调节层状分子基磁体[NO2BzQ1][FeRuxFe（1-x）（ox）3]的合成与磁性研究

合成了组成不同的一类新的层状分子基磁体[NO2BzQ1][FeRuxFe(1-x)(ox)3]，并测定了它们的变温磁化率，结果显示，磁体磁性随着Ru^Ⅲ／Fe^Ⅲ比例的不同而发生变化。     

分子基磁体[NCBzPy][Ni(dmit)2]的合成、表征和磁学性质

合成了一种新的取代苄基吡啶盐[NcBzpy]cl(1),1和NiCl2,dmit^2-反应生成分子基磁体[NCBzPy][Ni(dmit)2](2),其结构用元素分析、IR和UV进行了表征。并测定了2在2K～300K的变温磁化率,结果显示。相邻Ni^3 之间存在铁磁偶合作用。     

双金属层状配位聚合物{[NO2 BzQl][MCr(ox)3]}∞的合成、光谱表征和磁性研究

合成了两种新的草酸根桥联的双金属层状配位聚合物,{[NO2BzQl][MCr(ox)3]}∞,其中[NO2BzQl]+为1-(p-nitrobenzyl)quinolinium,ox2-为Oxalate,M为Ni2+或Cu2+,并经元素分析、红外光谱表征.变温磁化率测定结果表明,在这两种层状配位聚合物中,相邻的金属离子之间存在反铁磁偶合作用.应用Curie-Weiss公式拟合相应的变温磁化率数据为:C=0.662 emu K/mol,θ=-1.658 K,R=2.0×10-5(Ni2+);C=0.17 emu K/mo1,θ=-0.693 K,R=1.86×10-6(Cu2+).     

[Nd(ONO2)6][Cu(Im)(Phen)2]2(OH)·4H2O的合成、晶体结构及磁性质

用Nd(NO3)3·6H2O、Im(C3H4N2)、Phen(C12H8N2)和Cu(NO3)2·3H2O为原料,两步反应合成了标题化合物.该化合物晶体属P1空间群,晶胞参数a=1.012 6(2) nm,b=1.179 2(2)nm,c=1.398 5 nm,α=111.32(3)°,β=93.17(3)°,γ=90.33(3)°,Z=1,R=0.043.测定了化合物的UV-Vis-NIR及IR光谱和变温磁化率,发现标题化合物在低温下具有反铁磁性质.     

[Mn(phen)2(H2O)2]2[Cr(OX)3][HOCH2CH2O].4H2O的合成、晶体结构及性质

在二甲亚砜(DMSO)中,以MnCl_2·2H_2O和K_3[Cr(OX)_3]·3H_2O为原料,合成了离子型配合物[Mn(phen)_2(H_2O)_2]_2[Cr(OX)_3][HOCH_2CH_2O]·4H_2O.晶体结构测定表明,该晶体属单斜晶系,P2/c空间群.晶体学参数:a=1.0602(3),b=1.3515(3),c=2.1508(3)nm,β=102.57(2)°,V=3.008(1)nm~3,Z=2,Dc=1.49g/cm~3,F(000)=1392.最后的偏差因子R=0.067.测定了化合物的UV-Vis-NIR,IR,XPS,ESR光谱和变温磁化率,讨论了相应的性质.     

分子导体:[NCBzPy][TCNQ]2和[FBzPy][TCNQ]2的合成及光谱研究

合成了两种新的取代苄基吡啶盐[NCBzPy]Cl(1)和[FBzPy]cl(2),1(或2)与LiTCNQ,TCNQ进一步反应生成[NCBzPy][TCNQ]2(3){或[FBzPy][TCNQ]2(4)}。IR研究表明：TCNQ盐中存在TCNQ^o和TCNQ^-,并形成了一维TCNQ分子柱,且TCNQ^o和TCNQ^-之间存在相互作用,有部分电荷发生转移。     

[NEt4][Mn(salophen)(H2O)2]2[Fe(CN)6]· H2O· CH3OH超分子化合物的合成和结构

室温下将 [NEt4 ]3[Fe (CN) 6 ]和 [Mn (salophen) (H2 O) (CH3OH ) ]ClO4 反应 ,得到了超分子化合物[NEt4 ][Mn(salophen) (H2 O) 2 ]2 [Fe(CN) 6 ]·H2 O·CH3OH (salophenH2 =双水杨醛缩邻苯二胺 ) ,并对其进行了晶体结构测定 .结果表明 ,该晶体属三斜晶系 ,空间群P1- ,晶胞参数a =1.2 15 0 ( 4)nm ,b =1.483 4( 6)nm ,c =1.662 5 ( 6)nm ,α =81.896( 7)° ,β =76.980 ( 8)° ,γ =81.12 0 ( 6)°,V =2 .872 ( 2 )nm3,Z =2 ,Dc=1.3 88g·cm-3.晶体的各部分间以氢键连接成网状超分子体系     

