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1.
It is shown that luminescence detection of multiphoton ionization-fragmentation of the molecular CrO 4 2− anions adsorbed on the surface of dispersed SiO2 is possible under excitation with the fundamental frequency of a Nd:YAG pulsed laser (λ=1.064 μm). The structure and the process of formation of the adsorbed complexes under thermal activation of the surface and the nature of luminescence transitions in CrO 4 2− anions are studied in detail. It is shown that luminescence is excited as a result of the recombination of photoelectrons and ionized chromate ions. Multiphoton ionization of the ions occurs under three-photon resonance conditions. The resonance level is an antibonding state of the adsorption complex formed with the participation of an oxygen vacancy on the SiO2 surface. The dynamics of the multiphoton luminescence excitation process includes autoionization (stimulated by intercomplex electronic excitation) in superexcited states, fragmentation of chromate anions, and annealing of surface oxygen vacancies. The rate equations for three-photon-resonance multiphoton ionization are studied. The cross sections for two-and one-photon transitions on the nonresonance steps of multiphoton absorption are obtained. It is concluded that the nonlinear polarizability of the donor-acceptor adsorption bond in “chromate anion-oxygen vacancy” complexes is very important. Zh. éksp. Teor. Fiz. 111, 1748–1774 (May 1997)  相似文献   

2.
The selectivity dependence of multiphoton dissociation of CF3I on the conditions of excitation (pulse duration, concentration of the isotope under excitation and gas pressure) has been studied. It has been shown that the main mechanism of selectivity loss isV-V exchange during a laser pulse. The elaborated model is in good agreement with the experiment.  相似文献   

3.
We report the preparation of D2 molecules in v=2 level in molecular beam condition. A single longitudinal mode laser system was used for excitation of D2 from (v=0, j=0) to (v=2, j=0) with the scheme of stimulated Raman pumping. An excitation efficiency of 25.2% has been achieved, which was determined by the scheme of resonance-enhanced multiphoton ionization. Dependence of relative excitation efficiency on laser energy has been measured. We found that the increasing rate of excitation efficiency became slower as pulse energy of Stokes laser increase, while the excitation efficiency still increases approximately linearly with pump pulse energies up to 60 mJ. The spectral line shapes of Raman transition was also measured at different laser energies and considerable dynamical Stark effect was observed. A single peak was found on the three dimension surface of relative excitation efficiency, indicating the process occurred in the present study is a process of stimulated Raman pumping instead of stimulated adiabatic Raman passage.  相似文献   

4.
The picosecond interband two-photon laser excitation of PbWO4 crystals at a temperature of 10 K leads to electronic excitation energy accumulation, which results in almost 100% induced absorption in the 450–750 nm spectral range. The relaxation time of this induced absorption exceeds 100 min. The electronic excitation energy accumulated in the PbWO4 crystal at T = 10 K excites the intrinsic luminescence with a decay time longer than 45 min. The decay kinetics and the spectra of the intrinsic luminescence of the PbWO4 crystal at a temperature of 10 K were measured under two-photon and single-photon excitation. The luminescence under two-photon and single-photon excitation revealed a difference in the structure of the spectra.  相似文献   

5.
We performed numerical simulation of a random laser in a spherical multiple scattering medium in order to examine the saturation absorption in the excitation process and the resultant increasing process of the gain volume under the random laser action. The size of the gain volume increases with 1/3 power of the excitation pulse energy in the weak excitation region, and then approaches a critical value Lth when the excitation pulse energy is increased above the threshold. The dependence of Lth, as well as the dependence of the threshold excitation pulse energy on the dye concentration, transport mean free path, stimulated emission cross section and excited state lifetime were also examined. These results of the simulation well correspond to the experimental results by a two-beam spatial-correlation method.  相似文献   

