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Measurement of residual stress in a multi-layer semiconductor heterostructure by micro-Raman spectroscopy 被引量:13
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作者 Wei Qiu Cui-Li Cheng +7 位作者 Ren-Rong Liang Chun-Wang Zhao Zhen-Kun Lei Yu-Cheng Zhao Lu-Lu Ma Jun Xu Hua-Jun Fang Yi-Lan Kang 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2016年第5期805-812,共8页
Si-based multilayer structures are widely used in current microelectronics. During their preparation, some inhomogeneous residual stress is induced, resulting in competition between interface mismatching and surface e... Si-based multilayer structures are widely used in current microelectronics. During their preparation, some inhomogeneous residual stress is induced, resulting in competition between interface mismatching and surface energy and even leading to structure failure. This work presents a methodological study on the measurement of residual stress in a multi-layer semiconductor heterostructure. Scanning electron microscopy(SEM), micro-Raman spectroscopy(MRS), and transmission electron microscopy(TEM) were applied to measure the geometric parameters of the multilayer structure. The relationship between the Raman spectrum and the stress/strain on the [100] and [110] crystal orientations was determined to enable surface and crosssection residual stress analyses, respectively. Based on the Raman mapping results, the distribution of residual stress along the depth of the multi-layer heterostructure was successfully obtained. 展开更多
关键词 Residual stress Multi-layer semiconductor heterostructure micro-raman spectroscopy(MRS) Strained silicon Germanium silicon
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中煤级煤Micro-Raman结构对甲烷吸附的响应
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作者 陈小珍 李美芬 曾凡桂 《煤炭学报》 EI CAS CSCD 北大核心 2022年第7期2678-2686,共9页
煤与甲烷、二氧化碳等流体作用后的体积膨胀及其机制一直是煤层气地质学和煤与瓦斯突出防治研究中的重要课题之一。以往的研究主要集中在宏观吸附膨胀及变形,并从力学的角度解释其膨胀机制。实际上,煤作为由大分子构成的分子体系,与甲... 煤与甲烷、二氧化碳等流体作用后的体积膨胀及其机制一直是煤层气地质学和煤与瓦斯突出防治研究中的重要课题之一。以往的研究主要集中在宏观吸附膨胀及变形,并从力学的角度解释其膨胀机制。实际上,煤作为由大分子构成的分子体系,与甲烷、二氧化碳的相互作用是一种分子现象,其膨胀变形的本质应该是分子体系发生了变化,因此揭示煤大分子结构对煤体吸附膨胀的响应特征是认识其机制的基础。应用显微-拉曼光谱法对吸附甲烷前后的8个中煤级煤样(镜质组最大反射率R_(o)=1.08%~1.80%)进行了结构表征,并运用Origin 8.5软件对煤样吸附甲烷前后的拉曼光谱曲线进行了分峰拟合,在此基础上计算了煤样吸附前后的拉曼光谱结构参数。结果表明:原煤和吸附煤的G峰与D峰的峰位差d(G-D)随着煤级的增加有增大趋势,G峰半峰宽(FWHM-G)呈减小趋势,表明在反射率1.08%~1.80%阶段,煤结构有序度和微晶尺寸随煤级增加而逐渐增加;大芳香环(≥6)的相对含量(A_(D)/A_(G))出现先增加后减小的趋势,这是以较大芳香环的生成为主转为向石墨结构生成为主的结果;随着煤级增加,原煤的大芳香环结构中“杂质”(A_(S)/A_(D))及氢化芳环上的C—C的含量(A_(S)/A_(total))均有减小的趋势,反映出煤结构中sp^(2)-sp^(3)杂化烷基碳或氢化芳环逐渐减少,有序度逐渐增加;当R_(o)>1.3%时,吸附煤相对原煤的d(G-D)及A_(D)/A_(G)减少,小芳香环相对含量(A_(GR+VR+VL)/A_(D)),A_(S)/A_(D),A_(S)/A_(total)和FWHM-G增加,表明甲烷吸附变形引起环数较大的芳香环和微晶结构破裂形成较小的芳香环。这一结果对于认识煤大分子结构与甲烷的相互作用机制提供了理论依据。 展开更多
关键词 micro-raman 吸附变形 结构演化 中煤级煤 西山煤田
