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1.
采用叠加模型和双旋-轨耦合参量模型,建立了结构参数与EPR参量之间的定量关系;较好地解释了[VO(H2O)5]2 络离子的局域结构和EPR参量;研究结果发现,(NH4)2C4H4O6:VO2 晶体中络离子[VO(H2O)5]2 的键长为R//≈0.130nm,R⊥≈0.195nm;在(NH4)2C4H4O6:VO2 晶体中,局域结构沿C4轴方向呈压缩的八面体结构;所得EPR参量的理论计算与实验测量数据符合很好。  相似文献   

2.
李超英  涂虬  顾磊  郑雪梅 《人工晶体学报》2014,43(11):2982-2986
在晶体场理论的基础上,由重叠模型建立了杂质中心结构参数与电子顺磁共振(EPR)参量之间的定量关系;利用3d9离子正交(D2h)伸长八面体对称EPR参量的高阶微扰公式计算了K2Cd(SO4)2·6H2O∶Cu2+的g因子gi(i=x,y,z)和超精细结构常数Ai.研究表明,K2Cd(SO4)2·6H2O晶体中络离子[Cu(H2O)6]2+的Cu2-H2O键长分别为Rx≈0.181 nm,Ry≈0.199 nm,Rz≈0.232 nm,局域结构为沿C4轴方向呈正交伸长八面体(D2h)结构.所得EPR参量理论计算与实验符合较好,并对上述结果进行了讨论.  相似文献   

3.
本文基于晶体场理论,建立了10×10阶的3d~1离子的全组态能级矩阵,由全对角化法(CDM)计算了ZPPH (ZnKPO_4·6H_2O)∶ VO~(2+)晶体的吸收光谱与顺磁g因子;同时,运用3d~1离子在C_(4v)对称下的能级公式和电子顺磁共振(EPR)参量高阶微扰(PTM)公式,计算了ZPPH∶ VO~(2+)晶体的光学吸收谱和EPR参量g因子g_(//),g_⊥和超精细结构常数A_(//),A_⊥,所得理论结果与实验符合.两种理论方法对比研究表明:对3d~1(V~(4+))电子组态,微扰法所得结果是全对角化法所得结果的一种很好近似.对所得结果的合理性进行了讨论.  相似文献   

4.
基于晶体场理论和电荷转移机制,采用双旋-轨耦合参量模型的3d~1离子在D_(4h)对称的晶场中自旋哈密顿参量的高阶微扰公式和晶场能级公式,计算了(ZnKPO_4·6H_2O)∶VO~(2+)晶体的光吸收谱和自旋哈密顿参量。本文不仅考虑了晶场机制,同时也考虑了电荷转移机制。计算结果与实验数据是一致的。说明电荷转移机制对(ZnKPO_4·6H_2O)∶VO~(2+)晶体的自旋哈密顿参量的结果有不可忽略的作用。  相似文献   

5.
LiTaO3:Cr3+晶体中Cr3+离子占位及其EPR参量的理论研究   总被引:3,自引:5,他引:3  
利用Racah不可约张量算符法和Winger定理,建立了d3(C*3v)电子组态的能量矩阵及其全组态EPR理论;借助Newman的叠加晶场模型和自旋哈密顿理论,研究了EPR参量与LiTaO3:Cr3+晶体结构参数之间的定量关系.在此基础上,研究了LiTaO3:Cr3+的EPR参量及其电子光谱,理论与观测一致.定量研究表明:LiTaO3:Cr3+晶体中,Cr3+离子取代了Ta5+离子而不是Li+离子.  相似文献   

6.
六次甲基四胺(C6H12N4,HMTA)部分取代六水合硫酸镍(NSH)晶体结构中的配位水,合成Ni(C6H12N4)2SO4·4H2O(NSH-HMTA)晶体材料.采用称量法测定了NSH-HMTA晶体的溶解度曲线,应用水溶液降温法在温度区间56 ~44℃之间生长出6 mm×6 mm×2 mm尺寸的晶体,生长速度约为0.5 mm/d.通过等离子发射光谱分析所生长晶体中镍离子含量,X射线单晶衍射用于验证晶体的结构.采用热重法(TGA)和差热分析法(DTA)测定晶体脱水温度和分解温度分别为93℃、1 14℃.测量晶体的紫外-可见光谱特性,其紫外波段透过峰位于波长为307 nm处,比NSH晶体(287 nm)红移了约20 nm,HMTA与Ni2+配位提高了Ni2+的3A2g光谱项的能级,3A2g→3T1g(P)所需能量更低,导致吸收谱红移.  相似文献   

