分子导体(PyEt)[Ni(dmit)2]2的合成、结构与导电性

合成了一种新的导电分子晶体PyEt[Ni(dmit)₂]₂ (dmit=4,5-dimercapto-1,3-dithiole-2-thione). X射线衍射测定表明, 该晶体属于单斜晶系, C2/c空间群. PyEt[Ni(dmit)₂]₂晶体中, 导电组元[Ni(dmit)₂]^0.5−沿c方向面对面平行堆积成分子柱, 各分子柱沿a方向肩并肩并行伸展构成(010)面的二维导电层. 测得二维导电层上某方向的室温电导率为10 S∙cm^−1. 从282~269 K, 该晶体表现出金属导电性, 269 K以下则为半导体. 用实测的晶体结构和计算的能带结构对这种导体→半导体的相变予以解释: 金属导电性对应于均匀的分子柱和直线点列型Ni原子链; 而半导体导电性则对应于交错的分子柱和锯齿型Ni原子链.     

分子导体(PyH)[Ni(dmit)_2]_2的合成、结构与导电性

合成了一种新的导电分子晶体(PyH)[Ni(dmit)_2]_2 (Py = pyridine, dmit = (C_3S_5)~(2-) = 4,5-dimercapto-1,3-dithiole-2-thione)，用元素分析、红 外光谱对其进行了表征，并用四圆X射线衍射方法确定了结构，该晶体属于三斜晶 系，P-1空间群；晶胞参数为: a = 0.59227(4) nm，b = 0.82279(6) nm, c = 1. 67535(9) nm, α = 90.233(5)°, β = 92.107(5)°, γ = 104.654(6)°; V = 0.78925(9) nm~3, Z = 1. (PyH)[Ni(dmit)_2]_2晶体中，导电组元[Ni(dmit)_2] ~(-0.5) 沿b轴方向形成具有二聚体结构的柱状堆积，在(001)面形成以肩并肩分子 间的S…S强相互作用为特征的二维导电层，这种二维导电层上的室温电导率为0. 13 Ω~(-1)·cm~(-1)，在c轴方向，(PyH)~+与[Ni(dmit)_2]~(-0.5)之间除库仑作 用外，还存在N-H…S，C-H…S氢键相互作用。单晶(001)面上变温电阻的测定结果 表明，在90 K到室温的温度范围内，(PyH)[Ni(dmit)_2]_2具有半导体导电行为， 导电激活能为0.15 eV。     

(Me_3NEt)[Pd(dmit)_2]_2和(NEt_4)[Pd(dmit)_2]_2的结构、能带及导电性

合成了导电分子晶体(Me3NEt)[Pd(dmit)2]2和(NEt4)[Pd(dmit)2]2, 测定了它们的晶体结构和电导-温度曲线. 在能带计算基础上解释了(Me3NEt)[Pd(dmit)2]2的室温电导率(σ= 58(Ω·cm)-1)高于(NEt4)[Pd(dmit)2]2 (σ= 2.2(Ω·cm)-1)的原因. (Me3NEt)[Pd(dmit)2]2属单斜晶系, P21/m空间群; (NEt4)[Pd(dmit)2]2属三斜晶系, P1 空间群. 两种晶体的导电组元皆为平面型配位阴离子[Pd(dmit)2]0.5-, 它们以面对面形式的二聚体 存在. 凭借肩并肩形式的S…S分子间相互作用, 二聚体进一步形成二维导电分子层. 两种配合物的二维导电分子层的微小结构差异导致电导率一个数量级的差别. 变温电导测定还表明, 两种晶体皆为小能隙的半导体.     

