共查询到20条相似文献,搜索用时 140 毫秒
1.
聚乙烯醇纤维金属配合物的合成和表征 总被引:3,自引:0,他引:3
以聚乙烯醇纤维(PVA)为配体原料,分别与FeCl3、NiCl2、CuCl2和Pb(Ac)2反应,制备了宏观上仍保持原纤维形态的PVA Fe(Ⅲ)、PVA Ni(Ⅱ)、PVA Cu(Ⅱ)、PVA Pb(Ⅱ)纤维配合物(用PVA M表示).用红外光谱仪分别对PVA和4种配合物在4000~400cm-1范围进行傅立叶变换红外光谱测量,对各PVA M的FTIR主要吸收峰做了经验归属,并与PVA的相应吸收峰做对比分析,结果表明,与金属离子形成配合物后,PVA分子中O—H氢键缔合状态被破坏,向高波数位移了65~86cm-1,PVA中的羟基氧与金属离子发生配位作用.PVA Fe(Ⅲ)的XPS显示,PVA中O1s只出现532.5eV单峰,而PVA Fe(Ⅲ)中O1s分裂为531.4eV和532.3eV两个峰,且Fe2p只有一个峰710.9eV,比FeCl3的结合能值711.2eV下降,说明OH氧与Fe3+形成配位键. 相似文献
2.
对生物滤池中不同高度的生物膜和出水悬浮物的碳氢氮三元素和红外光谱进行了分析比较.元素分析结果表明,悬浮物的无机成份比生物膜高.悬浮物和生物膜的红外吸收光谱图主要由蛋白质的吸收带、碳水化合物的吸收带组成.1655 cm-1处的吸收峰为酰胺Ⅰ带,是C=O的伸缩振动,1542 cm-1的吸收峰是酰胺Ⅱ带,是N-H的弯曲振动和C-N的伸缩振动,1240 cm-1是酰胺Ⅲ带,是C-N的伸缩振动和N-H的弯曲振动引起的.1460 cm-1处的吸收峰为CH3和CH2的弯曲振动峰.悬浮物的蛋白质特征峰强度比生物膜低,而1050cm-1处的吸收峰强度比生物膜大. 相似文献
3.
应用变温红外光谱法和二维红外光谱法对聚酰胺-66在303~393K范围内的晶区和非晶区结构及热稳定性进行研究。变温一维红外光谱和变温二阶导数红外光谱的试验结果表明,聚酰胺-66的晶区结构对温度变化较为敏感,而非晶区结构相对稳定。非晶区结构的热稳定性在二维红外光谱试验中得到进一步的证实。从聚酰胺-66的分子结构观察,随着温度的升高,其晶区结构(主要对应O=C-NH-)最先改变,而非晶区结构(主要对应-C-C-)则较为稳定。非晶区的异步二维红外光谱试验结果表明,其晶区结构的吸收波数为1 141cm-1(νamorphous-1)和1 138cm-1(νamorphous-2);而非晶区结构的吸收波数为939cm-1(νcrystal-1)和931cm-1(νcrystal-2)。对聚酰胺-66的非晶区结构和晶区结构还同时进行同步二维红外光谱试验,结果表明:随着温度的升高,两者的红外吸收峰的变化快慢顺序为931cm-1(νcrystal-2)1 141cm-1(νamorphous-1)939cm-1(νcrystal-1)1 138cm-1(νamorphous-2)。 相似文献
4.
镁热还原法制备圆片状氮化硼多晶微粉 总被引:1,自引:1,他引:0
采用三氧化二硼(B2O3)、氯化铵(NH4Cl)和镁粉为反应物,以三氧化二铁(Fe2O3)为催化剂,利用镁热还原法在700~850℃下反应,制备了氮化硼多晶微粉.X射线衍射(XRD)分析表明,产物为六方相,晶格常数a=0.2499 nm,c=0.6682 nm.产物的红外光谱中在790和1380 cm-1处出现了六方氮化硼的特征吸收峰.利用扫描电子显微镜(SEM)观察到产物为圆片状颗粒,平均直径约为0.9μm,平均厚度约为100 nm.讨论了Fe2O3的存在对产物形成的影响. 相似文献
5.