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Spectra of spontaneous Raman scattering in taper-drawn micro/nano-fibers 被引量:1
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作者 徐颖鑫 崔亮 +5 位作者 李小英 郭骋 李宇航 徐忠扬 王力军 方伟 《Chinese Physics B》 SCIE EI CAS CSCD 2016年第12期266-270,共5页
We study the spontaneous Raman scattering (RS) in taper-drawn micro/nano-fibers (MNFs) by employing the photon counting technique. The spectra of RS in five MNFs, which are fabricated by using different heating fl... We study the spontaneous Raman scattering (RS) in taper-drawn micro/nano-fibers (MNFs) by employing the photon counting technique. The spectra of RS in five MNFs, which are fabricated by using different heating flames (hydrogen flame or butane flame) and with different diameters, are measured within a frequency shift range of 1435 cm- 1_3200 cm- 1. From the measured spectra, we observe the RS peaks originated from silica and a unique RS peak with a frequency shift of - 2905 cm-1 (- 87.2 THz). Unlike the former ones, the latter one is not observable in conventional optical fibers. Furthermore, the unique peak becomes obvious and starts to rapidly increase with the decrease of the diameter of MNFs when the diameter is smaller than 2 μm, and the intensity of the unique peak significantly depends on the heating flame used in the fabricating process. Our investigation is useful for the entanglement generation or optical sensing using taper-drawn MNFs. 展开更多
关键词 nonlinear optics micro/nano-fibers raman scattering
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Comparison between Double Crystals X-ray Diffraction and Micro-Raman Measurement on Composition Determination of High Ge Content Si_(1-x)Ge_(x) Layer Epitaxied on Si Substrate 被引量:1
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作者 Lei ZHAO Yuhua ZUO Buwen CHENG Jinzhong YU Qiming WANG 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2006年第5期651-654,共4页
It is important to acquire the composition of Si1-xGex layer, especially that with high Ge content, epitaxied on Si substrate. Two nondestructive examination methods, double crystals X-ray diffraction (DCXRD) and mi... It is important to acquire the composition of Si1-xGex layer, especially that with high Ge content, epitaxied on Si substrate. Two nondestructive examination methods, double crystals X-ray diffraction (DCXRD) and micro-Raman measurement, were introduced comparatively to determine x value in Si1-xGex layer, which show that while the two methods are consistent with each other when x is low, the results obtained from double crystals X-ray diffraction are not credible due to the large strain relaxation occurring in Si1-xGex layers when Ge content is higher than about 20%. Micro-Raman measurement is more appropriate for determining high Ge content than DCXRD. 展开更多
