GaP∶NLED外延片微区光致发光和拉曼散射研究

在国内首次通过微区光致发光结合拉曼散射的方法研究了GaP∶N五层结构的绿色发光外延片 ,用非破坏性的光学方法得到了载流子浓度的纵向分布 ,确定了发光最强的部位在P-区而且不同的样品有不同的光致发光强度随厚度的衰减曲线 ,以此为表征 ,从国内外样品的比较中查找出提高国产样品的改进方向。     

近海微塑料含量的相干反斯托克斯拉曼光谱成像研究

由于塑料工业的发展,微塑料成为一种主要的环境污染物.它在自然界中不易降解,对人类的生存环境及健康都存在不可忽视的潜在危险.因此,环境中微塑料的检测和分析,成为了近年来研究的热点问题.目前人们大多数采用浮选法、密度分离法、离心法等方法提取微塑料,然后放在显微镜下进行目视观察,并结合拉曼光谱分析、傅里叶红外光谱分析、高光谱...     

金刚烷的高压拉曼光谱研究

对金刚烷(C_(10)H_(16))进行了常温原位高压拉曼光谱研究,最高压力为25 GPa。通过分析高压拉曼光谱,结合拉曼频移随压力的变化情况,得出在实验压力范围内C_(10)H_(16)发生了多次相变。0.6 GPa时,C_(10)H_(16)由常温常压下的无序相(α相)转变为有序相(β相);继续加压至1.7 GPa时,第2次结构相变开始,直至3.2 GPa,第2次相变完全结束;第3次相变开始于6.3 GPa,结束于7.7 GPa;22.9 GPa时发生了第4次结构相变。另外,首次在拉曼光谱上探测到第3次相变过程中晶格振动峰的变化,说明第3次相变并非前人报道的等结构相变。     

X射线荧光光谱及拉曼光谱法研究五谷营养成分

采用X射线荧光光谱分析法(XRF)和激光拉曼光谱法(Raman),测定了小米、玉米、黄米、大米和小麦5种常用主食(五谷)中营养成分及钾、镁、钙、铁、锌、锰、铝、铜等多种微量元紊的含量.X射线荧光光谱分析法测量结果表明,五谷中所含微量元素非常丰富且种类基本相同,但各元素含量存在很大差异.5种谷类中K元素含量均为最高,含量...     

GaP:N LED外延片微区光致发光和拉曼散射研究

在国内首次通过微区光致发光结合拉曼散射的方法研究了GaP:N五层结构的绿色发光外延片,用大破坏性的光学方法得到了载流子浓度的纵向分布,确定了发光最强的部位在P^－区而且不同的样品有不同的光致发光强度随厚度的衰减曲线,以此为表征,从国内外样品的比较中查找出提高国产样品的改进方向。     

胆红素络合物的表面增强拉曼光谱研究

本文通过对近红外激发傅里叶变换拉曼光谱(NIR-FT-Raman)与表面增强拉曼散射(Surface Enhanced Raman Scattering,SERS)技术的联用,测得胆红素及其络合物Na2BR,CaBR与CuBR在银溶胶中的SERS光谱.结果表明,这一类与胆结石密切相关的生物分子络合物具有不同的配位方式,且在银胶表面采取不同的吸附取向,并从配位化学角度初步解释了黑色结石的黑色成因.     

拉曼光谱与拉曼效应的量子模型结构分析

散射光谱这种新谱线对应于散射分子中能级的跃迁,为研究分子结构提供了一种重要手段,引起学术界极大兴趣,拉曼也因此荣获1930年诺贝尔物理学奖。并称这种谱线为拉曼光谱。介绍了拉曼光谱的基本原理、拉曼光谱的应用以及其发展,由于拉曼光谱非常弱,实验要求比较高,最后介绍了实验仪器及利用拉曼光谱研究分子的结构。     

显微拉曼光谱检验射击残留物

建立了一种使用显微拉曼成像光谱仪检验发射火药、火药燃烧后产物和射击残留物的方法.取警用仿9×19巴拉贝鲁姆手枪弹发射药颗粒和QSZ92式9毫米手枪发射药燃烧后的产物,同时提取射击者手部射击残留物、枪管内射击残留物和目标靶物上射击残留物.使用显微拉曼成像光谱仪对采集的发射火药、火药燃烧后产物和射击残留物样本进行拉曼检...     

