{[K(18-C-6)][K(H_2O)_2]}[Cd(CN)_4]的合成与结构分析

合成了配合物 { [K(18- C- 6 ) ][K(H2 O) 2 ]} [Cd(CN) 4 ](1) ,并通过元素分析、红外光谱、单晶 X-射线衍射进行了结构分析。配合物属单斜晶系 ,空间群 P2 (1) / n。晶体学数据 :a=0 .936 5 3(18) nm,b=1.6 178(3) nm,c=1.74 81(3) nm,β=91.332 (3)°,V=2 .6 479(9) nm3 ,Z=4 ,Dcalcd=1.4 5 3g/ cm3 ,F(0 0 0 ) =12 0 8,R1=0 .0 317,w R2 =0 .0 5 6 7。配合物中 [K(18- C- 6 ) ],[K(H2 O) 2 ]和 [Cd(CN) 4 ]基团通过 K N键和 K —π相互作用形成三维网状结构     

苯并18-冠-6配合物[K(B18-C-6)]SCN的合成与结构分析

苯并 18 -冠 - 6 (B18- C- 6 )与 K2 [Cd(SCN) 4 ]反应 ,得到了 [K(B18- C- 6 ) ]SCN配合物。通过元素分析、红外光谱、单晶 X射线衍射进行了结构分析。该配合物为单斜晶系 ,空间群 P2 (1) / c,晶体学数据 :a=0 .996 0(3) nm,b=2 .5 0 97(7) nm,c=0 .8374 (2 ) nm,β=10 6 .5 19(5 )°,V=2 .0 0 6 7(10 ) nm3 ,Z=4 ,F(0 0 0 ) =86 4,R1=0 .0 4 2 9,w R2 =0 .0 5 75。结构分析表明 ,该配合物由一个 [K(B18- C- 6 ) ]配阳离子和一个 SCN阴离子组成 ,配合物的两个分子通过 K+ - π相互作用形成一维链状结构     

[Na(18-C-6)]2[Cu(i-mnt)2]的合成与结构分析

研究了18-冠-6与Na2[Cu(i-mnt)2][i-mnt=异丁二腈烯二硫醇阴离子,S2CC(CN)2-2]的反应,得到的配合物[Na(18-C-6)]2[Cu(i-mnt)2](1)通过元素分析、红外光谱、X射线单晶衍射进行了结构分析.配合物为单斜晶系,空间群P2(1)/c.晶体学结构数据a=1.2819(11),b=1.1793(10),c=1.4928(13)nm,β=99.121(16)°,V=2.228(3)nm3,Z=2,Dcaled.=1.369g/cm3,F(000)=958,R1=0.0521,wR2=0.1003.1中的[Cu(i-mnt)2]基团通过配体i-mnt的氮原子与两个[Na(18-C-6)]基团中的钠原子成键,形成稳定的中性配合物.     

二苯并18-冠-6配合物[NH4(DB18-C-6)]2[Pd(SCN)4]的合成与结构分析

研究了二苯并18-冠-6(DB18-C-6)与(NH4)2[Pd(SCN)4]的反应,通过元素分析、红外光谱、单晶X射线衍射对生成的配合物[NH4(DB18-C-6)]2[Pd(SCN)4](1)进行了结构分析.1为三斜晶系,空间群P-1,晶体学数据:a=0.8705(3)nm,b=1.1954(4)nm,c=1.3044(4)nm,α=73.216(5)°,β=78.897(5)°,γ=81.105(6)°,V=1.2682(7)nm3,Z=1,F(000)=568,R1=0.0301,wR2=0.0431.配合物由二个[NH4(DB18-C-6)]+配阳离子和一个[Pd(SCN)4]2-配阴离子组成,二者通过N-H…N氢键形成中性配合物,配合物中不存在阳离子-π相互作用.     

[{Na(18-C-6)}2(H2O)][Ni(i-mnt)2]的合成与结构分析

研究了18-冠-6与Na2[Ni(i-mnt)2]{i-mnt=异丁二腈烯二硫醇阴离子,[S2C2(CN)2]2-}的反应,得到的配合物[{Na(18-C-6)}2(H2O)][Ni(i-mnt)2](1),通过元素分析、红外光谱、X射线单晶衍射进行了结构分析。配合物为三斜晶系,空间群P-1。晶体学结构数据:a=1.0991(12)nm,b=1.1011(12)nm,c=1.1305(12)nm,α=70.44(2)°,β=87.44(2)°,γ=62.552(19)°,V=1.134(2)nm3,Z=1,F(000)=488,R1=0.3771,wR2=0.1497。(1)中的[Ni(i-mnt)2]基团通过配体i-mnt的氮原子与两个[Na(18-C-6)]基团之中的钠原子成键,形成稳定的中性配合物。     