关键词 Si1-xGex Ge content Composition determination Double crystals X-ray diffraction (DCXRD) micro-raman measurement
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不同煤级煤纳米力学性能的Micro-Raman结构响应
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作者 韩雅婷 孙蓓蕾 《煤矿安全》 CAS 北大核心 2022年第11期7-14,共8页
煤的力学性质具有非均质性及多尺度效应,从纳米尺度认识煤力学性质及与其组成结构之间的关系,是理解煤储层的压裂改造机制及裂纹扩展机理的关键。利用原子力显微镜和显微拉曼对不同煤级煤的镜质组进行测试,获得煤样的力学和结构参数。... 煤的力学性质具有非均质性及多尺度效应,从纳米尺度认识煤力学性质及与其组成结构之间的关系,是理解煤储层的压裂改造机制及裂纹扩展机理的关键。利用原子力显微镜和显微拉曼对不同煤级煤的镜质组进行测试,获得煤样的力学和结构参数。结果表明:镜质组的弹性模量E在0.66~7.58 GPa之间,且弹性模量随镜质组最大反射率Ro的增加而增加;同时随着Ro的增大,拉曼结构参数呈现有规律的变化;将弹性模量E与拉曼结构参数建立关系,发现(G-D)峰位差、多环芳烃的相对含量与致弹性模量均呈现明显的正相关关系,FWHM-G与E呈现负相关关系,反映了结构有序度的增加会导致弹性模量增大,表明随着成熟度的增加,促使大分子结构排列紧密且分子间作用力增大,导致弹性模量也随之增大。 展开更多
关键词 煤储层压裂 煤结构 原子力显微镜 显微拉曼 纳米力学性能
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Microstructural Probing of (1-x) GeS_(2-x)Ga_2S_3 System Glasses By Raman Scattering 被引量:4
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作者 陶海征 《Journal of Wuhan University of Technology(Materials Science)》 SCIE EI CAS 2005年第3期8-10,共3页
Roman scattering measurement of ( 1 - x ) GeS2-x Ga2S3 system glasses was conducted in order to understand the microstructural change caused by the addition of Ga2S3 . According to the change of Raman spectra with t... Roman scattering measurement of ( 1 - x ) GeS2-x Ga2S3 system glasses was conducted in order to understand the microstructural change caused by the addition of Ga2S3 . According to the change of Raman spectra with the addition of Ga2S3, two main structural transformations were deduced : the gradual enhancement of ethane- like structural units S3 Ge- GeS3 ( 250 cm ^- 1) and S3 Ga- GaS3 (270 cm ^- 1 ) and the appearance of charge imbalanced units [ Ga2 S2 ( S1/2 )4 ]^2- and [Ga( S1/2 )4 ]^- . And this change of structural aspect seems to give as a clue to understanding the cause of the increased rare-earth solubility. 展开更多
关键词 1 - x GeS2-x Ga2S3 system glasses raman microstructure
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Low-energy(40 keV) proton irradiation of YBa_2Cu_3O_(7-x) thin films:Micro-Raman characterization and electrical transport properties
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作者 王三胜 李方 +8 位作者 吴晗 张玉 穆罕默德苏尔曼 赵鹏 乐小云 肖志松 姜利祥 欧学东 欧阳晓平 《Chinese Physics B》 SCIE EI CAS CSCD 2019年第2期406-413,共8页
To investigate the damage profiles of high-fluence low-energy proton irradiation on superconducting materials and related devices, Raman characterization and electrical transport measurement of 40-keV-proton irradiate... To investigate the damage profiles of high-fluence low-energy proton irradiation on superconducting materials and related devices, Raman characterization and electrical transport measurement of 40-keV-proton irradiated YBa_2Cu_3O_(7-x)(YBCO) thin films are carried out. From micro-Raman spectroscopy and x-ray diffraction