两个发光铽(Ⅲ)配合物的晶体结构和荧光性质

采用水热法合成了两个稀土配合物[Tb(3-SBA)(IP)OH(H2O)]·H2O(1)和[Tb(dpdc)1.5(IP)(H2O)]n(2)(3-SBA=3-羧基苯磺酸根,dpdc=2,2′-联苯二甲酸根,IP=1H-咪唑[4,5-f][1,10]-邻菲啰啉),并用X-ray单晶衍射仪测定了它们的晶体结构。配合物1是由3-羧基苯磺酸根和羟基交替连接Tb(Ⅲ)离子形成的一维链。配合物2是由2,2′-联苯二甲酸根桥联Tb(Ⅲ)离子形成的一维链。配合物1与2在紫外灯下均发出强的绿色荧光,其荧光光谱中有四个发射峰,位于492,544,584和619nm,分别对应于Tb(Ⅲ)离子的5 D4→7 FJ(J=6-3)跃迁,其发射光谱中均不存在配体荧光。配体吸收紫外光,有效地转移能量给Tb(Ⅲ)离子。配合物1与2中Tb(Ⅲ)离子的5 D4发光显示了单指数衰减,寿命分别为0.287和0.439ms,发光量子产率分别为9.28%和7.07%。     

2,9-二正丁基-1,10-菲咯啉双核铜(Ⅰ)配合物的合成、晶体结构及光学性质

以2,9-二正丁基-1,10-菲咯啉(dnbp)和碘化亚铜为原料,在四氢呋喃溶液中反应合成了一种新型中性双核铜(Ⅰ)配合物[CuI(dnbp)]2。采用X射线单晶衍射、核磁共振氢谱、紫外-可见吸收光谱表征其结构,荧光光谱测定其发光性能。结果表明:该配合物分子由两个Cu(Ⅰ)离子通过两个碘离子桥联形成畸变的菱形Cu2I2核心和dnbp螯合配体构成,配合物中I—Cu—I的夹角较小(106.08°),两个Cu(Ⅰ)离子的距离很长(0.319 4 nm),表明它们的相互作用可以忽略。上述结构的特征主要由dnbp配体大的空间位阻造成。配合物晶体属于三方晶系,空间群为R-3,晶胞参数a=4.404 14(11)nm,b=4.404 14(11)nm,c=1.085 92(4)nm,γ=120°,V=18.241 1(9)nm3。配合物在二氯甲烷溶液中出现350～500 nm的吸收峰,归属于金属离子到配体的电荷转移跃迁(MLCT)。室温下,当激发波长为365 nm时,其最大发射波长为653 nm,发光寿命为3.1μs,光致发光量子产率为0.013。发光机制属于金属离子和卤素到配体电荷转移激发态的磷光发射。低温下,配合物最大发射波长蓝移至645 nm,发射峰变窄。     

新型β-二酮配体及其Eu(Ⅲ)三元配合物的合成、表征及发光性能的研究

采用Claisen缩合反应合成了一种新型的β-二酮化合物1-(4-溴苯)-3-苯基丙烷-1,3-二酮(L),并以其为第一配体,邻菲罗啉(Phen)为第二配体,合成出新型稀土Eu(Ⅲ)三元配合物。通过元素分析、红外光谱、紫外光谱、荧光光谱对合成的配体及三元配合物进行了表征。红外光谱的分析表明:配体L含有β-二酮结构,且烯醇式含量高;配合物中L的氧原子以及Phen中的氮原子与稀土离子进行了配位。紫外光谱的分析表明配合物中的能量传递主要来自第一配体。通过荧光光谱研究了配合物的发光性质,结果显示配合物表现出Eu3+的特征发射,主发射峰为Eu3+的5D0→7F2发射,属于窄带发射,单色性较好,是具有潜在应用价值的红色发光材料。     