α′-(BEDT-TTF)2C6H4(SO3)2的合成、结构与导电性

用恒电流电化学结晶法合成了一种新的基于BEDT-TTF的电荷转移盐α′-(BEDT-TTF)2C6H4(SO3)2[BEDT-TTF=双亚乙基二硫四硫富瓦烯,C6H4(SO3)2 2 -=对苯二磺酸根].通过四圆X射线衍射方法测定了α′@(BEDT-TTF)2C6H4-(SO3)2的结构.晶体属于单斜晶系,P2/n空间群;晶胞参数:α=0.77937(17)nm,b=0.66989(11)nm,c=3.4422(7)nm,β＝91.135(12)°,V=1.7968(6)nm3.该晶体中BEDT-TTF+自由基沿α轴方向形成具有二聚体结构的交错排列型柱状堆积,沿b轴方向由肩并肩强分子间相互作用形成一维分子链.电荷补偿阴离子C6H4(SO3)2 2 -则在α方向存在较强的作用.沿c轴方向,BEDT-TTF+自由基层和阴离子层交替排列形成夹心式结构.α′-(BEDT-TTF)2C6H4-(SO3)2在ab面的某方向的室温电导率为0.5913 Q-1@m-1,电阻率-温度测定曲线表明它具有半导体导电行为.在150K附近,晶体发生了某种相变.     

分子导体θ-(ET)(C7H7SO3)·3H2O的合成、结构和导电性

用恒电流电化学结晶的方法合成了一种新的基于电子给体BEDT-TTF(双亚乙基二硫四硫富瓦烯) 的电荷转移盐θ-(ET)(C7H7SO3)·3H2O (ET为BEDT-TTF的简写,C7H7SO-3=对甲苯磺酸根).用四圆X衍射的方法测定了θ-(ET)(C7H7SO3)·3H2O的结构.晶体属于三斜晶系,P-1空间群;a=0.8682(1) nm, b= 1.2027(1) nm, c=2.5890(3) nm, α=87.025(6)°, β=89.117(8)°, γ=69.071(7)°, V=2.5216(5) nm3, R=0.0580.晶体中ET自由基沿a轴方向堆积成柱,相邻两个分子柱中的ET分子平面的夹角为49.30°.在b轴方向存在着分子柱侧向间的S…S近距作用.ET阳离子层与对甲苯磺酸根阴离子层沿c轴方向上交替排列.位于阳离子层与阴离子层之间的许多H2O形成了有利于晶体导电性的二维氢键网络.θ-(ET)(C7H7SO3)·3H2O在(001)晶面上某方向上的室温导电率为0.011 S·cm-1,所测变温电导曲线表明,该晶体在120～278 K温度区间内表现为半导体导电行为,导电激活能Ea=0.316 eV.从278～286 K表现为金属导电性.在276 K附近存在金属-半导体相变.     

ET类分子导体3d轨道对晶体能带及导电性的影响

采用扩展休克尔 -紧束缚方法 (EHTB)研究了ET类分子导体 [ET =bis (ethylenedithio) tetrathiafulvalene]的能带 .讨论了硫原子 3d轨道对能带结构的影响 ,添加 3d轨道导致ET分子柱间的横向作用大为增强 ,并与纵向作用处于同一数量级 ,这一结论解释了晶体二维导电性的实验结果 .计算得到 (ET) 2 C3 H5SO3 ·H2 O ,(ET) 2 HgCl3 ·TCE两个晶体的带隙分别为0 5 79,0 .5 72eV ,与实验得到的导电激活能 0 .3 19,0 .3 0 8eV符合较好 .     

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。     

á-(BEDT-TTF)_2C_6H_4(SO_3)_2的合成、结构与导电性

用恒电流电化学结晶法合成了一种新的基于BEDT TTF的电荷转移盐α′ (BEDT TTF) 2 C6H4 (SO3 ) 2 [BEDT TTF =双亚乙基二硫四硫富瓦烯 ,C6H4 (SO3 ) 2 -2 =对苯二磺酸根 ].通过四圆X射线衍射方法测定了α′ (BEDT TTF) 2 C6H4 (SO3 ) 2 的结构 .晶体属于单斜晶系 ,P2 /n空间群 ;晶胞参数 :a =0 .77937(17)nm ,b =0 .6 6 989(11)nm ,c =3.44 2 2(7)nm ,β =91.135 (12 )°,V =1.796 8(6 )nm3 .该晶体中BEDT TTF+ 自由基沿a轴方向形成具有二聚体结构的交错排列型柱状堆积 ,沿b轴方向由肩并肩强分子间相互作用形成一维分子链 .电荷补偿阴离子C6H4 (SO3 ) 2 -2 则在a方向存在较强的作用 .沿c轴方向 ,BEDT TTF+ 自由基层和阴离子层交替排列形成夹心式结构 .α′ (BEDT TTF) 2 C6H4 (SO3 ) 2 在ab面的某方向的室温电导率为 0 .5 913Ω-1·m-1,电阻率 -温度测定曲线表明它具有半导体导电行为 .在15 0K附近 ,晶体发生了某种相变     

