La掺杂Ni0.5Zn0.5FeO4铁氧体的制备与微波吸收性能

采用高分子凝胶法制各了Ni0.5Zn0.5LaxFe2-xO4(x=0,0.05,0.1)铁氧体,采用XRD,TEM和HP8510网络分析仪对其结构、形貌、电磁和微波吸收性能进行了研究.结果表明,当煅烧温度为600℃时,立方晶系尖晶石结构的Ni0.5Zn0.5La0.05Fe1.95O4相初步形成,La在尖晶石结构中固溶量有限.与Ni0.5Zn0.5Fe2O4铁氧体相比,掺杂La的Ni-Zn铁氧体的tanδm值降低,tanδε滥升高.与Ni0.5Zn0.5Fe2O4铁氧体相比,x=0.1样品的吸波性能降低,而x=0.05样品的吸波性能提高,其电磁波反射率小于-10 dB的频宽可达2.7 GHz,最小反射率为-15.6 dB.     

铈掺杂镍锌铁氧体的制备与性能研究

用高分子凝胶法制备了稀土元素铈掺杂的镍锌铁氧体粉Ni0.5Zn0.5CexFe2-xO4,并对产物结构和电磁性能进行了表征。结果表明,当Ce3+的掺杂摩尔数x为0.1时,800℃煅烧后会形成立方晶系尖晶石结构的镍锌铁氧体晶相。与Ni0.5Zn0.5Fe2O4铁氧体相比,在8.2~12.4 GHz频率范围内掺杂铈元素的Ni0.5Zn0.5Ce0.1Fe1.9O4铁氧体的tanδm值降低,而其tanδe值升高,平均值可达0.527。     

溶胶-凝胶法制备镍锌铁氧体及其电磁损耗性能

以Zn(NO3)2×6H2O, Ni(NO3)2×6H2O, Fe(NO3)3×9H2O及柠檬酸为原料,采用溶胶-凝胶法制备前驱体,在1200℃下对其煅烧3 h,合成了NixZn1-xFe2O4(x=0, 0.3, 0.5, 0.7)铁氧体. 产品表征结果表明,所有NixZn1-xFe2O4均属立方晶系尖晶石结构,结晶完整,在580 cm-1附近均具有铁氧体的红外吸收特征峰,晶粒大小均在100 nm左右. 在0.2~1.8 GHz测试频率范围内,Ni0.7Zn0.3Fe2O4和Ni0.5Zn0.5Fe2O4铁氧体对电磁波的吸收损耗性能相对较好,Ni0.7Zn0.3Fe2O4的电磁损耗角正切值tgd为0.67~1.59, Ni0.5Zn0.5Fe2O4为0.37~1.51,随Ni含量增加,其电磁损耗逐渐增强.     

尖晶石型锰锌铁氧体的电子结构和磁性的计算与实验研究(英文)

采用基于密度泛函理论的第一性原理平面波超软赝势法,计算了尖晶石型Zn1-xMnxFe2O4(x=0,0.5,1)铁氧体的电子结构和磁性,计算结果表明:ZnFe2O4铁氧体为绝缘体,MnFe2O4和Zn0.5Mn0.5Fe2O4铁氧体为半金属,ZnFe2O4铁氧体的能隙为0.89eV,小于实验值。此外,计算研究了Zn1-xMnxFe2O4(x=0,0.5,1)铁氧体中Zn的含量对其磁性的影响。结果表明,随着Zn含量的增加Zn1-xMnxFe2O4(x=0,0.5,1)铁氧体的磁矩先增大后减小,这与实验结果一致。     

Co0.5Zn0.5Fe2O4/PANI复合物的制备及其电磁性能

采用水热法制备尖晶石结构的Co0.5Zn0.5Fe2O4纳米颗粒,再采用原位聚合法制备Co0.5Zn0.5Fe2O4/聚苯胺(PANI)复合物,对其结构及电磁性能进行了表征. 结果表明,复合物中Co0.5Zn0.5Fe2O4与PANI之间存在键的作用;在频率2~18 GHz范围内,与纯Co0.5Zn0.5Fe2O4相比,复合物的介电常数实部与虚部均增大,磁导率的实部与虚部均减小;复合物的最大吸收峰比纯Co0.5Zn0.5Fe2O4明显提高,最大吸收峰在频率11~13 GHz范围内约为15 dB.     

