PAN基碳纤维在表面处理中的拉曼光谱研究

采用激光拉曼光谱研究了PAN基碳纤维在表面处理中的微结构变化,分析了表面处理前后碳纤维的一级拉曼光谱特性。结果表明：拉曼光谱中主要的D峰和G峰的拉曼频移、半高宽以及各个不同拉曼频移位置对应肩峰的积分面积比是表征碳纤维物相结构变化的重要参数。经过不同的表面处理,PAN基碳纤维的一级拉曼光谱参数发生了一定程度变化,D峰和G峰的拉曼峰位向高波数偏移,表征石墨微晶尺寸的R值有所提高,这说明在表面处理后碳纤维的石墨微结构受到刻蚀,微晶尺寸有所减小,石墨微晶的边界活性增大;此外,表征碳纤维结构有序程度和缺陷多少的D峰和G峰的半高宽均有减小,表征无定型碳结构或某种有机官能团的A峰和D″峰的相对积分面积减小,这说明与乱层石墨结构相比,碳纤维中存在的无定型碳结构更容易被刻蚀,经过表面处理之后无定型碳的物相比例减小,这与碳纤维XRD图谱中表观结晶度提高的规律相一致。因此,利用激光拉曼光谱可研究碳纤维物相结构的变化规律。     

PAN基碳纤维在石墨化过程中的拉曼光谱

采用激光拉曼光谱研究了PAN基碳纤维在石墨化(2 000～3 000 ℃)过程中的结构变化;比较了石墨化前后纤维表面和断面拉曼光谱特征。结果表明：高温石墨化后,碳纤维的一级拉曼光谱有3个峰(D,G和D′),表征碳纤维结构有序程度的拉曼参数主要有D和G峰的半高宽(FWHM)、G峰的拉曼位移和D与G峰的积分强度比R(I_D/I_G)。随着热处理温度的提高,D和G峰的半高宽、G峰的拉曼位移和R值均逐渐减小,即使经过3 000 ℃高温处理后,D峰仍然存在,R值为0.19,说明纤维中仍存在无序结构。另外,R值与纤维中石墨微晶的基面宽度L_a成反比,石墨化后纤维取向性的增加使得表面和断面的拉曼光谱有明显的差异。因此,可利用激光拉曼光谱来定量表征碳纤维的石墨化程度和取向。     

傅里叶变换红外光谱在胃癌淋巴结转移诊断中的应用研究

观察傅里叶变换红外光谱技术无创、原位、快速诊断胃癌淋巴结转移的可行性。联合使用衰减全反射探头及傅里叶变换红外光谱仪测量新鲜离体胃周淋巴结红外光谱,发现每条光谱在吸收波长3 000～1 000 cm-1之间循序出现13条谱带,依据病理检测结果将淋巴结分为转移组及非转移组,比较两组淋巴结红外光谱的峰位和相对峰强等指标结果,最后进行标准统计学分析。36例胃癌患者,共检测淋巴结720枚,其中转移性淋巴结180枚,未转移540枚;与非转移淋巴结相比,转移淋巴结红外光谱有如下特征：(1)与核酸相关的峰强比I_{1 240}/I_{1 460}(p=0.015)和I_{1 080}/I_{1 460}(p=0.034)显著升高,提示转移淋巴结细胞的核酸含量增多;(2)与蛋白相关的I_{1 640}/I_{1 460}(p=0.001)和I_{1 546}/I_{1 460}(p=0.027)峰强比值升高,表明转移淋巴结组织的蛋白质含量明显升高;(3)与脂类相关的I_{2 855}/I_{1 460}和I_{1 740}/I_{1 460}显著降低(p＜0.001),提示癌组织脂类含量相对减少;(4)I_{1 160}/I_{1 460}(p=0.023)显著降低,表明恶性细胞糖类物质的减少。研究结果显示,傅里叶变换红外光谱分析技术有望成为术中原位、在体和快速诊断胃癌淋巴结转移的新方法。     

