96 resultados para 765-14


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A perfect single crystal of nylon-2,14 was prepared from 0.02% (w/v) 1,4-butanediol solution by a "self-seeding" technique and isothermal crystallization at 120 and 145 degreesC. The morphology and structure features were examined by transmission electron microscopy with both image and diffraction modes, atomic force microscopy, and wide-angle X-ray diffraction (WAXD). The nylon-2,14 single crystal grown from 1,4-butanediol at 145 degreesC inhabited a lathlike shape with a lamellar thickness of about 9 nm. Electron diffraction and WAXD data indicated that nylon-2,14 crystallized in a triclinic system with lattice dimensions a = 0.49 nm, b = 0.51 nm, c = 2.23 nm, alpha = 60.4degrees, beta = 77degrees, and gamma = 59degrees. The crystal structure is different from that of nylon-6,6 but similar to that of other members of nylon-2Y.

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A novel organic-inorganic hybrid vanadium oxide [V4O10(o-phen)(2)], involving all vanadium atoms present in +5 oxidation, has been hydrothermally synthesized and characterized by elemental analysis, IR, UV-vis, ESR, XPS spectra and TG-DTA thermal analysis. The single-crystal X-ray diffraction shows that the red-brown crystal is formed in the triclinic system, space group P (1) over bar, a = 9.782(2), b = 6.5124(14), c = 19.765(4) Angstrom, alpha = 89.94(2)degrees, beta = 100.66(2)degrees, gamma = 89.86(2)degrees. The title compound exhibits an infinite one-dimensional ladder-type tetravanadate skeleton with organonitrogen donors of o-phenanthroline ligands coordinated directly to the vanadium oxide framework.

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分析了室温下晶体在紫外、可见区的吸收、荧光和红外光谱,利用Judd Ofeld理论计算了PrPP和La0.2Pr0.8PP晶体中Pr3+的实验振子强度,PrPP和La0.2Pr0.8PP晶体中Pr3+离子振子强度变化不大,说明在该晶体中Pr3+的浓度猝灭效应较小。红外光谱和结构分析确定了晶体的结构为单斜晶系,并观察到Pr3+的3P0 3H6跃迁的红色发射很强。

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用水热法研究了La12xPr xP5O14(LaPrPP)(0 < x < 1,原子百分含量)晶体的生长,测定了La0.2Pr0.8PP晶体结构为 单斜晶系,空间群为P21/c。晶体的密度为3.27g/cm3,分解温度为915℃。分析了室温下晶体在紫外、可见区的吸 收、荧光和红外光谱,利用Judd2Ofeld 理论计算了PrPP 和La0. 2Pr0. 8PP 晶体中Pr3 + 的实验振子强度,得到一些规律性结果,观察到Pr3 + 的3 P0 —3 H6 跃迁的红色发射很强。

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使用复杂晶体上化学键理论计算了 RBa2 Cu4 O8(R=Dy,Ho,Er,Tm ,Yb)和 Y2 Ba4 Cu7O14 .3 的化学键参数 .结果表明 ,Cu O链上的 Cu O键共价性大于它们在 Cu O2 面的共价性 .当金属元素与氧形成五配位时 ,其共价性的数值大于这些元素在六配位时的情形

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Petroleum sulfoxide-NH4SCN extraction chromatography was developed for the separation of Y from other rare earth elements. Some chromatographic parameters were chosen and separation factors between Y and other rare earth elements were determined. A column of resin coated with petroleum sulfoxide was used. The Y in the sample was eluted with NH4SCN, then titrated with EDTA. The recovery was 67%-120% and relative standard deviation +/-4.0%-19.4%. This method can be applied to the determination of trace amounts of rare earth impurities in Y2O3 with a purity of 99.999 9%-99. 999 99%.

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用水热法合成了 H8[P4 W14 O58Na4 (H2 O) 2 0 ]· 16 H2 O,通过 X射线单晶衍射、元素分析和IR进行了结构表征 ,用 TG- DTA研究了热稳定性 .晶体属三斜晶系 ,P1空间群 ,a=1.1379(2 )nm,b=1.36 32 (3) nm,c=1.6 2 71(3) nm;α=78.2 0 (3)°,β=71.2 0 (3)°,γ=71.6 2 (3)°;V=2 .2 52 5(8) nm3 ,Z=1,Mr=4 374 .38,Dc=3.2 2 5mg/ cm3 ,μ=18.0 0 7mm-1,F(0 0 0 ) =1972 ,R=0 .0 74 2 ,Rw=0 .2 0 0 4 .标题化合物的阴离子是由两个 PW7O2 9Na2 (H2 O) 10 亚单元通过与两个磷原子上键合的氧连接而成 ,分子内形成了一个 0 .6 6 14nm× 0 .3189nm的微孔.

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Pr~(3+)离子的能级结构丰富,在紫外可见区有很好的荧光发射。因此,以Pr~(3+)为激活离子的发光材料研究工作引起了人们的关注。轻稀土五磷酸盐晶体结构为单斜晶系,空间群为P_(1/2)/C,稀土离子处在隔离的多面体中,离子间的作用减弱,即使在化学计量比的PrP_5O_(14)仍得到激光输出。本文采用水热法生长出La_(1-x)Pr_xP_5O_(14)

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本文研究了电感耦合等离子体原子发射光谱分析Kalman滤波法测定高纯氧化铥中的14种其他稀土杂质的方法。Kalman滤波法有效地消除光谱干扰,可利用受干扰的光谱灵敏线,因而可提高灵敏度,是一种在大量基体存在下测定痕量杂质的有效方法。

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本文研究了电感耦合等离子体原子发射光谱分析Kalman滤波法测定高纯氧化铕中的14种其他稀土杂质的方法。Kalman滤波法有效地消除光谱干扰,可利用受干扰的光谱灵敏线,因而可提高灵敏度,是一种在大量基体存在下测定痕量杂质的有效方法。

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本文采用蒸发溶液法生长出高质量的GdP_5O_(14)晶体,测定了其结构属于单斜晶系、空间群P2_1/c。用荧光光谱仪实验测定GdP_5O_(14)的激发光谱和发射光谱,并计算了Gd ̄(3+)在晶体中的能级。

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本文采用蒸发溶液法生长出一系列 Ce_xGd_(1-x)P_5O_(14)晶体,测定了它们的结构均属于单斜晶系、空间群 P2_1/c,用稳态和时间分辨荧光光谱法研究了该晶体中不同 Gd 含量时的发光性能,观察到随着(1-x)值增加,包含有 Gd~(3+)发射在内的314nm 峰增强和 Ce~(3+)的荧光寿命的有规律递减,说明了存在着 Ce~(3+)至 Gd~(3+)的能量传递。

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水溶液中用硫酸亚铁-异丙苯过氧化氢氧化还原引发体系合成了丙烯酰胺(AM)/2-丙烯酰胺基十六烷磺酸铵(AMC_(16)SNH_4)无规共聚物。用元素分析、IR、~(13)C-NMR和~1H-NMR对其进行了表征。对水溶液性质的研究结果表明,与部分水解聚丙烯酰胺相比,这种新型共聚物有着优异的耐盐性、耐温性和贮存稳定性。

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本文用X射线衍射方法研究 LnP_5O_(14)(Ln=La,Pr,Nd,Sm,Tb)晶体相变表明,相变是晶轴 c 和α夹角β随温度升高逐渐减小的过程,也就是晶体的畸变角δ随温度下降而增加。相变温度随稀土离子半径由 La 到 Tb 减小呈线性增加,最后讨论了晶体缺陷随温度的变化关系。