密度泛函理论在分子磁学中的应用

通过对桥联双核铁的磁耦合常数的计算，探讨了密度泛函理论计算条件对计算 结果的影响。基于密度泛函理论下的破损态方法，着重讨论了双核 Fe(III)_2的 d~5-d~5电子通过氧桥的超交换作用。研究发现分子的反铁磁通道主要是Fe(III) d_yz和d_z~2与μ-O的p轨道形成的，具有π*/π*和σ*/σ*特征的超交换通道。     

密度泛函理论在分子磁学中的应用1.单氧桥联双核铁(Ⅲ)[Cl3FeOFeCl3]2-磁耦合作用

通过对桥联双核铁(Ⅲ)[Cl3FeOFeCl3]2-的磁耦合常数的计算,探讨了密度泛函理论计算条件对计算结果的影响.基于密度泛函理论下的破损态方法,着重讨论了双核Fe(Ⅲ)2的d5-d5电子通过氧桥的超交换作用.研究发现分子的反铁磁通道主要是Fe(Ⅲ)的dyz和dz2与μ-O的p轨道形成的,具有π*/π*和σ*/σ*特征的超交换通道.     

密度泛函理论在分子磁学中的应用1.单氧桥联双核铁(III)[Cl_3FeOFeCl_3]~(2-)磁耦合作用

通过对桥联双核铁 (III) [Cl3FeOFeCl3] 2 - 的磁耦合常数的计算 ,探讨了密度泛函理论计算条件对计算结果的影响 .基于密度泛函理论下的破损态方法 ,着重讨论了双核Fe(III) 2 的d5 d5 电子通过氧桥的超交换作用 .研究发现分子的反铁磁通道主要是Fe(III)的dyz和dz2 与 μ O的p轨道形成的 ,具有π /π 和σ /σ 特征的超交换通道     

氰酸根桥联双核铜配合物磁构效关系的密度泛函研究

在密度泛函理论的框架下,采用对称性破损态方法,以{Cu2(C2H4N2)2(N, N-μ-NCO)2}2+为模型化合物,研究氰酸根EO方式桥联双核铜配合物的磁构效关系,进一步证实了通过CuNCu间的三中心d-p-dσ反键的超交换作用与磁偶合构效关系的本质联系. 计算了氰酸根桥联配合物磁交换偶合常数J与桥联角θ的关系,并与叠氮酸桥联配合物进行了比较.     

双核金属茂合物Zn2(η5-E5)2(E=N, P, As, Sb)电子结构和三阶非线性光学性质的理论研究

运用密度泛函PBE0方法研究了双核金属茂合物Zn2(η5-E5)2(E=N, P, As, Sb)的电子结构, 运用自然键轨道(NBO)方法对该体系的电荷分布及成键特征进行了分析. 此类体系中存在Zn—Zn的σ单键, 为近似纯s成分的成键方式. 用含时密度泛函理论(TDDFT ) 完全态求和(SOS) 方法计算了该体系的三阶非线性光学系数, 结果表明, γ值与最大吸收波长λmax成正比, 在各个分量中, 对〈γ〉起主要贡献的是γzzzz, 最大吸收波长对应的电子跃迁是从Zn—Zn的σ成键轨道到Zn—Zn的σ*反键轨道.     

氧桥联稀土钆双核配合物磁学性质的密度泛函理论研究

采用密度泛函理论结合对称性破损态方法,选用氧桥联稀土钆双核配合物为研究对象,通过与实验值比较,探讨了不同泛函与基组对计算磁耦合常数的影响.结果表明,在B3LYP/TZV水平下(Gd为SARC-TZV),相对论效应采用DHK2方法,计算结果与实验测量值-0.022 5cm~(-1)最接近.不同体系测试结果显示,可在该水平下预测新合成稀土钆双核配合物的磁学性质.Mulliken自旋密度分析可知磁中心Gd以自旋极化为主.键级分析表明,2个磁中心之间的磁耦合作用通过桥联氧原子的超交换作用实现.分子磁轨道分析显示2个磁中心间存在较强的轨道相互作用,其磁轨道主要是由钆原子的4f_z~3,4f_z~2_x轨道和桥联氧原子的2pz轨道组成.     