红外杂化单光束谱的性质

同一样品不同厚度(b₁和b₂)的两单光束谱ø_b1和ø_b2经线性组合得到杂化单光束谱ø_α=αø_b1+(1-α)ø_b2=αø₀e-Kb₁+(1-α)ø₀e-Kb₂,α为杂化系数。通过改变杂化系数α,就可获得任意强度的杂化谱ø_α。系统研究了杂化光谱ø_α的性质。研究表明,只要控制合适的条件,则厚度为(b₂-αb₂+αb₁)的真实样品的单光束谱ø_b(b=b₂-αb₂+αb₁)与杂化谱ø_α高度相似,ø_α的失真程度可忽略不计。也就是说,厚度在b₁～b₂间任一厚度b的真实样品的单光束谱都可用杂化谱ø_α来表达,ø_α≈ø_b。因此,不需制备厚度为b的样品,通过改变杂化系数α就可获得研究者所希望强度的单光束谱ø_b。杂化谱方法有望在扣除背景干扰等方面得到广泛应用。     

胆管癌新鲜离体组织的傅里叶变换红外光谱研究

该研究探讨了运用傅里叶变换红外(FTIR)光谱技术对胆管癌进行术中原位、无创和快速诊断的可行性。联合应用傅里叶变换红外光谱仪和衰减全反射(ATR)探头,测定了26例胆管癌和43例良性胆管疾病新鲜离体组织的红外吸收光谱,发现每条光谱在3 800～1 000 cm-1之间循序出现了12个谱带。测量各个谱带的峰位、峰强和峰面积值,然后计算出各谱带的相对峰强和相对峰面积比值,最后进行标准统计学分析。比较胆管癌与良性胆管组织的光谱发现有以下特征：(1)2 925 cm-1谱带明显地向低波数移位(P=0.033);(2)峰强比I_{1 083}/I_{1 460}(P=0.005)和峰面积比S1 083/S_{1 460}(P=0.001),S_{1 240}/S_{1 460}(P=0.025)明显升高,说明癌组织中核酸相对脂类含量明显增加;(3)峰强比I_{1 550}/I_{1 083}(P=0.000)和峰面积比S_{1 550}/S_{1 083}(P=0.000)明显下降,提示蛋白质相对核酸的含量下降。研究结果表明,FTIR有望成为一种术中原位、在体和快速诊断胆管癌的新方法。     

FTIR光谱法整体评价蜂王浆新鲜度的研究

测定了在不同温度下经过不同时间贮存后的蜂王浆的FTIR光谱,以新采收蜂王浆的红外谱图为参考标准谱,利用光谱比对软件进行了一系列的相关分析。结果表明：不同贮存条件下的蜂王浆红外光谱图中酰胺Ⅰ带(1 700～1 600 cm-1)波段的相关系数和相对峰强度I_{1 647}/I_{1 541},I_{1 647}/I_{1 409},I_{1 647}/I_{1 247}和I_{1 647}/I_{1 054}都随着蜂王浆贮存时间延长和温度升高而降低,且与贮存时间存在着良好的线性关系,变化幅度顺序为28＞16＞4＞-18 ℃。因此,初步选定红外光谱图中酰胺Ⅰ带的相关系数和4个相对峰强度(I_{1 647}/I_{1 541},I_{1 647}/I_{1 409}、I_{1 647}/I_{1 247}和I_{1 647}/I_{1 054})作为新鲜度的评价指标,相关系数的阈值设定为0.910 0,4个相对峰强度的阈值分别设定为1.744,2.430,3.345和1.412。只要有1个或多个指标低于相应的阈值,可初步判定此蜂王浆是不新鲜的。该方法利用FTIR光谱法并结合计算机辅助解析技术能从宏观上、整体和快速地评价蜂王浆的新鲜度。     