[{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。     

2,6-双二苯基膦吡啶银(Ⅰ)配合物的光谱研究

利用电子吸收光谱和发射光谱,研究具有光致发光性能的三配位Ag(Ⅰ)配合物[Ag2(μ-PNP)3](ClO4)2(PNP=2,6-双二苯基膦吡啶)的光谱性质,电子吸收光谱中约260和300 nm处的肩峰吸收分别被指定为l→aπ(l代表膦的孤对电子,aπ是苯环的反键轨道)和l→π·(π·表示吡啶的π反键轨道)跃迁.室温下受紫外可见光激发,配合物的乙腈溶液显示了发光性质,其发射峰位于525 nm,这是由配体激发态引起的.利用吸收和发射光谱,研究了配合物光物理性质在不同客体分子如AuPPh3Cl,AgCF3SO3和[Cu(CH3CN)4](ClO4)存在下光物理性质的改变情况.在配合物中,配体PNP和Ag(Ⅰ)形成一个空穴,可以结合外来的离子,从而引起光物理性质的改变,这种改变,使[Ag2(μ-PNP)3](ClO4)2可以作为作为客体离子的检测探针或传感器.     

1-正丁基咪唑合钴(Ⅱ)配合物的合成及其晶体结构分析

由1-正丁基咪唑(C7H12N2)和氯化钴(CoCl2)合成了一种新的配合物1-正丁基咪唑合钴配合物[Co (C7H12N2)6]Cl2.采用元素分析、红外光谱和X射线单晶衍射对配合物结构进行了表征.结果表明,所合成的配合物C42H72Cl2CoN12属于单斜晶系,空间群P2,晶胞参数:a=8.540(3)nm,b=16.851(5)nm,c=17.237(5)nm;α=90.00°,β=104.037(5)°,γ=90.00°;V=2406.5 (13)nm3,Z=2,Dc=1.207g· cm-3,F(000)=938,μ=0.509mm-1,R1 =0.0526,wR,=0.1664.     

2,7-二(3-(氰基)苯基)-9,9-二乙基芴的合成、晶体结构及光学性质(英文)

合成了一种新型的芴类衍生物2,7-二(3-(氰基)苯基)-9,9-二乙基芴。通过元素分析、红外(IR)、核磁共振(1H NMR)以及X射线单晶衍射对其组成和结构进行了表征。结果表明该化合物属于正交晶系,P空间群,晶胞参数:a=1.380 0(3)nm,b=2.230 6(4)nm,c=0.726 33(15)nm,α=β=γ=90°,V=2.235 8(8)nm3,Z=4,F(000)=896,μ=0.073 mm-1,S=1.013,R=0.046 9,wR=0.104 2。同时,我们对该化合物的紫外-可见吸收光谱和荧光光谱做了研究。在室温下,当激发光波长为330 nm时,该化合物的固态薄膜发射强烈的蓝色荧光,其发射波长为408 nm。此芴类衍生物在CH2Cl2溶液中的荧光量子效率为0.64,在固态薄膜中的斯托克斯位移为56 nm。该化合物有望成为一种优良的蓝色发光材料。     

[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。     

一维硫酸镉-双咪唑配合物的合成、结构及谱学性质研究

采用水热合成的方法,得到一种新颖镉的配合物{[Cd(H2biim)2(SO4)].3H2O}n(1,H2biim=2,2’-biimidazole)。通过X-ray单晶衍射分析可知,在该化合物中,SO24-桥连Cd(Ⅱ)离子在c轴上形成"之"字形一维无机CdSO4链。双咪唑配体通过与镉的配位作为支链悬挂在链的两侧,链与链之间分别通过π—π堆积和氢键作用,拓展为三维超分子网络。二维红外相关光谱分析表明SO24-的对称伸缩振动及咪唑环上的N—C伸缩和反伸缩振动,以及NC伸缩振动对热微扰均有响应。稳态荧光分析显示,配合物在397nm光激发下,在498nm处出现了强的蓝光,该发射带归属为配体到金属的荷移跃迁。     

