108 resultados para ER-2O-3


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Er3+ -doped Gd2SiO5 (Er:GSO) single crystal with dimensions of circle divide 35 x 40 mm(3) has been grown by the Czochralski method. The absorption and fluorescence spectra of the Er:GSO crystal were measured at room temperature. The spectral parameters were calculated based on Judd-Ofelt theory, and the intensity parameters Omega(2), Omega(4) and Omega 6 are obtained to be 6.168 x 10(-20), 1.878 x 10(-20), and 1.255 x 10(-20) cm(2), respectively. The emission cross-section has been calculated by Fuechtbauer-Ladenbury formula. (c) 2007 Elsevier B.V. All rights reserved.

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The contamination and distribution of polychlorinated dibeinizo-p-dioxins and dibenzofurans (PCDD/Fs) from two agricultural fields of a heavily polluted lake area in China (Ya-Er Lake) are presented. The vertical distribution pattern of total PCDD/Fs in soil cores reveals that the maximum concentration was in the layer of 20-30 cm. The concentrations in the top layer of soil at the two sites were similar (17.48 ng/kg at Site 1 and 18.10 ng/kg at Site 2), but the maximum concentration of Site 1 (120.8 ng/kg) was two times higher than that of Site 2 (64.39 ng/kg). The maximum concentration of PCDD/Fs in mud cores in rice fields (0-50 cm) at Sites 1 and 2 was in the layer of 0-10 cm. The maximum PCDD/F concentration in the top layer in mud at Site 1 (203.1 ng/kg) was higher than that at Site 2: (143.3 ng/kg). Significant correlations were found between the mind PCDD/Fs and the organic carbon content (R = 0.9743, P< 0,05 at Site 1; R = 0.9821, P< 0.05 at Site 2), the two variables being highly correlated (R = 0.9049, P< 0.05, at Site 1; R = 0.9916, P< 0.05 at Site 2). All correlation coefficients were significant at the 95% level. Concentrations were highly correlated with organic carbon, indicating that sorption to organic carbon was the dominant mechanism. Using principal component analysis, the homologue profiles of soil, mud, and plants (rice and radish) were compared. The PCDD/F patterns in plants were found not to be correlated to those in soil and mud. This suggests that atmospheric deposition may be the main source of PCDD/Fs in rice grain. However, mixed exposure involving uptake mechanisms and atmospheric deposition is considered main the source of PCDD/F pollution in radishes. (C) 2002 Elsevier Science (USA).

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The sediment of Ya-Er Lake had been heavily polluted by polychlorinated dibenzo-p-dioxins and dibenzofurans (PCDD/Fs) from the former chloralkali industry. The total amounts of PCDD/Fs and I-TEQ decreased along the water flow direction and also decreased from top to bottom layers of sediment cores. Sediment of Pond 1 was dominated by PCDF, especially TCDF. In contrast, in the other four ponds, PCDD dominated in all layers and octachlorinated dibenzo-p-dioxin (OCDD) predominated in all of the homologues. When homologue profiles from sediments and water samples were compared using principal component analysis (PCA), the first two principal components represented 95.2% of the variance in the data. The first component explained 75.9% of the variance and the second one 19.3%. Two clusters were most distinct, presenting a shift in PCDD/Fs composition from PCDF to heptachlorinated dibenzo-p-dioxin (HpCDD) and OCDD in sediments and water from Pond I to Ponds 2-5. The pattern variation between Pond 1 and Ponds 2-5 in Ya-Er Lake was most likely due to the change of process in the chemical plant after the dams between the ponds were built. The results of the present study also showed that log K-oc of PCDD/Fs calculated from data of sediment and water in the field were comparable with theoretical log K-oc. The results also implied that the concentrations of PCDD/Fs in water and sediments could be predicted from each other by log K-oc. (C) 2001 Elsevier Science Ltd. All rights reserved.