直肠组织的高分辨魔角旋转核磁共振波谱研究

文章对6例直肠癌变及正常组织进行高分辨魔角旋转核磁共振波谱研究,结果显示直肠癌变和正常组织的核磁共振氢谱存在明显差异。这可以通过特征峰面积与0.88处峰积分面积的比值上的差异看出：（1）在化学位移0.75～1.55之间,癌组织各种氨基酸[缬氨酸,异亮氨酸,亮氨酸]与脂肪酸甲基的比值（I₂/I₁）,癌组织乳酸盐与脂肪酸甲基的比值(I₄/I₁)都明显增大。（2）在化学位移1.55～2.90之间,癌变组织中亮氨酸、赖氨酸、异亮氨酸与脂肪酸甲基的比值（I₇/I₁）, 谷氨酸、谷氨酰胺、缬氨酸、琥珀酸与脂肪酸甲基的比值((I₉+I₁₁)/I₁)、天冬氨酸与脂肪酸甲基的比值((I₁₂+I₁₄)/I₁)都较正常组织明显增大。（3）在化学位移2.90～3.49之间,癌变组织氨基酸与脂肪酸甲基的比值（I₁₅/I₁）、胆碱类与脂肪酸甲基的比值((I₁₆+I₁₇)/I₁)、牛磺酸与脂肪酸甲基的比值((I₁₈+I₁₉)/I₁)都较正常组织明显增大。（4）在化学位移3.49～4.50之间,其他代谢物与脂肪酸甲基的比值（I₂₀/I₁）,以及甘油基与脂肪酸甲基的比值（I₂₂/I₁）在癌变组织中都有增大的趋势。（5）化学位移4.5～10之间,癌变组织的核苷酸发生了变化,癌变组织的不饱和脂肪酸与脂肪酸甲基的比值（I₂₄/I₁）明显减小。（6）在化学位移-8～0.75之间,癌变组织的谱峰有减少的趋势。通过上述分析可知,通过癌变与正常组织代谢物NMR谱峰的差异,可以区分癌变和正常组织。说明核磁共振波谱技术可能发展成为一种诊断直肠癌的新方法。     

激发态Rb原子间的碰撞能量转移

脉冲激光器激发Rb原子到5P_1/2态,通过碰撞能量转移Rb(5P_1/2)+Rb(5S_1/2)Rb(5P_3/2)+Rb(5S_1/2)产生5P_3/2原子,研究了5P_1/2+5P_1/2,5P_3/2+5P_3/2,5P_1/2+5P_3/2的碰撞能量合并产生态的过程。5P_1/2态原子密度利用Rb空心阴极灯通过光学吸收方法得到,而5P_3/2态密度通过5P_3/25S_1/2(D2线)与5P_1/25S_1/2(D₁线)跃迁的荧光比得到。因为5P_3/2+5P_3/2或5P_1/2+5P_3/2的能量和与5D态的能量差远小于5P_1/2+5P_1/2与5D态的能量差,因此5P_3/2+5P_3/2,5P_1/2+5P_3/2的过程将影响5P_1/2+5P_1/2的测量结果。由于精细结构能量转移的时间比5D态寿命小得多,故5P_1/2+5P_1/2,5P_1/2+5P_3/2和5P_3/2+5P_3/2产生的5D5P荧光是同时产生的。在不同的池温下测量了积分荧光信号的相对强度,5P态原子有效寿命由辐射陷获的理论得到,结合激发态原子密度得到了5P_1/2+5P_1/2,5P_1/2+5P_3/2和5P_3/2+5P_3/2碰撞能量合并截面分别为7.810-15,2.9×10-14和3.1×10-14 cm2。结果表明5P_1/2+5P_3/2与5P_3/2+5P_3/2产生5D_3/2态的截面基本是相等的。     

光学厚Rb蒸气界面附近后向荧光光谱研究

在存在表面耗散层的纯Rb光学厚蒸气中,利用小功率可调谐半导体激光器泵浦Rb(5P_3/2)的超精细结构能级,测量和分析了780 nm(5P_3/2→5S_1/2)和795 nm(5P_1/2→5S_1/2)后向荧光的强度和线形,耗散层(近区)起光谱滤波器的作用。有两种可能产生5P_1/2态原子的机制,第一种机制是Rb(5P_3/2)+Rb(5S_1/2)→Rb(5P_1/2)+Rb(5S_1/2);第二种机制是Rb(5D)+Rb(5S)→Rb(5P)+Rb(5P),对于每一种机制,给出了后向敏化荧光的理论公式。研究后向荧光时,必须要确定荧光强度与激光功率的关系和荧光线形。激光频率扫描超精细结构共振线,得到的敏化后向荧光795 nm线形与共振荧光780 nm线形相似,其荧光强度与荧光功率有线性关系。因此,基本上可以用第一种机制解释5P_1/2态布居机制。理论证明了,第二种机制产生的敏化后向荧光强度应与激光功率平方成比例,这与实验结果是不同的,第二种机制不能解释耗散层界面后向敏化荧光的产生。     