2-(3’,4’-二羧基苯氧基)苯甲酸配体桥联的锌(Ⅱ)配合物的合成、结构及荧光性质

以2-(3’,4’-二羧基苯氧基)苯甲酸(H3DPBA)和1,3-二(4-吡啶基)-丙烷(bpp)为配体,与Zn(Ac)2通过水热反应,获得了一维链状配合物Zn(DPBA)(bpp)。该配合物的一个不对称单元包括一个Zn(Ⅱ)离子,一个DPBA配体和一个bpp配体。Zn(Ⅱ)离子与四个氧原子及一个氮原子配位,其配位数为5。固态配合物在375nm处出现强的发射峰,来自于配体的π~*—π跃迁。与配体的荧光发射光谱比较,配合物的荧光发射峰发生了蓝移,而且配合物的荧光发射强度有大幅度增强。讨论了配合物在常见溶剂中和金属阳离子中的荧光性质。实验结果表明不同有机小分子或不同金属阳离子对配合物的荧光强度有不同程度的影响,有机小分子硝基苯和Fe~(3+)使配合物荧光猝灭,该Zn(Ⅱ)-配合物可用于硝基苯的检测以及水和乙醇体系中Fe~(3+)的检测。     

2，6—双二苯基膦吡啶银（I）配合物的光谱研究

利用电子吸收光谱和发射光谱，研究具有光致发光性能的三配位Ag(I)配合物[Ag2(μ-PNP）3](ClO4)2(PNP=2,6-双二苯基膦吡啶）的光谱性质，电子吸收光谱中约260和300nm处的肩峰吸收分别被指定为l→aπ（l代表膦的孤对电子，aπ是苯环的反键轨道）和l→π^*（π^*表示吡啶的π反键轨道）跃迁。室温下受紫外可见光激发，配合物的乙腈溶液显示了发光性质，其发射峰位于525nm，这是由配体激发态引起的。利用吸收和发射光谱，研究了配合物光物理性质在不同客体分子如AuPPh3Cl,AgCF3SO3和[Cu(CH3CN)4](ClO4)存在下光物理性质的改变情况。在配合物中，配体PNP和Ag(I)形成一个空穴，可以结合外来的离子，从而引起光物理性质的改变，这种改变，使[Ag2(μ-PNP)3](ClO4)2可以作为作为客体离子的检测探针或传感器。     

镧系离子(Eu3+,Tb3+)氧氟沙星配合物的合成和光谱表征

本文报道了镧系离子Eu3 + ,Tb3 + 同喹诺酮羧酸类衍生物氧氟沙星形成配合物的合成。用元素分析法和ICP确定了配合物的组成为Ln(oflo) 3 Cl3 ·8H2 O。红外光谱表明氧氟沙星配体羧基同中心离子发生螯合 ,并可能与邻位羰基形成六元环稳定结构。荧光光谱表明 ,Eu配合物具有很宽的激发谱带 (2 0 0～ 45 0nm) ,明显区别于其他羧酸类的稀土配合物 ;中心离子Eu3 + 发射谱位于 5 79 0nm(5D0 7F0 ) ,5 92 2nm(5D0 7F1) ,6 12 2nm(5D0 7F2 ) ;而Tb3 + 配合物则同时有配体和中心离子的荧光发射     

Air Stability of Cs2CO3:Ag/Ag Cathode for Organic Light-Emitting Diodes

We report the superior stability of the composite Cs2CO3 ：Ag/Ag cathode structure, which can be used in efficient organic light-emitting diodes （OLEDs）. Devices with the Cs2CO3：Ag （1：10, 5nm）/Ag （95nm） cathode show a considerably improved lifetime compared with the control device with the Cs2CO3 （0.5 nm）/Ag （100 nm） cathode. The composite Cs2CO3 ：Ag/Ag film is proved to be stable in the atmosphere. X-ray diffraction （XRD） is applied to analyze the crystalline structure of the Cs2CO3：Ag film, and it is demonstrated that CsAg alloy is formed, leading to the improved stability of the thin film and the devices.     

