Na3La2(BO3)3:Sm3+的合成及其光谱特性

本文采用固相反应法,合成了一系列掺Sm^3 的Na3La2(BO3)2[Na3(La1-xSmx)2(BO3)3]发光,X－射线粉末衍射数据分析表明它们属于正交晶系,空间群为Amm2,测量了红外光谱,荧光光谱,观察到在599nm,645nm处有较强的荧光发射,并研究了发光强度与Sm^3 离子浓度（x)的关系,确定了Sm^3 离子在Na3La2(BO3)3基质中发光的适宜浓度。     

Structural,dielectric and magnetic properties of cobalt based spinel ferrites

CoYb_xFe_2-xO₄ (x = 0.00, 0.025, 0.05, 0.075, 0.10) spinel ferrites were synthesized by co-precipitation technique. Structural, dielectric and magnetic properties were measured. X-ray diffraction analysis showed that all the prepared spinel ferrites possessed cubic spinel structure. Dielectric constant, AC conductivity and dielectric loss decreased with the addition of rare earth ions. The impedance analysis explained the role of grains and grain boundaries with in prepared samples. Cole-Cole plots helped to measure the values of grains and grain boundary's resistance. The magnetic properties proved the soft nature of these ferrites. Saturation magnetization and remanence decreased while coercivity was enhanced with the addition of ytterbium concentration. All these parameters suggested that these prepared samples might be suitable for high frequency applications.     

Magnetic properties of rare earth ion (Sm) added nanocrystalline Mg-Cd ferrites, prepared by oxalate co-precipitation method

Nanocrystalline ferrite powder having the general formula Mg_1−xCd_xFe₂O₄+5% Sm³⁺ (x=0, 0.2, 0.4, 0.6, 0.8 and 1.0) was synthesized by chemical oxalate co-precipitation technique. The synthesized powder was characterized by X-ray, IR and SEM techniques. The XRD analysis confirms cubic spinel phase with orthoferrite secondary phase. The lattice constant increases with increase in Cd²⁺ content (x). It is smaller than that for pure Mg-Cd ferrites. The average crystallite size lies in the range 28.69-32.66 nm. Saturation magnetization and magnetic moment increase with cadmium content up to x=0.4 and decrease thereafter. This is attributed to the existence of localized canted spin. The decrease in saturation magnetization and magnetic moment beyond x=0.4 is due to the presence of triangular spin arrangement on B-site. Coercivity and remanent magnetization decrease while Y-K angles increase with Cd²⁺ content. The Sm³⁺ addition improves the magnetic properties.     

Eu~(3+)作探针研究铋铕共掺硼硅酸盐玻璃光学特性

利用高温烧结法制备了铕/铋铕共掺硼硅酸盐玻璃系列样品,测量了样品的激发光谱、发射光谱和声子边带谱,利用Eu3+离子作为探针进一步研究了敏化剂Bi3+的掺入对Eu3+发光的影响.结果表明:本文制作的玻璃样品的电子-声子耦合系数比以往报道过的硼铅等玻璃材料的值都要小,但在硼硅酸盐玻璃中掺入Bi3+会使Eu3+的无辐射跃迁概率增加;Bi3+对Eu3+有敏化作用,Bi3+的掺入使材料的共价性增强,对称性降低,这又使得Eu3+的发光整体变强.所以,在硼硅酸盐玻璃体系中,Eu3+发光的增强不仅仅是由于Bi3+对Eu3+的能量传递,而是以上各因素综合作用的结果.     

染料敏化太阳能电池Eu~(3+),Sm~(3+)掺杂TiO_2下转换光阳极的制备及性能

用溶胶-凝胶法制备了Eu,Sm共掺TiO_2粉体,将其与P25复合,制备了下转换光阳极,用于染料敏化太阳能电池,利用其下转换特性提高电池的光电性能.用荧光光谱对粉体的发光性能进行表征,荧光光谱显示:Eu,Sm共掺TiO_2粉体受463nm光激发可以发射550~700nm的可见光,具有下转换功能.当Eu~(3+)的摩尔掺杂含量为1%,Sm~(3+)的摩尔含量为0.5%时,制备的Eu~(3+),Sm~(3+)共掺下转换光阳极,短路电流达到14.08mA/cm2,与使用Eu~(3+)掺杂TiO_2的下转换光阳极电池相比,提高了32.08%,转换效率也达到5.29%.     