studies, the main component of proton-radiation-induced defects is found to be the partial transition of superconducting orthorhombic phase to the semiconducting tetragonal phase and non-superconducting secondary phase. The results indicate that the defects induced in the conducting CuO_2 planes, such as increased oxygen vacancies and interstitials, can result in an increase in the resistivity but a decrease in the transition temperature TCwith the increase in the fluence of proton irradiation, which is confirmed in the electrical transport measurements. Especially, zero-resistance temperature TC_0 is not observed at a fluence of 10^(15)p/cm^2.Furthermore, the variation of activation energy U_0 can be explained by the plastic-flux creep theory, which indicates that the plastic deformation and entanglement of vortices in a weakly pinned vortex liquid are caused by disorders of point-like defects. Point-like disorders are demonstrated to be the main contribution to the low-energy proton radiation damage in YBCO thin films. These disorders are likely to cause flux creep by thermally assisted flux flow, which may increase noise and reduce the precision of superconducting devices. 展开更多
关键词 SUPERCONDUCTORS PROTON radiation micro-raman spectra electrical transport
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Micro-Raman Spectroscopy for Stress Evaluation of 3C-SiC Epitaxially Grown on Si Substrate by Hot Wall CVD
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作者 ZHUWen-liang ZHUJi-liang PEZZOTTIGiuseppe 《材料热处理学报》 EI CAS CSCD 北大核心 2004年第05B期803-806,共4页
A series of cubic SiC single crystals were heteroepitaxially grown by the hot-wall chemical vapor deposition (CVD) using a HMDS-C3H8-H2 system on 2 inch silicon substrates with the orientations of (100), (111), (110) ... A series of cubic SiC single crystals were heteroepitaxially grown by the hot-wall chemical vapor deposition (CVD) using a HMDS-C3H8-H2 system on 2 inch silicon substrates with the orientations of (100), (111), (110) and (211), respectively. Even though an initial carbonization was carried out to reduce the large lattice mismatch, residual stress could not be completely relieved, partly also due to the difference of their thermal expansion coefficients. Raman scattering studies for the specimens were performed to estimate the internal stress in the SiC epilayer and the substrate. Raman spectra were mapped out on the sample surface as well as on the cross section using an automated x-y stage with a spatial resolution capable of 100 nm. For all the samples, two Raman peaks corresponding to the transverse optical (TO) and longitudinal optical (LO) phonon modes were observed, even though the intensity varied with the polarization configurations. In the SiC epilayers, tensile stresses decrease away from the interface, while compressive stresses exist in the substrate, with the magnitudes dependent on the growth orientation. The lattice strains were discussed in terms of the elastic deformation theory for the comparison. 展开更多