显微拉曼光谱在珍珠鉴定中的应用

本文用显微拉曼对三种珍珠 (天然海水珍珠、人工养殖海水珍珠、人工养殖淡水珍珠 )做了测试与分析。结果表明 :虽然主峰相同 ,然而这三种珍珠的拉曼谱有不可置疑的差别。另外 ,珍珠粉和整粒珍珠也有明显差异。测试中还发现 ,与拉曼谱同时记录到的光荧光谱也是有关珍珠的宝贵信息。因此 ,显微拉曼光谱仪记录到的材料振动谱和荧光谱为珍珠的分析研究及日常鉴定提供了可靠的信息资料。     

互叶白千层不同部位油细胞分布及显微拉曼光谱研究

为避免复杂的制样提取过程,在天然状态下获得植物样品油细胞中精油的成分,用显微拉曼光谱仪,得到互叶白千层同一植株不同部位的油细胞的分布及油细胞中的主成分。对各部位的显微镜观察发现在软枝干中不存在油细胞或者很少,老叶中的油细胞没有新叶中的多。在老叶油细胞上获得的谱峰中,1 675和726 cm-1为4-萜烯醇的特征峰, 归属为C═C伸缩振动和环的变形振动;1 700和754 cm-1为γ-松油烯的特征峰,归属为C═C伸缩振动和环的变形振动;1 609 cm-1为α-松油烯的特征峰,归属为C═C伸缩振动;1 522,1 156和1 011 cm-1为β-胡萝卜素的的特征峰,分别归属为C═C伸缩振动、C-C伸缩振动和C-C面内摇摆振动。在新叶油细胞上获得的谱峰中,745 cm-1为顺香桧烯水合物的特征峰,归属为环变形振动;1 609 cm-1为α-松油烯的特征峰;1 525,1 160和1 008 cm-1为β-胡萝卜素的的特征峰;老叶与新叶油细胞中的主成分不完全相同,老叶中油细胞精油为γ-松油烯-4-萜烯醇-α-松油烯型,而新叶中油细胞中的精油为顺香桧烯水合物-α-松油烯型。老叶、新叶的共有物为：α-松油烯、β-胡萝卜素。β-胡萝卜素及顺香桧烯水合物为首次在互叶白千层中发现。利用该方法可迅速的确定植株油细胞的主成分,为互叶白千层精油提取提供有益参考。     

Micro-Raman and ion channeling study of crystal damage in Si induced by focused Co ion beam implantation

The lattice damage of silicon produced by ion implantation at extremely high current density of 0.8 A/cm² (2.5᎒¹⁸ cm^-2 s^-1) was investigated. In a focused ion beam system, implantation was carried out with 70 keV Co ions, fluences of 1.2᎒¹⁶ cm^-2 and 6.7᎒¹⁵ cm^-2 into Si (111) at room temperature and elevated temperatures between 355 °C and 400 °C. Radiation damage measurements were performed by Rutherford backscattering/channeling spectroscopy and micro-Raman analysis. The radiation damage was studied as a function of pixel dwell-time and implantation temperature. The critical temperature for amorphization increases with current density. Although the fluence of the focused ion implantation was constant, crystalline layers were obtained for short and amorphous layers for long pixel dwell-times. The critical dwell-time of crystalline/amorphous transition increases with implantation temperature. From the results a typical time for defect annealing of 10^-5 s at 400 °C and an activation energy of (2.5ǂ.6) eV were deduced.     

Raman spectroscopy study of damage induced in fluorapatite by swift heavy ion irradiations

Raman spectroscopy was used to study the radiation damage of fluorapatite single crystals and sinters. Krypton and iodine ion irradiations were performed at high energies (∼1 MeV amu⁻¹) for fluences ranging between 1 × 10¹¹ and 5 × 10¹³ cm⁻². Evolution of the symmetric stretching mode of the PO₄³⁻ tetrahedral building blocks (strongest Raman mode observed at 965 cm⁻¹) versus ion fluence was investigated. After irradiation, this peak decreases in intensity and a second broader peak appears at lower wavenumber. The well‐resolved peak has been assigned to the crystalline phase, and the broader one to the amorphous phase. The integrated intensity ratios of these two peaks versus fluence are in good agreement with the damage fractions determined by X‐ray diffraction (XRD). Fits of the amorphous fraction versus fluence show that the amorphization mechanisms is dominated by a single‐impact process for iodine ions and by a double‐impact process for krypton ions in the case of single crystals and sinters. For both irradiations, complete amorphization could not be obtained. The amorphous fraction saturates at a maximum value of 88% for sinters and 72% for single crystals. This is attributed to a recrystallization effect which is more important in single crystals than in sinters. For both types of samples, the crystalline peak shifts slightly to a lower wavenumber with fluence, and then shifts back to its initial value for an amorphous fraction larger than 60%. This feature is attributed to a stress relaxation, as shown in the XRD data, which is accompanied by a decrease of the crystalline peak full‐width at half‐maximum. Copyright © 2011 John Wiley & Sons, Ltd.     