双核浆叶式钨配合物电子结构和电子光谱的理论研究

用密度函数理论中的B3LYP方法,对甲脒做配体的过渡金属双核浆叶式配合物W2（form)4((form)^-=[(p-tol)NCHN([p-tol)^-]^-)进行了分子轨道计算,结果表明,W－W键具σ^2π^4δ^2四重键的性质,W－W间的成键和反键分子轨道顺序为σ＜π＜δ＜σ^*＜π^*＜δ^*。用单激发组态相互作用（CIS）方法计算了W2(form)4的电子吸收光谱,得到这种配合物的最低能吸收光谱为λ＝496nm,这是δ（dxy）→σ^*(spz)跃迁产生的,属于金属内部的电荷迁移。     

CO在α-U(001)表面的吸附

采用密度泛函理论中的广义梯度近似,计算了CO在α-U(001)表面的吸附、解离和扩散.结果表明:CO分子以CU3OU2构型化学吸附在α-U(001)表面,吸附能为1.78-1.99eV;吸附后表层U原子向上迁移,伴随着褶皱的产生;CO分子与表面U原子的相互作用主要是U原子的电子向CO分子最低空轨道2π*转移,以及CO2π*/5σ/1π-U6d轨道间杂化而生成新的化学键;CO解离吸附较分子吸附在能量上更为有利,h1(C)+h2(O)和h1(C)+h1(O)(h:空位)解离态吸附能分别为2.71和3.08eV;近邻三重穴位之间C、O原子的扩散能垒分别为0.57和0.14eV,预示O原子较C原子更易在U(001)表面扩散迁移.     

邻苯二甲酸单甲酯桥联双核铜(Ⅱ)配合物磁性的理论研究

采用对称性破损态方法结合密度泛函理论,选用典型的强反铁磁双核配合物作为研究对象,通过与实验数据相比较,探讨了不同密度泛函方法与基组对计算铜配合物[Cu2(mMP)4(H2O)2]·H2O交换耦合常数的准确度.结果表明,4种混合密度泛函DFT(B3LYP,B3P86,B3PW91和PBE0)的计算结果都能和实验所观察到的值-324cm-1符号一致,但B3PW91方法得到的结果和实验结果吻合程度最好,同时采用方法B3PW91方法计算所得的交换耦合常数Jab对基组的依赖性较大.研究表明,2个Cu(Ⅱ)离子之间的反铁磁相互作用主要源于单占据分子轨道SOMOs大的能量劈裂和桥联配体O-C-O轨道的重叠.     

洛汾碱衍生物的电子结构及光谱性质的理论研究

采用密度泛函理论(DFT)的B3LYP/6-31G*方法,对4种洛汾碱类化合物的几何构型进行了优化,在此基础上计算分子的电子结构,并结合有限场FF方法研究了二阶非线性光学(NLO)性质.用含时密度泛函理论(TD-DFT)对上述化合物分子进行吸收光谱的研究.研究表明在4,5-二-苯基-2-对甲酰苯基咪唑生色团中4,5苯环上引入硝基和3位N原子引入苄基改变分子的共轭平面,使二阶非线性极化率总有效值(βtot)减小,吸收峰总体蓝移.同时还发现,在CH2Cl2溶剂中a和c分子的λmax主要来源于HOMO→LUMO的π一π*跃迁,b和d分子的λmax主要来源于HOMO→LUMO+2的π→π*跃迁.     

A diamagnetic dititanium(III) paddlewheel complex with no direct metal-metal bond

Reaction of Ti[N(But)Ar]3 (Ar = 3,5-C6H3Me2 or Ar' = C6H5) with CO2 at -40 degrees C produces diamagmetic Ti(III) paddlewheel complexes with long Ti-Ti separations (>3.4 Angstrom), thus excluding direct Ti-Ti bonding. 1H NMR spectroscopy shows that the compounds are diamagnetic in solution in the temperature range of -65 to +70 degrees C. In the solid state, the diamagnetism was found to persist between 2 and 300 K. Calculations at the density functional theory level suggest that the diamagnetism results from antiferromagnetic coupling by superexchange through the ligand pi system.     