关键词 显微喇曼光谱学 应力测定 3C-SIC 热壁CVD 外延生长
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A polarized micro-Raman study of a 0.65PbMg_(1/3)Nb_(2/3)O_3-0.35PbTiO_3 single crystal
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作者 张丽艳 朱恪 刘玉龙 《Chinese Physics B》 SCIE EI CAS CSCD 2012年第1期482-487,共6页
Polarized micro-Raman spectra of a 0.65PbMgl/3Nb2/303 0.35PbTiO3 (0.65PMN-0.35PT) single crystal poled in the [001] direction are obtained in a wide frequency range (50 2000 cm^-1) at different temperatures. The b... Polarized micro-Raman spectra of a 0.65PbMgl/3Nb2/303 0.35PbTiO3 (0.65PMN-0.35PT) single crystal poled in the [001] direction are obtained in a wide frequency range (50 2000 cm^-1) at different temperatures. The best fit to the Raman spectrum at 77 K is achieved using 17 Lorenzians to convolute into it, and this is proved to be a reasonable fit. According to the group theory and selection rules of overtone and combinational modes, apart from the seven Raman modes that are from first-order Raman scattering, the remaining ones are attributed to being from second-order Raman scattering. A comparison between the experimental results and theoretical predictions shows that they are in satisfactory agreement with each other. Our results indicate that at 77 K the sample belongs to the rhombohedral symmetry with the C^53v(R3m) space group (Z = 1). In our study, on heating, the 0.65PMN 0.35PT single crystal undergoes a rhombohedral → tetragonal → cubic phase transition sequence. The two phase transitions occur at 340 and 440 K, which correspond to the disappearance of the soft mode near 106 cm-1 recorded in VV polarization and the vanishing of the band around 780 cm^-1 in VH polarization, respectively. 展开更多
关键词 0.65PMN-0.35PT polarized micro-raman second-order raman scattering phase tran-sition
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Study of Thermal Conductivity of Porous Silicon Using the Micro-Raman Method
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作者 Amaria Ould-Abbas Mama Bouchaour Nasr-Eddine Chabane Sari 《Open Journal of Physical Chemistry》 2012年第1期1-6,共6页
In this work, we are interesting in the measurement of thermal conductivity (on the surface and in-depth) of Porous silicon by the micro-Raman spectroscopy. This direct method (micro-Raman spectroscopy) enabled us to ... In this work, we are interesting in the measurement of thermal conductivity (on the surface and in-depth) of Porous silicon by the micro-Raman spectroscopy. This direct method (micro-Raman spectroscopy) enabled us to develop a systematic means of investigation of the morphology and the thermal conductivity of Porous silicon oxidized or no. The thermal conductivity is studied according to the parameters of anodization and fraction of silicon oxidized. Thermal transport in the porous silicon layers is limited by its porous nature and the blocking of transport in the silicon skeleton what supports its use in the thermal sensors. 展开更多