6.
By the spectral and kinetic characteristics of the luminescence of vapors of polyatomic molecules (anthracene, anthraquinone, fluorenone) initiated by selective IR multiphoton excitation (IR MPE) of molecules in the ground electronic state S 0 the relaxation processes proceeding under vibrational excitation of molecules to energies exceeding the energies of the lower excited electronic states have been investigated. The changes in the spectral and kinetic characteristics with increasing CO2 laser energy density and vapor P v and foreign gas pressure P FG are analyzed. They are similar to the characteristics obtained for normal fluorescence of these molecules with changing vibrational energy E vib content. On the basis of experimental data and model calculations it has been concluded that at the laser radiation densities used in the case of IR MPE the molecules reach energies considerably exceeding the energies of the electronic levels. It is shown that a nonadiabatic connection between the electronic states leads to the population of mixed electronic states isoenergetic to the vibrational levels of the ground electronic state and to emission of delayed luminescence spectrally identical to the normal luminescence of these molecules. It has been found that when high vibrational levels are populated, new relaxation channels, such as reverse electron relaxation, emission from high vibrational levels of the ground electronic state, and multiquantum vibrational energy transfer at collisions leading to a rapid establishment of vibrational equilibrium become important.  相似文献   

7.
Energy transfer processes are very important in solid-state laser systems because they can cause an enhancement of the luminescence emission resulting in a reduction of the laser threshold. In this work, a detailed investigation to understand the basic processes of energy transfer between Tm and Ho ions in LiYF4, a solid-state laser crystal, was made. Data includes absorption, luminescence excitation and response to pulsed excitation. Dynamics of the energy transfer was analyzed by considering the kinetic evolution of the emissions of both ions. It was found that the energy transfer process between the 3 F 4 spectral manifold of Tm and the 5 I 7 spectral manifold of Ho results in thermal equilibration of these two manifolds. Received: 20 May 1999 / Revised version: 20 August 1999 / Published online: 27 January 2000  相似文献   

8.
Dai DC  Xu SJ  Shi SL  Xie MH  Che CM 《Optics letters》2005,30(24):3377-3379
At room temperature, multiphoton absorption- (MPA-) induced photoluminescence in ZnO strongly driven by a femtosecond (fs) near-infrared laser is studied. Two-photon absorption and three-photon absorption are proved to be responsible for the intense luminescence, when the wavelength of the fs excitation laser is above and below the half-bandgap of ZnO, respectively. Strong MPA absorption in ZnO is unambiguously evidenced by the interferometric autocorrelation measurements of the luminescence signal.  相似文献   

9.
In this letter we report results of a selective multiphoton excitation of O2 in the 9–12 eV region by a neodymium glass laser. The main feature of this experiment is the major presence of the ion specie O2+ in the interaction volume with the values 10 ± 1 for the nonlinear interaction order. This result can be interpreted as a double mechanisms namely: a one step process, the direct absorption from the ground state or a two step process via an intermediate resonant state which has been attributed as the second (B3Σu?, v′=2) state of O2 located at 10.56 ± 0.03 eV. The probability of multiphoton formation of O2+ for a flux value of 1,5 × 1012 W/cm2 is equal to 2 × 107±1 sec?1.  相似文献   

10.
The interaction of a 60 fs 790 nm laser pulse with beams of Ar+, C+, H2 +, HD+ and D2 + are discussed. Intensities up to 1016 Wcm-2 are employed. An experimental z-scanning technique is used to resolve the intensity dependent processes in the confocal volume.Received: 6 January 2003, Published online: 15 July 2003PACS: 32.80.Fb Photoionization of atoms and ions - 33.80.Rv Multiphoton ionization and excitation to highly excited states (e.g., Rydberg states) - 42.50.Hz Strong-field excitation of optical transitions in quantum systems; multiphoton processes; dynamic Stark shift  相似文献   

11.
The study of luminescence of high-purity multicomponent silicate glasses excited by radiation of a N2 laser (λ=337 nm, P≈12kW) showed darkening of a sample and a monotone decrease in luminescence intensity and the transmitted radiation intensity from pulse to pulse. Additional illumination with radiation of an Ar+ laser (λ=514.5 nm) caused an increase in luminescence intensity. An increase in absorption and a decrease in luminescence intensity were found to be caused by two-photon absorption and electron-hole pair production.  相似文献   

12.
Luminescence of silver nanoparticles photodeposited on titan dioxide nanoparticles of mesoporous film is studied. Luminescence was registered under the two-photon excitation by femtosecond laser pulses of Ti:sapphire laser. It occurs that Ag/TiO2 mesoporous films have high concentration of bright luminescence spots which reveal stability to degradation under long illumination. Various configurations of silver nanoparticles are analyzed to explain the physics of bright luminescence spots (“hot spots”). Luminescence intensity reveals “hot spots” dependence on excitation laser pulse polarization. Properties of Ag/TiO2 system show its promising usage for single molecule spectroscopy and biological objects visualization.  相似文献   