(Me3NEt)[Pd(dinit)2]2和(NEt4)[Pd(dinit)2]2的结构、能带及导电性

合成了导电分子晶体(Me3NEt)[Pd(dmit)2]2和(NEt4)[Pd(dmit)2]2,测定了它们的晶体结构和电导-温度曲线.在能带计算基础上解释了(Me3NEt)[Pd(dmit)2]2的室温电导率(б=58(Ω@cm)-1)高于(NEt4)[Pd(dmit)2]2(б=2.2(Ω@cm)-1)的原因.(Me3NEt)[Pd(dmit)2]2属单斜晶系,P21/m空间群;(NEt4)[Pd(dmit)2]2属三斜晶系,P 1空间群.两种晶体的导电组元皆为平面型配位阴离子[Pd(dmit)2]0 5-,它们以面对面形式的二聚体[Pd(dmit)2]21-存在.凭借肩并肩形式的S…S分子间相互作用,二聚体进一步形成二维导电分子层.两种配合物的二维导电分子层的微小结构差异导致电导率一个数量级的差别.变温电导测定还表明,两种晶体皆为小能隙的半导体.     

Synthesis, Structure and Conductivity of （PyH）[Ni（dmit）2]2

A new molecular conductor (PyH)[Ni(dmit)2]2 (dmit = 4, 5-dimercapto-1, 3-dithiole-2-thione) has been prepared and its crystal structure has been determined. Crystallographic parameters for (PyH)[Ni(dmit)2]2: C17H6NNi2S20; triclinic system; P-1 space group; a = 5.9227 (4) , b =8.2279 (6), c = 16.7535 (9) A, a = 90.233 (5) , 0 = 92.107 (6) , y= 104.654 (6) ; V= 789.25 (9) A3; Z = 1; Dc = 2.068 g/cm3; F (000) = 491. The conductivity at one direction on (001) plane at room temperature was measured to be 0.13 ii^-cmf1. The resistivity-temperature curve in the temperature range of 90-290 K shows that this compound behaves as a semiconductor.     

Synthesis, structure, and conductivity of molecular conductor (PyEt)[Ni(dmit)_2]_2

A new electrical conductive crystal PyEt[Ni(dmit)2]2 (dmit=4,5-dimercapto-1,3-dithiole-2-thione) has been synthesized and its X-ray structure has been determined to be in monoclinic system, C2/c space group. In PyEt[Ni(dmit)2]2 crystal, the conducting component [Ni(dmit)2]0.5- is face-to-face packed forming molecular column along the c-direction, and these molecular columns are then side-by-side extended along the a-direction forming a kind of two-dimensional conducting sheet on (010). The measured conductivity at room temperature along a certain direction on (010) plane is 10 S .cm-1. From 282 to 269 K, the crystal shows metallic behavior but changes to semiconductor below 269 K. Based on the measured crystal structure and calculated band structure, this conductor-semiconductor phase transformation can be primarily interpreted: The metallic conductivity is corresponding to the uniform molecular column and the atomic-lattice-chain structure of Ni chain, while the semi-conductive behavior to staggered mo     

Towards Single-component Molecular Conductor [Ni(dmit)_2] by Charge Disproportionation:2[Ni(dmit)_2]~(-0.5)[Ni(dmit)_2]+[Ni(dmit)_2]~-