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The concentrations of polychlorinayed dibenzo-p-dioxins and dibenzofurans (PCDD/F) in surface sediment, soil, human hair, acid fish muscle from Ya-Er Lake area, China, were analyzed. The results showed that there were very high concentrations of PCDD/F existing in these samples. The results also indicated that Ya-Er Lake, which received a large amount of waste water from a nearby chloroalkali plant, was heavily polluted by PCDD:F. The present study demonstrated that those congeners, which possess at least three chlorine atoms in the lateral position with a fourth chlorine atom in the neighborhood bond of the third single chlorine atom, such as 1,2,7,8-TCDF and 2,3.6,7-TCDF, were very resistant to biodegradation due to the "neighbor effect" of every two chlorine atoms. The present study suggested that human hair may be a suitable alternative bioindicator for detecting PCDD/F exposure. (C) 2001 Elsevier Science Ltd. All rights reserved.

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Bioaccumulation of PCDD/F in the foodweb was investigated in the Ya-Er Lake area, which was heavily polluted by PCDD/F. The high concentrations of PCDD/F in sediment can be transferred and bioaccumulated by aquatic organisms and humans through various pathways. Benthonic invertebrate animals and aquatic plants with a lot of fibers in the root can accumulate PCDD/F from sediment and water. Snail (Bellamya aeruginosa), shrimp (Macrobranchium sp.) and freshwater mussel (Acuticosta chinensis (Lea)) took up PCDD/F from the water and maintained the emission patterns, whereas fish tended to selectively accumulate 2,3,7,8-substituted isomers. The tissues of fish-eating bird and duck (Anas platyrhynchos) were very highly contaminated by PCDD/F due to ingestion of fish and other aquatic organisms from sediment. The residual concentration in breast milk depended on the original concentration of PCDD/F in the food. A resident in Ya-Er Lake area showed a daily intake of PCDD/ F of about 9.14 pg TEQ/kg body weight/day. This is higher than the tolerable daily intake (TDI) for PCDD/F (1 pg TEQ/kg body weight/day), which was recommended by the World Health Organization (WHO). (C) 2001 Elsevier Science Ltd. All rights reserved.

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Sources and distribution of polycyclic aromatic hydrocarbons (PAH) in the Ya-Er Lake area (Hubei, China) sediment cores of 3 ponds in the shallow Ya-Er Lake were investigated for 16 PAH. Analytical procedure included extraction by ultrasonication, clean-up by gel-permeation and quantification by HPLC with fluorescence detection. The total PAH amount in sediment samples of the Ya-Er Lake ranged from 68 to 2242 mu g/kg. Concentrations decreased from pond 1 to pond 3 and from upper to lower sediment layers. In addition a soil sample from Ya-Er Lake area showed a total PAH amount of 58 mu g/kg. The PAH pattern in lower sediment layers were similar to that of the soil sample which indicates an atmospheric deposition into the sediments prior to 1970 only. The PAH profile of upper sediment samples, which differs completely from that of lower layers, may be explained by a gradually increasing input of mixed combustion and raw fuel sources since 1970. Therefore the origin of increased PAH contamination in Ya-Er Lake during the last 3 decades has been probably an industrial waste effluent in pond 1.

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Silicon nitride films were deposited by plasma-enhanced chemical-vapour deposition. The films were then implanted with erbium ions to a concentration of 8 x 10(20) cm(-3). After high temperature annealing, strong visible and infrared photoluminescence (PL) was observed. The visible PL consists mainly of two peaks located at 660 and 750 nm, which are considered to originate from silicon nanocluster (Si-NCs) and Si-NC/SiNx interface states. Raman spectra and HRTEM measurements have been performed to confirm the existence of Si-NCs. The implanted erbium ions are possibly activated by an energy transfer process, leading to a strong 1.54 mu m PL.