PVA-Fe(Ⅲ)、Zn(Ⅱ)、Cd(Ⅱ)、Hg(Ⅱ)配合物的合成、表征及抗菌性能 总被引:5,自引:0,他引:5
以聚乙烯醇(PVA)为高分子配体,与金属离子在溶液中进行配位反应,合成了PVA-Fe(Ⅲ)、PVA-Zn(Ⅱ)、PVA-Cd(Ⅱ)、PVA-Hg(Ⅱ)配合物.通过IR、Raman和XPS测试技术对配合物进行表征.IR结果显示,各配合物νc-o从纯PVA的1094cm-1向低波数方向移动8~11cm-1,νc-c由纯PVA的1430cm-1向低波数方向移动3~8cm-1;Raman显示,PVA-re(Ⅲ)、PVA-Zn(Ⅱ)、PVA-Cd(Ⅱ)、PVA-Hg(Ⅱ)配合物均在200~400cm-1处出现金属-氧键新峰;PVA-Fe(Ⅲ)的XPS显示O1s(533.0ev)、C1s(285.0eV)、Fe2p(712.0eV)的结合能与PVA[O1s(532.5eV)、C1s(284.6eV)]及FeCl3[Fe2p(711.2eV)]比较,发生了显著变化.以上结果表明,PVA分子侧链上的羟基氧提供孤对电子对与金属离子的空轨道形成配位键.配合物的抗菌实验结果显示,PVA-Hg(Ⅱ)对大肠杆菌、枯草芽孢杆菌和金黄色葡萄球菌具有很强的灭菌效果,PVA-Zn(Ⅱ)的灭菌效果较弱. 相似文献
6.
M0,±6(M=Os,Ir,Pt)团簇结构与性质的密度泛函理论研究 总被引:1,自引:1,他引:0
采用密度泛函理论(DFT)中的杂化密度泛函(B3LYP)方法,在LANL2DZ基组水平上对M06,±(M=Os,Ir,Pt)团簇的各种可能构型进行了几何结构优化,得出各团簇的最稳定构型,并对其能量、振动频率、热力学性质、核独立化学位移(NICS)和极化率进行了理论研究.结果表明,M06,±(M=Os,Ir)团簇的基态都是三棱柱结构,Pt-6团簇的基态是平面三角形结构;M06,±(M=Os,Ir,Pt)团簇生成焓都为负值,热力学上是稳定的;NICS值都为负值,表明M06,±(M=Os,Ir,Pt)团簇都具有芳香性,其中Os6-团簇的芳香性最强;从光谱分析来看,Os6的IR和Raman谱的较强吸收峰的个数最多,Ir6的IR和Raman谱的最强吸收峰都只有一个,IR最强吸收峰在137.O和143.5 cm-1之间,Raman谱最强的吸收峰位于169.5 cm-1处;Pt6的IR和Raman谱的最强吸收峰分别位于50.2和194.7 cm-1处. 相似文献
7.
采用密度泛函理论(DFT)中的杂化密度泛函(B3LYP)方法,在LANL2DZ基组水平上对M06,±(M=Os,Ir,Pt)团簇的各种可能构型进行了几何结构优化,得出各团簇的最稳定构型,并对其能量、振动频率、热力学性质、核独立化学位移(NICS)和极化率进行了理论研究.结果表明,M06,±(M=Os,Ir)团簇的基态都是三棱柱结构,Pt-6团簇的基态是平面三角形结构;M06,±(M=Os,Ir,Pt)团簇生成焓都为负值,热力学上是稳定的;NICS值都为负值,表明M06,±(M=Os,Ir,Pt)团簇都具有芳香性,其中Os-6团簇的芳香性最强;从光谱分析来看,Os6的IR和Raman谱的较强吸收峰的个数最多,Ir6的IR和Raman谱的最强吸收峰都只有一个,IR最强吸收峰在137.0和143.5 cm-1之间,Raman谱最强的吸收峰位于169.5 cm-1处;Pt6的IR和Raman谱的最强吸收峰分别位于50.2和194.7 cm-1处. 相似文献
8.
