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1.
The Compton scattering of attosecond X-ray pulses on a hydrogen atom has been studied theoretically in terms of the spectral angular scattering probability during the action of a pulse. The dependence of scattering on the carrier frequency, pulse duration, and scattering angle has been analyzed. It has been shown that the probability of the process at certain parameters of the problem is a nonlinear function of the pulse duration. 相似文献
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We have calculated and analyzed the probability of ultrashort electromagnetic pulse (USP) scattering on small metal clusters in the frequency range of plasmon resonances during the field action. The main attention is devoted to dependence of the probability of scattering on the pulse duration for various detunings of the USP carrier frequency from the plasmon resonance frequency. Peculiarities of the USP scattering from plasmon resonances with various figures of merit are revealed. 相似文献
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受激布里渊散射(SBS)具有脉冲压缩的特性,受激布里渊散射的脉冲宽度随着抽运能量的增大而变小,在水中可以达到几百皮秒的量级.本文在实验上观察到一种受激布里渊散射的脉冲宽度随抽运能量增大而变大的现象,这里称之为反常压缩.SBS的脉冲反常压缩和脉冲压缩与抽运光的强弱会聚情况有关.利用数值模拟,模拟了强弱会聚情况下抽运光在水中的传输规律,强弱会聚情况的抽运光对受激布里渊散射形成的有效增益长度不同:抽运光强会聚时有效增益长度短,形成SBS脉冲宽度的反常压缩;弱会聚时有效增益长度长,也就是正常的SBS脉冲压缩. 相似文献
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Scattering of ultrashort electromagnetic pulses on the dense strongly coupled plasma is under consideration in the frame of hard ion sphere model. The electron distribution inside the ion sphere is obtained from self‐consistent solution of the Shrodinger equation for bound electrons and the Poisson equation for free electrons. The electron density distribution is determined by plasma electron temperatures. The ion density of Al plasmas under consideration is of the order of 1020–1022 cm?3, the electron temperature changes between 54 and 816 eV. Dynamical polarizability of the hard sphere determining the scattering cross sections is calculated using the modified local plasma frequency approximation. The spectrum of scattering cross section has maxima in the vicinity of the mean plasma frequency. Dependencies of scattering probability on carrier frequency and pulse duration are analysed in detail. The transition of the total scattering probabilities from nonlinear time dependence at small times to standard linear ones with the increase of pulse duration is demonstrated. 相似文献
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The probability of emission of a single-photon via Raman scattering of laser pulse on the three-level Λ - type atom in microcavity is studied. The duration of the pulse is considered to be short enough, so that the hyperfine structure of the upper level remains totally unresolved, while that of the lower level is totally resolved. The coherent laser pulse is assumed to be in resonance with the transition between one hyperfine-structure component of the lower atomic level and all hyperfine-structure components of the upper level, while the quantized cavity field is assumed to be in resonance with the transition between the other hyperfine-structure component of the lower level and all components of the upper one. The dependence of the photon emission probability on the mutual orientation of polarization vectors of the cavity mode and of the coherent laser pulse is analyzed. Particularly, the case is investigated, when the total electronic angular momentum of the lower atomic level equals 1/2, which is true for the ground states of alkali atoms employed in the experiments on deterministic single-photon emission. It is shown, that in this case the probability of photon emission equals zero for collinear polarizations of the photon and of the laser pulse, and the probability obtains its maximum value, when the angle between their polarizations equals 60°. 相似文献
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研究了光子晶体光纤中调制不稳定性效应.从非线性薛定谔方程出发,计算和分析了光子晶体光纤中反常色散区以及正常色散区内的调制不稳定性现象,详细讨论了超短脉冲的脉宽、峰值功率、高阶色散和高阶非线性效应(如脉冲内喇曼散射、自陡峭效应)对调制不稳定性产生的影响.结果表明:二阶色散对调制不稳定性的影响要远大于三阶色散,同时也发现随着初始脉冲宽度的减小,调制不稳定性旁瓣增大但是强度有所降低.另外还发现高阶非线效应如自陡峭和喇曼效应会在不同程度上抑制调制不稳定性. 相似文献
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The scattering of a partially coherent plane-wave pulse on a Gaussian-correlated, quasi-homogeneous random medium is investigated. The analytical expressions for the temporal coherence length and the pulse duration of the scattered field are derived. We demonstrate that the scattering-induced changes in the temporal coherence length and the pulse duration may be used to determine the correlation function of the scattering potential of the medium. 相似文献
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P. A. Apanasevich 《Journal of Applied Spectroscopy》1967,6(2):115-121
Rate equations are used to compute a weak stimulated Raman scattering pulse in the case where the scattered radiation energy can be neglected in the over-all energy balance. Expressions for the shape, position and height of the maximum, duration, and spectral width of the scattering pulse as functions of the parameters of the driving laser, scattering material, and observation conditions are derived. 相似文献
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The scattering of photon by electron in the presence of the field of the low-intensity circularly-polarized pulsed laser wave
is analyzed at a laser pulse duration that is significantly greater than the characteristic oscillation time. The conditions
for the resonance process in which the intermediate particle is located in the vicinity of the mass surface are determined.