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In this study, we report the dependences of infrared luminescence properties of Er-implanted GaN thin films (GaN:Er) on the kinds of substrates used to grow GaN, the growth techniques of GaN, the implantation parameters and annealing procedures. The experimental results showed that the photoluminescence (PL) intensity at 1.54 mum was severely influenced by different kinds of substrates. The integrated PL peak intensity from GaN:Er /Al2O3 (00001) was three and five times stronger than that from GaN:Er /Si (111) grown by molecular beam epitaxy (MBE) and by metalorganic chemical vapor deposition (MOCVD), respectively. The PL spectra observed from GaN:Er/Al2O3 (0001) grown by MOCVD and by MBE displayed a similar feature, but those samples grown by MOCVD exhibited a stronger 1.54 mum PL. It was also found that there was a strong correlation between the PL intensity with ion implantation parameters and annealing procedures. Ion implantation induced damage in host material could be only partly recovered by an appropriate annealing temperature procedure. The thermal quenching of PL from 15 to 300 K was also estimated. In comparison with the integrated PL intensity at 15 K, it is reduced by only about 30 % when going up to 300 K for GaN:Er/Al2O3 sample grown by MOCVD. Our results also show that the strongest PL intensity comes from GaN:Er grown on Al2O3 substrate by MOCVD. (C) 2004 Elsevier B.V. All rights reserved.

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We extend the use of Raman spectroscopy to investigate the modes of Er-implanted and Er + O co-implanted GaN, and discuss the influence of O ions on Er3+ -related infrared photoluminescence (PL). It is found that Er3+ implantation introduces new Raman peaks in Raman spectra at frequencies 300 and 670 cm and one additional new peak at 360cm is introduced after Er + O implantation. It is proposed that the broad structure around 300 cm(-1) mode originates from disorder-activated scattering (DARS). The