掺杂的Ni-Zn铁氧体磁性材料的制备与性能

以分析纯Fe2O3,NiO,ZnO,Al2O3,Pr6O11和WO3为原料,以Ni0.5Zn0.5MxFe2–xO4(M=Al,Pr,W;x=0～0.04)为基本配方,采用一步合成法制备了Ni–Zn铁氧体陶瓷,研究了掺杂对Ni–Zn铁氧体相组成、显微形貌和电磁性能的影响。结果表明:掺杂Al3+,Pr3+和W6+的Ni–Zn铁氧体均能形成结晶完好的尖晶石相结构。材料致密,无晶粒异常长大。适当的金属阳离子替代可有效降低材料的磁损耗和介电损耗,提高截止频率,同时使铁氧体保持较高初始磁导率,高饱和磁化强度,高Curie温度等优良性能,从而制得高性能大功率高频Ni–Zn系铁氧体磁芯。     

尖晶石型铁氧体Cu_xZn_(1-x)Fe_2O_4(x=0~0.5)的制备及光催化性能的研究

采用溶胶-凝胶法制备了尖晶石型铁氧体Cu x Zn1-x Fe2O4。利用XRD,SEM对纳米颗粒的结构、形貌进行了表征。结果表明,所合成的样品为尖晶石型铁氧体,形貌呈规则颗粒,随着Cu掺杂量的增加可使样品粒径减小。通过对甲基橙的降解情况对其光催化活性进行了研究。结果表明,经过Cu2+掺杂可加快甲基橙降解速率,少量掺杂的Cu x Zn1-x Fe2O4样品,光催化活性可以提高。     

不同稀土Nd3+掺杂含量对锰锌铁氧体吸波性能的影响

采用水热合成法制备出锰锌稀土复合铁氧体Mn0.4Zn0.6NdxFe2-xO4(x=0,0.03,0.06,0.09),以X射线衍射仪(XRD),矢量网络分析仪(VNA)和透射电子显微镜(TEM)为表征手段,研究不同稀土Nd3+掺杂含量对锰锌铁氧体微观结构及吸波性能的影响.实验表明:当掺杂量x=0.03时,制备的样品纯相单一,具有类球形结构,反射损耗值最低为-8.36 dB.随着Nd3+含量的不断增加,晶格常数减小,反射损耗值逐渐增大,样品的吸波性能不佳,说明掺杂适量的Nd3+能够提高材料的吸波性能.     

溶胶-凝胶法制备Zn(0.5-x)Mg(0.5-x)Ca2xFe2O4铁氧体超微粉

利用柠檬酸前驱物溶胶-凝胶法合成了掺杂Ca的尖晶石型纳米晶铁氧体Zn(0.5-x)Mg(0.5-x)Ca2xFe2O4(x为0～0.25),表征了其结构性能与电磁特性.结果表明:掺杂Ca对Zn(0.5-x)Mg(0.5-x)Ca2xFe2O4的磁化强度和矫顽力均有影响.     

尖晶石型铁氧体CoFe_（2-x）Ni_xO_4（x=0.1～0.5）结构及光催化性能的研究

采用溶胶-凝胶法制备了铁氧体CoFe2-xNixO（4x=0.1~0.5）系列样品。利用XRD,SEM对纳米颗粒的结构、形貌进行了表征。结果表明,所合成的样品为尖晶石型,呈圆球状,粒径均匀,直径约为50nm。通过甲基橙的降解情况对其脱色率进行了研究。结果表明,经过B位Ni2＋掺杂的CoFe2-xNixO（4x=0.1~0.5）系列样品,其脱色率明显提高。     

The influence of Nd substitution in Ni–Zn ferrites for the improved microwave absorption properties

