Vertex correction effects on nonlinear optical response

The effects of vertex corrections due to frequency modulation are exactly evaluated on the emission spectra from the two-level electronic system pumped by the laser of arbitrary intensity and the absorption spectra of the weak probe field of this system. Here the frequency modulation is assumed to obey the Gaussian-Markoffian process. The two-time correlation function of the polarizations which describe the emission and absorption spectra is represented as the product of two propagators and a vertex correction. This correction is described in the form of the summation of the products of the matrix continued fractions. This correction is numerically demonstrated to be quite large for the emission spectrum in the case of the slow or strong frequency modulation and weak laser field, and for the absorption spectrum in the case of intermediate modulation and laser intensity.     

The polarized reflection and absorption spectra of perylene crystals in monomeric and dimeric forms

The electronic absorption spectra of perylene crystals in the α- and β-forms were measured by the normal incidence reflection method in the spectral region from 20 000 to 60 000 cm^?1. From the absorption spectrum polarized perpendicular to [1$\text{1}$0] axis of the α-form crystal, the bands around 24 000 cm^?1 were determined to be polarized along the long molecular axis. Two strong bands with different polarizations were observed around 50 000 cm^?1 for each of the α- and β-perylene crystals and were assigned to the transitions to the ¹B_2u and ¹B_3u states. The observed polarized absorption spectra as a whole were consistent with the theoretical results by Hummel and Ruedenberg and the reflection method was found to be suitable to the polarized absorption measurement of strong bands of crystals. The observed factor-group splittings were compared with the theoretical values, the oriented gas model being found to be applicable to the β-form crystal.     

稀土氟碳酸盐矿物的光致发光谱和吸收谱研究

测定并讨论了产自四川冕宁矿区的氟碳铈矿和产自内蒙白云鄂博稀土矿区的黄河矿、氟碳钙铈矿、氟碳铈钡矿的光致发光谱。结果表明,稀土氟碳酸盐矿物在488.0nm和514.5nm激光激发下的光致发光中心是Nd3+,发光谱中的所有谱带均出自Nd3+的辐射跃迁。在488.0nm激光激发下,稀土氟碳酸盐矿物在495nm到733nm谱区的发光谱带强而尖锐,但在514.5nm激光激发下,这个谱区的谱带明显变弱或消失,转而出现783nm到907nm谱区的强发光谱带。可见光吸收谱表明稀土氟碳酸盐矿物对可见光的吸收也与矿物中的Nd3+有关。     

On the luminescence of TlCl+KCl phosphor

The measurements on the luminescence spectra of TlCl+KCl mixed phosphor under low energy cathode rays at 80° K have been presented here. The reflectance as well as excitation spectra of this mixed phosphors have also been studied. The X-ray diffraction studies of the samples along with the optical studies show that the mixed phosphor consists of two phases: (1) KCl:Tl (2) TlCl:K. It has been observed that the emission bands due to thallous chloride are gradually quenched with the increase in potassium chloride content of the phosphor; further, the emission bands supposed to be due to KCl:Tl phosphors gradually appear. Since some of the emission bands obtained with KCl:Tl phosphors at high thallium content are also present in the luminescence spectra of thallous chloride it is suggested that such bands should be attributed to undissociated thallous chloride present in KCl:Tl phosphor. The quenching of thallous chloride emission by the incorporation of potassium chloride in the system has been explained as being due to the absence of stoichiometric excess of thallium in such mixed system. The results also show that the absorption spectra of the mixed system is determined by the minor components KCl:Tl. This indicates that the absorption spectra of KCl:Tl phosphor should not be affected by the presence of undissociated thallous chloride.     

Magnetic Circular Dichroism Spectra of p-Disubstituted Benzenes Possessing Both Electron-Donating and Accepting Groups

Abstract

The magnetic circular dichroism (MCD) and absorption spectra of some p-disubstituted benzenes possessing both electron-donating and accepting groups were measured. The electronic spectra of the above compounds are characterized by the appearance of two absorption bands, one of which appears at 25000–40000 cm^?1 region with large intensity, and another at 40000–50000 cm^?1 region with rather small intensity. These absorption bands, especially the latter one, have been investigated by means of the MCD spectra and molecular orbital calculations based on the Pariser-Parr-Pople method.     