Raman peak at 670 cm is assigned to nitrogen vacancy related defects. The 360 cm peak is attributed to the O implantation induced defect complexes (vacancies, interstitial, or anti-sites in the host). The appearance of the 360 cm(-1) mode results in the decrease of the Er3+ -related infrared PL of GaN: Er + O.

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Deep level transient spectroscopy measurements were used to characterize the electrical properties of metal organic chemical vapor deposition grown undoped, Er-implanted and Pr-implanted GaN films. Only one deep level located at 0.270 eV below the conduction band was found in the as-grown GaN films. But four defect levels located at 0.300 eV, 0.188 eV, 0.600 eV and 0.410 eV below the conduction band were found in the Er-implanted GaN films after annealing at 900 degrees C for 30 min, and four defect levels located at 0.280 eV, 0.190 eV, 0.610 eV and 0.390 eV below the conduction band were found in the Pr-implanted GaN films after annealing at 1050 degrees C for 30min. The origins of the deep defect levels are discussed. After annealing at 900 degrees C for 30min in a nitrogen flow, Er-related 1538nm luminescence peaks could be observed for the Er-implanted GaN sample. The energy-transfer and luminescence mechanism of the Er-implanted GaN film are described.

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目前,国内外对于铕和铽等稀土配合物的可见区发光和应用都有大量研究,但对具有近红外发光(800-1700 nm)性能的稀土配合物的研究还处于起步阶段。由于稀土的近红外发光在光纤通讯、激光系统及诊断学等方面应用具有特殊的优点,越来越引起人们的兴趣和重视。 稀土近红外发光配合物的致命弱点是其光、热和化学稳定性较差,从而限制了其在很多领域的实际应用。而溶胶-凝胶材料和介孔材料具有良好的光、热和化学稳定性,能改善客体分子的结构环境和化学微环境,从而能有效提高客体分子的发光性能。因此,本论文将具有优良近红外发光性能的稀土配合物分别与上述两种基质复合,从实验和理论研究稀土近红外发光杂化材料的性能和应用价值,制备出具有良好稳定性的高效稀土近红外发光杂化材料,以期为光纤通讯、激光等领域提供潜在的候选材料。围绕这一宗旨,开展了如下工作: 通过原位技术分别得到了掺杂和嫁接[Ln(dbm)3phen]化合物(Ln = Er, Nd, Yb)的杂化凝胶材料,Ln-D-P gel和Xerogel-Ln。通过对其近红外发光性能的研究,表明材料中配体能很好的保护稀土离子,并将能量有效的传递给稀土离子。采用Judd-Ofelt理论对所得部分材料进行了光谱分析,基于实验数据和理论分析表明其具有潜在的光放大和激光应用价值。 