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1.
Three‐peak Autler‐Townes (A‐T) splitting in the resonant multiphoton ionization photoelectron spectrum for a rotating Li2 molecular system in femtosecond pulse laser fields is studied by using two‐dimension time‐dependent quantum wave packet method. The A‐T splitting results from rapid Rabi oscillation caused by intense femtosecond laser pulses. Because of the effects of molecular rotation and alignment, the Rabi oscillation in the population distribution will be damped in a certain degree. The three‐peak A‐T splitting can only be observed for a strongly aligned molecule with rapid Rabi oscillation. The three‐peak A‐T splitting dynamics can be affected by intensity, duration, temporal profile of laser pulse, and initial molecular rotational temperature. The conditions to observe the A‐T splitting are discussed in detail. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010  相似文献   

2.
硫氧化碳OCS是线性三原子分子,这类小分子的激发态、离子态能级结构、能级之间的相互作用及电离过程,是研究中所关心的问题.Tanaka等[1]和Kopp[2]测量了OCS的VUV吸收光谱,Frey和Schlag等[3]以同步辐射光源,用光电离共振(PIR)谱方法、Kovac[4]和Wang,Shirley等[5]以Hel为电离光源,分别采用传统的光电子能谱和高分辨光电子能谱技术研究了CO2、CS2和OCS分子从电子振动基态吸收单个光子而电离的过程.Yang和Anderson等问为了作选态的离子一分子反应利用可调谐激光rt光子吸收将OCS选择激发到某一中间态,OCS再吸收光子后…  相似文献   

3.
We have recorded high-resolution HeI and HeII photoelectron spectra of the valence bands of six MX2 compounds (M = Zn, Cd: X = Cl, Br, I) in the gas phase. Transition-state Xα SW calculations on all six compounds confirm the assignments. For the first time, we have clearly resolved the spin-orbit splitting of the IIg and IIu states in the bromide and iodide spectra: and calculated Πu splittings, using a simple MO LCAO model and the Dxh double group, are in very good agreement with the experimental values. The relative intensities of the photoelectron peaks change markedly from HeI to HeII spectra, and Xα SW cross section calculations on ZnCl2 predict these intensity changes rather well.  相似文献   

4.

The delay time dependence of photoelectron spectra and state populations of three-level ladder K2 molecule is investigated by pump-probe pulses via time-dependent wave packet approach. The periodical motion of the wave packet with oscillating period 500 fs results in the periodical variation of photoelectron spectra. The photoelectron spectra show Autler-Townes double splitting at zero delay time, and no splitting at positive delay time. The periodical change of state populations with delay time can be ascribed to the coupling effect between the two pulses. It is found that the selectivity of the state populations may be attained by regulating the delay time. The results can provide some important basis for realizing the optical control of molecules experimentally.

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5.
List of subject     
We report the high resolution emission (S1 → S0, T1 → S0) and laser single site singlet excitation (S1 ← S0) spectra for the various insertion sites of coronene in n-heptane cooled to 1.5 K. The observation of site splitting of doubly degenerate vibrations and weak electric dipole forbidden 0, 0 bands in the S1 → S0 and T1 → S0 spectra indicates that the ground state, the first excited singlet and lowest triplet states are all distorted. In these spectra, the intensity distribution of the various sites in the 0, 0 bands suggests that the distortion is different from site to site but similar in S0, S1 and T1. Identical ordering of the sites in S1 S0 and S1 S0 spectra as well as the observation of weak shifts in the vibrational frequencies in the two states implies the absence of strong pseudo Jahn-Teller forces in the first excited singlet state. We propose, further, that this is also true for the triplet state. This conclusion is supported by the similarity in zero-field splitting parameters of coronene and deuterated coronene. Taken together, these results indicate strongly that the distortion of coronene in n-heptane is primarily crystal field induced and is not greatly changed upon excitation of the molecule to its lowest excited states.  相似文献   

6.
We study the behavior of Rydberg series of resonances excited by intense laser fields. Our approach is based on a semiclassical formalism for the evolution in time of the atomic states coupled by the laser. The atomic system is described by a two-channel model in a Multichannel Quantum Defect Theory approach. We calculate the total ionization and the photoelectron spectrum after a certain interaction time. We present results both for on-resonance and off-resonance excitation of the series. We employ a more or less realistic pulse shape that corresponds to a narrow Fourier bandwidth. We show that the effects of the non-resonant members of the series on the photoelectron spectra can be important and we study it both as a function of laser intensity and as a function of the interaction time. We also show that our model correctly describes the Rabi oscillations between the ground state and the excitedAI state when the field is sufficiently strong.  相似文献   

7.
Results are presented of a study on the application of a N2 laser to the spectrochemical analysis of microareas. It is found that when the pressure of the surrounding gas is reduced to 1 Torr (133 Pa) or thereabouts, the plasma induced by the bombardment of N2 laser light yields sharp atomic line spectra with a negligibly low background signal, facilitating quantitative analysis with reasonable precision. A simple and rapid detection method is employed in which the atomic emission spectrum from the plasma produced under successive bombardment (10 Hz) is recorded directly on a chart by means of scanning the wavelength of a monochromator. By using iron-steel standard samples of known content, it is demonstrated that a plot of the intensity of the 425.4 nm emission line of Cr against the Cr content shows a linear relationship.  相似文献   

