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1.
We have determined the temperature from SRS spectra of N2-N2, N2-CO2, O2-O2, and CO2-CO2 recorded in wide pressure and temperature ranges. The fitting procedure takes simultaneously into account the Dicke effect and motional narrowing. We have quantified the accuracy of the MEG and ECS-P models for rotational relaxation. The temperature extracted from each model is compared with thermocouple measurements. The influence of vibrational broadening and shifting is discussed in detail.  相似文献   
2.
The CARS spectrum of the v1 band of 12CH4 at a pressure of 14 mbar was recorded using cw excitation in the cavity of a ring argon ion laser. The analysis of the intensity profile of the obarred spectrum led to the detection of inconsistencies with the hitherto proposed calculated positions of transitions with J = 7 to J = 10 and to a relocation of the corresponding lines.  相似文献   
3.
With the aim of temperature diagnostic, femtosecond time-resolved CARS (coherent anti-Stokes Raman spectroscopy) is applied to probe H2 in H2-N2 mixtures. In a first part, a Lorentzian profile is used to model the femtosecond CARS response. A difference between the experimental broadening and the expected one is observed in the collision regime. The observed broadening increases strongly in an inhomogeneous way with respect to the perturber concentration. This is of considerable importance for temperature measurements. In a second part, we show that in the collision regime, this inhomogeneous broadening is due to the speed dependence of the collisional parameters and the memory effects of the radiator speed. A new modelization of the time-resolved CARS response taking into account the speed memory effects is presented and applied to the temperature diagnostic in H2-N2 mixtures. The numerical results are in good agreement with experiments.  相似文献   
4.
Spectroscopic constants of the X 1Σg+ ground state of 14N2 are deduced from CARS spectra recorded in a 4 Torr d.c. N2 glow discharge. Vibrational states up to ν = 14 have been observed but only the 11 lower levels which have a good signal-to-noise ratio have been processed. The Dunham constants that were deduced yield vibrational band centre positions in good agreement with those of Lofthus and Krupenie.  相似文献   
5.
Abstract— As is known the chlorophyll fluorescence of photosynthetizing plants is strongly quenched by carotenoid triplet states if the exciting light intensity is high enough (> 10 kW/m2). This light-induced quenching process was studied by measuring the relative yield of chlorophyll fluoresccncc excited with a pulsed argon laser at 20 C in light adapted algae as function of time (within lo μ s ) and exciting light intensity (<400 kW/m2). The experimental yield against time and yield against intensity curves have been adequately explained by a statistical model of Photosystem 2 (PS 2) units based upon the existence of freely moving excitons according to which the carotenoid triplet quenchers are randomly distributed and are perfect traps for excitons. Accepting the hypothesis that carotenoid triplet quenching occurs only in PS 2 units. it could be concluded that the height of the true zero level of PS 2 fluorescence is somewhat lower than the half value of the fluorescence level of the dark adapted state.  相似文献   
6.
We report a theoretical and experimental investigation of the dynamical Stark effect in a tetrahedral molecule, silane (SiH(4)). We use a tetrahedral formalism and Floquet theory to calculate the absorption spectra for the molecule dressed by an intense nonresonant pulsed laser. Experimentally, the dynamical Stark effect is observed for transitions of the nu(2)/nu(4) vibrational polyad of SiH(4) by means of nanosecond diode laser absorption spectroscopy and a Nd:YAG laser excitation. Copyright 2000 Academic Press.  相似文献   
7.
Abstract— The decay of luminescence of Chlorella in repetitive steady-state flashing light displays two categories of phase, broadly characterized as ‘fast’ and ‘slow’. They are strongly contrasted in amplitude and lifetime; the transition from fast to slow occurs a few milliseconds after the flash.
  • 1 The slow phases observed in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) are clearly of the deactivation type. i.e. the luminescence intensity is quantitatively correlated with the rate of relaxation of the System II reaction center to its photoactive state. The significance of the deactivation type is a reverse flow of the light-produced ⊕ and ? charges through the luminescence-producing recombination path. This mechanism is probably not limited to the DCMU-poisoned systems. The light regime (flash duration, flashing period, induction effects) modifies specifically the amplitude of the slow phases; this effect is strikingly not dependent on the presence of DCMU. Although the light-driven pH gradient is the likely explanation, it is argued that its action bears more directly on the exciton and/or emission yield of luminescence rather than on the rate of recombination itself.
  • 2 Most of the fast-phase components are ascribed under normal conditions to stabilization steps involving the donor side of the System II reaction centers. However, when the reaction center turnover is much reduced (DCMU) or completely abolished (DCMU + NH2OH, after preillumination), a fast luminescence phase is still visible. This phase is barely affected by the light regime (notably the flash duration). It must be attributed to an anomalous residual photochemical turnover of the reaction centers. Another type of fast photochemical turnover has been characterized with NH2OH-pretreated cells. A two-quantum functioning of some sort seems required to account for the anomalous photochemical turnover. The importance of the luminescence loss during the fast phases and its possible connection with the ‘misses’ of the O2-evolving system are discussed.
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8.
The measurement of relative intensities in CO2 combination bands spectrum is performed using wavelength modulation spectroscopy (WMS) and a DFB (distributed feedback) diode laser operating at 1.6 μm. The diode laser is stabilized with an external Fabry–Pérot interferometer and absorption spectroscopy is performed in a multipass gas cell. A spectrum containing spectral lines of both 13CO2 and 12CO2 isotopic species is recorded. The variation of laser power during frequency scanning and the line shape are taken into account to accurately extract line intensities from experimental data. The isotopic concentration ratio is deduced from the intensity ratio. Both ratios are measured with an accuracy of about 0.5% in pure CO2. Received: 9 June 2000 / Published online: 8 November 2000  相似文献   
9.
Following the scheme recently proposed by Remacle and Levine [Phys. Rev. A 73, 033820 (2006)], we investigate the concrete implementation of a classical full adder on two electronic states (X 1A1 and C 1B2) of the SO2 molecule by optical pump-probe laser pulses using intuitive and counterintuitive (stimulated Raman adiabatic passage) excitation schemes. The resources needed for providing the inputs and reading out are discussed, as well as the conditions for achieving robustness in both the intuitive and counterintuitive pump-dump sequences. The fidelity of the scheme is analyzed with respect to experimental noise and two kinds of perturbations: The coupling to the neighboring rovibrational states and a finite rotational temperature that leads to a mixture for the initial state. It is shown that the logic processing of a full addition cycle can be realistically experimentally implemented on a picosecond time scale while the readout takes a few nanoseconds.  相似文献   
10.
We show that a linear molecule subjected to a short specific elliptically polarized laser field yields post-pulse revivals exhibiting alignment alternatively located along the orthogonal axis and the major axis of the ellipse. The effect is experimentally demonstrated by measuring the optical Kerr effect along two different axes. The conditions ensuring an optimal field-free alternation of high alignments along both directions are derived.  相似文献   
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