选择了两种含全氟化烷基链的β-二酮配体Hhfth和Htfnb,通过功能化的phen-Si配体,将三元配合物[Ln(hfth)3phen] (Ln = Er, Nd, Yb, Sm)和[Pr(tfnb)3phen]成功共价嫁接到介孔MCM-41和SBA-15杂化材料中,得到的衍生材料Ln(hfth)3phen–MCM-41、Pr(tfnb)3phen–MCM-41和Ln(hfth)3phen–SBA-15、Pr(tfnb)3phen–SBA-15都保持了高度有序的介孔p6mm结构,并展现出稀土离子特征的近红外发射。所得稀土配合物功能化的材料的发射光谱能完全覆盖对光通讯极具应用价值的1300-1600nm区域。 通过对Er(dbm)3phen–M41(X, Y) (X = 1~14, Y = 3, 6, 12, 18, 24 h)材料系统的比较研究,选择了X = 12, Y = 6作为合成目标材料的优化参数,通过功能化的phen-Si配体将[Ln(dbm)3phen]配合物共价嫁接于有序介孔MCM-41和SBA-15中(Ln = Er, Nd, Yb),所得两类材料Ln(dbm)3phenM41和Ln(dbm)3phenS15都保持了很好的介孔有序性,并具有良好的近红外发光性能。通过对Ln(dbm)3phenM41和Ln(dbm)3phenS15两类材料发光行为的比较,以及两类材料中稀土离子的含量及孔结构的分析,推出以SBA-15为载体得到的材料在相对发光强度和荧光寿命上,均比以MCM-41为载体的材料有所提高。 通过对8-羟基喹啉配体进行改性,合成了具有双功能的配体Q-Si,继而合成了共价嫁接8-羟基喹啉衍生物的介孔杂化材料Q–SBA-15,其形貌均一,并具有高度有序的介孔p6mm结构。通过配体交换反应,得到了嫁接稀土喹啉配合物的具有近红外发光性能的介孔杂化材料LnQ3–SBA-15 (Ln = Er, Nd, Yb),其仍然保持高度有序的介孔结构,且外形呈现与母体材料Q–SBA-15相似的弯曲圆柱状。激发配体的吸收,LnQ3–SBA-15材料都分别展现出相应稀土离子特征的近红外发射,并详细分析和讨论了所得介孔杂化材料的近红外发光性能。

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本工作用固相反方法、以炭保护或在N_2-H_2还原气氛中,两次灼烧,合成了一系列烯土取代的卤磷酸盐发光体,其反应是M_2~ICO_3 + M_3~(II)(PO_4)_2 + M_2~(III)O_3 + (NH_4)_2HPO_4 + M~(II)F_2 → M_x~IM_(10-2x)~(II)M_x~(III)(PO_4)_6F_2 + NH_3 + H_2O式中:M~I = Li~+, Na~+, K~+; M~(II) = Ca~(2+), Sr~(2+); M~(III) = Y~(3+), La~(3+), Gd~(3+); X = 0.5, 1, 2, 3。通过X-射线分析法和以Eu~(3+)作为荧光离子探针方法确定了样品的物相和晶体结构,表明它与M_(10)~(II)(PO_4)_6F_2同属六方晶系(Pb_3/m)。并用图解外推法求得样品的晶胞参数a和c分别为9.41和6.89 A。在研究了M~I, M~(II)和M~(III)为不同阳离子,X为不同值时,取代物的物相和结构变化以及对Ce~(3+)发光和能量传递影响规律的基础上,以Na_2Ca_6La_2(PO_4)_6F_2为基本体系比较详细地研究了Ce~(3+)的发光,Ce~(3+)-Mn~(2+), Ce~(3+)-Re~(3+) (Re~(3+) = Pr~(3+)、Nd~(3+)、Sm~(3+)、Tb~(3+)、Dy~(3+)、Tm~(3+)、Ho~(3+)、Er~(3+))以及Ce~(3+)-Mn~(2+)-Re~(3+) (Re~(3+) = Dy~(3+), Nd~(3+))的能量传递。实验发现,Na_2Ca_6La_2(PO_4)_6F_2:Ce~(3+)是较强的紫外光发射体,发射谱带是由338和358nm两个宽带峰组成的,相应于~2D-~2F_(5/2)和~2D-~2F_(1/2)跃迁。发射强度和~2D-~2F_(6/2),~2D-~2F_(7/2)两种辐射跃迁几率相对大小与温度,Ce~(3+)的浓度有关;F~-含量对发射强度也有强烈的影响。我们认为,浓度和温度的影响是由于Ce~(3+)-Ce~(3+)的能量迁移作用。实验发现,Ce~(3+)能有效地敏化Mn~(2+)的发光,得到高效的黄色荧光发射体。Ce~(3+)对Re~(3+)的作用可以分为三类:A). Ce~(3+)-Sm~(3+)、Tb~(3+)、Dy~(3+)、Tm~(3+);B).Ce~(3+)-Nd~(3+),Pr~(3+);C). Ce~(3+)-Ho~(3+), Er~(3+)。在A,B类型中,Ce~(3+)能有效地敏化这些稀土离子,但能量传递效率(η_T)_A > (η_T)_B。