超级材料--高维分子基铁磁体的设计与合成

高维分子基铁磁体的设计与合成是自然界向化学家的挑战。本文在简述了高维分子基铁磁体的重要性后,侧重介绍了设计与合成高维磁体的常用桥基、合成方法以及最新研究进展。     

[Nd（ONO2）6][Cu（Im）（Phen）2]2（OH）.4H2O的合成,晶体结构…

用Ｎｄ（ＮＯ３）３．６Ｈ２Ｏ、Ｉｍ（Ｃ３Ｈ４Ｎ２）、Ｐｈｅｎ（Ｃ１２Ｈ８Ｎ２）和Ｃｕ（ＮＯ３）２．３Ｈ２Ｏ为原料，两步反应合成了标题化合物，该化合物晶体属Ｐ１空间群，晶胞参数ａ＝１．０１２６（２）ｎｍ，ｂ＝１．１７９２（２）ｎｍ，ｃ＝１．３９８５ｎｍ，ａ＝１１１．３２（３）°，β＝９３．１７（３）°，γ＝９０．３３（３）°，Ｚ＝１，Ｒ＝０．０４３，测定了化合物的ＵＶ－Ｖｉｓ－ＮＩＲ及ＩＲ光谱和变温     

单分子磁体[Mn4(CF3COO)4(hmp)6]的合成、晶体结构及磁学性质

以[Mn12O12(CF3COO)16(H2O)4]·2CF3COOH·4H2O和2-羟甲基吡啶(hmpH)为起始物, 在四氢呋喃溶液中合成了一种新的四核锰配合物[Mn4(CF3COO)4(hmp)6]. X射线单晶衍射结果表明, 该配合物属于单斜晶系, P21/c空间群, 晶胞参数a=1.3663(3) nm, b=1.4705(3) nm, c=1.4734(3) nm, β=98.51(3) °, V=2.9276 nm3, Z=2. 配合物中有两个CF3COO-基团与七配位Mn2中心相连, 其中一个为单齿配体, 另一个是双齿配体. 直流磁化率研究结果表明, 该配合物具有较高的自旋基态, 而交流磁化率依赖于外场频率变化极值的出现表明该配合物是一种单分子磁体.     

单分子磁体及其磁学表征*

单分子磁体是介于分子基磁体和纳米磁性材料的学科交叉点.对其不同寻常磁特性的研究不仅有助于纳米磁性离子物理学和化学的发展,而且有望最终用于高密度信息储存设备.本文就单分子磁体的研究背景和意义、单分子磁体的种类、结构及磁学表征作一概述.     

配位聚合物{[CoL][FeⅡFeⅢ(ox)3·1.5H2O]}∞的合成、波谱表征和磁学性质

A new Schiff base complex， CoL(ClO₄)·3H₂O (1) {L represents condensed from equal molar ratio of sali-cylaldehyde and diethylenetriamine} was synthesized and characterized. Further， a new coordination polymer， {[CoL][Fe^ⅡFe^Ⅲ(ox)₃·1.5H₂O]}_∞ (2)， was synthesized and characterized， where ox^2-=oxalate. The results of the IR and M?ssbauer spectra of 2 revealed that the coordination polymer exists 2-D layer structure in the solid state， and anions layer was formed by [^ⅡFe^Ⅲ(ox)₃]^- unit. The magnetic properties of 2 have been measured and the results indicate that there is magnetic ordering in the low temperature， which may arise from intermolecular ferromagnetic interactions or spin canted effects.     

Molecular and Crystal Magnetic Engineering of Polymetallic Coupling System: From Magnetic Molecules to Molecular Magnets

One of the main challenges in the field of molecular materials is the design of molecular ferromagnets. General design strategy includes two steps, that is molecular magnetic engineering and crystal magnetic engineering. The first step is the synthesis of ferromagnetically coupled polymetallic systems. The second step is the assembly of polymetallic systems with muti‐dimensional structure and exhibiting a ferromagnetic transition. This paper summarized the strategies of molecular design and crystal engineering allowed to obtain such systems and our efforts in the fields of molecular magnetism and molecular‐based magnets.     