采用基因定点突变的方法, 构建了细菌视紫红质(Bacteriorhodopsin, BR)的3种突变体蛋白, 即单突变体BRE194Q、三突变体BRI119T/T121S/A126T和四突变体BRI119T/T121S/A126T/E194Q. 测定了突变体和野生型BR在水溶液和聚乙烯醇(PVA)膜中的紫外-可见吸收光谱和拉曼光谱, 采用显微视频录像技术记录了PVA膜中野生型和3个突变体样品的M态寿命. 与野生型BR相比较, 在水溶液中, 单突变体的可见吸收光谱的最大吸收峰发生了轻微红移, 三突变体和四突变体的最大吸收峰则分别发生了11.0和12.0 nm的明显蓝移. 在PVA膜中, 3个突变体BR的可见吸收光谱的最大吸收峰均发生蓝移, 四突变体BR的最大吸收峰为557 nm, 蓝移达15.0 nm. 四突变体BR在水溶液中的共振拉曼光谱不仅表现有与M态特征相关的1567和1573 cm-1谱带, 还有L态特征带1334 cm-1及N态特征带1200, 1328, 1530和1549 cm-1. 在PVA膜中的样品与在水溶液中的比较, 四突变体共振拉曼光谱的1334和1549 cm-1带消失, 同时1187 cm-1带的强度下降. 显微视频录像技术记录的PVA膜中样品的M态寿命表明, 野生型BR的M态寿命最短, 单突变体的M态寿命小于1.0 s, 三突变体的寿命为3.0 s, 四突变体的寿命为2.0 s. 相似文献
9.
利用溶胶-凝胶方法合成了Ce0.8Pr0.2O2-δ固溶体, XRD结果表明,经200 ℃焙烧就已经形成立方萤石结构固溶体,晶粒尺寸为8.1 nm, 随焙烧温度的升高,晶粒尺寸增大. X射线光电子能谱(XPS)结果表明,样品中存在氧离子缺位,铈离子主要为Ce4 离子,镨离子以混合价态Pr3 和Pr4 存在. 固溶体Ce0.8Pr0.2O2-δ的拉曼谱(Raman)观察到4个峰,458和1140 cm-1峰为特征F2g振动谱带,较宽的570和187 cm-1峰对应氧离子缺位及引起的不对称振动. 交流阻抗谱表明固溶体Ce0.8Pr0.2O2-δ在600 ℃时的电导率为1.44×10-3 S·cm-1, 活化能为Ea=0.67 eV (650~800 ℃), Ea=0.91 eV (400~600 ℃). 相似文献
10.
纳米六方相氮化铝的合成和光学性能研究 总被引:1,自引:0,他引:1
报道了以AlCl3和Mg3N2为反应物, 在500 ℃条件下, 用简易的设备, 合成六方相AlN纳米材料. 样品的XRD和XPS图谱表明, 实验得到的AlN样品是纯的六方相AlN, 其中的杂质相含量均小于仪器的探测灵敏度. TEM图表明, AlN样品呈多孔网络状结构, 网络的骨架大小在10~20 nm之间. 对AlN样品的光学性能的研究表明, AlN样品的禁带宽度值约为6.12 eV; 红外吸收谱以680 cm-1为中心形成一个很宽的红外吸收带; 其拉曼散射峰较AlN薄膜和AlN单晶向低波数方向移动. 相似文献
11.
Raman spectroscopy was applied to characterize the species deposited from the mass-selected C60 ion beam which was accelerated to 900 eV. The substrates for the deposition were (0001) surface of highly oriented pyrolitic graphite and (111) surface of gold crystal. The species do not exhibit the Raman scattering features of buckminsterfullerene, but displays peaks at 1585 and 1332 cm-1 instead. The former peak is the chararteristic Ranan peak of hexagonal graphite, and the latter can be attributed to the amorphous carbon in sp3 hybridization. The result reveals that C60 was collapsed to form a new phase when it collides on the solid surface. 相似文献
12.
13.
14.
15.
Infrared spectra of SF_6 trapped in cryogenic matrix of argon have been measured. Five peaks are observed at the frequencies of 938.51, 938.05, 937.55, 939.82 and 936.22 cm~(-1) for the v_3 mode. Varying the concentration of SF_6 in argon matrix and diffusion studies indicate that the 937.55 cm~(-1) peak is due to SF_6 aggregate and the others arise from monomer. The changes in relative intensities with annealing show that there are at least three different trapping sites for monomeric SF_6 in argon lattice. The result that the increase in intensity of the peak at 938.03 cm~(-1) parallels the decrease in that of the peak at 938.51 cm~(-1) implies a temperature-induced-change in the site population. 相似文献
16.
《Chemical physics letters》2003,367(1-2):136-140
Single crystalline wurzite GaN nanowires were successfully synthesized on the NiO catalyzed alumina substrate through a simple thermal chemical vapor deposition method. The mixture of Ga and GaN powder was used as the source material of Ga for synthesizing GaN nanowires. The diameter of nanowires ranged 50–60 nm and the length was about hundreds of micrometers. The nanowires were single crystal with hexagonal wurzite structure. The peaks of Raman spectra of GaN nanowires appeared broadened and asymmetric compared with those of bulk GaN. PL spectra under excitation at 325 nm showed a strong emission at 3.315 eV from near band-edge transition and a broad weak emission at 2.695 eV related to deep level defects. 相似文献
17.