Single vibronic level fluorescence of CrO2Cl2 excited by a tunable cw dye laser

Fluorescence of gaseous chromyl chloride has been excited using a tunable cw dye laser, and fluorescence spectra have been recorded for excitation in 20 different absorption bands. The vibrational structure of these spectra shows activity of all of the totally symmetric vibrations, but there is no evidence for activity of any non-totally symmetric vibration as previously proposed from absorption spectra. We conclude that the absorption band system near 5800 Å comprises at least two electronic transitions.     

Electronic structure and resonant X-ray emission spectra of carbon shells of iron nanoparticles

The electronic structure of carbon shells of carbon encapsulated iron nanoparticles carbon encapsulated Fe@C has been studied by X-ray resonant emission and X-ray absorption spectroscopy. The recorded spectra have been compared to the density functional calculations of the electronic structure of graphene. It has been shown that an Fe@C carbon shell can be represented in the form of several graphene layers with Stone-Wales defects. The dispersion of energy bands of Fe@C has been examined using the measured C Kα resonant X-ray emission spectra.     

Electronic energy structure of SiO2: An application of the recursion method

The electronic structures of α-quartz, β-cristobalite and stishovite have been calculated using semiempirical tight-binding Hamiltonian and the recursion method. The model describes fairly well the valence states and lower conduction bands as well as trends in band gaps and effective charges. For comparison, the electronic structure of α-quartz has been calculated in Harrison's universal first-neighbour parametrization.     

Specific effects of a polar solvent in optical absorption spectra of 5,12-tetracenequinone

We have measured the optical absorption spectra of 5,12-tetracenequinone (5,12-naphthacenequinone) in polar protic (methanol) and nonpolar (n-hexane) solvents. It has been shown that shifts of some bands in the polar solvent compared to the nonpolar one are caused by the formation of high hydrogen bonds between methanol molecules and the molecules under study. The occurrence of hydrogen bonds leads to changes in the energy gaps between occupied and unoccupied molecular orbitals of 5,12-tetracenequinone and, as a consequence, to corresponding changes in energies of electronic transitions. Based on analysis of the absorption spectra in different solvents in combination with the data of calculations of electronic spectra and taking into account changes in the orbital pattern under the action of the solvent, we have determined exact electronic configurations of electronically excited singlet states of 5,12-tetracenequinone.     

The Infrared and Raman Spectra of β-and α-Tricalcium Phosphate (Ca3(Po4)2)

Factor group analysis was applied to interpret the vibrational spectra of β-and α-tricalcium phosphate (Ca₃(PO₄)₂). The analysis predicts the number of bands formed due to the splitting of the fundamental vibrational modes of the PO₄ ^3-ion. The number of the infrared and Raman bands predicted by this analysis for the two phases are drastically different and can be ascribed to the difference in atomic arrangements in the two phases resulting in greater shielding of the PO₄ ^3-ions in the β-phase than in the α-phase. Discrepancies in the number of predicted and experimentally-observed bands can be attributed to the weak intensities of some vibrational modes or the convolution of vibrations and limited spectral resolution.     

Luminescence of solid cyclic polynitramines

The solid form of the cyclic polynitramines known as RDX and HMX have a weak absorption band in the near ultraviolet which is not observed in spectra of the solvated compounds. Fluorescence measurements on solid samples of these materials show a weak emission, the excitation spectrum of which corresponds to this absorption band. Phosphorescence measurements on the solids at 77 K reveal a long-lived emission, the excitation spectrum again corresponding to the weak absorption band. The absorption and the luminescence bands are attributed to charge-transfer self-complex formation in the solid state, and estimates of the energies of the emissive singlet and triplet excited states are given.     