Sm3+掺杂稀土硼酸盐玻璃的光谱参数计算和荧光光谱分析

制备了具有高效可见荧光发射的Sm3 掺杂稀土硼酸盐(LBLB)玻璃,对玻璃的吸收和荧光光谱展开了测试与分析.根据Judd-Ofelt理论对吸收光谱进行了拟合,求得Sm3 离子的晶场调节参数Ωt=(2,4,6)分别为6.81×10-20,4.43×10-20和2.58×10-20 cm2,并进一步计算出各能级跃迁的谱线强度、自发辐射跃迁概率、辐射寿命和荧光分支比等光谱参数.紫外光激发下,Sm3 掺杂LBLB玻璃发出明亮的橙红色光.激发光谱表明,氩离子激光器是Sm3 掺杂LBLB玻璃有效的激发光源.     

Effect of Ca substitution on structural,magnetic and dielectric properties of BiFeO3

Bi_1-xCa_xFeO₃ (x = 0.40, 0.50) compounds are synthesized by conventional solid-state reaction method. The effect of Ca²⁺ substitution is investigated on structural, dielectric and magnetic properties. Rietveld refinement confirms that crystal structures of both the samples are tetragonal with P4mm symmetry. The highest values of remnant magnetization (M_r ) and coercive field (H_c ) are 0.002 emu/g and 0.23 kOe, respectively, for x = 0.50. The electric modulus formalism is used to distinguish and separate out the relaxation process which is dominated by the transport phenomenon. The relaxation process has activation energy ～0.32 eV which is found to be related to both the hopping mechanisms, i.e. electronic and oxide ions.     

X-ray and dielectric studies of Sm2(MoO4)3

The polycrystalline samples of Sm₂(MoO₄)₃ have been prepared by heating appropriate quantities of oxides. The X-ray powder diffraction technique has been used to provide information about lattice parameter, space group and basic structure. The dielectric constant has been measured as a function of frequency (560 Hz-13 MHz) and temperature (30–220°C) to know the ferroelectric transition temperature.     

Cr~(3+)离子在Na_2MgAlF_7中的发光

实验考查了Cr~(3+)离子在Na_2MgAlF_7多晶粉末中的发光特性。~4T_2能级的发光复盖近红外的700nm至1050nm的宽阔谱域。77K时,荧光寿命为310μs,荧光衰减曲线稍偏离单指数式。在200K以上发生较严重的温度猝灭。荧光谱表现出一些结构,对此做了讨论。     

Crystal field effects on the saturation magnetic moment of Sm3+ ion in ferronagnetic samarium compounds

The effects of cubic crystal fields on the saturation magnetic moment of Sm³⁺ ion in ferromagnetic compounds have been investigated. In samarium compounds with magnetic elements, the exchange fieldH _ex acting on Sm³⁺ ion is taken to be proportional to the sublattice magnetization of the magnetic element, while in compounds with nonmagnetic elementsH _ex is taken to be proportional to the spin average of the Sm³⁺ ion and is determined self-consistently. In both types of compoundsH _ex is assumed to be along [001] direction. The saturation magnetic moment is calculated by taking into account the admixture of excited (J=7/2 andJ=9/2) levels into the ground (J=5/2) level of Sm³⁺ ion by crystal fields and exchange fields. It is shown that depending upon the strength, the crystal fields quench or enhance the magnetic moment from the free ion value, and in some cases force Sm³⁺ ion to behave effectively like an (L+S) ion rather than an (L−S)ion. The crystal fields may have important bearing on the performance of samarium compounds as permanent magnet materials.     

染料敏化太阳能电池Sm~(3+)掺杂TiO_2下转换光阳极的制备及性能

用溶胶-水热法制备了Sm3+掺杂的Ti O2粉体(Ti O2∶Sm3+),将其按不同质量分数掺杂到P25基体中,制备了具有下转换功能的光阳极,并将其用于染料敏化太阳能电池中,提高了电池的光电性能。荧光光谱显示,Ti O2∶Sm3+粉体可以将紫外光转换为570~700 nm的可见光。当下转换光阳极中Ti O2∶Sm3+粉体的掺杂质量分数为80%时,短路电流密度达到13.12 m A/cm2,与纯P25光阳极相比,提高了26.5%,转换效率也提高了23.5%。     