Syntheses, crystal structures, and magnetic properties of [Ln(III)2(Succinate)3(H2O)2].0.5H2O [Ln = Pr, Nd, Sm, Eu, Gd, and Dy] polymeric networks: unusual ferromagnetic coupling in Gd derivative

Lanthanide-organic coordination polymeric networks of [Ln(III)2(suc)3(H2O)2].0.5H2O [suc = succinate dianion, Ln = Pr (1), Nd (2), Sm (3), Eu (4), Gd (5), and Dy (6)] have been synthesized and characterized by single-crystal X-ray diffraction analyses. The structural determination reveals that complexes are isomorphous, all crystallizing in monoclinic system, space group I2/a(.) The complexes possess a 3D architecture with Ln ion in a nine-coordination geometry attained by eight oxygen atoms from succinate and one oxygen atom from an aqua ligand. Low-temperature magnetic study indicates that ferromagnetic interaction is present in case of Gd(III) and Dy(III). Antiferromagnetic interaction is observed for the rest of the complexes. Density functional theory calculations are performed which support the existence of a superexchange ferromagnetic coupling in Gd(III) ions, whereas classical crystal field model has been applied to study the complexes 1, 2, 3, and 6.     

Exchange coupling through diamagnetic [Fe(CO)4]2- bridging ligands in a xenophilic cluster

The electronic structure of so-called 'xenophilic' clusters, which contain both organometallic fragments and Werner-type paramagnetic transition metal centres, presents a challenge to simple theories of bonding. Density functional theory shows clearly that the cluster Mn(2)(thf)(4)(Fe(CO)(4))(2) is best described as an exchange-coupled Mn(II)(2) dimer, the closed-shell organometallic [Fe(CO)(4)](2-) fragments acting simply as bridging ligands. The high-spin configuration of the Mn(II) ions leads to single occupation of the Mn-Fe σ* orbitals and therefore substantially weaker metal-metal bonding than in conventional low-valent organometallic clusters. The transition metal fragments are effective mediators of superexchange (J(calc) = -44 cm(-1)), leading to the measured effective magnetic moment of ~5 μ(B) at 300 K, considerably lower than the limiting value of 8.37 μ(B) for two uncoupled S = 5/2 Mn(II) centres.     

具有不同芳氧基取代酞菁钯聚集行为研究

为了研究具有不同芳氧基取代酞菁的聚集行为，合成了5种酞菁如 1,8,15,22- 四(2,4-二氯芳氧基)酞菁钯(Pel);1,8,15,22-四芳氧基酞菁钯(Pc2);1,8,15,22-四 (2,4-二特丁基芳氧基)酞菁钯(Pc3);1,8,15,22-四(2.5-二特丁基芳氧基)酞菁钯 (Pc4)和1,8,15,22-四(2,6-二溴-4-甲基芳氧基)酞菁钯(Pc5).酞菁的聚集行为由芳 氧基的性质不同决定。在四氢呋喃(THF)溶液中浓度在10~(-6)-10~(-5)mol·dm~(- 3)范围内，计算 得到5种酞菁的聚集常数分别为1.61*10~(-5)mol~(-1)·dm~3, 3. 87*10~(-5)mol~(-1)·dm~3, 2.60*10~(-5)mol~(-1)·dm~3, 1.21*10~(-5)mol~(- 1)·dm~3, 2.57*10~(-5)mol~(-1)·dm~3. 除了Pc1外，其余酞菁的单体和二聚体 吸收行为类似。在薄膜状态下，不同取代基对酞菁的吸收性质影响较大。成膜后5 种酞菁的吸收光谱都发生了改变，其中Pc1的吸收开关改变量大，而Pc5的吸收位置 改变最大。     

Ultrafast photoinduced intramolecular charge separation and recombination processes in the oligothiophene-substituted benzene dyads with an amide spacer

Photoinduced intramolecular charge separation (CS) and recombination (CR) processes of the tetrathiophene-substituted benzene dyads with an amide spacer (4T-PhR, R = 4-H (1), 4-CN (2), 3,4-(CN)2 (3), 4-NO2 (4), 3,5-(NO2)2 (5)) in solvents of different polarities were investigated using various fast spectroscopies. It was revealed that the CS rates depend on the ability of the acceptor and solvent polarity. Ultrafast CS with the rate of 5 x 10(12) s(-1) was revealed for 5 in PhCN and MeCN. The ultrafast CS can be attributed to the large electronic coupling matrix element between the donor and the acceptor despite the relative long donor-acceptor distance. The existence of the state with large electron density on the spacer between 14T*-PhR and LUMO should facilitate the CS process in the present dyad system. It was also revealed that the CR rates in these dyads were rather fast because of the enhanced superexchange interaction through the amide spacer.     