四取代酞菁金属配合物的紫外-可见吸收光谱和荧光发射光谱研究

报道了16种含哌嗪或含哌啶四取代酞菁金属配合物{R4PcM,R=2-[4-(2-磺基乙基)哌嗪-1-基]乙氧基(SPEO—)、2-(哌啶-1-基)乙氧基(PEO—);取代位置分别在α位和β位;M=Zn(Ⅱ),Ni(Ⅱ),Co(Ⅱ), Cu(Ⅱ)}的UV-Vis吸收光谱和荧光发射光谱的测定,探讨了中心金属离子、取代基种类及其取代位置、溶剂等因素对酞菁金属配合物UV-Vis吸收光谱和荧光发射光谱性质的影响。结果表明:R4PcM的Q带λ_max落在681～718 nm范围内,与相同中心金属离子的无取代酞菁金属配合物(669～671 nm)比较都发生了不同程度的红移,荧光发射光谱与UV-Vis吸收光谱呈镜像关系,特别的是两种β位取代中心金属离子为Zn(Ⅱ)的酞菁金属配合物[β-(SPEO)₄PcZn,β-(PEO)₄PcZn]具有极高的摩尔消光系数、较大的荧光量子产率和较长的荧光寿命,有望开发成新型的光动力诊疗用光敏剂。     

Interpretation of electronic spectra by configuration analysis: Absorption spectra of monosubstituted naphthalenes

The electronic absorption spectra of four monosubstituted naphthalenes, α-, β-naphthols, and α-, β-naphthylamines have been investigated by means of configuration analysis with particular attention to the dependence of spectra on the position of substitution and on the electron-donating power of the substituent. The results of molecular orbital calculations based on the Pariser-Parr-Pople method are analyzed in terms of locally excited states and intramolecular charge-transfer configurations. The characteristic changes in location and polarization of the L_b, L_a, and B_b bands caused by substitution at the α- or β-position are adequately explained by the analysis. Two strong absorption bands of α-substituted naphthalenes, which appear in place of the B_b band of naphthalene, are shown to result from a mixing of the $\text{B}{}_{\mathrm{3u}}{}^{\mathrm{+}}\text{(B}{}_{\mathrm{b}}\text{)}$ and $\text{A}{}_{\mathrm{g}}{}^{\mathrm{?}}$ states. The amino group exerts a great influence on the electronic structure of the parent molecule, so that the B_b band cannot be identified in the spectrum of β-naphthylamine.     

Tm3+激活无水芒硝在真空紫外光激发下的发光性质

采用高温固相反应方法在空气中制备了Na2SO4:Tm2+发光材料.用X射线衍射对晶体结构进行了表征.发射光谱由Tm3+内4f12电子跃迁的窄峰组成.激发光谱分别由Tm3+离子4f12→4f115d跃迁(183nm),O2--Tm3+之间的电荷转移带(170 nm)引起的强激发谱和基质吸收(130,223,258 nm)...     

Encapsulation of Labetalol, Pseudoephedrine in β-cyclodextrin Cavity: Spectral and Molecular Modeling Studies

The absorption and fluorescence spectra of labetalol and pseudoephedrine have been studied in different polarities of solvents and β-cyclodextrin (β-CD). The inclusion complexation with β-CD is investigated by UV-visible, steady state and time resolved fluorescence spectra and PM3 method. In protic solvents, the normal emission originates from a locally excited state and the longer wavelength emission is due to intramolecular charge transfer (TICT). Labetalol forms a 1:2 complex and pseudoephedrine forms 1:1 complex with β-CD. Nanosecond time-resolved studies indicated that both molecules show triexponential decay. Thermodynamic parameters (ΔG, ΔH, ΔS) and HOMO, LUMO orbital investigations confirm the stability of the inclusion complex. The geometry of the most stable complex shows that the aromatic ring is deeply self included inside the β-CD cavity and intermolecular hydrogen bonds were established between host and guest molecules. This suggests that hydrophobic effect and hydrogen bond play an important role in the inclusion process.     