Nanocrystalline Ni–Zn ferrites with different neodymium contents (Ni_0.5Zn_0.5Nd_xFe_2-xO₄) were synthesized by sol-gel route combined with self-propagating combustion (SPC) method. The presence of surface functional groups, crystal structure and morphology of the samples were studied by FT-IR, XRD and SEM. The results show that the prepared samples are composed of spinel phase under the condition of low neodymium content, like the pure Ni–Zn ferrite. While neodymium oxide appears after the content of Nd³⁺ exceeds a certain limit (x > 0.04) and there exist two phases in the ferrite. The results of vibrating sample magnetometer (VSM) and vector network analyzer (VNA) show that adjusting the content of Nd is significant in improving the dielectric properties and microwave absorption capacity of the materials, specifically at low frequencies. When x < 0.04, the enhancement of dielectric loss ability of spinel ferrites by doping Nd³⁺ is the dominant factor affecting microwave absorption ability of samples. The secondary phase Nd₂O₃ hardly appears under this condition, thus the weakening effect of Nd³⁺ addition on magnetic loss ability is not obvious. When x = 0.04, the optimal absorption peak of the material reaches −20.8 dB at 4.4 GHz with a thickness of 8.5 mm and the effective absorption bandwidth (R_L < −10 dB) was 3.2 GHz. On the contrary, when x > 0.04, the magnetic loss ability decreases rapidly (e.g., Ms decreases from 82.47 emu/g to 59.77 emu/g). Meanwhile, the dielectric loss increases slowly and the microwave absorption capacity decreases.     

Structural,spectral, dielectric and magnetic properties of Ni0.5MgxZn0.5-xFe2O4 nanosized ferrites for microwave absorption and high frequency applications

Ni_0.5Mg_xZn_0.5−xFe₂O₄ (x=0, 0.1, 0.2, 0.3, 0.4 and 0.5) (NiMgZn) nano-sized ferrites were synthesized via sol-gel route. The average cation radius, bond lengths (A and B sites), shared (d_AE, d_BE) and unshared edges (d_BEU) of the NiMgZn nanoferrites were determined from the XRD data. FTIR studies confirmed the spinel structure of NiMgZn nanoferrites. The force constant at tetrahedral and octahedral sites were calculated. The surface morphology was investigated from the micrographs. The dielectric parameters such as dielectric constant, dielectric loss factor, loss tangent and Q values with different concentration of Mg in NiZn nanoferrite were evaluated. It was found that the NiMgZn sample at x=0.5 showed high Q values with low dielectric losses at higher frequencies. The squareness ratio and coercivity values confirmed the super paramagnetic behaviour of the NiMgZn nano-sized ferrites. However, the saturation and remanence increased with the increasing Mg contents whereas coercivity values follow the Stoner-Wolforth model for NiMgZn at x=0, 0.2, 0.3 and 0.4. The NiMgZn nano-sized ferrites samples at x=0.1 and 0.5 show the variations in coercivity values which may be due to the strong LS coupling and super-exchange interactions of the metal cations at tetrahedral and octahedral sites. The dielectric and magnetic studies of NiMgZn nano-sized ferritesexplored their application in various technological and industrial fields such as magnetic storage, microwave absorption and high frequency applications.     

Ba1-3x/2Lax(Mg1/3Ta2/3)O3陶瓷的微波介电性能

采用固相合成法制备了Ba1-3x/2Lax(Mg1/3Ta2/3陶瓷,研究了La掺杂对钽镁酸钡的结构和微波介电性能的影响.结果表明:A位取代能改进其烧结性能.在x≤0.02时,烧结样品为单相的钙钛矿结构,B位离子1:2有序;当x>0.02时出现第二相Ba0.5TaO3.B位离子有序度随着x的增大先增加后减小,在x=0.04时出现最大值.x≤0.02时介电常数变化较小,而后其值逐渐增大.品质因数与谐振频率的乘积(Q×f)值随着x的增大先增大后减小,在x=0.02时取得最大值;谐振频率温度系数(τf)值随着x增大而增大.     

Preparations and characterizations of Ca doped Ni–Mg–Mn nanocrystalline ferrites for switching field high-frequency applications

