Dynamical theory of spectroscopy with pulse excitation ——Application to continuum Raman of IBr

In the coupling system, the dynamical theory of Raman spectroscopy with pulse excitation was developed, and applied to the continuum Raman of IBr. The structure of Raman excitation profile of IBr was explained, which does not follow the new reflection principle.     

Abnormal Raman spectral phenomenon of silicon nanowires

The Raman spectra of two one-dimensional silicon nanowire samples with different excitation wavetengths were measured and an abnormal phenomenon was discovered that the Raman spectral features change with the wavetengths of excitation. Closer analysis of the crystalline structure of samples and the changes in Raman spectral features showed that the abnormal behavior is the result of resonance Raman scattering setection effect.     

Raman spectra of SiC nanorods with different excitation wavelengths

With increasing excitation wavelength from 514 to 782 nm, a significant difference in the Raman spectra of SiC nanorods was observed as compared to bulk material. The intensity ratio of the LO mode to that of the IF mode increases with the excitation wavelength increasing. This has been identified as resonant Raman scattering caused by Fröhlich interaction.     

单晶体材料WTe2的Raman光谱

利用波长为532 nm的激光分别沿单晶体材料WTe₂的b轴和c轴进行激发获得相应的Raman光谱, 结合第一性原理计算, 对两种激发条件下单晶体材料WTe₂的Raman光谱进行研究, 并根据单晶体材料WTe₂的偏振Raman光谱及理论计算结果, 分别对测量获得单晶体材料WTe₂的Raman光谱进行归属. 实验结果表明, 沿单晶体材料WTe₂的b轴比c轴激发获得的Raman光谱变化明显.     

Controlling inelastic light scattering quantum pathways in graphene

Inelastic light scattering spectroscopy has, since its first discovery, been an indispensable tool in physical science for probing elementary excitations, such as phonons, magnons and plasmons in both bulk and nanoscale materials. In the quantum mechanical picture of inelastic light scattering, incident photons first excite a set of intermediate electronic states, which then generate crystal elementary excitations and radiate energy-shifted photons. The intermediate electronic excitations therefore have a crucial role as quantum pathways in inelastic light scattering, and this is exemplified by resonant Raman scattering and Raman interference. The ability to control these excitation pathways can open up new opportunities to probe, manipulate and utilize inelastic light scattering. Here we achieve excitation pathway control in graphene with electrostatic doping. Our study reveals quantum interference between different Raman pathways in graphene: when some of the pathways are blocked, the one-phonon Raman intensity does not diminish, as commonly expected, but increases dramatically. This discovery sheds new light on the understanding of resonance Raman scattering in graphene. In addition, we demonstrate hot-electron luminescence in graphene as the Fermi energy approaches half the laser excitation energy. This hot luminescence, which is another form of inelastic light scattering, results from excited-state relaxation channels that become available only in heavily doped graphene.     

水的受激Raman散射

利用532 nm脉冲激光研究水的受激Raman散射, 并利用激光诱导产生的等离子体解释了前向、 后向和侧向水受激Raman散射的差异. 结果表明: 水与甲醇和乙醇的受激Raman阈值基本相同,  大于苯、 甲苯和二硫化碳的受激Raman阈值; 当能量为140 mJ时, 出现前向Stokes和反Stokes 3 426 cm^-1谱线, 后向和侧向出现3 400,3 268 cm^-1的受激Stokes谱线.     

Brauer特征标的扩张

设G为有限群,N△G且G/N可解.用Irr(G)表示G的不可约(复)特征标集合.如果θ∈Irr(N)为G-不变特征标且(θ(1),|G∶N|)=1,I.M.Isaacs证明了,θ可扩张当且仅当行列式特征标det(θ)可扩张.在此基础上考虑关于此定理的p-Brauer特征标的形式.用IBr(G)表示G的不可约p-Brauer特征标的集合.假设θ∈IBr(N)为G-不变的且(|G∶N|p′,θ(1))=1,其中p为1个固定的素数,则θ可扩张到G当且仅当det(θ)可扩张到G.     