7.
以芒柄花素为先导化合物,合成了水溶性的[Co(H2O)6](C18H15O4SO3)2·4H2O,并采用IR, 1H NMR, TG-DTA, XRD和单晶X射线衍射法对其结构进行了表征.单晶X射线衍射结果表明:[Co(H2O)6]2+、C18H15O4SO 3和H2O之间存在多种氢键,形成晶体结构中的亲水区.异黄酮骨架间反平行排列,面对面和边对面芳香堆积作用同时存在于其中,构成晶体结构中的疏水区.磺酸根是连接亲水区和疏水区的桥梁.氢键、芳香堆积作用以及阴阳离子之间的静电引力共同将标题化合物组装成具有三维网络结构的超分子.  相似文献   

8.
利用Newman的晶场叠加模型,建立了晶体微观结构与电子顺磁共振(EPR)参量之间的定量关系.采用全组态完全对角化方法,对YAG:V2+晶体的局域晶格畸变及其EPR参量进行了系统的研究,结果表明:V2+离子掺入YAG晶体后,V2+离子的局域结构产生压缩三角晶格畸变,沿[111]晶轴方向V2+离子上方的三个O2-配体与下方的三个O2-配体均偏离[111]轴1.96°,从而成功地解释了YAG:V2+晶体的EPR参量.同时研究也表明,SS与SOO磁相互作用对EPR参量的贡献不可忽略.  相似文献   

9.
魏群 《人工晶体学报》2006,35(2):224-227,236
在考虑微小磁相互作用(包括SS、SOO和OO作用)的基础上,采用全组态完全对角化方法,建立了A l2O3晶体中V2 离子的局域结构与自旋哈密顿参量定量关系,对A l2O3:V2 晶体基态和激发态零场分裂以及基态g因子等自旋哈密顿(SH)参量给出了统一的解释。结果表明,V2 离子进入A l2O3晶体后,上下配体氧平面分别沿C3轴向远离三角中心的方向移动了0.0021nm和0.0020nm。理论计算结果与实验值符合甚好。  相似文献   

10.
基于离子簇模型,采用d9离子在四角伸长八面体对称中电子顺磁共振(EPR)参量的高阶微扰公式,计算了SrCl2中四角Ag2+中心的EPR参量(g因子g//,g⊥和超精细结构常数A因子A//,A⊥).由于体系的共价性及配体Cl-较大的旋轨耦合系数,在这些公式中同时考虑了配体轨道及旋轨耦合作用对EPR参量的贡献.公式里的能级分裂由重叠模型和杂质中心的局部结构确定.研究发现,掺杂后由于尺寸失配,杂质Ag2+沿着C4轴有一个很大的非中心位移,到最近邻的Cl-平面距离约为0.060 nm.计算所得的EPR理论值与与实验值符合的很好.  相似文献   

11.
In this article, diaquatetrakis (thiocyanato) manganese(II) mercury(II)‐N‐methyl‐2‐pyrrolidone, MnHg(SCN)4(H2O)2.2(C3H6CONCH3), (abbreviated as MMTWMP), a new organometallic nonlinear optical crystal material is reported. The structure, optical and thermal characterizations were determined by elemental analysis, infrared and Raman spectroscopy, X‐ray powder diffraction, thermogravimetric analysis, differential scanning calorimetry, special heat, SHG measurements and UV/Vis/NIR optical transmission spectra. It belongs to the tetragonal crystallographic system, with cell parameters: a = 12.1294, c = 8.2238Å, V = 1211.27Å3. Single crystals with dimensions up to 8 × 7 × 5 mm3 have been obtained. The morphology of the crystals was indexed. The MMTWMP crystal exhibits good physicochemical stability at normal temperature and pressure. Its UV transparency cutoff is 360 nm, which is shifted to the violet by 13 nm, as compared with MnHg(SCN)4 (MMTC); the optical transmission is 44.82% at 404 nm, which is by 17.46% higher than that of MMTC.  相似文献   

12.
采用提拉法(CZ法),生长出质量良好的Er3+:NaY(W0.9Mo0.1O4)2晶体.通过X射线粉末衍射,红外光谱分析,并与NaY(WO4)2相比较,得到Er3+:NaY(W0.9Mo0.1O4)2晶体的结构与NYW类似,仍为四方晶系的白钨矿结构,I4(1)/α空间群.测定了晶体的实际组成,得到晶体中各元素均按理论值进行掺杂,计算了掺杂离子的分凝系数约为1.15.在光谱性质上,测试了晶体的吸收光谱,及晶体在50~1000cm-1波数范围内的拉曼光谱,并计算了各吸收峰的半峰宽及吸收系数A.  相似文献   

