants and the atomic positions are in good agreement with experimental data. The total density of states and partial density of states of jadeite have been discussed. The energy gap has been calculated along the Γ direction found to be 5.338 eV, which shows that jadeite has wide direct band gap. The optical properties, such as the dielectric function, refractive index, extinction coefficient, reflectivity coefficient, loss function and absorption coefficient for [100] and [001] directions have been described for the first time in the energy range 0–40 eV. The elastic constants, bulk modulus, Young׳s modulus, anisotropic factor and Poisson׳s ratio have been calculated. Furthermore, the Vickers hardness and Debye temperature of jadeite have been predicted. The calculated values of all above parameters are compared with the available experimental values.  相似文献   

12.
The cubic BiGaO3 and BiInO3 perovskite oxides have been investigated for their structural stability, mechanical and opto-electronic properties by employing the density functional theory. The exchange-correlation effects have been modeled with Perdew–Burke–Ernzerhof generalized gradient approximation, while the improved evaluation of electronic properties has been achieved by using the Tran–Blaha modified form of semi-local Becke–Johnson functional. Structural properties are calculated and the thermodynamics stability of BiGaO3 and BiInO3 in the cubic perovskite structure has been established in terms of enthalpies of formation. Furthermore, elastic coefficients such as Cij, bulk modules B, anisotropy factor, shear modulus G, Young’s modulus Y, Poisson’s ratio ν, and B/G ratio are predicted. Band structure calculations reveal that investigated compounds have an indirect band gap between the occupied O 2p and unoccupied Bi 6p orbitals. The optical response of BiGaO3 and BiInO3 are also inspected by computing the complex dielectric function, refractive index, absorption coefficient, extinction coefficient, reflectivity and optical conductivity for radiation with energy up to 16 eV. The important thermoelectric properties of the compounds are described in terms of thermal conductivity, electrical conductivity, Seebeck coefficient and figure of merit.  相似文献   

13.
正Effect of rhenium doping is examined in single crystals of MoSe_2 viz.MoRe_(0.005)Se_(1.995), MoRe_(0.001)Se_(1.999) and Mo_(0.995)Re_(0.005)Se_2,which is grown by using the direct vapor transport(DVT) technique. The grown crystals are structurally characterized by X-ray diffraction,by determining their lattice parameters a and c,and X-ray density.Also,the Hall effect and thermoelectric power(TEP) measurements show that the single crystals exhibit a p-type semiconducting nature.The direct and indirect band gap measurements are also undertaken on these semiconducting materials.  相似文献   

14.
Nanocrystalline CdO thin films were prepared onto a glass substrate at substrate temperature of 300 °C by a spray pyrolysis technique. Grown films were annealed at 250, 350, 450 and 550 °C for 2.5 h and studied by the X-ray diffraction, Hall voltage measurement, UV-spectroscopy, and scanning electron microscope. The X-ray diffraction study confirms the cubic structure of as-deposited and annealed films. The grain size increases whereas the dislocation density decreases with increasing annealing temperature. The Hall measurement confirms that CdO is an n-type semiconductor. The carrier density and mobility increase with increasing annealing temperature up to 450 °C. The temperature dependent dc resistivity of as-deposited film shows metallic behavior from room temperature to 370 K after which it is semiconducting in nature. The metallic behavior completely washed out by annealing the samples at different temperatures. Optical transmittance and band gap energy of the films are found to decrease with increasing annealing temperature and the highest transmittance is found in near infrared region. The refractive index and optical conductivity of the CdO thin films enhanced by annealing. Scanning electron microscopy confirms formation of nano-structured CdO thin films with clear grain boundary.  相似文献   

15.
为了提高 SnO_2-LiZnVO_4系湿敏材料的性能,采用共沉淀法制备出 SnO_2-K_2O-LiZnVO_4系纳米湿敏粉体。考察了液相掺杂 K+对材料湿敏性能、复阻抗特性和电容特性的影响。实验结果表明,采用共沉淀法制备纳米粉体并使K+液相掺杂量为 2.5%(摩尔分数),可使湿敏材料低湿电阻小、灵敏度适中,适当的 K+添加量可明显改善 SnO_2-LiZnVO_4系纳米材料的感湿特性。  相似文献   