8.
The Hel photoelectron spectra of the three allyl amines show low ionization potential bands arising from nitrogen lone-pair n electrons and ethylenic π-bond electrons. Analysis of the spectra using MINDO/3 calculations and comparisons with ionization data of related molecules shows that π-π interactions are considerable, but n-π interactions are small. The π-π splitting in triallyl amine is consistent with a near-planar C3 symmetry structure for the gas phase molecule.  相似文献   

9.
Using two different TDDFT methods, we study the role of electronically excited states and two-electron dynamics in high harmonic generation (HHG) of H2. The two methods produce slightly different electronic structures as reflected in the calculated ionization potentials. They nevertheless give similar HHG spectra. The difference between the two methods increases with the laser intensity, while their predictions remain qualitatively consistent.Our results suggest that two-electron dynamics can extend the HHG cutoff. Specifics of such extension depends on the internuclear distance and the laser intensity. We propose an ion excitation plus tunneling ionization mechanism to explain these extensions.The involvement of excited states is further revealed when we analyze each harmonic as a function of the internuclear distance. We see resonant peaks that are due to multiphoton excitation. These peaks exist above the ionization threshold as well.  相似文献   

10.
Patterned self-assembled monolayers (SAMs) of alkanethiolates (AT) on Au and Ag substrates were imaged and characterized by scanning photoelectron microscopy (SPEM). The patterns were prepared in situ by direct writing with the zone-plate-focused X-ray beam provided by the SPEM station. Whereas both AT/Au and AT/Ag behaved alike upon the irradiation, which resulted in similar contrasts in the fabricated patterns and similar microspot spectra from the irradiated areas, the intensity relationship between the patterned and nonpatterned areas changed by different pathways for the Au and Ag substrates after the exposure of the patterns to ambient. The SPEM data imply that weakly bound molecular fragments are desorbed from the irradiated areas upon air exposure in the case of Ag, whereas adsorption of airborne molecules from ambient occurs for the Au substrate. The origin of the observed differences is presumably related to the specific branching patterns of irradiation-induced modification of AT/Au and AT/Ag.  相似文献   

11.
Ceria-titania interfaces play a crucial role in different chemical processes but are especially promising for the photocatalytic splitting of water using light in the visible wavelength region when Pt is added to the system. However, the complexity of this hierarchical structure hampers the study of the origin of its outstanding properties. In this article, the structural, electronic and optoelectronic properties of CeO2/TiO2 systems containing 1D, 2D, and 3D particles of ceria are analyzed by means of density functional calculations. Adsorption sites and vacancy effects have been studied to model Pt adsorption. Density of states calculations and absorption spectra simulations explain the behavior of these systems. Finally, these models are used for the screening of other metals that can be combined with this heterostructure to potentially find more efficient water splitting photocatalysts.  相似文献   

12.
We theoretically investigate the physical mechanism of quantum control on a K(2) molecule with an ultrafast strong laser pulse by solving the time-dependent Schr?dinger equation exactly using a wave packet approach. The structures of the triple splitting in the 3-photon ionization spectra of a K(2) molecule are presented to analyze the information of a selective population of dressed states. In this work, it is found that the tunability of the dressed states energies is achieved by regulating the laser intensity and the high selectivity of the dressed state population is attained by altering the envelope and wavelength of the intense laser pulse.  相似文献   

13.
Previously published X-ray emission spectra (Mg Kβ1,3; MgL2,3M and OKα) from magnesium oxide are aligned on a common energy scale using atomic orbital ionisation energies determined by X-ray photoelectron spectroscopy. All three spectra show two principal components which derive from the same two bands of molecular orbitals. The two components of both magnesium spectra have equal intensity; in the oxygen spectrum the high energy peak is the most intense: these observations are rationalised using a simple molecular orbital model based on the MgO610?unit. It is necessary to consider the interactions of this unit with further magnesium and oxygen atoms and also π -type perturbations between Mg—O σ bonds in order to explain the structure of the observed emission spectra (but there is no recourse to forbidden 3d → 1s transitions).  相似文献   

14.
We describe a collinear velocity-map photoelectron imaging spectrometer, which combines a Wiley-McLaren time-of-flight mass analyzer with a dual-valve laser vaporization source for investigating size-selected cluster and reaction intermediate anions. To generate the reaction anions conveniently, two pulsed valves and a reaction channel are employed instead of premixing carrier gas. The collinear photoelectron imaging spectrometer adopts modified velocity-map electrostatic lens, and provides kinetic energy resolution better than 3%. The performance of the instrument is demonstrated on the photodetachment of Si4- at 532 and 355 nm, and Si3C- at 532 nm, respectively. In both cases, photoelectron spectra and anisotropy parameters are obtained from the images. For Si4-, the spectra show two well-resolved vibrational progressions which correspond to the ground state and the first excited state of the neutral Si4 with peak spacing of 330 and 312 cm-1, respectively. Preliminary results suggest that the apparatus is a powerful tool for characterizing the electronic structure and photodetachment dynamics of cluster anions.  相似文献   