Investigation of thermoluminescence in Li_2B_4O_7 phosphors doped with Cu, Ag and Mg

Li_2B_4O_7 (LBO):Cu,Ag,Mg phosphors have been prepared by the sintering technique. The roles of the Ag and Mg dopants in the phosphors have been studied using the methods of thermoluminescence (TL) glow curves and TL 3D spectra. The results indicated that proper concentrations of Ag and Mg can enhance the TL of LBO:Cu. It was also indicated that the intensity of TL peak at ~130℃ is reduced with the in- creasing Ag concentration, and enhanced with the increasing Mg concentration. From the TL 3D spectra, three emission bands (λ1 = 421 nm, λ2 = 380 nm, λ3 = 350 nm) were observed: the intensity of low energy emission band is reduced and that of the high energy is enhanced with the increasing dopant Ag; on the contrary, the intensity of low energy emission band is enhanced and that of the high energy one is reduced with the increasing dopant Mg.     

多孔配位聚合物[Nd2(C6H8O4)3(H2O)2]n·n(4,4'-bpy)的合成及晶体结构

合成了标题配位聚合物, 借助于元素分析、 红外光谱和X射线单晶衍射等分析方法确定了其晶体结构, 并测定了其TDA-DTA. 该配位聚合物属正交晶系, Pbcn空间群, 晶胞参数为a=2.201 2 nm(6), b=0.777 8 nm(2), c=1.972 4 nm(5), α=β=γ=90°, V=337.70 nm(15)3, Z=4, Dc=1.796 g·cm-3, μ=3.108 mm-1, F(000)=1 800, R1=0.043 0, wR2=0.056 0. 波谱分析结构显示, 通过己二酸配体羧基氧原子桥联Nd3+离子形成三维多孔结构, 4,4'-bpy通过氢键连接存在于孔道中.     

Cl+HN3产生NCl(a1Δ)和NCl(b1∑)的实验研究

 对利用微波放电直接解离Cl₂生成Cl, Cl与HN₃反应生成NCl(a^1Δ )和NCl(b^1∑)的过程进行了实验研究。得到了较强的NCl(a^1Δ 和NCl(b^1∑)自发辐射光谱,考察了Cl₂流量和He/Cl₂配比对NCl(a^1Δ 和NCl(b^1∑)生成的影响。发现对于一定的He流量,Cl₂流量对NCl(a^1Δ 和NCl(b^1∑)生成的影响存在一最佳范围,而最佳He/Cl₂配比不是一定值,而是随He流量升高而变大,在实验所考察的He流量范围（5~40 L/min）内,最佳He/Cl ₂配比在30∶1~100∶1之间。     

Adsorption of oxygen and carbon dioxide on cesium-reconstructed Ag(1 1 0) surface

The adsorption of oxygen and carbon dioxide on cesium-reconstructed Ag(1 1 0) surface has been studied with scanning tunneling microscopy (STM) and temperature programmed desorption (TPD). At 0.1 ML Cs coverage the whole surface exhibits a mixture of (1 × 2) and (1 × 3) reconstructed structures, indicating that Cs atoms exert a cooperative effect on the surface structures. Real-time STM observation shows that silver atoms on the Cs-covered surface are highly mobile on the nanometer scale at 300 K. The Cs-reconstructed Ag(1 1 0) surface alters the structure formed by dissociative adsorption of oxygen from p(2 × 1) or c(6 × 2) to a p(3 × 5) structure which incorporates 1/3 ML Ag atoms, resulting in the formation of nanometer-sized (10–20 nm) islands. The Cs-induced reconstruction facilitates the adsorption of CO₂, which does not adsorb on unreconstructed, clean Ag(1 1 0). CO₂ adsorption leads to the formation of locally ordered (2 × 1) structures and linear (2 × 2) structures distributed inhomogeneously on the surface. Adsorbed CO₂ desorbs from the Cs-covered surface without accompanied O₂ desorption, ruling out carbonate as an intermediate. As a possible alternative, an oxalate-type surface complex [OOC–COO] is suggested, supported by the occurrence of extensive isotope exchange between oxygen atoms among CO₂(a). Direct interaction between CO₂ and Cs may become significant at higher Cs coverage (>0.3 ML).     