[K(15-C-5)2]2[Ni(i-mnt)2]·2H2O的合成与结构分析

研究了15-冠-5与K2[Ni(i-mnt)2]{i-mnt=异丁二腈烯二硫醇阴离子,[S2C2(CN)2]2-}的反应,得到的配合物[K(15-C-5)2]2[Ni(i-mnt)2]·2H2O(1)通过元素分析、红外光谱、X射线单晶衍射进行了结构分析。配合物为三斜晶系,空间群P-1。晶体学结构数据:a=1.2674(5)nm,b=1.6317(7)nm,c=1.7771(7)nm,α=102.397(7)°,β=104.828(8)°,γ=93.659(7)°,V=3.442(2)nm3Z=2,F(000)=1412,R1=0.0727,wR2=0.1283。(1)中的[Ni(i-mnt)2]基团通过配体i-mnt的氮原子与两个[K(15-C-5)2]基团之中的钾原子成键,形成稳定的中性配合物。     

[Na(15-C-5)]2[Pd(SCN)4]配合物的合成与结构分析

研究了15-冠-5(15-C-5)与Na2[Pd(SCN)4]的反应,得到的配合物[Na(15-C-5)]2[Pd(SCN)4]通过元素分析、红外光谱、单晶X射线衍射进行了结构分析.该配合物为单斜晶系,空间群C2/c,晶体学数据: a=1.3525(6)nm,b=1.3729(6)nm,c=2.0312(9)nm,β=102.985(6)°,V=3.675(3)nm3,Z=4,F(000)=1696,R1=0.0288,wR2=0.0457.结构分析表明,该配合物由两个[Na(15-C-5)]+配阳离子和一个[Pd(SCN)4]2-配阴离子组成,二者通过Na-N相互作用形成二维网状结构.     

铁(Ⅱ)异腈配合物与三甲基胺氮氧化物氧原子转移反应动力学及其机理研究

在CH2 Cl2 介质中研究了铁 (Ⅱ )异腈配合物 [FeL5(CN) ]Br(1 ,L = CNCH2 Ph)和trans [FeL4(CN) 2 ] (2 ,L = CNCH2 Ph)等与氧原子转移试剂 (CH3) 3NO的反应动力学行为 ,研究结果表明 :配合物 1与 (CH3) 3NO反应遵从二级速率定律 ,反应速率 =k2 [铁异腈配合物 ]× [(CH3) 3NO]。反应的活化熵ΔS≠ 和活化焓ΔH≠ 分别为- 2 5 34± 1 67cal·(mol·K) - 1 和 1 2 71± 0 49kcal·mol- 1 ,而配合物 2不与氧原子转移试剂反应。认为反应以缔合机理进行。     

配合物[Zn(PSA)2(H2O)2]的合成及其晶体结构研究

合成了配合物单晶[Zn(PSA)2(H2O)2],其中PSA-为4-苯基丁酸根.配合物为单斜晶系,Cc空间群,a=3.8340(11)nm,b=0.51865(15)nm,c=1.0734(3)nm.a=90°,β=103.064(4).,r=90°,C20H26O6Zn.Mr=427.79,Z=4,V=2.0791(10)nm3,D=1.212g/cm3,F(000)=900,-46≤h≤43,-4≤k≤6,-13≤l≤13,R1=0.0780,wR2=0.2029.PSA-以两个氧原子与中心离子Zn(Ⅱ)离子形成四元螯合环,PSA与PSA反式构型.配合物分子之间存在氢键弱相互作用.     

苯并15冠5钯配合物:[K(B15C5)_2]_2[Pd(SCN)_4]的合成与结构研究

合成了苯并 15冠 5与钯生成的配合物 :[K( B15C5) 2 ]2 [Pd( SCN) 4],并通过元素分析、红外光谱及 X射线单晶结构分析进行了表征。配合物为单斜晶系、空间群 P2 1/ n。晶体学数据 :a=1.2 0 4 30 ( 7) ,b=1.932 99( 10 ) ,c=1.56680 ( 9) nm,β=10 8.1190 ( 10 )°,V=3.4 665( 3) nm3,Z=2 ,F( 0 0 0 ) =142 4 ,R1=0 .0 50 0 ,w R2 =0 .1549。配合物由两个 [K( B15C5) ]+2 配阳离子和一个 [Pd( SCN) 4]2 -配阴离子组成。四个硫氰酸根的硫原子与钯原子配位 ,[Pd( SCN) 4]2 -为平面方形构型。 K+与 2个冠醚环的 10个氧原子成键而形成夹心型结构。两个苯并 15冠 5的苯环相对钾原子呈反式排列     

First Observation of Hyperfine Structure in K(2)

The hyperfine structure of the (v'-v") = (27-0) band of the b(3)Pi(u0(+)) <-- X(1)Sigma(+)(g) transition has been observed by laser excitation spectroscopy in a highly collimated molecular beam. Hyperfine parameters for magnetic dipole and electric quadrupole interaction are derived from least-squares fitting of the hyperfine pattern and deperturbation between A(1)Sigma(+)(u) and b(3)Pi(u0(+)). Copyright 2000 Academic Press.     