Tuning the Magnetic Properties of Columnar Benzo[e][1,2,4]triazin-4-yls with the Molecular Shape

A homologous series of disc-like 1,3,6-trisubstituted benzo[e][1,2,4]triazin-4-yls 1[n] was synthesized and their structural, thermal, optical, magnetic, and electric properties were investigated. The results demonstrate that all members of the series display a Col_h phase with clearing temperatures depending on the length of the alkoxy chains at the N(1) position, hence the shape of the disc. Powder XRD and magnetic data indicate a gradual change in the column diameter and magnetic behavior in the series in transition from half-disc in 1[0] (antiferromagnetic interactions) to full-disc geometry in the 1[12] homologue (ferromagnetic interactions with J/k_B=+7.5 K). Studies of binary systems revealed that a 1 : 1 mixture of 1[0] and 1[12] exhibits modest stabilization of the Col_h phase with an expanded range, and magnetic behavior typical for 1[0] in the rigid phase obtained from the melt. Electric measurements demonstrated hole mobility of ∼10⁻³ cm² V⁻¹ s⁻¹ and dark conductivity of ∼10⁻¹¹ Scm⁻¹ in the mixture and individual compounds. The latter is enhanced up to 4 times by simultaneous illumination with UV light.     

A Study of Magnetic Relaxation in Dysprosium(III) Single-Molecule Magnets

Although the development of single-molecule magnets (SMMs) is rapid, there are only two families of high energy barrier (U_eff) dysprosium(III) SMMs known so far: the cyclopentadienyl (Cp) family with a sandwich structure and the pentagonal-bipyramidal (PB) family with D_5h symmetry. These high-barrier SMMs, which usually possess U_eff>500 cm⁻¹ allow the separate study of the four magnetic relaxation paths, namely, direct, quantum tunnelling, Raman and Orbach processes, in detail. Whereas the first family is chemically more challenging to modify the Cp rings, it is shown herein that the latter family, with the common formulae [DyX¹X²(L_eq)₅]⁺, such as X¹/X²=⁻OCMe₃, ⁻OSiMe₃, ⁻OPh, Cl⁻ or Br⁻; L_eq=THF/pyridine/4-methylpyridine, can be readily fine-tuned with a range of axial and equatorial ligands by simple substitution reactions. This allows unambiguous confirmation that the U_eff mainly depends on the identity of X¹ and X², rather than on L_eq. More importantly, the fitted parameters are barrier dependent. If X¹ is an O donor and X² is a halide, 500<U_eff<600 cm⁻¹, log τ_0avg (s)=−10.66, log C_avg (s⁻¹ K⁻ⁿ)= −5.05, n_avg=4.1 and T_H=9 K (in which τ₀ is the pre-exponential factor for the Orbach relaxation process, C and n are parameters used to describe Raman relaxation, and T_H is the highest temperature at which magnetic hysteresis is observed). For cases in which both X¹ and X² are O donors, 900<U_eff<1300 cm⁻¹, log τ_0avg (s)=−11.63, log C_avg (s⁻¹ K⁻ⁿ)= −6.03, n_avg=4.1 and 18<T_H<25 K. Based on these results, it can be further concluded that U_eff not only has a linear correlation to the axial Dy−X bond lengths, but also to T_H for these PB SMMs. This represents the first systematic study of a family of lanthanide SMMs and derives the first magneto-structural correlation in Dy SMMs.     

Synthesis,Magnetic Properties,and STM Spectroscopy of Cobalt(II) Cubanes [CoII4(Cl)4(HL)4]

Reaction of cobalt(II) chloride hexahydrate with N‐substituted diethanolamines H₂L^2–4 ( 3 ) in the presence of LiH in anhydrous THF leads under anaerobic conditions to the formation of three isostructural tetranuclear cobalt(II) complexes [Co^II₄(Cl)₄(HL^2–4)₄] ( 4 ) with a [Co₄(μ₃‐O)₄]⁴⁺ cubane core. According to X‐ray structural analyses, the complexes 4 a , c crystallize in the tetragonal space group I4₁/a, whereas for complex 4 b the tetragonal space group P$\bar 4$ was found. In the solid state the orientation of the cubane cores and the formation of a 3D framework were controlled by the ligand substituents of the cobalt(II) cubanes 4 . This also allowed detailed magnetic investigations on single crystals. The analysis of the SQUID magnetic susceptibility data for 4 a gave intramolecular ferromagnetic couplings of the cobalt(II) ions (J₁≈20.4 K, J₂≈7.6 K), resulting in an S=6 ground‐state multiplet. The anisotropy was found to be of the easy‐axis type (D=?1.55 K) with a resulting anisotropy barrier of Δ≈55.8 K. Two‐dimensional electron‐gas (2DEG) Hall magnetization measurements revealed that complex 4 a is a single‐molecule magnet and shows hysteretic magnetization characteristics with typical temperature and sweep‐rate dependencies below a blocking temperature of about 4.4 K. The hysteresis loops collapse at zero field owing to fast quantum tunneling of the magnetization (QTM). The structural and electronic properties of cobalt(II) cubane 4 a , deposited on a highly oriented pyrolytic graphite (HOPG) surface, were investigated by means of STM and current imaging tunneling spectroscopy (CITS) at RT and standard atmospheric pressure. In CITS measurements the rather large contrast found at the expected locations of the metal centers of the molecules indicated the presence of a strongly localized LUMO.     