Ca-doped Ni–Mg–Mn spinel ferrites with compositions of Ni_0·5Mg_0·3Mn_0.2Ca_xFe_2-xO₄ (x = 0, 0.1, 0.2, 0.3, 0.4, 0.5) were prepared via sol-gel auto-ignition technique. TGA/DTA, FTIR, XRD, FESEM, and VSM were employed to evaluate the thermal, spectral, structural, morphological, and magnetic features of Ca-doped Ni–Mg–Mn spinel ferrites. TGA/DTA curves show the weight loss in the sample. This weight loss was attributed to the oxidation and decomposition of the sample contents at a temperature of 500 °C. XRD reveals a single-phase structure of the Ni–Mg–Mn nano ferrites. A single-phase orthorhombic structure was confirmed for Ca-doped Ni–Mg–Mn ferrites. Structural parameters such as lattice parameter, ‘da’, ‘db’, ‘dc’, and ‘dv’ were evaluated using unit cell software. The absorption peaks at 427 to 538 cm^?1 confirmed the spinel structure, which was evaluated using FTIR. FESEM analyses showed that the agglomerations increased with the doping of Ca in Ni–Mg–Mn ferrites. Remanence, Y–K angles, saturation, coercive force, magnetic squareness, magnetic moment, and anisotropy constant were determined for Ca-doped Ni–Mg–Mn spinel ferrite samples. It is noticed that saturation increases from 29.157 to 51.322 emu/g, whereas remanence increased from 5.34 to 9.40 emu/g, respectively. The permeability, anisotropy constant, and magnetic moments were also found to increase with Ca doping. However, the Y–K angles increased with Ca concentration in Ni–Mg–Mn nano ferrites. In addition, the switching field distribution (SFD) and high-frequency response of all the Ca-doped Ni–Mg–Mn samples were also evaluated. Ca-doped Ni–Mg–Mn samples are suggested to be suitable for switching, filters, inductors, and microwave absorption applications because of the superparamagnetic nature of the prepared spinel ferrites.     

Synthesis of La-doped NiO nanofibers and their electrochemical properties as electrode for supercapacitors

La-doped NiO nanofibers were synthesized by the electrospinning method. The X-ray diffraction (XRD) pattern showed that La doping does not change the crystal structure up to the doping ratio of La/Ni=1.5%. Electrochemical properties of La-doped NiO nanofibers were investigated using cyclic voltammetry and galvanostatic charge/discharge. The results showed that the La doping can enhance the charge/discharge specific capacitance and electrochemical stability of the NiO nanofibers. Especially, the sample with doping ratio of La/Ni=1.5% could reach a discharge specific capacitance of 94.85 F g⁻¹ at a constant current density of 5 mA cm⁻².     

Structural evolution,sintering behavior and microwave dielectric properties of Al(1-x)(Si0.5Zn0.5)xPO4 ceramics

Al_(1-x)(Si_0.5Zn_0.5)_xPO₄ (0 ≤x≤0.6) ceramics were prepared via solid state reaction process. Their structural evolution, sintering behavior and microwave dielectric properties were investigated by X-ray diffraction (XRD), scanning electron microscopy (SEM) and with a network analyzer. Phase pure AlPO₄ could not be obtained for the undoped composition. However, microscopically homogeneous single phase solid solution formed within the compositional range of 0 < x ≤ 0.05. Immiscibility with two-phase structure within apparently single phase solid solution could be observed for other doped compositions (0.1 ≤ x ≤ 0.6). Small level of doping with (Si_0.5Zn_0.5)³⁺ (x≤0.4) stabilized the orthorhombic cristobalite-like AlPO₄ (C-AlPO₄) phase; while further doping led to the transformation from orthorhombic α-C-AlPO₄ into cubic β-C-AlPO₄ phase. The doping with (Si_0.5Zn_0.5)³⁺ considerably improved the sinterability and reduced the sintering temperature to ?900 °C when x = 0.6. The dielectric permittivity slightly increases and the Q × f value decreases with the increasing doping concentration. All composition demonstrate low permittivity (?_r ?4) and negative value of τ_f. Good combined microwave dielectric properties with ?_r ?3.9, Q × f?25,000 GHz and τ_f ? -25 ppm/^oC could be obtained for the x = 0.2 composition after sintering at 1200 °C/2h.     

Co取代对Nd(Zn0.5Ti0.5)O3微波介质陶瓷结构与性能的影响

采用传统固相法制备Nd[(Zn1?xCox)0.5Ti0.5]O3 (0≤x≤0.9)微波介质陶瓷,研究Co2+在B位取代Zn2+对Nd(Zn0.5Ti0.5)O3微波介质陶瓷的结构和微波介电性能的影响. 结果表明,在研究的组分范围内,Nd[(Zn1?xCox)0.5Ti0.5]O3陶瓷均能形成单斜钙钛矿型固溶体,随Co取代量增加,陶瓷的相对介电常数?r逐渐减小,谐振频率温度系数?f逐渐向负值移动,品质因数Q×f先增大后下降,在x=0.3 mol时达到最大值215130 GHz, Q×f大幅增加是有序度作用所致. 在1410℃下烧结4 h, Nd[(Zn0.7Co0.3)0.5Ti0.5]O3陶瓷具有优异的微波介电性能,?r=31.2, Q×f=215130 GHz, ?f=?35.7×10?6℃?1.