鸡粪堆肥有机质转化的荧光定量化表征

采用荧光分析技术和数学分析方法,对不同阶段鸡粪堆肥样品提取出的水溶性有机物进行了特征荧光参数定量化表征。结果显示：随着堆肥的进行,类腐殖质荧光峰与类蛋白荧光峰荧光强度的比值I₃₃₀/I₂₈₀、465 nm激发波长下发射光谱中470～640 nm范围内荧光积分面积A_470～640及240 nm激发波长下发射光谱中后四分之一波段与前四分之一波段的荧光强度积分面积比A_{435～480 nm}/A_{300～345 nm}均不断增大,表明堆肥腐殖化程度加大。三维荧光光谱显示,随着堆肥的进行类蛋白峰强度不断降低,而类富里酸峰强度不断增大,至堆肥结束类蛋白荧光基本消失;紫外区与可见区类富里酸峰荧光强度的比值r_{(A, C)}随着堆肥的进行总体呈明显下降趋势,但出现了较大波动。相关性分析显示,I₃₃₀/I₂₈₀,A_470～640及A_{435～480 nm}/A_{300～345 nm}两两间显著相关,而r_{(A, C)}受其他因素影响较大,与上述３个参数未达到显著相关水平。结果表明,I₃₃₀/I₂₈₀,A_470～640及A_{435～480 nm}/A_{300～345 nm}均能有效表征堆肥腐殖化进程。     

Quantitative structure–property relationships of polyacrylonitrile-based graphite fibers revealed by laser confocal Raman spectroscopy

A series of polyacrylonitrile-based graphite fibers with different tensile modulus and electrical resistivity were characterized by laser confocal Raman spectroscopy. The Raman spectra of the graphite fibers were deconvolved into five constituent bands using Lorentzian peak fitting function. The Raman spectra parameters, including band position, full width at half maximum, and integrated band area, were extracted and correlated with the tensile modulus and electrical resistivity. Most of the Raman parameters changed monotonically with the tensile modulus and electrical resistivity. A good linear relationship between the electrical resistivity and the structural order was found.     

Raman scattering characterization of a carbon coating after low-energy argon ion bombardment

The characteristic of Raman scattering spectra of a carbon coating, which was modified by radio frequency argon plasma, has been investigated. The argon ion bombardment causes changes in the microstructure and amount of stress in the coating. Raman scattering spectra are discussed in terms of intensity, bandwidth and wavenumber. The evolvement of Raman spectra shows the following behavior with increasing bombardment time: the intensity changes of the disordered D band, amorphous D″ band and graphite G band could be separated into several stages; low-energy argon ion bombardment over a short period can reduce the number of defects in the carbon coating, while a larger bombardment period can increase the number of defects; the widths of the D and G bands both increase, while that of the D″ band decreases; the wavenumbers of all the three bands fluctuate according to the changes in electronic configuration and amount of stress in the carbon coating.     

Raman identification of lonsdaleite in Popigai impactites

Micro‐Raman spectroscopy and X‐ray diffraction method (XRD) were used to characterize impact carbonaceous rocks excavated from the Popigai crater (Siberia). The deconvolution of the first‐order Raman spectra of the rocks containing different amounts of carbon phases (diamond, lonsdaleite and graphite) allowed the identification of lonsdaleite spectrum. The most intensive band at 1292–1303 cm⁻¹ was ascribed to A_1g vibration mode of lonsdaleite, whereas the less intense band at 1219–1244 cm⁻¹ was attributed, in agreement with previously reported ab initio calculations, to E_2g vibration mode. The established correlation between the intensities of Raman and XRD peaks permits a rough estimation of lonsdaleite/diamond phase ratio in the impact rocks using micro‐Raman measurements. The second‐order Raman spectra of lonsdaleite–diamond rocks were recorded. Copyright © 2014 John Wiley & Sons, Ltd.     