Surface-enhanced Raman scattering and polarized photoluminescence from catalytically grown CdSe nanobelts and sheets 总被引:2,自引:0,他引:2
Venugopal R Lin PI Liu CC Chen YT 《Journal of the American Chemical Society》2005,127(32):11262-11268
We have successfully fabricated single-crystalline CdSe nanowires, nanobelts, and sheets by a chemical vapor deposition (CVD) method assisted with laser ablation. The synthesized CdSe nanostructures have hexagonal wurtzite phase as characterized by X-ray diffraction (XRD). CdSe nanobelts can range in length from several tens to a hundred micrometers, in thickness from 40 to 70 nm, and a tapered width which is approximately 3 microm at one end and tapers off to approximately 100 nm at a catalytic gold particle. Both selected area electron diffraction (SAED) and high-resolution transmission electron microscopic (HRTEM) measurements show that the single-crystalline hexagonal belts and sheets grew along the [0.1-1.0] direction with side surface of +/-(0 0 0 1) and top surface of +/-(2 -1 -1 0). While the growth mechanism of nanobelts complies with a combination of vapor-liquid-solid (VLS) and vapor-solid (VS) processes, the formation of sheets is primarily based on the VS mechanism. For comparison, the phonon modes of CdSe nanobelts and bulk powder have been measured by surface-enhanced Raman scattering (SERS) and normal Raman scattering (NRS) spectroscopies with off- and near-resonant excitations. A blue-shift of 2.4 cm(-1) for the longitudinal optical (LO) phonon of CdSe nanobelts, relative to bulk CdSe, is attributed to a lattice contraction in the belt structure, which is confirmed by the XRD measurement. Room-temperature microphotoluminescence (PL) at approximately 1.74 eV from single CdSe nanobelts shows a 3-fold enhancement compared to that from bulk CdSe powder and displays a partial polarization dependence of emission angles. 相似文献
18.
Theoretical results of normal coordinate analysis of polybenzamide performed with two conformational isomerized models, the cis trans and the all-trans conformation, have been adopted to examine a number of infrared spectra of films of the polymer treated in a subsequent annealing process and a cooling process. It shows, in this investigation, that two sets of infrared spectral profiles around 1400 cm~(-1) and 900 cm~(-1) behave quite attractively. Their spectral behaviours have been correlated to the conformational defect variation in samples, and reasonably predicted by the normal coordinate calculation. 相似文献
19.
本文用循环伏安法和现场红外光谱方法研究了铜电极上CN~-和SCN~-的电化学行为。对于0.5mol~(-1)L~(-1)NaCN+0.5 mol L~(-1)NaF/Cu体系, 电极电势在-1.60至0.30 V(相对SCE)范围内, 2030—2230 cm~(-1)范围内可得到三个吸收峰, 位置分别为2076, 2094和2170 cm~(-1)。2076和2170 cm~(-1)峰分别对应于溶液中CN~-和表面沉积难溶化合物CuCN。2094 cm~(-1)峰是吸附态CN~-和溶液中配合物Cu(CN)_3~2二物种的红外吸收叠加。对于0.5 molL~(-1)NaSCN+0.5 molL~(-1)NaF/Cu体系, 在上述电势范围内可得到2060, 2177和2170 cm~(-1)三个红外吸收峰, 分别对应于溶液中的SCN~-, 吸附态的SCN~-和表面难溶化合物CuNCS。 相似文献
20.
Sodium (Na) doped Zinc oxide (ZnO) thin films have been deposited on a glass substrate by the sol–gel spin coating method. Effect of doping with various percentages of Na at a particular annealing temperature of 500 °C is studied. The samples were characterized by X-ray diffraction (XRD), micro-photoluminescence, Raman and Polarized Raman spectroscopy. The X-ray diffraction and micro-Raman spectroscopy confirmed the presence of Na substitution in zinc oxide and the wurtzite structure of the lattice is retained. An enhancement of resonant Raman scattering processes as well as longitudinal optical phonon overtones up to the fifth order were observed in the micro Raman spectra. The similar values of depolarization ratios obtained from Polarized Raman studies recommend no change in the symmetry. Photoluminescence showed a strong emission peak in the near UV at 3.2 eV and negligible visible emission. 相似文献