在Ce~(3+)-Ho~(3+)、Ce~(3+)-Er~(3+)类型中,Ho~(3+)、Er~(3+)不产生可见辐射,Ce~(3+)的发射强度也显著降低。在Ce~(3+)-Mn~(2+)-Re~(3+)三元中心体系中,Ce~(3+)的能量可直接传递给Mn~(2+)和Re~(3+)中心,还可通过Ce~(3+)-Mn~(2+)-Re~(3+)的途径传递。通过研究中心离子的浓度效应,温度效应、测定激发光谱、荧光光谱、荧光衰减曲线的荧光寿命,能够证实:在Ce~(3+)-Mn~(2+)、Ce~(3+)-Re~(3+)、Ce~(3+)-Mn~(2+)-Re~(3+)的能量传递属于无辐射共振传递相互作用类型。符合M. Yokata等人提出的偶极-偶极相互作用扩散限制传递历程。我们还利用Ce~(3+)、Ce~(3+)-Mn~(2+)、Ce~(3+)-Re、Ce~(3+)-Mn~(2+))-Re~(3+)激活体系中Ce~(3+)的发射强度和荧光寿命等数据计算了Ce~(3+)的能量传递效率。发现两种结果相差较大,为了准确地表达Ce~(3+)的敏化效果,在分析上了产生这种误差的原因后,提出了两种传递效率表示式(η_f, η_R)。

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我们利用湿法制备了单一稀土氟化物LnF_3(Ln = La 、Ce、Nd、Gd、Tb、Dy、Er、Yb、Y), 并采用高温固相反应制备了稀土掺杂氟化物Ln_(1-x)MxF_(3-δ)(Ln = La、Ce、Gd、Yb、Y M = Ca、Sr、Ba)。用X射张衍射方法研究了它们的晶体结构。对单一稀土氟化物,LaF_3、CeF_3、NdF_3为六方晶系,GdF_3、TbF_3、DyF_3、DrF_3、YbF_3、YF_3为正交晶系。对掺杂氟化物,La_(0.95)Ba_(0.05)F_(3-δ)、Ce_(0.95)Ca_(0.05)F_(3-δ)、Yb_(0.70)Sr_(0.30)F_(3-δ)为固溶体,Ce_(0.95)Ca_(0.05)F_(3-δ)的晶胞参数比CeF_3的略为变小;Gd_(0.85)Ca_(0.15)F_(3-δ)、Y_(0.71)Ca_(0.29)F_(3-δ)为新化合物,Gd_(0.85)Ca_(0.15)F_(3-δ)的晶体结构由GdF_3的正交晶系变为六方晶系,其晶胞参数为:a=3.973A, C=7.124A, γ=120°, Y_(0.71)Ca_(0.29)F_(3-δ)化合物的晶体结构与YF_3相同为正交晶系,晶胞参数却较小:a=3.683A、b=6.978A, c=3.396A。 我们对氟化物的烧结陶瓷片进行了直流电导率测量。对单一稀土氟化物,结果表明六方结构的化合物的电导率高于正交结构的,对于相同结构的氟化物,一般地,稀土离子半径越大,电导率越高;对于掺杂氟化物,由于二价碱土金属离子掺杂可以提高氟离子空位浓度,因此掺杂物的电异率均高于对应的单一稀土氟化物,其中Gd_(0.85)Ca_(0.15)F_(3-δ)掺杂后变成更利于离子导电的六方结构。采用压片工艺,以La_(0.95)Ba_(0.05)F_(3-δ)、Ce_(0.95)Ca_(0.05)F_(3-δ)、Gd_(0.85)Ca_(0.15)F_(3-δ)和Y_(0.71)Ca_(0.29)F_(3-δ)为固体电解质材料制备电位输出式氧传感器件,并利用调节N_2、O_2流量比控制氧分压的方法,对器件的敏感性能进行测试。结果表明该类器件可在150 ℃的低温下对氧气敏感,器件的输出电位差与氧分压的对数值有较好的线性关系。器件的响应时间在2分与9分之间。该类器件的敏感机理是:氧气先吸附敏感电极上,发生还原反应后生成的氧负离子在敏感电极与固体电解质界面上发生晶格置换反应,使得氧分压的改变通过快离子即氟离子在两个界面上(另一界面为参比电极与固体电解质界面)的电化学势差的变化与输出电位差值的改变联系起来,从而实现利用输出电位差测定氧分压的目的。根据使用的敏感电极材料,可以有单电子反应和双电子反应两种敏感机理。器件是由参比电极、固体电解质、敏感电极三个部分构成。我们采用固定其中二个部分的材料,改变第三个部分的用料的方法,对器件的敏感性进行了对比研究:A、我们首先固定固体电解质为Ce_(0.95)Ca_(0.05)F_(3-δ)、敏感电极材料为Pt黑,采用不同的参比电极材料Bi+BiF_3、Sb+SbF_3、Mg+MgF_2、Zn+ZnF_2制备了器件。性能测试结果表明使用Bi+BiF_3参比电极材料的器件稳定性和敏感性都比其它器件好。器件的输出电位差取决于参比电极氟化物的标准生成自由能的大小。B、固定Bi+BiF_3为参比电极材料,Ce_(0.95)Ca_(0.05)F_(3-δ)为固体电解质,使用不同的敏感电极材料Pt黑、Pd粉、Ag粉和RuO_2制备器件。