It was commonly thought that a molecular conductor or semiconductor should be composed of at least two components to make the conducting component in partially charged state. However, this idea became questionable by the recent report of the single-component molecular conductor [Ni(tmdt)2]1 as well as several reports about single-component molecular semiconductors such as [Ni(ptdt)2]2 and [Ni(C10H10S8)2]3. In fact, as early as 1985, [Ni(dmit)2] as a by-product in synthesizing TTF[Ni(dmit…     

Towards Single-component Molecular Conductor [Ni（dmit）2 ] by Charge Disproportionation： 2[Ni（dmit）2]^0.5→[Ni（dmit）2 ]＋ [Ni（dmit）2]^-

A new method of synthesizing single-component molecular conductor [Ni(dmit)2] bythe reaction 2(Me4N)[Ni(dmit)2]2→ [Ni(dmit)2] (Me4N)[Ni(dmit)2] is reported. [Ni(dmit)2]exhibits a semiconductive behavior above 167 K, while from 167 K down to the measuring limit of 60 K, it exhibits metallic conductivity.     

Synthesis,structure, and conductivity of molecular conductor (PyEt)[Ni(dmit)<Subscript>2</Subscript>]<Subscript>2</Subscript>

A new electrical conductive crystal PyEt[Ni(dmit)₂]₂ (dmit = 4,5-dimercapto-1,3-dithiole-2-thione) has been synthesized and its X-ray structure has been determined to be in monoclinic system, C2/c space group. In PyEt[Ni(dmit)₂]₂ crystal, the conducting component [Ni(dmit)₂]^0.5- is face-to-face packed forming molecular column along the c-direction, and these molecular columns are then side-by-side extended along the a-direction forming a kind of two-dimensional conducting sheet on (010). The measured conductivity at room temperature along a certain direction on (010) plane is 10 S · cm^-1. From 282 to 269 K, the crystal shows metallic behavior but changes to semiconductor below 269 K. Based on the measured crystal structure and calculated band structure, this conductor-semiconductor phase transformation can be primarily interpreted: The metallic conductivity is corresponding to the uniform molecular column and the atomic-lattice-chain structure of Ni chain, while the semi-conductive behavior to staggered molecular column and the atomic-zigzag-chain structure of Ni chain.     

Structures, energy bands and conductivities of (Me_3NEt)[Pd(dmit)_2]_2 and (NEt_4)[Pd(dmit)_2]_2

The electrical conductive molecular crystals (Me3NEt)[Pd(dmit)2]2 and (NEt4)[Pd (dmit)2]2 (dmit = 4,5-dimercapto-1,3-dithiole-2-thione) have been prepared, and their crystal structures and conductivity-temperature curves have been determined. The fact that the conductivity at room temperature of (Me3NEt)[Pd(dmit)2]2 (a = 58 Ω· cm-1) is much higher than that of (NEt4)-[Pd(dmit)2]2(cr= 2.2 Q~1 ?cm'1) has been rationally explained by the results of energy band calculations. (MeNEt3)[Pd(dmit)2]2 belongs to monoclinic system, P21/m space group and (NEt4)[Pd (dmit)2]2 belongs to triclinic system, P1 space group. The structural conducting component of the crystals is the planar coordinative anion [Pd(dmit)2]05- which forms the face-to-face dimmer [Pd(dmit)2]2-. These dimers have been further constructed to be a kind of two-dimensional (2-D)conductive molecular sheet by means of S…S intermolecular interactions. The tiny difference of the above 2-D molecular sheets of the two title crystals has resulted in one     

The Inorganic-free Organic Conductor α''''-(ET)_2C_6H_4(SO_3)_2 : Its Synthesis, Structure, and Conductivity

Having more than twenty years?glory, ET series still keep the most promising family in various kinds of organic conductors. Most of ET based molecular conductors consist of organic cationic ET+0.5 radical and certain anionic inorganic component such as the superconductor k-(ET)2Cu[N(CN)2]Cl (TC = 12.8K, 0.3kbar)1. Recently, the first purely organic superconductor b-(ET)2SF5CH2CF2SO3 (TC = 5.2K)2 has been reported, which aroused our interest on this kind of inorganic-free organic c…