Structural and magnetic property of Mn:ZnO bulk ceramic doped with rare earth (Gd/Sm) atoms

This paper reports the paramagnetic behavior of Mn doped ZnO co-doped with rare earth (Gd and Sm) atoms. The formation of secondary rare earth oxides (Gd₂O₃ and Sm₂O₃) is confirmed from the X-ray diffraction patterns. The rare earth oxides in the system forbids the grain growth and interconnection between the grains. The weak link between the grains suppresses the long range exchange interaction between the Mn ions and hence, reduces the ferromagnetic ordering. Owing to the large mismatch between ionic radii of rare earth and transition metal atoms inside the matrix, the rare earth element cannot contribute to promote ferromagnetic behavior in Mn doped ZnO, irrespective of their high individual magnetic moments.     

Er~(3+)和Yb~(3+)/Er~(3+)掺杂对石英光纤中倍频的影响

实验研究了掺Er~(3+)和Yb~(3+)/Er~(3+)石英光纤中的倍频过程.测量了不同Er~(3+)和Yb~(3+)/Er~(3+)掺杂量的光纤倍频转换效率和光纤倍频预处理前后Er~(3+)发射可见荧光的强度,探讨了Er~(3+)和Yb~(3+)掺杂对光纤中倍频过程的影响.     

CaZrO_3∶Ln(Ln=Pr~(3+),Sm~(3+),Tb~(3+),Dy~(3+),Tm~(3+))荧光粉的制备与光谱调控

采用高温固相法合成了稀土离子Pr3+、Sm3+、Tb3+、Dy3+、Tm3+掺杂的正交相CaZrO3荧光粉。利用X射线粉末衍射(XRD)对样品的结构进行表征,并通过荧光光谱对其发光性质进行了研究。在适当近紫外或蓝光激发下,CaZrO3∶Pr3+产生很强的绿光发射,CaZrO3∶Sm3+可发射550~700 nm的红橙光,Tm3+在CaZrO3中可获得良好的蓝光发射。研究结果表明,通过改变CaZrO3中的掺杂离子可实现其发光颜色的调控,稀土离子掺杂CaZrO3荧光粉是很有潜力的新型发光材料。     

HO3+单掺杂及其与Yb3+、Er3+共掺杂硼硅酸盐玻璃上转换发光的光谱分析

采用高温固相烧结法制备了HO3+单掺杂、HO3+/Yb3+共掺杂、HO3+/Er3+共掺杂和Ho3+/Yb3+/Er3+共掺杂等系列硼硅酸盐玻璃,测量了样品的激发光谱和发射光谱.结果表明:Ho3+单掺杂样品的激发光谱与发射光谱的强度随其浓度增加而逐渐减弱,原因是高浓度掺杂导致Ho3+离子产生猝灭效应;Ho3+/Yb3+...     

白光LED用Ce3+/Sm3+共掺玻璃和微晶玻璃的发光特性及能量传递研究

采用高温熔融法制备了一系列Ce³⁺/Sm³⁺共掺透明微晶玻璃,并研究了其发光特性。在微晶玻璃中Ce³⁺呈现出基于4f-5d跃迁的较强的宽带蓝光发射,通过调节Ce³⁺/Sm³⁺离子的掺杂浓度,Ce³⁺/Sm³⁺离子共掺微晶玻璃发光的色度逐渐发生变化,当CeO₂/Sm₂O₃掺杂的量比为1:1时,制得的微晶玻璃发光色坐标为(0.315, 0.296)。通过光谱和荧光衰减曲线,研究了Ce³⁺离子到Sm³⁺离子的能量传递,在SAZKNGC_0.6S_0.6微晶玻璃中,Ce³⁺离子向Sm³⁺离子传递能量效率约为20%。结果表明,Ce³⁺/Sm³⁺共掺微晶玻璃是白光LED的一种潜在基质材料。     

Structure and magnetic properties of RAlSi(R=light rare earth)