性能测试结果表明:Pt材料器件的精确度较高,Pd材料器件的响应最快(2分),RuO_2材料器件的敏感性较好。使用Ag、RuO_2敏感电极材料的器件采用的是单电子反应敏感机理:O_2 + e <-> O_2~-, O_2~- + V_F + F_(F-bar)~- <-> O_(F-bar) + O_F + F_(F-bar)。而使用Pt、Pd敏感电极材料的器件采用双电子反应敏感机理:O_2 + 2e <-> 2O~-, 2O~- + F_(F-bar) <->O_(F-bar) + F~-。C、我们固定Bi+BiF_3为参比电极材料,Pt和RuO_2为敏感电极材料,使用La_(0.95)Ba_(0.05)F_(3-δ)、Ce_(0.95)Ca_(0.05)F_(3-δ)、Gd_(0.85)(Ca_(0.015)F_(3-δ)、Yb_(0.70)Ca_(0.29)F_(3-δ)制备了两个系列的器件。结果表明,无论是使用Pt还是使用RuO_2为敏感电极材料,都有下列的结论:用Ce_(0.95)Ca_(0.05)F_(3-δ)的器件的精确度较高,La_(0.95)Ba_(0.05)F_(3-δ)材料器件的敏感性最好,而Gd_(0.85)(Ca_(0.015)F_(3-δ的响应最快(Pt器件2分,RuO_2器件5分)。并未发现同时具备各种较好性能的器件,与敏感电极材料对器件性能的影响相比,固体电解质材料的影响要小。对于材料完全相同的器件,我们还对工艺条件影响作了初步研究。制备器件的工艺条件由于各种难以控制的因素不会每次、每批完全相同,工艺条件的差别也会影响器件的各方面性能。研究结果表明,工艺差别对器件的输出电位差值和响应时间的影响较大,对敏感性能的影响则较小。

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胺类萃取剂具有其独特优点,特别是伯胺,因含有活泼氢,既能作为“阴离子交换剂”,又能与被萃的含氧金属络阴离了形成氢键而溶剂化,同时伯胺为一路易斯碱,可作为配体与某些金属离子形成配位键等,因而已广泛地用于金属离子的提纯与分离工业中。然而,1)为了寻找新的、更有效的萃取及协同萃取体系,以适应分析分离各种金属离子,改善金属离子的分离工艺;2)研究萃取和协同萃取的一般规律,探寻其内在规律性,充实完善萃取化学原理的内容;3)研究多元配合物的组成、结构和机理;4)系统地研究和比较不同结构胺类萃取剂与其它萃取剂对金属离子的萃取及协同萃取的相互作用,探讨多元配合物的形成条件等,因此,研究伯胺N_(1923)与其它萃取剂在不同酸度、不同条件,不同体系中对Zn(II)、Cd(II)、Re(III)的萃取及协同萃取具有一定意义。本文分别研究了伯胺N_(1923)与中性磷试剂对ZnCl_2、CdCl_2、Zn(SCN)_2的协同萃取;伯胺N_(1923)与HPMBP对RE(III)的协同萃取以及伯胺N_(1923)在不同介质中对Sc(III)的萃取机理等,并用得到了一些有意义的结果与结论。一、伯胺N_(1923)与中性磷萃取剂(TBP, DBBP)对Zn(II)、Cd(II)的协同萃取1. 伯胺N_(1923)与TBP、DBBP对ZnCl_2的协萃取 研究了伯胺N_(1923)与TBP、DBBP的正庚烷溶液从盐酸介质中对ZnCl_2的萃取机理,用斜率法、等摩尔系列法确定了协萃配合物组成为:(RNH_3Cl)_3·ZnCl_2·B、(RNH_3Cl)_2·ZnCl_2·B (B = TBP·DBBP)协萃反应为:ZnCl_2 + (RNH_3Cl)_3_((o)) + TBP_((o)) →~(K_(12)(TBP) (RNH_3Cl)_3·ZnCl_3·ZnCl_2·TBP_((o)) ZnCl_2+Z/3(RNH_3Cl)_(3(o)) + DBBP_((o)) → (RNH_3Cl)_2 · ZnCl_2·DBBP_((o))协萃配合物生成反应为:(RNH_3Cl)_3·ZnCl_(2(o)) + TBP_((o))→~(B_(12)(TBP) (RNH_3Cl)_3·ZnCl_2·TBP_((o)) (RNH_3Cl)_3·ZnCl_(2(o)) + DBBP_((o)) →~(B_(12)(DBBP) (RNH_3Cl)_2·ZnCl_2·DBBP_((o)) + RNH_3Cl_((o))同时发现,中性磷试剂对Zn(II)的协萃效应大小影响有下列关系:DBBP>TBP。并求得了协萃反应平衡常数和协萃配合物生成反应平衡常数。在研究溶剂对协同效应影响时发现,对芳香烃及其衍生物,分配比(D)与溶剂介电常数(ε)的关系为D_∝1/ε,而对芳香烃及其衍生物,分配比(D)与介电常数(ε)的关系为D_∝ε。讨论了温度对协萃反应的影响,对协萃配合物的IR、NMR谱也进行了研究。2.