关键词 Mono-Crystal SILICON POROUS SILICON Thermal CONDUCTIVITY micro-raman Spectroscopy
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Micro-Raman and SEM Analysis of Minerals from the Darhib Mine, Egypt
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作者 Giuliana Gatto Rotondo Larysa Darchuk +1 位作者 Marcel Swaenen René Van Grieken 《Journal of Analytical Sciences, Methods and Instrumentation》 2012年第1期42-47,共6页
The Darhib mine is one of the several talc deposits in the Hamata area of southeastern Egypt. Several specimens of minerals coming from this mine were subjected to complementary investigation by micro-Raman spectromet... The Darhib mine is one of the several talc deposits in the Hamata area of southeastern Egypt. Several specimens of minerals coming from this mine were subjected to complementary investigation by micro-Raman spectrometry and scanning electron microscopy. The difficulty in their identification is the appearance of most of them: they are all very small and only visible under the mineral binocular microscope(×10 - ×40). They appear as small crystals in fissures and holes and a visual determination on colour and crystal gives only a guess of what kind of mineral it could be. Therefore, only after analyzing them by micro-Raman and scanning electron microscopy it was possible to identify their structure and they can be divided in three main groups: one is quite generic and several minerals of different species were identified, such as quartz, talc, mottramite and chrysocolla, very common in the talc mine (these ones are Si-based minerals);the other one is constituted by four samples which are Zn and/or Cu rich, which means minerals of the rosasite or aurichalcite groups;the last group is constituted by two samples containing mainly Pb.. 展开更多
关键词 MINERALS micro-raman SEM TALC Mines
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Rb(NTO)·(H_2O)的合成,表征,FT-IR和Raman光谱 被引量:7
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作者 胡满成 高世扬 +1 位作者 刘志宏 夏树屏 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2001年第2期197-201,共5页
首次用碳酸铷与NTO在水溶液中直接合成了Rb+ 与NTO- 的配合物。采用元素分析和化学分析确定配合物的组成为Rb(NTO)·(H2 O)。用X 射线粉末衍射谱的测试与分析对该配合物进行了结构和性质的表征。给出了FTIR和Raman光谱 ,分析了各种... 首次用碳酸铷与NTO在水溶液中直接合成了Rb+ 与NTO- 的配合物。采用元素分析和化学分析确定配合物的组成为Rb(NTO)·(H2 O)。用X 射线粉末衍射谱的测试与分析对该配合物进行了结构和性质的表征。给出了FTIR和Raman光谱 ,分析了各种谱线的归属。从结构角度讨论了配合物中不同键的形成。 展开更多
关键词 NTO 合成 配合物 表征 raman 炸药 红外光谱 3-硝基-1 2 4三唑-5酮 拉曼光谱
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显微Raman光谱法对Al_2O_3-SiO_2-H_2O系反应过程的探索表征 被引量:1