13.
Selective laser excitation of the luminescence of a thin film of the π-conjugated polymer poly(p-phenylene) at room temperature is achieved. Monochromatic excitation is selective only for excitation in the long-wavelength wing of the absorption spectrum. This is manifested as a shift of the luminescence spectrum with excitation frequency. The experimental results are interpreted on the basis of model calculations. Pis’ma Zh. éksp. Teor. Fiz. 63, No. 3, 171–175 (10 February 1996)  相似文献   

14.
The absorption of three linesP(30) (1037.4 cm–1),P(36) (1031.5 cm–1) andP(40) (1027.4cm–1) of the pulsed CO2 laser (0001–0200 transition) by SiF4 was examined at various pulse energies, pulse durations, temperatures, optical path lengths and pressures of this compound and several non-absorbing gases. In addition, the low-intensity infrared absorption spectrum of tetrafluorosilane was compared with high-intensity absorption data for all lines of the laser. The experimental dependences demonstrate nonlinear features of the absorption phenomena originating from the high power of the incident radiation and collisions of absorbing molecules with surroundings. These effects are included in the analytical formula, being an extended form of the Lambert-Beer law. which reasonably approximates all experimental data. The importance of the results obtained for understanding general features of multiphoton absorption and for revealing potential applications of SiF4 as a sensitizer for the infrared region is presented in brief.  相似文献   

15.
Following pulsed laser excitation of As-doped Ge with impurity concentrations between 1015-1017cm-3, we observe the electron-hole drop (EHD) and excitonic luminescence decay. The spectrum resolved no-phonon (NP) EHD luminescence kinetics are found to depend on its spectral position. “Plateaus” on the kinetic curves for the high energy side of NP-spectrum are observed at high excitation. The data suggest this luminescence is due to the states which are in dynamical equilibrium during some time after excitation pulse.  相似文献   

16.
Abstract

Investigations of the luminescence decay of Ce3+- and Tb3+-ions in solid solutions of the system K3La1?x?yCexTby(P04)2 were carried out at 298 K and 10 K using a laser pulse spectrometer or synchrotron radiation as excitation sources. A comparison of the decay times determined in the host absorption range (160 nm) and in the Ce3+- and Tb3+- ion levels shows a delayed decay of the host excitation. The results are discussed in regard to energy transfer.  相似文献   

17.
The luminescence kinetics of solutions of pseudoisocyanine iodide (PIC) J aggregates is studied upon excitation by pico- and subnanosecond laser pulses into the main superintense long-wavelength absorption band. The dependences of the transmission and luminescence energy on the pump energy are measured. It is found that the shape of the luminescence kinetics depends on the recording and excitation spectral regions, which is obviously related to the energy transfer between coherently coupled fragments of J aggregates.  相似文献   

18.
The applicability of a pyroelectric detector (PED) to multiphoton absorption measurements (MPA) under ir laser excitation of molecules was examined. The possibility of MPA measurement of SF6 molecules in the pressure range of 10−3÷10−1 Torr with a time resolution of ∼ 7 μs has been shown. It has been demonstrated that the degree of vibrational relaxation of highly vibrationally excited molecules at PED surface does not depend on excitation level under the studied conditions.  相似文献   

19.
在978nm激光二极管的激发下,Mo掺杂的TiO2材料表现出很强的宽带上转换发光 ,该发光来源于[MoO42-基团的激发态3T1, 3T2能级到基态1A1能级的电子跃迁.通过研究发光强度与抽运功率的关系及上转换发光的上升时间曲线,发现TiO2∶Mo体系的上转换发光中存在着雪崩机制,应用转 关键词: 上转换 光子雪崩 转移函数理论  相似文献   

20.
The energy level structure of F 3 + laser color centers in crystals of LiF is discussed. A high-power laser (λ ex=920 nm) is used to excite luminescence from LiF crystals with F 3 + centers via two-photon absorption, and the dependence of the polarization and intensity of this luminescence on the polarization of the laser light is measured and calculated. It is shown that the two-photon transition involves the excitation of a previously unknown state of the F 3 + center—a spin singlet whose wave function has 1 A 1 symmetry. Fiz. Tverd. Tela (St. Petersburg) 39, 1373–1379 (August 1996)  相似文献   

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