伯胺N_(1923)与TBP对Zn_(SCN)_2的协同萃取研究了伯胺N_(1923)与TBP的庚烷溶液从硝酸底液中对Zn(SCN)_2的萃取机理,用等摩尔系列法、斜率法确定了TBP和Zn(SCN)_2以及伯胺N_(1923)与TBP对Zn(SCN)_2的协萃配合物组成分别为:Zn(SCN)_2·3TBP. (RNH_3)_2Zn(SCN)_4·TBP,协谇反应为:Zn(SCN)_4~(2-) + (RNH_3NO_3)_(2(o)) + TBP_((o)) → (RNH_3)_2Zn(SCN)_4·TBP_((o)) + 2NO_3~-协萃配合物三种可能生成反应为(RNH_3)_2Zn(SCN)_(4(o)) + TBP_((o)) → ~(B'12) (RNH_3)_2Zn(SCN)_4·TBP_((o)) (a) (RNH_3NO_3)_(2(o)) + Zn(SCN)_2·3TBP_((o)) + 2SCN~-→~(β"12)→(RNH_3)Zn(SCN)_4βTBP_((o))+2TBP_((o))+2NO_3~- (b) (RNH_3NO_3)_(2(o)) + (RNH_3)_2Zn(SCN)_(4(o)) + 2SCN~- + Zn(SCN)_2.3TBP_((o)) →~(β"12)→R(RNH_3)_2Zn(SCN)_4.TBP_((o)) + 2NO_3~- + TBP_((o)) (c) 求得了协萃反应及生成反应的平衡常数,并由生成反应常数可知:β"'_(12) > β'_(12) > β"_(12),即反应(c)对协萃配合物的生成贡献最大,其次反应(a),最小的是反应(b),同时还发现,不同阴离子对协萃效应影响有下列关系:SCN~- > Cl~_。并对协萃配合物的IR谱进行了研究,讨论了温度对协萃反应的影响。3. 伯胺N_(1923)与TBP、DBBP对Cd(II)的协同萃取研究了伯胺N_(1923)与TBP、DBBP的正庚烷溶液从盐酸介质中对Cd(II)的协同萃取,用等摩尔系列法、斜率法确定了协萃配合物组成为(RNH_3Cl)_2·CdCl_2·B,协萃反应及协萃配合物生成的反应分别为:CdCl_2 + 2/3 (RNH_3Cl)_(3(o)) + B_((o)) →~(K_(12)) → (RNH_3Cl)_2·CdCl_2·B_((o)) (RNH_3Cl_3)·CdCl_2_((o)) + B_((o)) →~(BR)(RNH_3Cl)_2·CdCl_2·B_((o)) + RNH_3Cl_((o))求得了协萃反应及生成反应平衡常数,计算了协萃反应的热力学函数值,结果还发现与Zn(II)协同萃取比较,协同效应大小有下列关系:Zn(II) > Cd(II),由实验结果证实了“萃取效应大,则协萃效应小,反之,萃取效应小,则协同效应大”这一结论。并对协萃配合物的IR、NMR谱进行了研究。二. 伯胺N_(1923)与HPMBP对RE(III)的协同萃取研究了伯胺N_(1923)与HPMBP的二甲苯溶液在盐酸介质中对RE(III)的协萃机理(RE~(3+ = La~(3+), Pr~(3+), Eu~(3+), Gd~(3+), Tb~(3+), Er~(3+), Yb~(3+)和Y~(3+))用斜率法及等摩尔系列法确定了协萃配合物组成为RNH_3Ln(PMBP)_4。求得了关于Pr(III)的协萃反应及生成反应的平衡常数值,协萃反应及生成反应分别为:Ln~(3+) + 4HPMBP_((o)) + RNH_3Cl_((o)) → RNH_3LN(PMBP)_(4(o)) + 4H~+ + Cl~- Ln(PMBP)_(3(o)) + RNH_3Cl_((o)) → RNH_3Ln(PMBP)_(4(o)) + H~+ + Cl~- 结果还发现协萃系数(R)随稀土元素的原子序数(Z)递变而出现“双峰效应”(未见文献报道),而且随RNH_3Cl浓度增加到某一一出现反协同效应。同时研究了关于Pr(III)协萃配合物的IR、NMR谱。三、伯胺N_(1923)在硝酸盐及硫氰酸盐混合介质中对Sc(III)的萃取研究了RNH_3NO_3在硝酸盐和硫氰酸盐混合介质中萃取Sc(III)的机理,结果发现,钪是以Sc(OH)_2~+形式萃入有机相的,且SCN~-, NO_3~-对RNH_3nO_3萃取Sc(III)具有协同效应,并且斜率法、连续变化法及PH值测定确定了萃取反应为:Sc(OH)_2~+ + SCN~- + 2(RNH_3NO_3)_(2((o)) → (RNH_3nO_3)_4.Sc(OH)_2SCN_((o)) Sc(OH)_2~+ + SCN~- + NO_3~- + (RNH_3NO_3)_(2(o)) → (RNH_3NO_3)_2.Sc(OH)(SCN)NO_3 + OH~-求得了反应的平衡常数及热力学函数值。