新型3-五元碳环螺环氧化吲哚类化合物的合成及其抗人白血病细胞活性

以氧化吲哚与邻芳基二甲醛为原料,经Knoevenagel缩合(或Michael,环化反应),制得7个3-五元碳环螺环氧化吲哚(4a~4c,产率67%~86%,d/r值4∶1~10∶1)和4d~4g;4d~4g与哌啶(或四氢吡咯)和多聚甲醛经胺甲基化反应,合成了4个3-五元碳环螺环氧化吲哚(5d~5g),产率55%~67%,d/r值10∶1~20∶1,其结构经~1H NMR,~(13)C NMR和HR-MS(ESI-TOF)表征。采用MTT法研究了4a~4c和5d~5g对人白血病细胞(K562)的体外抗肿瘤活性。结果表明:4b,5d和5f对K562抑制活性较好,IC50分别为29.3μmol·L~(-1),27.4μmol·L~(-1)和34.2μmol·L~(-1),与阳性对照药顺铂(26.8μmol·L~(-1))相当。     

二甲亚砜-二(4,4,4-三氟-1-(2-噻酚基)丁二酮-1,3)合铜单晶的ESR研究

由于过渡金属配合物的顺磁共振研究可以导出金属未成对电子的磁性质和金属离子与配体之间的成键信息。在对体系各种不同状态的研究中,以晶体的ESR数据最为准确可靠。β-二酮配合物一直是化学工作者开展研究的活跃领域。当中心金属离子为铜(Ⅱ)时,ESR     

Bi2Sr2CuO6的电子结构和铜氧对间电荷涨落

自发现含铋铜氧化物的高温超导性以来,采用各种复杂程度方法对电子结构的计算已经在文献中报道.它们集中讨论了能带结构,态密度和Fermi面的性质,但很少报道铜氧对间的电荷涨落。而价态变动对超导电性起着至关重要的作用,因此本文对Bi_2Sr_2CuO_6进行了紧束缚带计算,探讨了电子缺陷和氧呼吸式振动对铜和氧电荷分布的影响。     

Ln(terpy)]3+ (Ln = Sm, Gd) entity forms isolated magnetic chains with [W(CN)8]3-

The reaction between Ln(NO3)3*xH2O, Cs3[W(V)(CN)8]*H2O and 2,2':6',2'-terpyridine (terpy) leads to the original isomorphous cyano-bridged [Ln(III)(terpy)(DMF)4][W(V)(CN)8] *6H2O [Ln = Gd (1), Sm (2)] 1-D chains. The crystal structures of {Ln(III)W(V)} chains and consist of alternating {[W(CN)8]} and {[Ln(terpy)]} building blocks. The neighbouring 1-D chains are weakly linked through pi-pi stacking interactions of the aromatic rings leading to 2-D supramolecular layers. The layers are linked through hydrogen bonds between H2O molecules and terminal cyano ligands. Magnetic studies revealed a weak antiferromagnetic coupling (J = -2.3(2) K) within the {Gd(III)W(V)} chains in . The positive effective coupling constant J = +2.0(5) K between the total angular momentum of the Sm(III) centre and the spin of the W(v) ion is equivalent to an antiferromagnetic character of the spin coupling between both centres in the {Sm(III)W(V)} chains of 2. The magnetic measurements suggest that they display an isolated magnetic chain behaviour.     

Theoretical Studies on the Spin Exchange Interaction in Copper(II) Complexes Coordinated with Nitronyl Nitroxide

In the recent years, a wide variety of transition metal complexes with the nitronyl radical ligands have been reported1,2. These systems display the various magnetic behaviors (ferro- or antiferro-magnetism) between the unpaired electrons on the radical ligands and on the paramagnetic metal ion center. However, few theoretical studies on the metal-radical complexes were reported and quite few are known about the nature of the exchange coupling interactions. In this work, we are interested i…