Synthesis and magnetism of μ-isophthalato dinuclear lanthanide(III) complexes

Seven new μ-isophthalato dinuclear lanthanide(III) complexes, namely [Ln₂(IPHTA)(Me₂-phen)₄-(ClO₄)₂](ClO₄)₂ (Ln=La, Nd, Sm, Eu, Gd, Ho, Er), where Me₂-phen denotes 2,9-dimethyl-1,10-phenanthroline (Me₂-phen), IPHTA represents isophthalate dianion, have been synthesized and characterized by elemental analyses, molar conductance measurements, IR, ESR and electronic spectra. The variable-temperature magnetic susceptibilities of [ Gd₂ (IPHTA) (Me₂-phen)₄ ( ClO₄ )₂ ] ((ClO₄ )₂ complex were measured in the temperature range of 4–300 K and the observed data were successfully simulated by the equation based on the spin Hamiltonian operator, H = -2JS₁. J₂. giving the exchange parameter J = -0.19 cm^?1. This result is commensurate with a weak antiferromagnetic spin-exchange interaction between Gd(III)-Gd(III) im within the complex.     

Dependence of the Interface Magnetism in a Ferromagnetic Superlattice on the Geometric Structure

A new method which combines the mean-field renormalization group with the discretized path-integral representation is proposed to study interface magnetism in a ferromagnetic superlattice consisting of two alternating materials. A simple spin-1/2 transverse Ising model with the nearest-neighbour coupling is assumed. The dependence of the interface magnetism in the superlattice on the geometric structure and the coupling strengths between the interface and bulk layers are studied.     

NMRON Study of Magnetically Ordered (166m Ho)HoF3

A NMRON study of magnetically ordered HoF₃ using in-situ neutron activated ^166m Ho (I=7) isoelectronic probes in a spherical single crystal is presented. The optimal sensitivity to resonant change in the gamma-ray anisotropy of the 810 keV daughter gamma-ray emission has been utilised to track the lowest nuclear Zeeman substate resonance over an applied magnetic field range from 0.300 to 0.524 T, corresponding to the frequency range 1.56 to 1.78 GHz. The 2nd lowest substate resonance has also been observed at 0.3 T leading to a value P/h=−32.9(14) MHz for the ^166m Ho quadrupolar splitting which is consistent with predictions of a dominant negative pseudo-quadrupole interaction in this system. The Ho³⁺ electronic moment, in zero applied magnetic field, is projected to be 16% smaller than measured previously with neutron diffraction. This revised version was published online in September 2006 with corrections to the Cover Date.     

多核配合物高自旋基态分子的设计--一个理论和实践的总结

多核配合物高自旋基态分子的设计和合成是分子磁学的一项重要研究内容.作者结合本课题组的工作,总结了合成高自旋基态分子的几种重要模型,包括磁轨道正交、自旋极化、非正规自旋态及自旋失措模型.简要介绍了它们的基本原理和应用这些模型取得成功的一些实例,为分子磁工程的实现提供了一些可行的策略和方法.     

Magnetization reversal of ultrathin Fe film grown on Si（111） using iron silicide template

Ultrathin Fe films were epitaxially grown on Si（lll） by using an ultrathin iron silicide film with p（2 × 2） surface reconstruction as a template. The surface structure and magnetic properties were investigated in situ by low energy electron diffraction （LEED）, scanning tunnelling microscopy （STM）, and surface magneto-optical effect （SMOKE）. Polar SMOKE hysteresis loops demonstrate that the Fe ultrathin films with thickness t 〈 6 ML （monolayers） exhibit perpen-dicular magnetic anisotropy. The characters of M-H loops with the external magnetic field at difference angles and the angular dependence of coercivity suggest that the domain-wall pinning plays a dominant role in the magnetization reversal process.[第一段]     