具有二维纳米孔径结构Ni3(H2O)6(TMA)3-(TMA)23-·2H2O(TMA=均苯三甲酸)的合成、晶体结构和磁性研究

A novel coordination polymer nickel 1,3,5-benzenetricarboxylate (TMA) Ni₃(H₂O)₆(TMA)^3-(TMA)₂^3-·2H₂O with two-dimensional porous structure was synthesized and characterized. It crystallizes in the hexagonal system, space group P6₅22, with a=1.665 2(10) nm, c=2.045 4(11) nm, V=4.912(5) nm³, Z=6, D_c=1.916 g·cm^-3, μ(Mo Kα)=0.181 8 mm^-1, F(000)=2 892. The final R₁=0.066 4, wR₂=0.175 6 for 2 710 observed reflections [I>2σ(I)] out of 2 904 unique reflections . This coordination polymer reveals not only two-dimensional porous structure but also particular magnetic properties. CCDC: 274177.     

One‐Dimensional Ferromagnetically Coupled Bimetallic Chains Constructed with trans‐[Ru(acac)2(CN)2]−: Syntheses,Structures, Magnetic Properties,and Density Functional Theoretical Study

Four cyano‐bridged 1D bimetallic polymers have been prepared by using the paramagnetic building block trans‐[Ru(acac)₂(CN)₂]^? (Hacac=acetylacetone): {[{Ni(tren)}{Ru(acac)₂(CN)₂}][ClO₄]?CH₃OH}_n ( 1 ) (tren=tris(2‐aminoethyl)amine), {[{Ni(cyclen)}{Ru(acac)₂(CN)₂}][ClO₄]? CH₃OH}_n ( 2 ) (cyclen=1,4,7,10‐tetraazacyclododecane), {[{Fe(salen)}{Ru(acac)₂(CN)₂}]}_n ( 3 ) (salen^2?=N,N′‐bis(salicylidene)‐o‐ethyldiamine dianion) and [{Mn(5,5′‐Me₂salen)}₂{Ru(acac)₂(CN)₂}][Ru(acac)₂(CN)₂]? 2 CH₃OH ( 4 ) (5,5′‐Me₂salen=N,N′‐bis(5,5′‐dimethylsalicylidene)‐o‐ethylenediimine). Compounds 1 and 2 are 1D, zigzagged NiRu chains that exhibit ferromagnetic coupling between Ni^II and Ru^III ions through cyano bridges with J=+1.92 cm^?1, z J′=?1.37 cm^?1, g=2.20 for 1 and J=+0.85 cm^?1, z J′=?0.16 cm^?1, g=2.24 for 2 . Compound 3 has a 1D linear chain structure that exhibits intrachain ferromagnetic coupling (J=+0.62 cm^?1, z J′=?0.09 cm^?1, g=2.08), but antiferromagnetic coupling occurs between FeRu chains, leading to metamagnetic behavior with T_N=2.6 K. In compound 4 , two Mn^III ions are coordinated to trans‐[Ru(acac)₂(CN)₂]^? to form trinuclear Mn₂Ru units, which are linked together by π–π stacking and weak Mn???O* interactions to form a 1D chain. Compound 4 shows slow magnetic relaxation below 3.0 K with ?=0.25, characteristic of superparamagnetic behavior. The Mn^III???Ru^III coupling constant (through cyano bridges) and the Mn^III???Mn^III coupling constant (between the trimers) are +0.87 and +0.24 cm^?1, respectively. Compound 4 is a novel single‐chain magnet built from Mn₂Ru trimers through noncovalent interactions. Density functional theory (DFT) combined with the broken symmetry state method was used to calculate the molecular magnetic orbitals and the magnetic exchange interactions between Ru^III and M (M=Ni^II, Fe^III, and Mn^III) ions. To explain the somewhat unexpected ferromagnetic coupling between low‐spin Ru^III and high‐spin Fe^III and Mn^III ions in compounds 3 and 4 , respectively, it is proposed that apart from the relative symmetries, the relative energies of the magnetic orbitals may also be important in determining the overall magnetic coupling in these bimetallic assemblies.