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作者 王旻 覃维祖 《硅酸盐学报》 EI CAS CSCD 北大核心 2008年第5期724-727,共4页
用显微Raman光谱法在Al2O3-SiO2-H2O体系不除去所含水分的情况下对样品进行了检测,避免了脱水处理过程对样品微结构的损伤。研究了反应产物和微结构随时间进展的变化情况,对同一样品进行了定点跟踪观察,Raman光谱检测结果和在显微镜下... 用显微Raman光谱法在Al2O3-SiO2-H2O体系不除去所含水分的情况下对样品进行了检测,避免了脱水处理过程对样品微结构的损伤。研究了反应产物和微结构随时间进展的变化情况,对同一样品进行了定点跟踪观察,Raman光谱检测结果和在显微镜下观测结果很好地对应。结果表明:对于配比为m(钾水玻璃):m(偏高岭土):m(粉煤灰):m(硅灰)=10:9:1:1,石膏掺量为3.7%的实验样品,在搅拌后4 h之内,二水石膏溶解于体系,Ca2+浓度提高,[SiO4]4-聚合度下降,偏高岭土中的五配位铝逐渐消失;在搅拌后4 h至1 d中,大量的含水凝胶物形成,材料也因此开始有强度,样品表面变得致密;在搅拌后1 d至7 d中,结晶态K2SO4形成,样品表面致密程度大幅提高,材料的强度也随之提高。 展开更多
关键词 显微raman光谱 铝硅酸盐 定点跟踪观测法
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Cu-ZnO-ZrO_2甲醇水蒸气重整催化剂的原位Raman表征 被引量:1
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作者 云虹 张慧 +1 位作者 陈建华 陈鸿博 《化学学报》 SCIE CAS CSCD 北大核心 2004年第18期1729-1732,共4页
应用显微Raman光谱对Cu ZnO ZrO2 (Zr 2 4% ,w)催化剂催化甲醇水蒸气重整 (SRM)反应进行原位表征 ,并将结果与相同催化剂上的甲醇合成 (MS)反应进行对比 ,结果表明 :在SRM反应时 ,催化剂表面出现四个宽峰 ,其中 5 44 8和 65 2 8cm-1... 应用显微Raman光谱对Cu ZnO ZrO2 (Zr 2 4% ,w)催化剂催化甲醇水蒸气重整 (SRM)反应进行原位表征 ,并将结果与相同催化剂上的甲醇合成 (MS)反应进行对比 ,结果表明 :在SRM反应时 ,催化剂表面出现四个宽峰 ,其中 5 44 8和 65 2 8cm-1分别为CuO ZnO和ZrO2 的Raman吸收峰 ,而 13 61 8cm-1为HCOO—Cu对称伸缩振动吸收峰 ,在 15 90 3cm-1附近的谱峰归属于甲酸物种中OCO的不对称伸缩振动 .在由CO CO2 H2 合成气合成甲醇时 ,在 13 5 0cm-1和分别在 15 5 0 ,15 85 ,15 95cm-1出现两个甲酸根表面物种和甲酸盐的振动吸收谱带 .因此 ,在Cu ZnO ZrO2 催化剂上的甲醇合成和甲醇水蒸气重整存在相同的甲酸根中间体 ,这一结果将有助于对甲醇合成和甲醇水蒸气重整反应机理的理解 . 展开更多
关键词 甲醇 水蒸气重整 显微raman光谱 -氧化锌-氧化铬催化剂 合成
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BaCe_(1-x)Eu_xO_(3-δ)电解质的Raman谱与TG-DTA研究 被引量:1
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作者 王金霞 简家文 《中国稀土学报》 CAS CSCD 北大核心 2009年第4期514-518,共5页
合成了初始摩尔比为Ba/(Ce+Eu)=1.0和1.1的钙钛矿型氧化物BaCe1-xEuxO3-δ(x=0.05,0.10,0.15,0.20)。XRD分析表明,过量Ba的样品Ba/(Ce+Eu)=1.1已成钙钛矿单相,样品Ba/(Ce+Eu)=1.0有微量CeO2相存在。Raman谱分析表明,微量CeO2相的产生是... 合成了初始摩尔比为Ba/(Ce+Eu)=1.0和1.1的钙钛矿型氧化物BaCe1-xEuxO3-δ(x=0.05,0.10,0.15,0.20)。XRD分析表明,过量Ba的样品Ba/(Ce+Eu)=1.1已成钙钛矿单相,样品Ba/(Ce+Eu)=1.0有微量CeO2相存在。Raman谱分析表明,微量CeO2相的产生是由于高温烧结时引起一定量BaO的蒸发引起的;样品Ba/(Ce+Eu)=1.1中过量的Ba对高温烧结时BaO的蒸发起到了补偿作用。热重(TGA)和差热分析(DTA)显示,样品长期放置在空气中,会与空气中的CO2发生一定的反应。 展开更多
关键词 氧化物 粉末衍射 raman 热重-差热 稀土
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FCVAD合成Ta-C(N)薄膜及其Raman和XPS分析 被引量:2
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作者 王广甫 张荟星 《发光学报》 EI CAS CSCD 北大核心 2003年第5期535-539,共5页
掺N非晶金刚石Ta-C(N)薄膜是合成β-C3N4研究中出现的一种新型固体薄膜材料,近年来由于其优异的电化学性能受到越来越多的关注。我们用磁过滤阴极真空弧等离子体沉积(FCVAD)方法在不同N2分压下,在Si衬底上合成了Ta-C(N)薄膜。Raman和XP... 掺N非晶金刚石Ta-C(N)薄膜是合成β-C3N4研究中出现的一种新型固体薄膜材料,近年来由于其优异的电化学性能受到越来越多的关注。我们用磁过滤阴极真空弧等离子体沉积(FCVAD)方法在不同N2分压下,在Si衬底上合成了Ta-C(N)薄膜。Raman和XPS分析表明Ta-C:N薄膜中的N主要以C—N的方式与C结合。N2分压越大,N/C原子比越高,最高可达31.1%。但同时sp3键含量越低,并且合成Ta-C:N薄膜的速度越慢。 展开更多
关键词 磁过滤阴极真空弧沉积 掺杂 固体薄膜材料 -碳薄膜 氮原子 X射线分析 raman光谱分析
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利用原子-腔场的Raman相互作用制备类自旋多腔场纠缠态 被引量:3