正规三元组上的模特征标性质

在有限群模表示理论中,模特征标诱导和限制下的动态表现以及对应关系是有意义的问题,尤其是考虑如何把常表示的结论推广到模表示上,得到相应的模特征标结果一直是表示论中的重要课题.对于有限群G,如果N和M均为G的正规子群且N包含M,M.L.Lewis称(G,N,M)为群G的正规三元组,并且对其上的常特征标问题进行了探讨.首先给出了模特征标的一些基本性质,然后在正规三元组(G,N,M)条件下,得到了IBr(N)和IBr(M)中元素限制和诱导的若干动态表现,讨论了其上不可约模特征标的不变性和唯一性问题,并且进一步获得了互素正规三元组(X,N,M)上的几个模特征标对应关系.     

单个红细胞的拉曼光谱研究

研究了不同物种的血红细胞的拉曼光谱,采用一个波长为785nm的半导体激光束来囚禁血红细胞和激发血红细胞的拉曼光谱。结果显示不同物种血红细胞的拉曼光谱在1603cm^-1苯丙氨酸和色氨酸的C=C平行振动模及1616cm^-1酪氨酸和色氨酸的C=C拉伸模有明显的差异,这可以用来作为不同种血红细胞鉴定的特征标记。表明激光镊子拉曼光谱技术可以成为血红细胞分析的有效手段。     

2×2熔锥光纤表面增强拉曼散射实验

基于光纤渐逝波原理,结合表面增强拉曼散射(surface-enhanced Raman scattering,SERS)技术,实验研究一种银溶胶涂覆的2×2熔锥光纤的SERS特性.熔锥光纤由一对单模光纤经过熔融拉制而成,固化在其表面的银溶胶为表面活性基底,起拉曼增强作用.随着锥区长度的增加,纤芯逐渐减小,其对光的束缚能力变弱,从而透射出较强的可作为拉曼激发光源的渐逝波.实验中,以R6G为待测溶液,在耦合锥区探测到低浓度目标分子R6G的拉曼光谱,其最低检测浓度达到了10-8 mol/L。     

强激光场中脉冲激发的连续拉曼光谱理论

在强场中发展了时间相关的光谱理论，提出了一个有很好性质的近似，籍此长脉冲激发体系的计算将变得非常容易，讨论了强场下的连续拉曼光谱，发现产生类荧光散射的入射频率范围比弱场大。     

金属纳米颗粒／微纳结构金属膜增强拉曼研究进展

被称为“指纹谱”的分子拉曼谱及拉曼散射成像在生物及化学单分子识别领域具有重要应用。问题的关键是分子的拉曼散射截面小,利用金属纳米颗粒（LSP）局域场增强特性及其与金属膜（SPP）相互作用可产生比 LSP （ SPP）更强的局域场及尖角结构金属纳米颗粒的“热点天线”效应,可实现单分子拉曼信号的激发与辐射双共振增强效应。本文综述有关金属纳米颗粒和微纳结构金属膜相耦合增强分子拉曼信号的研究进展。     

Tb~(3+)掺杂β-Ga_2O_3纳米粉末的结构和光致发光性质的研究

采用溶胶-凝胶法制备Tb3+掺杂β-Ga2O3纳米粉末.用X-射线衍射(XRD)、拉曼(Raman)、光致发光激发谱(PLE)和发光谱(PL)对其进行了一系列的表征. XRD 和 Raman 的结果表明: Tb3+离子的掺入没有改变β-Ga2O3结构.用350 nm的激发光去激发Tb3+掺杂β-Ga2O3纳米粉末,样品的最强峰在543 nm (5D4-7F5)附近,对应着Tb3+离子的绿光发射.此外,还讨论了能量传递机制.     

人工自旋轨道耦合玻色-爱因斯坦凝聚体的元激发

文章研究了准一维人工自旋轨道耦合玻色-爱因斯坦凝聚体中的元激发. 利用平均场理论和波戈留波夫近似方法,分别计算了此原子凝聚体在依赖于拉曼耦合强度的零动量相和平面波相的激发谱. 结果表明,在零动量相时体系激发谱的2个分支都呈现出对称结构;相反地,在较小拉曼耦合强度时的平面波相,激发谱呈现出旋子最低结构,从而预示了体系从平面波相到条纹相的相变. 文中证明了在平面波相和零动量相的相变附近,低频元激发的声速急剧下降并消失于相变点. 文章全面分析了人工自旋轨道耦合原子凝聚体的元激发特性,为实验研究该类崭新的多体系统提供理论支持.     