含铅空位PbWO4晶体光学性质的模拟计算

为了研究钨酸铅晶体中铅空位对光学性质的影响,利用完全势缀加平面波局域密度泛函近似,按照能量最低原理采用共轭梯度方法,对含铅空位的PbWO4(PWO)晶体进行结构优化处理。计算了含铅空位的PWO晶体的电子结构、复数折射率、介电函数及吸收光谱,并与完整的PWO晶体进行了比较。结果表明：完整的PWO晶体在可见和近紫外区域内无吸收,而含铅空位的PWO晶体在可见和近紫外区域出现2个明显的吸收峰,这2个吸收峰可分解成4个高斯线型的吸收带,它们的峰值分别为350nm、405nm、550nm和670nm。可以得出这样的推论：PWO晶体中350nm、420nm、550nm和670nm吸收带的出现都与铅空位的存在有关。     

激发态质子转移分子2-(2'-羟基苯基)苯并噻唑在不同溶剂中的光谱特性

观测了2-(2’-羟基苯基)苯并噻唑(HBT)在不同极性溶剂中的吸收光谱和荧光光谱,详细研究了溶剂极性对HBT发生激发态分子内质子转移(ESIPT)影响的机制。吸收光谱表明在常态条件下,HBT在各种溶剂中都以烯醇式构型和酮式构型共同存在,但以烯醇式构型占绝大多数。荧光光谱表明在纯环己烷溶剂中,HBT被紫外光激发时,绝大多数烯醇式构型发生ESIPT转变为酮式构型,分子的ESIPT效率最大。在含有乙醇的极性溶剂中,HBT烯醇式会形成溶剂化的烯醇式构型,阻碍分子发生ESIPT反应。溶剂中乙醇含量愈多极性愈强,溶剂化烯醇式的成份就愈多,HBT的ESIPT效率就愈低。以400 nm光激发HBT溶液时,在510 nm处发现酮式构型荧光,从而确认了400 nm处的弱吸收是酮式构型的吸收;且在436和456nm处还有新的荧光峰,分析其可能来源于酮式构型去质子化阴离子的发射。     

Electronic spectrum of praseodymium monoxide

Emission and absorption spectra of praseodymium monoxide were investigated. In the 5000–11,200 Å region the bands of 22 systems were found. The rotational structure of four bands belonging to two systems was analyzed. It has been shown that in absorption there are observed transitions at least from two electronic states having close values of vibrational and rotational constants.     

Directional photoemission from tungsten

Photoemission energy distribution spectra have been scanned for photoelectrons emitted normal to two different crystal faces of tungsten, namely (100) and (110). The energy distributions and the derivative spectra show large differences between emission from the two faces. Whereas strong surface state emission is observed from the (100) face, no surface states are associated with the (110) face. The spectra show features characteristic of direct and also nondirect transitions, but these features appear very different for the two faces. Using existing band structure calculations, the spectral structure is assigned to electronic transitions between bands along the Δ axis for the (100) face and the Σ axis for the (110) face. The experiments show that directional photoemission spectra taken normal to a crystal surface make it possible to investigate electronic energy bands along symmetry directions in the Brillouin zone.     

环氧丙烷爆燃转爆轰过程反应产物的光谱法确定

采用由增强型ICCD光谱探测器、SpectraPro-275光谱仪和DG535同步控制器组成的瞬态光谱测量系统,在解决了测试系统时间同步问题、弱光探测问题、提高光谱分辨率问题和波长定标及防止误触发问题后,在长4.0 m,内径为0.10 m的爆炸激波管侧窗,拍摄到了持续时间仅为数ms的环氧丙烷爆燃转爆轰过程的曝光时间为1～16 μs的瞬态发射光谱。测量系统的光谱分辨本领达到了0.2 nm 。根据由碳、氢和氧组成的小分子和自由基的特征辐射谱带带头波长值,经过对所测光谱进行分析和辨认,确定了在环氧丙烷的爆燃转爆轰过程中有OH,CH,C₂,C₃,CO,CO₂,CHO和CH₂O这些反应产物出现。这些反应产物的确定,是进一步分析环氧丙烷爆燃转爆轰过程的微观机理必不可少的实验依据。