13.
Infrared spectra of K2Ni(SeO4)2·6H2O and (NH4)2Ni(SeO4)2·6H2O containing SO42‐ ions and those of K2Ni(SO4)2·6H2O and K2Ni(SeO4)2·6H2O containing NH4+ ions are presented and discussed in the region of ν3 and ν1 of the sulfate ions and in the region of ν4 of the NH4+ ions, respectively. The SO42‐ ions matrix‐isolated in the selenate matrices (approximately 1 mol%) exhibit three bands for ν3 and one band for ν1 in agreement with the low site symmetry C1 of the host selenate ions. The NH4+ guest ions included in the potassium sulfate matrix are characterized also with three bands for ν4. However, the ammonium ions in (NH4)2Ni(SeO4)2·6H2O as well as those included in K2Ni(SeO4)2·6H2O display four infrared bands corresponding to ν4 due probably to some kind of disorder of the ammonium ions. The extent of energetic distortion of the isomorphously included sulfate ions as deduced from the values of Δν3 and Δνmax is commented. The spectroscopic experiments reveal that the SO42‐ guest ions are weaker distorted in the selenate matrices as compared to the same ions in the neat sulfates due to the larger unit‐cell volumes of the selenate compounds. The band positions of the water librations in the host potassium compounds are affected by the included ammonium cations. The formation of hydrogen bonds between the NH4+ guest ions and the XO42‐ host ions leads to a decrease in the proton acceptor capabilities of the anions and as a result the hydrogen bonds weaken on going from the neat potassium compounds to the mixed crystals. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

14.
Cross‐like Pr2(C2O4)3·10H2O micro‐particles were synthesized through a simple precipitation method at room temperature. The products were characterized by X‐ray diffraction (XRD), X‐ray photoelectron spectroscopy (XPS), field‐emission scanning electron microscopy (FESEM), thermogravimetry–differential thermal analysis (TG‐DTA) and photoluminescence (PL). The possible formation mechanism of the cross‐like Pr2(C2O4)3·10H2O micro‐particles was discussed, and Pr6O11 with similar morphology was obtained by calcining the oxalate precursor. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

15.
利用无水氯化钙-钛酸四正丁酯-无水乙醇体系,通过加入一定摩尔配比的C3N4粉体用溶剂热法制备了C3N4-CaTi2O4(OH)2复合材料粉体.利用X射线衍射(XRD),比表面积(BET)和扫描电子显微镜(SEM)对样品的显微结构进行检测分析,并利用紫外-可见吸收光度计分析了样品对光的吸收特性,研究不同摩尔配比的C3N4粉体复合量对CaTi2O4(OH)2样品的物相结构、微观形貌以及其光催化性能的影响,并考察了不同光源对所制备样品性能的影响.实验结果表明:C3N4粉体的引入显著提高了CaTi2O4(OH)2样品的光催化活性,且当CaTi2O4(OH)2:C3N4物质的量之比为1:0.75时,复合样品的光催化降解率在250nm光源照射下K可达到最大值0.02338min-1.  相似文献   

16.
掺杂晶体SrLaAlO4:Cr3+局域结构的研究   总被引:10,自引:7,他引:3  
采用半自洽场 (semi-SCF) d轨道波函数模型和点电荷模型,利用高阶微扰公式,在晶体掺杂过渡金属离子后其结构对称性不会被破坏的条件下,由d-d跃迁光谱和EPR谱,确定SrLaAlO4: Cr3+晶体的局域结构.计算发现,掺入Cr3+后,晶体的键长为:R′⊥=0.1922nm, R′∥=0.2197nm.所得计算结果与实验值吻合得很好.  相似文献   

17.
通过水热合成法,成功合成了化合物[(CH3)2NH]3[H3PMo12O40],并通过单晶X射线衍射,IR,XRD,元素分析和电化学分析对该化合物进行表征.该化合物中,Keggin型磷钼酸之间通过氢键形成二维折叠层,这些层按照ABCD沿c轴方向堆积.二甲胺分子分布在层间,通过氢键连接相邻的来自不同层的两个Keggin型磷钼酸,将二维折叠层进一步拓展成三维超分子骨架.  相似文献   

18.
Abstract  [Na(H2O)2(C18H15O6SO3)]2 was synthesized by sulfated 5-hydroxy-6,7,4′-trimethoxyisoflavone with concentrated sulfuric acid. Single-crystal X-ray diffraction study indicates that it is a dimeric centrosymmetric species. The coordination polyhedron of each Na(I) atom exhibits a distorted trigonal bipyramidal geometry. The dimeric units are linked by intermolecular hydrogen bonds C–H⋯π, C–H⋯O and O–H⋯O to result in a three-dimensional framework. Graphical Abstract  [Na(H2O)2(C18H15O6SO3)]2 was synthesized by sulfated 5-hydroxy-6,7,4′-trimethoxyisoflavone with concentrated sulfuric acid. The coordination polyhedron of each Na(I) atom exhibits a distorted trigonal bipyramidal geometry. The dimeric centrosymmetric units are linked by intermolecular hydrogen bonds C–H⋯π, C–H⋯O and O–H⋯O to result in a three-dimensional framework. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.  相似文献   

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