硅掺杂氮化硼纳米管的制备及其光学性质

通过高温热解聚合物前驱体方法制备Si掺杂BN纳米管. 采用扫描电子显微镜（SEM）和透射电子显微镜（TEM）对样品的结构与形貌进行表征, 结果表明, 样品属于一端开口的竹节状BN纳米管, 通过变温光致发光谱及喇曼光谱研究了Si掺杂BN纳米管的光学性质.      

键联于核酸的激发态水溶铜卟啉共振拉曼光谱研究

本文测量了键联于核酸的激发态水溶铜卟啉共振拉曼光谱.结果表明,位于1550cm~(-1)和1346cm~(-1)附近的两条谱带归属于受激铜卟啉拉曼带,其强度与核酸和铜卟啉的种类、核酸所含的(AT)_n结构和受激铜卟啉沟槽键联于核酸的能力有关.文中对插入DNA中GC位置上的基态铜卟啉在受激状态下能沟槽键联于—ATAT一位置这一现象作了定性的解释.     

Quaternary structure-induced photoreduction of haem of haemoglobin.

Spectroscopic studies have provided extensive information on the primary process of visual pigments and photoexcitation of chlorophyll as well as their effects on photoreactivity on the higher-order structures of protein has been observed only rarely. Resonance Raman spectroscopy can reveal the vibrational frequencies of the chromophore in a molecule provided the excitation wavelength is in the absorption band of that molecule. As the visible absorption bands of haemproteins are due to pi pi* transitions of the porphyrin ring, we can selectively observe the vibrational frequencies of iron porphyrin during in situ interactions with immediate amino acid residues of protein when the wavelength of excitation light is close to the Soret or Q band. Correlation of some vibrational frequencies of haem with the oxidation and spin states of the haem iron has been studied in detail and an empirical rules has been established. This method is therefore especially suitable for the study of an effect of higher-order structures of protein on the chromophore. We report here a photoreaction facilitated by a particular quaternary structure of protein--in various haemoglobins resonance Raman spectroscopy showed that reversible photoreduction of haem took place in the T state but not the R state.     

安徽史前孙家城和黄家堰等遗址出土玉器的无损科技研究

孙家城和黄家堰等遗址是安徽史前文化的重要遗址,针对这些遗址出土的玉器,从材质无损鉴别的方法、化学成分、加工微痕迹以及受沁情况等方面进行了分析.结果显示采用785 nm激发光源的拉曼光谱可以有效克服荧光背景,结合632.8 nm 激发光源可以很好地应用于古代玉器的无损材质鉴别;采用G(o)bel Mirror的X射线衍射...     

Experimental quest for orbital waves

One challenge in condensed-matter physics is the experimental confirmation of a new kind of elementary excitation orbital waves, or orbitons, which are predicted to exist in an orbitally ordered state. Saitoh et al. have observed three peaks at 160, 144 and 126 meV in the Raman scattering of orbitally ordered lanthanum manganate (LaMnO(3)), and interpret these as evidence of orbitons. However, we find similar peaks in the optical conductivity, sigma(omega), of LaMnO(3) and point out that the direct observation of orbitons in sigma(omega) is prohibited by a selection rule. This suggests that the Raman peaks observed by Saitoh et al. arise from multiphonons, and that the existence of orbitons has yet to be experimentally confirmed.     

结晶紫表面增强拉曼与时间关系研究

【目的】研究银包金纳米颗粒(Ag@AuNP)对结晶紫信号的增强效果与时间的关系。【方法】用新型纳米材料银包金纳米颗粒作为拉曼增强基底,采用785nm激光激发结晶紫表面增强拉曼光谱,统计光谱特征峰强度变化趋势。【结果】结晶紫725cm-1,801cm-1,914cm-1,1177cm-1,1392cm-1,1588cm-1等特征峰强度在0~30min内随时间的延长而逐渐升高,达到一个平台后随时间(30~36min)的增加基本保持不变。【结论】最优最快的结晶紫表面增强光谱的测定时间约为30min,该结论丰富了表面增强拉曼的研究成果。