The existence of three resonance ranges is demonstrated. The first one corresponds to the resonance of direct diagram, and
two ranges correspond to the resonance of exchange diagram via electron and positron intermediate states. The conditions under
which only the resonance of the direct diagram takes place are determined, and the probability of such process is calculated.
It is demonstrated that the resonance probability can be significantly greater than the probability of the Compton effect
in the absence of the external field. 相似文献
14.
The use of a 100 ns pulse Nd:YAG laser is proposed to perform single-shot measurements by spontaneous Raman scattering. The long pulse duration is obtained thanks to a White cell placed inside the laser oscillator. This lengthens the pulse duration within the laser cavity, keeping almost the same beam quality as standard Nd:YAG lasers. The laser system is described, the advantages are compared with extra-cavity stretched lasers, and single-shot measurement of concentration in gas is demonstrated. 相似文献
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An experimental study of quantum mechanical pulse energy fluctuations in stimulated Raman scattering from hydrogen is presented. The probability density function P(W) for Stokes pulse energy W is measured for highly transient scattering in both the linear and nonlinear gain regimes. While large pulse energy fluctuations (100%) occur in the linear gain regime, the fluctuations are reduced to about 20% in the nonlinear regime where the laser pulse is depleted significantly. The results are in excellent agreement with the theoretical predictions of Lewenstein. 相似文献
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The vibrational amplitude and the intensity of the Stokes light generated by transient stimulated Raman scattering rise and decay very rapidly. The time duration of the Stokes pulse and of the phonon pulse is much shorter than the pump pulse duration. It is shown that both phonon and Stokes pulses can be used to probe the shape of ultrashort light pulses. 相似文献
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C. Jordan K. A. Stankov G. Marowsky E. J. Canto-Said 《Applied physics. B, Lasers and optics》1994,59(4):471-473
Femtosecond pulses at 496 nm were Raman-shifted in methane with 20% efficiency. The pulse duration could be reduced up to 6.5 times from 560 fs at the fundamental to 85 fs at the Stokes frequency (580nm), which is the shortest pulse duration generated in this way. It was shown experimentally that chirped-pulse Raman scattering avoids the limitations arising from self-phase modulation. 相似文献
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X. M. Zhang J. T. Zhang R. X. Li Q. H. Gong Z. Z. Xu 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2006,37(3):457-462
Photoionization of hydrogen atoms in few-cycle laser pulses is studied
numerically. The total ionization probability, the instantaneous ionization
probability, and the partial ionization probabilities in a pair of opposite
directions are obtained. The partial ionization probabilities are not always
equal to each other which is termed as inversion asymmetry. The variation of
asymmetry degree with the CE phase, the pulse duration and the pulse intensity
is studied. It is found that the pulse intensity affects the asymmetry degree
in many aspects. Firstly, the asymmetry is more distinct at higher intensities
than that at lower intensities when the pulse duration exceeds 4 cycles;
secondly, the maximal asymmetry in lower intensities varies with the CE phase
visibly while at higher intensities not; thirdly, the partial ionization
probabilities equal to each other for some special CE phases. For lower pulse
intensities, the corresponding value of CE phase is always 0.5π and
1.5π, while for higher pulse intensities, the corresponding value varies
with the pulse intensity. Similar phenomena were observed in a recent
experiment using few-cycle radio-frequency (RF) pulses. 相似文献