16.
Effect of rhenium doping is examined in single crystals of MoSe2 viz. MoRe0.005Se1.995, MoRe0.001Se1.999 and Mo0.995Re0.005Se2, which is grown by using the direct vapor transport (DVT) technique. The grown crystals are structurally characterized by X-ray diffraction, by determining their lattice parameters a and c, and X-ray density. Also, the Hall effect and thermoelectric power (TEP) measurements show that the single crystals exhibit a p-type semiconducting nature. The direct and indirect band gap measurements are also undertaken on these semiconducting materials.  相似文献   

17.
18.
Nanocrystalline Zn1-x CoxO(where x varies from 0 to 0.04 in steps of 0.01) thin films were deposited onto glass substrate by the spray pyrolysis technique at a substrate temperature of 350 ℃. The X-ray diffraction patterns confirm the formation of hexagonal wurtzite structure. The crystal grain size of these films was found to be in the range of 11–36 nm. The scanning electron micrographs show a highly crystalline nanostructure with different morphologies including rope-like morphology for undoped ZnO and nanowalls and semispherical morphology for Co-doped Zn O. The transmittance increases with increasing Co doping. The optical absorption edge is observed in the transmittance spectra from 530 to 692 nm, which is due to the Co2C absorption bands corresponding to intraionic d–d shifts. The direct and indirect optical band gap energies decrease from 3.05 to 2.75 eV and 3.18 to 3.00 eV, respectively for 4 mol% Co doping. The electrical conductivity increases with increasing both the Co doping and temperature, indicating the semiconducting nature of these films. The temperature dependence thermal electromotive force measurement indicates that both undoped and Co-doped ZnO thin films show p-type semiconducting behavior near room temperature. This behavior dies out beyond 313 K and they become n-type semiconductors.  相似文献   

19.
Manganese indium sulphide (MnIn2S4) thin films were deposited using an aqueous solution of MnCl2, InCl3 and (NH2)2CS in the molar ratio 1:2:4 by simple chemical spray pyrolysis technique. The thin film substrates were annealed in the temperature range between 250 and 350 °C to study their various physical properties. The structural properties as studied by X-ray diffraction showed that MnIn2S4 thin films have cubic spinel structure. The formation of cube and needle shaped grains was clearly observed from FE-SEM analysis. The energy dispersive spectrum (EDS) predicts the presence of Mn, In and S in the synthesized thin film. From the optical studies, it is analyzed that the maximum absorption co-efficient is in the order between 104 and 105 cm−1 and the maximum transmittance (75%) was noted in the visible and infrared regions. It is noted that, the band gap energy decreases (from 3.20 to 2.77 eV) with an increase of substrate temperature (from 250 to 350 °C). The observations from photoluminescence studies confirm the emission of blue, green, yellow and red bands which corresponds to the wavelength range 370–680 nm. Moreover, from the electrical studies, it is observed that, as the substrate temperature increases the conductivity also increases in the range 0.29–0.41×10−4 Ω−1 m−1. This confirms the highly semiconducting nature of the film. The thickness of the films was also measured and the values ranged between 537 nm (250 °C) to 483 nm (350 °C). This indicates that, as the substrate temperature increases, the thickness of the film decreases. From the present study, it is reported that the MnIn2S4 thin films are polycrystalline in nature and can be used as a suitable ternary semiconductor material for photovoltaic applications.  相似文献   

20.
Structural, electrical, and optical properties of undoped and Zn doped lead sulfide (PbS) thin films are benign reported in this paper. The subjected films were grown on glass substrates at 25 °C by a chemical bath deposition (CBD) method. The concentration of Zn in the deposition bath represented by the ratio [Zn2+]/[Pb2+] was varied from 0% to 5%. It was found that the film׳s grains decreased in size with increasing Zn content in the film. XRD data showed the polycrystalline nature of the film its crystal orientation peak intensities decreased with higher doping concentration of Zn. Atomic force microscopy (AFM) measurements revealed that the surface roughness of the films decreased due to zinc doping as well. However, with increasing of the dopant concentration from 0% to 5%, the average transmittance of the films varied over the range of 35–75%. The estimated optical band (Eg) gaps of undoped and Zn doped PbS thin films were in the range of 0.72–1.46 eV. Hall Effect measurements electrical resistivity, carrier concentration and Hall mobility have been determined for the titled film as functions on the Zn content within the film׳s textures. The overall result of this work suggested that the Zn:PbS film is a good candidate as an absorber layer in the modern solar cell devices.  相似文献   

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