过渡金属元素Sc、Cr和Mn对Mg2Ge掺杂的第一性原理研究

基于密度泛函理论(DFT)的第一性原理计算,研究了过渡金属元素Sc、Cr和Mn掺杂对Mg₂Ge晶体光、电、磁性质的影响。结果表明,Sc掺杂能使Mg₂Ge的费米能级进入导带,呈n型简并半导体;Cr和Mn掺杂能使Mg₂Ge能带结构和态密度在费米能级附近产生自旋劈裂而形成净磁矩,表现为半金属磁体和稀磁半导体,体系净磁矩均来自杂质原子3d轨道电子及其诱导极化的Ge4p态和Mg2p态自旋电子。与本征Mg₂Ge相比,掺杂体系静态介电常数增大,扩展了吸收光谱,提升了近红外光波段吸收能力。     

提高级联爆磁压缩发生器功率放大能力的新途径

通过采用适当措施在爆磁压缩放大器的功率放大级充电回路完成间接馈电,即提供次级回路初始电流(即种子源)之后切断充电回路,从而减少不必要的磁压,以提高装置的功率放大能力.利用二维爆轰磁流体力学程序对此进行模拟计算,计算结果表明,采用这种方法可以有效地提高装置的功率放大能力.     

RhnAl(n=1-6)团簇结构和磁性的研究

用密度泛函理论中的广义梯度近似方法研究了RhnAl(n=1~6)团簇的结构和磁性。结果表明：Rhn-1Al和Rhn (n=2~7)团簇结构是相似的,结合能随团簇尺寸变化趋势一致,原子间的s,p,d轨道杂化使得RhnAl团簇更加稳定。几乎所有Rh原子都是电子受体,Al-Rh键长越小,Rh原子得电子就越多。团簇磁矩主要来自Rh原子的贡献,Rh原子的4d轨道磁矩是Rh原子磁矩的主要部分。Al原子失去的电子越多,则其磁矩就相对越小。     

磁性Fe_3O_4@PS@PAMAM-Ag复合催化粒子的制备及其可再生催化性能(英文)

采用聚苯乙烯(PS)包裹Fe3O4磁性纳米粒子,制得Fe3O4@PS复合微球,以此作为磁性载体,通过微球表面的羧基将聚酰胺-胺类树形大分子(PAMAM)连接到磁性载体上,然后使Ag纳米粒子镶嵌在树形分子层中,制得可再生的金属复合催化粒子Fe3O4@PS@PAMAM-Ag.并采用红外光谱、扫描电镜、电感耦合等离子体质谱(ICP-MS)和X射线光电子能谱等方法对复合催化粒子进行了表征,结果表明,树形分子可以较好地分散和稳定金属Ag纳米粒子,所制复合催化粒子表面Ag含量为1.64%,具有较高的催化还原对硝基苯酚的活性.同时,利用外加磁场可以方便快捷地从反应体系中分离出来,继续用于下一次反应中,复合催化粒子循环使用6次后,仍保持完全的催化性能.     

混配配合物[Cu(2-mpac)(SCN)(H_2O)·H_2O]_n的合成、结构与磁性研究

在水溶液中以Cu(NO3)·3H2O,2-mpac和KSCN反应得到了一个通过硫氰酸根桥连的混配配合物[Cu(2-mpac)(SCN)(H2O)·H2O]n(1)(2-mpac:5-methylpyrazine-2-carboxylie acid),利用元素分析,红外光谱,单晶X射线衍射,X射线粉末衍射以及热重分析对配合物1进行了表征.晶体学数据:三斜晶系,P-1空间群,a=0.5567(2)nm,6=1.0339(3)nm,c=1.0532(3)nm,α=64.030(2)°,β=77.620(3)°,γ=85.945(3)°,V=0.5321(3)nm3',Z=2,S=1.061,最终偏离因子[I>2σ(I)]R1=0.0444,wR2=0.0905,对于全部数据R1=0.0647,wR2=0.0988.变温磁化率研究表明配合物1中的Cu(Ⅱ)离子之间存在弱的反铁磁相互作用.