We prepared the semimetals RAl Si(R = light rare earth), and systematically study their crystal structures and magnetic properties. X-ray diffractions confirm the coexistence of the site-disordered phase with group space of I41/amd and the noncentrosymmetrically ordered phase with space group of I41 md in RAl Si alloy. The ordered phase is the main phase in RAl Si alloy. RAl Si alloys show nonmagnetic character for R = La, low temperature ferromagnetic order for R = Ce, Pr, and paramagnetic character for R = Nd, respectively. Sm Al Si shows metamagnetic transition at 10 K and ferromagnetic order at 143 K, respectively. Sm Al Si follows the van Vleck paramagnetic model in its paramagnetic region. The magnetization curves of RAl Si(R = Ce, Pr, Sm) follow the mixed model of ferromagnetism and paramagnetism, and the fitted saturation moment MSdepends on the moment of trivalent rare earth. The paramagnetic susceptibility χ of RAl Si is going up with increasing the atomic order numbers of rare earth elements. This reveals that the magnetic property of RAl Si originates from the rare earth.     

Structural,dielectric, electrical and piezoelectric properties of Ba<Subscript>4</Subscript>SrRTi<Subscript>3</Subscript>V<Subscript>7</Subscript>O<Subscript>30</Subscript> (R=Sm,Dy) ceramics

Polycrystalline samples of Ba₄SrRTi₃V₇O₃₀ (R=Sm and Dy), members of the tungsten-bronze family, were prepared using a high-temperature, solid-state reaction technique and studied their electrical properties (using complex impedance spectroscopy) in a wide range of temperature (31–500°C) and frequency (1 kHz-1 MHz). Preliminary structural (XRD) analyses of these compounds show the formation of single-phase, orthorhombic structures at room temperature. The scanning electron micrographs (SEM) provided information on the quality of the samples and uniform distribution of grains over the entire surface of the samples. Detailed studies of the dielectric properties suggest that they have undergone ferroelectric-paraelectric phase transition well above the room temperatures (i.e., 432 and 355°C for R= Sm and Dy, respectively, at frequency 100 kHz). Measurements of electrical conductivity (ac and dc) as a function of temperature suggest that the compounds have semiconducting properties much above the room temperature, with negative temperature coefficient of resistance (NTCR) behavior. The existence of ferroelectricity in these compounds was confirmed from a polarization study.      

Sol-gel synthesis, structural and optical properties of rare earth ions (Sm or Dy) activated Ca3Ga2Si3O12 powder phosphors

Structural, morphological and optical properties of rare earth ions (RE³⁺=Sm³⁺ or Dy³⁺) activated Ca₃Ga₂Si₃O₁₂ (CaGaSi) phosphors synthesized by the sol-gel method are reported. XRD results confirmed the cubic phase structure of RE³⁺:CaGaSi phosphors. From the SEM images of RE³⁺:CaGaSi phosphors, it is observed that the particles are agglomerated. Photoluminescence spectra of Sm³⁺:CaGaSi phosphors have shown bright orange red emission at 598 nm (⁴G_5/2→⁶H_7/2) with an excitation wavelength of λ_exci=401 nm. In the case of Dy³⁺:CaGaSi phosphors bright yellow emission has been observed at 574 nm (⁴F_9/2→ ⁶H_13/2) with λ_exci=451 nm. From the PL spectral results, the rare earth ion concentration of CaGaSi phosphors is optimized.     

Structural,magnetic and dielectric properties of (Li1+, Al3+) co-doped Ni0.5Zn0.5Fe2O4 ferrite ceramics prepared by the sol-gel auto-combustion method

(Li¹⁺, Al³⁺) co-doped Ni_0.5Zn_0.5Fe₂O₄ ferrites, Ni_0.5-xZn_0.5-xLi_xAl_xFe₂O₄ (x = 0.000, 0.025, 0.050 and 0.100), were synthesized by the sol-gel auto-combustion method. X-ray diffraction (XRD), field emission scanning electronic microscope (FESEM), vibrating sample magnetometer (VSM) and LCR meter were used to investigate the structural, magnetic and dielectric properties. Results of XRD and SEM indicate that both doping amount and calcination temperature play significant roles in crystal structure and grain growth. Also, it can be observed that the saturation magnetization and the coercivity change in a noticeable manner. The Ni_0.475Zn_0.475Li_0.025Al_0.025Fe₂O₄ ferrite sintered at 1200 °C has a relatively low coercivity value (62.93 Oe) and the largest saturation magnetization (110.95 emu/g). Besides, dielectric behavior is also improved by Li¹⁺ and Al³⁺ co-doping.