Origin of the low-frequency band in Raman spectra of multi-walled carbon nanotubes synthesized by the CVD method

The origin of the low-frequency band (250–300 cm^?1) in the Raman spectra of multi-walled carbon nanotubes (MWCNTs) produced by the CVD method has been studied. The studies performed by Raman spectroscopy, transmission electron microscopy, Auger spectroscopy, and X-ray photoelectron spectroscopy after chemical and thermal treatments allow the assumption that this band belongs to radial vibrations of carbon atoms in internal walls of MWCNTs.     

光纤共振和预共振喇曼光谱

在液芯光纤内产生共振和预共振喇曼效应,喇曼光谱强度可以大幅度提高,最高可达10⁹倍.本文介绍获得光纤(预)共振喇曼光谱的可行性、实验及实验结果.用远离吸收带的激光激发获得了α甲基吡啶预共振喇曼光谱.用小功率激光(0.8mW)、低浓度溶液(9.6×10¹²mol/L)还获得了β叶红素在CS₂中的共振喇曼光谱.     

Temperature-induced transformations in hydrogenated and fluorinated single-wall carbon nanotubes studied by Raman scattering

Raman spectra of hydrogenated and fluorinated single-wall carbon nanotubes (SWCNTs) are measured at ambient temperature before and after heat treatment. The spectra of the as-prepared hydrogenated SWCNTs show a giant structureless band in the visible region that screens the Raman peaks related to the carbon atom vibrations. The onset of this strong band follows the excitation laser line, which is typical of hot luminescence. The intensity of the luminescence background decreases exponentially with the annealing time, while the dependence of the luminescence decay time constant on the annealing temperature is of the Arrhenius type with the activation energy E _a = 465 ± 44 meV. The luminescence background in the Raman spectra of the fluorinated SWCNTs is comparable with the Raman peak intensity and decreases exponentially with the annealing time. The dependence of the decay time constant on the temperature is again of the Arrhenius type with the activation energy E _a = 90 ± 8 meV. The appearance of hot luminescence is related to the upshift of the fundamental energy gap in functionalized SWCNTs and the structural disorder induced by random binding of hydrogen or fluorine atoms. The luminescence background disappears upon annealing in vacuum or in air after removal of hydrogen (fluorine), while the annealed samples still demonstrate large structural disorder.     

Confocal Raman spectromicroscopy for tin-core/carbon-shell nanowire heterostructure

High density heterostructures of carbon nanotubes encapsulated single crystalline tin nanowires have been characterized by Raman spectromicroscopy. The morphology, composition and structure of the synthesized nanoheterostructures were examined by using scanning electron microscopy, transmission electron microscopy. The Raman spectra obviously manifest the crystalline nano-graphite within amorphous carbon walls in the heterostructures. The Raman image reproduces the pristine heterostructures of the CNTs as seen in SEM image, which illustrate the single nanowires oriented uniformly grown on micro-graphitic fibers. It was found that the resultant heterostructures are luminescent which was attributed to crystalline nano-graphite embedded in the amorphous carbon matrix, which is a consequence of excitons localization within an increasing number of sp² rich clusters. The contrast in the Raman image reflects nonuniform distribution of the graphite cluster size which acts as the radiative centers. The luminescent property was reviewed. The enhanced Raman spectra and luminescent property by the well-defined tin nanowires inside the heterostructures was revealed.     

How to obtain a reliable structural characterization of polished graphitized carbons by Raman microspectroscopy

A series of graphitized carbon materials, produced by the pyrolysis of an anthracene‐based coke at temperatures ranging from 1600 to 2900 °C, were studied by Raman microspectroscopy to assess the applicability of this technique to the particular case of polished carbon materials. The polishing process was shown to change significantly the first‐order Raman spectra (D band intensity increase) and therefore to induce unacceptable errors in the characterization of the intrinsic structure of these materials. The deconvolution of Raman spectra, related to the unpolished graphitized carbons at varying temperatures, highlighted a linear relationship between the intensity ratio I_D/I_G and the G band width. Thus, as the latter appears to be insensitive to the polishing, we highly recommend using it for a reliable assessment of the intrinsic structural disorder of polished carbon materials. Copyright © 2011 John Wiley & Sons, Ltd.