The effect of anti-hydrogen bond on Fermi resonance: A Raman spectroscopic study of the Fermi doublet ν1—ν12 of liquid pyridine

The effects of anti-hydrogen bond on the ν₁—ν₁₂ Fermi resonance (FR) of pyridine are experimentally investigated by using Raman scattering spectroscopy. Three systems, pyridine/water, pyridine/formamide, pyridine/carbon tetrachloride, provide varying degrees of strength for the diluent-pyridine anti-hydrogen bond complex. Water forms a stronger anti-hydrogen bond with pyridine than with formamide, and in the case of adding non-polar solvent carbon tetrachloride, which is neither a hydrogen bond donor nor an acceptor and incapable of forming hydrogen bond with pyridine, the intermolecular distance of pyridine will increase and the interaction of pyridine molecules will reduce. The dilution studies are performed on the three systems. Comparing with the values of Fermi coupling coefficient W of the ring breathing mode ν ₁ and triangle mode ν ₁₂ of pyridine at different volume concentrations, which are calculated according to the Bertran equations, in three systems, we find that the solution with the strongest anti-hydrogen bond, water, shows the fastest change in the ν₁—ν₁₂ Fermi coupling coefficient W with the volume concentration varying, followed by the formamide and carbon tetrachloride solutions. These results suggest that the stronger anti-hydrogen bond-forming effect will cause a greater reduction in the strength of the ν₁—ν₁₂ FR of pyridine. According to the mechanism of the formation of anti-hydrogen bond in the complexes and the FR theory, a qualitative explanation for the anti-hydrogen bond effect in reducing the strength of the ν₁—ν₁₂ FR of pyridine is given.     

The torsion potential function of hydrogen peroxide and disulfan molecules

A method for constructing the torsion potential function of hydrogen peroxide and disulfan molecules which takes into account the magnitudes of intramolecular interactions is suggested. The new representation of the potential is used to calculate the torsion spectra of the molecules indicated. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 67, No. 4, pp. 450–452, July–August, 2000.     

Detection of cellular damage by hydrogen peroxide using SV40-T2 cells on shear horizontal surface acoustic wave (SH-SAW) sensor

The rat lung epithelial cell line SV40-T2 was used to develop a cellular biosensing system to assay for environmental toxicants. The novel approach on which this system is based involves direct attachment of cultured rat or human cells onto a cell-adhesive matrix on the device through which shear horizontal surface acoustic waves (SH-SAW) are transmitted using 50 MHz SAW resonator. This novel design enables sensitive monitoring of changes of the electrophysical characteristics of cells, such as their conductivity and relative permittivity. A time-dependent change of phase of SAW and change of insertion loss (change of amplitude) were observed when the cells were treated with 0.5 or 1.0 mM H₂O₂. The change of insertion loss was biphasic, with an early phase (1–3 h) and a late phase (3–6 h). The late phase coincided with the destruction of cell–cell tight junctions detected by measurement of the transepithelial electrical resistance and paracellular permeability; in contrast, the early phase coincided with the destruction of intracellular actin filaments by H₂O₂. The early-phase effect of H₂O₂ on phase shift may be attributable to the change of intracellular permittivity by a change of cellular polarity. Immunofluorescence microscopy showed the disappearance of zonula occludens protein 1 from the region of cell–cell contact. These results suggest the correlation between the change of insertion loss as an SAW parameter and the destruction of tight junctions of the cells on the SH-SAW device in the late phase.     

Optical spectroscopy study of damage evolution in 6H-SiC by H_2~+ implantation

Lattice defects induced by ion implantation into Si C have been widely investigated in the decades by various techniques. One of the non-destructive techniques suitable to study the lattice defects in Si C is the optical characterization. In this work, confocal Raman scattering spectroscopy and photoluminescence spectrum have been used to study the effects of 134-ke V H_2~+ implantation and thermal treatment in the microstructure of 6 H-Si C single crystal. The radiation-induced changes in the microstructure were assessed by integrating Raman-scattering peaks intensity and considering the asymmetry of Raman-scattering peaks. The integrated intensities of Raman scattering spectroscopy and photoluminescence spectrum decrease with increasing the fluence. The recovery of the optical intensities depends on the combination of the implantation temperature and the annealing temperature with the thermal treatment from 700℃ to 1100℃. The different characterizations of Raman scattering spectroscopy and photoluminescence spectrum are compared and discussed in this study.     

一种新型共轭聚合物发光二极管老化的拉曼光谱研究

通过显微共焦拉曼光谱 ,对一种以新型的共轭聚合物半导体材料 3,4 (2 乙基己氧基 )苯基 1,3 丙二醇酯 (poly(2 (4 Ethylhexyl) phenyl 1,4 phenylenevinylene) (P PPV) )为发光层的聚合物发光二极管(PLEDs)器件进行了老化研究 ,无论是光致发光光谱还是拉曼光谱都提供证据说明造成器件老化的原因主要是发光层的聚合物的主链结构 ,即聚合物的共轭结构被破坏 ,这对提高以P PPV作为发光层的PLEDs器件的性能提出有用信息。