Ba(1-x)K(x)Mn2As2: an antiferromagnetic local-moment metal

The compound BaMn2As2 with the tetragonal ThCr2Si2 structure is a local-moment antiferromagnetic insulator with a Néel temperature T(N)=625 K and a large ordered moment μ=3.9μ(B)/Mn. We demonstrate that this compound can be driven metallic by partial substitution of Ba by K while retaining the same crystal and antiferromagnetic structures together with nearly the same high T(N) and large μ. Ba(1-x)K(x)Mn2As2 is thus the first metallic ThCr2Si2-type MAs-based system containing local 3d transition metal M magnetic moments, with consequences for the ongoing debate about the local-moment versus itinerant pictures of the FeAs-based superconductors and parent compounds. The Ba(1-x)K(x)Mn2As2 class of compounds also forms a bridge between the layered iron pnictides and cuprates and may be useful to test theories of high T(c) superconductivity.     

Synthesis, crystal structure, and spectroscopic study of K0.92(2) Zn0.08(2) H1.92(2) (PO4) (Zn-KDP)

The structure of K0.92₍₂₎ Zn_0.08(2) H_1.92(2) (PO₄) was determined using single-crystal X-ray diffraction. The crystal structure of the Zn-KDP belonged to the tetragonal space group $ \mathrm{I}\overline{4}2\mathrm{d} $ , with cell parameters of a?=?b?=?7.4487(5)?Å and c?=?6.9703(5)?Å, 386.73(5) Å3, Z?=?4, and R?=?0.023. Zn²⁺ ions were used as substitutes for K⁺ ions with hydrogen vacancy. The Zn-KDP single crystals were submitted to further Raman, infrared, and ¹H NMR studies to investigate chemical group functionalisation, possible bonding between the organic and inorganic materials, and partial substitution of K⁺ by Zn²⁺. The latter partial substitution was confirmed by the deviation of IR frequencies for O–H stretching, the variation of IR and Raman frequencies for stretching and bending vibrations ν(PO₄) of H₂PO₄, and the appearance of additional Raman (147, 386 and 481 cm^?1) vibrational bands. Electrical conductivity measurements were performed on polycrystalline pellets of Zn-KDP and pure KDP at room temperatures (RT) of up to 473K. In both cases, a conductivity jump close to 453K was observed, and a stronger increase of conductivity was measured.     

Light-induced structural changes in sodiumnitroprusside (Na2(Fe(CN)5NO)·2D2O) at 80 K

Groundstate and electronic excited state (MS_I) of deuterated sodiumnitroprusside (Na₂(Fe(CN)₅NO)·2D₂O) have been investigated by neutron diffraction as well as by optical and Mössbauer techniques. Significant structural changes occur predominantly in the O–N–Fe–C-bond. It has been shown, that the N–O bond-length is not the order parameter, as expected from other studies. We found an increase in the bond lengths Fe–N4 of 0.019(2) Å and N–O of 0.004(4) Å respectively, which is in qualitative agreement with changes determined by Raman spectroscopy and predictions based on diatomic correlations (Badger/Herschbach/Laurie). Additionally we observed a change in the Fe–C1 bond length of 0.012(3) Å in agreement with Raman meaurements.     

Phase Manipulation between c(4 x 2) and p(2 x 2) on the Si(100) surface at 4.2 K

Phase manipulation between c(4x2) and p(2x2) on the Si(100) surface has been demonstrated at 4.2 K for the first time using a low-temperature scanning tunneling microscope. We have discovered that it is possible to change the c(4x2) surface into the p(2x2) surface, artificially, through a flip-flop motion of the buckling dimers by using a sample bias voltage control. Also, scanning at a negative bias voltage or applying a pulse voltage can restore the c(4x2) surface. The STM images as a function of bias voltage and tunneling current reveal the interesting dynamics of the buckling dimers on the long debated surface. Our results will show that energetic tunneling electrons are most likely responsible for the observed phase transition from c(4x2) to p(2x2).     

Microscopic coexistence of superconductivity and magnetism in Ba(1-x)K(x)Fe2As2

It is widely believed that, in contrast to its electron-doped counterparts, the hole-doped compound Ba(1-x)K(x)Fe(2)As(2) exhibits a mesoscopic phase separation of magnetism and superconductivity in the underdoped region of the phase diagram. Here, we report a combined high-resolution x-ray powder diffraction and volume-sensitive muon spin rotation study of Ba(1-x)K(x)Fe(2)As(2) showing that this paradigm does not hold true in the underdoped region of the phase diagram (0≤x≤0.25). Instead we find a microscopic coexistence of the two forms of order. A competition of magnetism and superconductivity is evident from a significant reduction of the magnetic moment and a concomitant decrease of the magnetoelastically coupled orthorhombic lattice distortion below the superconducting phase transition.     

Exotic d-wave superconducting state of strongly hole-doped K(x)Ba(1-x)Fe2As2

We investigate the superconducting phase in the K(x)Ba(1-x)Fe2As2 122 compounds from moderate to strong hole-doping regimes. Using the functional renormalization group, we show that, while the system develops a nodeless anisotropic s(±) order parameter in the moderately doped regime, gapping out the electron pockets at strong hole doping drives the system into a nodal (cos k(x) + cos k(y))(cos k(x) - cos k(y)) d-wave superconducting state. This is in accordance with recent experimental evidence from measurements on KFe2As2 which observe a nodal order parameter in the extreme doping regime. The magnetic instability is strongly suppressed.