Characteristic difference between ITO/ZrCu and ITO/Ag bi-layer films as transparent electrodes deposited on PET substrate

The metallic-glass film of ZrCu layer deposited by co-sputtering was utilized as the metallic layer in the bi-layer structure transparent conductive electrode of ITO/ZrCu (IZC) deposited on the PET substrate using magnetron sputtering at room temperature. In addition, the pure Ag metal layer was applied in the same structure of transparent conductive film, ITO/Ag, in comparison with the IZC film. The ZrCu layer could form a continuous and smooth film in thickness lower than 6 nm, compared with the island structure of pure Ag layer of the same thickness. The 30 nm ITO/3 nm ZrCu films could show the optical transmittance of 73% at 550 nm wavelength. The 30 nm ITO/12 nm ZrCu films could show the better sheet resistance of 20 Ω/sq, but it was still worse than that of the ITO/Ag films. It was suggested that an alloy system with lower resistivity and negative mixing heat between atoms might be another way to form a continuous layer in thickness lower than 6 nm for metal film.     

Adsorption-desorption properties,coadsorption, and surface structural chemistry of chlorine and oxygen on Ag(331)

At 300 K oxygen chemisorbs on Ag(331) with a low sticking probability, and the surface eventually facets to form a (110)?(2 × 1) O structure with ΔΦ = +0.7 eV. This facetting is completely reversible upon O₂ desorption at ~570 K. The electron impact properties of the adlayer, together with the LEED and desorption data, suggest that the transition from the (110) facetted surface to the (331) surface occurs at an oxygen coverage of about two-thirds the saturation value. Chemisorbed oxygen reacts rapidly with gaseous CO at 300 K, the reaction probability per impinging CO molecule being ~0.1. At 300 K chlorine adsorbs via a mobile precursor state and with a sticking probability of unity. The surface saturates to form a (6 × 1) structure with ΔΦ = +1.6 eV. This is interpreted in terms of a buckled close-packed layer of Cl atoms whose interatomic spacing is similar to those for Cl overlayers on Ag(111) and Ag(100). Desorption occurs exclusively as Cl atoms with E_d ~ 213 kJ mol^?1; a comparison of the Auger, ΔΦ, and desorption data suggests that the Cl adlayer undergoes significant depolarisation at high coverages. The interaction of chlorine with the oxygen predosed surface, and the converse oxygen-chlorine reaction are examined.     

NCl（a^1△）／I（^2P3／2）传能体系的实验研究

利用微波放电C12／He等离子体作为Cl源，对反应NCl(a^1△) I(^2P3/2)→NCl(X^3∑) I(^2P3/2)进行了实验研究，得到了较大的I(^2P3/2)自发辐射荧光信号，检测到NCl(a^1△，b^1∑)自发辐射荧光光谱在存在少量I(^2P3/2)下发生的显著变化，其中NCl(a^1△)自发辐射荧光信号降低，同时由于I(^2P3/2)的作用，NCl(b^1∑)自发辐射荧光信号大幅度增加。在考察各反应气体流量对I(^2P3/2)自发辐射荧光信号的影响时发现，在本次实验条件下，各种气体的最佳流量：He为1—4mmol/s，I2为0．01—0．03mmol/s，Cl2为1．0mmol/s左右，而HN3流量略大于Cl2流量时信号升高幅度开始变缓，约为Cl2流量的两倍时信号不再有显著的变化。