15.
Orbital ionization energies are compared with the results of ab initio calculations for three-atomic linear BeCl2, XeF2, CrCl2 and five-atomic tetrahedral TiCl4, RuO4 molecules to investigate the effect of electron relaxation in ions on the informativity of photoelectron spectra of molecules and complex compounds. For all compounds except CrCl2 there is satisfactory agreement between theory and experiment in respect of the sequence and character of electronic levels and the orbital nature of chemical bonds. In the series of 3d metal tris-β-diketonates, for metal complexes of the second half of the series there are wide discrepancies between the photoelectron, Xα-DV, and ab initio data on the electronic structure of the complexes, which are due to electron relaxation in the ions. The calculations exaggerate the mixing of levels between the metal and ligands, since the energy splitting of the corresponding spin-orbitals (spin polarization) considerably exceeds the multiplet splitting of states corresponding to a vacancy on the ligand MO estimated from the photoelectron spectra. Translated fromZhurnal Struktumoi Khimii, Vol. 39, No. 6, pp. 1113–1120, November–December, 1998.  相似文献   

16.
用光电子成像技术研究了Cu^-的飞秒双光子光脱附过程.光脱附产生的光电子能量分布和角度分布通过光电子成像直接获得.实验发现,在光强为6.0×10^10W/cm^2下,双光子光脱附通道的光电子角度分布随激光波长出现剧烈的变化.通过低阶微扰理论和实验结果对比分析,Cu^-的双光子脱附产生的光电子角度分布特征可以归结于脱附过程中Cu^-的s和d轨道波函数之间的干涉效应.通过分析光电子角度分布特征,获得了不同波长下s和d轨道波函数对双光子脱附过程的贡献,该结果符合Wigner阈值理论的预期.  相似文献   

17.
Super‐atom molecular orbitals (SAMOs) are diffuse hydrogen‐like orbitals defined by the shallow potential at the centre of hollow molecules such as fullerenes. The SAMO excited states differ from the Rydberg states by the significant electronic density present inside the carbon cage. We provide a detailed computational study of SAMO and Rydberg states and an experimental characterization of SAMO excited electronic states for gas‐phase C60 molecules by photoelectron spectroscopy. A large band of 500 excited states was computed using time‐dependent density functional theory. We show that due to their diffuse character, the photoionization widths of the SAMO and Rydberg states are orders of magnitude larger than those of the isoenergetic non‐SAMO excited states. Moreover, in the range of kinetic energies experimentally measured, only the SAMO states photoionize significantly on the timescale of the femtosecond laser experiments. Single photon ionization of the SAMO states dominates the photoelectron spectrum for relatively low laser intensities. The computed photoelectron spectra and photoelectron angular distributions are in good agreement with the experimental results.  相似文献   

18.
Gaseous dibenzo-7-phosphanorbornadiene P-sulfide anions APS-(A=C14H10 or anthracene) were generated via electrospray ionization, and characterized by magnetic-bottle photoelectron spectroscopy, velocity-map imaging (VMI) photoelectron spectroscopy, and quantum chemical calculations. The electron affinity (EA) and spin-orbit (SO) splitting of the APS· radical are determined from the photoelectron spectra and Franck-Condon factor simulations to be EA=(2.62±0.05) eV and SO splitting=(43±7) meV. VMI photoelectron images show strong and sharp peaks near the detachment threshold with an identical electron kinetic energy (eKE) of 17.9 meV at three different detachment wavelengths, which are therefore assigned to autodetachment from dipole-bound anion states. The B3LYP/6-31++G(d, p) calculations indicate APS· has a dipole moment of 3.31 Debye, large enough to support a dipole-bound electron.  相似文献   

19.
HeI photoelectron (PE) spectra are re-recorded for SSF2 and FSSF. The assignment of bands has been made with the aid of band shapes, band intensities and ab initio calculations. In the PE spectrum of SSF2, two sharp peaks at 10.48 and 11.22 eV are considered to result from through-space interaction of lone-pair orbitals in the two S atoms and two sharp peaks at 12.50 and 12.90 eV from through-space interaction of lone-pair orbitals in the two F atoms. The larger splitting of the S atoms can be attributed to the larger 3p orbital of S. The lack of sharp peaks in the PE spectrum of FSSF shows that there is no orbital which embodies the character of a lone-pair. So the PE spectra of SSF2 and FSSF are examples embodying through-space interaction of lone-pair orbitals.  相似文献   

20.
By CNDO-CI calculations we have found that dicarbonyl compounds exhibit only two n → π* transitions in the visible or near UV. region, instead of four as expected from simpler MO-models. The dominant features of the long-wavelength electronic spectra may be characterized by the relative energy of the two n and the two lowest π* orbitals. In general we distinguish between three cases:
    相似文献   

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