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作者 陈昌永 《原子与分子物理学报》 CAS CSCD 北大核心 2002年第2期245-248,共4页
提出了一种利用Λ型三能级原子与相干态腔场的Raman相互作用制备类自旋多腔场纠缠态的方案。
关键词 原子-腔场 raman相互作用 制备 类自旋多腔场纠缠态 相干态 拉曼相互作用 量子光学 三能级原子
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5-羟色胺转运蛋白显像剂^(11)C-DASB的自动化合成及Micro PET/CT显像
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作者 张晓军 刘健 +2 位作者 李云钢 田嘉禾 张锦明 《同位素》 CAS 2015年第1期1-6,共6页
目的:自动化合成5-羟色胺转运蛋白显像剂11 C-DASB并进行大鼠Micro PET/CT显像;方法:通过改变甲基化试剂、溶解前体溶剂及反应条件,得到优化的标记条件作为碳-11多功能合成模块的输入参数,进行自动化合成11 C-DASB,大鼠静脉注射11 C-DAS... 目的:自动化合成5-羟色胺转运蛋白显像剂11 C-DASB并进行大鼠Micro PET/CT显像;方法:通过改变甲基化试剂、溶解前体溶剂及反应条件,得到优化的标记条件作为碳-11多功能合成模块的输入参数,进行自动化合成11 C-DASB,大鼠静脉注射11 C-DASB 45 min后进行显像;结果:采用11 C-CH3-Triflate作为甲基化试剂,通入新配制的含1mg去甲基DASB前体的500μL DMSO溶液内,80℃下加热2min,标准率为63.7%,大鼠显像表明,11 C-DASB特异性的浓聚于SERT富集区域;结论:经优化,11 C-DASB自动化合成可得到较高产率,大鼠显像表明,其特异性浓聚于SERT富集区域,有望作为5-羟色胺转运蛋白显像剂。 展开更多
关键词 ^11C-DASB 5-羟色胺转运蛋白 micro PET/CT
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MF-ZrF_(4)(M=Li,Na,K)体系离子结构的Raman光谱研究
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作者 于江玉 胡宪伟 +4 位作者 刘成员 康铱潇 张一帆 石忠宁 王兆文 《材料与冶金学报》 CAS 北大核心 2021年第4期310-314,共5页
碱金属氟化物-氟化锆体系是核反应熔盐堆冷却剂和燃料盐载体最具潜力的应用对象.采用Raman光谱法研究了MF-ZrF_(4)(M=Li,Na,K)体系的离子结构,探讨了温度和ZrF_(4)摩尔分数对体系中离子团的形式和相互转化规律的影响.研究表明,MF-ZrF_(4... 碱金属氟化物-氟化锆体系是核反应熔盐堆冷却剂和燃料盐载体最具潜力的应用对象.采用Raman光谱法研究了MF-ZrF_(4)(M=Li,Na,K)体系的离子结构,探讨了温度和ZrF_(4)摩尔分数对体系中离子团的形式和相互转化规律的影响.研究表明,MF-ZrF_(4)体系中主要存在ZrF^(4-)_(8),ZrF^(3-)_(7),ZrF^(2-)_(6),ZrF-5四种Zr-F结构,在较高温度时还存在Zr_(3)F^(8-)_(20),Zr_(2)F^(5-)_(13)和Zr_(2)F^(3-)_(11)络合离子团;随着温度的升高,体系中ZrF^(3-)_(7)离子团的相对含量减少,ZrF^(4-)_(8),ZrF^(2-)_(6)和ZrF-5离子团的相对含量增加;随着温度的升高或体系中ZrF_(4)摩尔分数的增大,ZrF^(4-)_(8),ZrF^(3-)_(7),ZrF^(2-)_(6),ZrF-5四种络合离子团的结构变得不稳定. 展开更多
关键词 碱金属氟化物-氟化锆 -氟络合离子团 raman光谱 离子结构
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^(18)F-氟赤硝基咪唑micro PET/CT评价裸鼠乳腺癌早期放疗疗效实验研究 被引量:3
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作者 苏晓雨 徐慧琴 +3 位作者 汪会 余文静 张丹 谯凤 《安徽医科大学学报》 CAS 北大核心 2019年第2期203-206,共4页
目的探讨^(18)F-氟赤硝基咪唑micro PET/CT评价裸鼠MDA-MB231乳腺癌早期放疗疗效的价值。方法建立16只裸鼠MDA-MB231乳腺癌模型,将其按照随机对照原则分为两组:对照组(A组)、放疗组(B组),每组8只。每组裸鼠行micro PET/CT显像,测定每只... 目的探讨^(18)F-氟赤硝基咪唑micro PET/CT评价裸鼠MDA-MB231乳腺癌早期放疗疗效的价值。方法建立16只裸鼠MDA-MB231乳腺癌模型,将其按照随机对照原则分为两组:对照组(A组)、放疗组(B组),每组8只。每组裸鼠行micro PET/CT显像,测定每只裸鼠肿瘤SUVmax值。完成显像后,常规HE染色观察每组肿瘤组织形态学特征,免疫组化方法测定每组肿瘤细胞乏氧诱导因子-1α(HIF-1α)的表达情况。结果放疗前,对照组与放疗组SUVmax值差异无统计学意义(t=0. 375,P> 0. 05)。放疗组放疗后48 h裸鼠肿瘤组织SUVmax值较放疗前(t=9. 958,P <0. 05)、放疗后24 h(t=16. 506,P <0. 05)明显降低,差异有统计学意义(F=58. 860,P <0. 05)。放疗后24 h SUVmax值也低于放疗前24 h(t=5. 405,P <0. 05),差异有统计学意义。HE染色结果显示放疗组肿瘤细胞坏死较对照组更加明显。免疫组化结果显示放疗组放疗后HIF-1α表达阳性率明显低于放疗前(t=14. 802,P <0. 05),差异具有统计学意义。相关性分析结果显示肿瘤SUVmax与HIF-1α的表达呈明显正相关性(r=0. 865,P <0. 05)。结论^(18)F-氟赤硝基咪唑micro PET/CT可以监测肿瘤内部的乏氧状态,并且可以评价裸鼠MDA-MB231乳腺癌的早期放疗疗效。 展开更多
关键词 18F-氟赤硝基咪唑 micro PET/CT 放疗疗效 乏氧诱导因子-
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