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EQEC'96. 1996 European Quantum Electronic Conference最新文献

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Hard X-Ray Emission from Plasmas Created by Subps Multiterawatt- Laser Pulses 次多太瓦激光脉冲产生的等离子体的硬x射线发射
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561590
M. Schnurer, P. Nickles, M. Kalachnikov, R. Nolte, P. Ambrosi, W. Sandner
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引用次数: 0
Photoisomerization Of DODCI Studied with a Spectrometer - Streak Camera System 用谱仪-条纹相机系统研究DODCI的光异构化
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561863
A. Penzkofer, M. Ramelsperger, M. Wittmann
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引用次数: 0
Photocarrier Dynamics and Terahertz Radiation From Semiconductor Surface Space-Charge Region 半导体表面空间-电荷区的光载流子动力学和太赫兹辐射
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561517
V.L. MaIevich
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引用次数: 0
Diffuse Optical Second Harmonic Generation in Thin Nonlinear Inhomogeous Films 非线性非均匀薄膜中扩散光学二次谐波的产生
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561774
D. A. Klimkin, A. A. Nikulin, A. Fedyanin, E. Mishina, O. Aktsipetrov
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引用次数: 0
Phase Control of Sub-10-Fs Pulses: Is It Feasible? 10- fs以下脉冲的相位控制是否可行?
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561876
Lin Xu, A. Poppe, C. Spielmann, F. Krausz
Chirped dielectric mirrors ol’lier a general solution for broadhand dispersion control and fcedhack i n femtosecond laser systems1. Since the first demonstration of a prismless femtosecond Ti:sapphire ( ‘ I 1:s) laser. fenttosccond “i:S laser oscillators generating sub-IO-is pulses2.3, parametric oscillators4 and Ti:S amplifiersS were built utilizing chirped mirrors for secondand higher-order dispersion compcnsation. ‘l‘hc shorlcst laser pulscs (7.5 fs) were ohtained from a mirror dispersion controlled Ti:sapphirc ring oscillator3 by replacing conventional dichroic mirrors by chirped mirrors transparent Ibr the innp wavelengths. Until now. however, only a few papers have been devoted to the theoretical^ and technological7 challanges in connection with their design and manufacture.
啁啾介质反射镜是飞秒激光系统中宽波段色散控制和fcedhack的通用解决方案。自首次展示无棱镜飞秒Ti:蓝宝石(i1:s)激光器以来。利用啁啾反射镜进行二次和高阶色散补偿,构建了产生亚io -is脉冲的芬秒“i:S”激光振荡器2.3、参数振荡器4和Ti:S放大器。利用镜面色散控制的钛蓝宝石环形振荡器3,用透明的innp波长的啁啾反射镜取代传统的二向色散反射镜,获得了1 ' hc最短激光脉冲(7.5 fs)。直到现在。然而,只有少数几篇论文致力于与它们的设计和制造有关的理论和技术挑战。
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引用次数: 0
Amplitude Instability of Coupled Lasers 耦合激光器的振幅不稳定性
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561829
M. Miller
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引用次数: 1
Excitability and Elliptically Polarized Standing Waves in the Vector Complex Ginzburg Landau Equation for a Birefrigent Cavity 双冷腔矢量复金兹堡-朗道方程中的激发态和椭圆极化驻波
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561571
M. San Miguel, A. Amenqual, D. Walgraef, E. Hernández‐García
Transverse pattern formation in dcgenerate optical parametric oscillation (DOPO) is a subject of' present interest [ I ] . In this work we carry out an analytical study of pattern formation i n DOPO and degenerate lour-wave mixing (DFWM), which is complemented by numerical integration of the microscopic cquations of both systems. In the limit of small pump and signal detunings both systems are described by the real SwiftHohenberg equation (SHE). This broadens the range of similarities existing between DOPO and DFWM, which comprise both temporal instabilities and quantum properties. On the other hand the derivation of the SHE gives support io the already observed leading role of rolls in DOPO 111. l'he predictions about the stability of these patterns given by the SHE are in good agreement with numerical simulations. Moreover. i t has been recently shown that the SHE contains stable hexagons with an additional zero-mode [ 2 ] . which have been also found by numerical simulation. Contrarily, for small signal and large pump detunings the SHE is modified by the appearance of additional nonlinear tenns, which signals the existence of a nonlinear resonance (NLR). These additional ternis are however different iii DOPO and DFWM, limiting the similarities existing between both systems.
在退化光学参量振荡(DOPO)中横向图样的形成是一个“当前感兴趣”的主题[1]。在这项工作中,我们对DOPO和简并低波混频(DFWM)的模式形成进行了分析研究,并对这两个系统的微观方程进行了数值积分。在小泵浦和信号失谐的极限下,这两个系统都用真实的SwiftHohenberg方程(SHE)来描述。这扩大了DOPO和DFWM之间存在的相似性范围,包括时间不稳定性和量子特性。另一方面,SHE的推导支持了在dopo111中已经观察到的卷的主导作用。SHE给出的关于这些模式稳定性的预测与数值模拟很好地吻合。此外。最近已经证明,SHE包含具有附加零模的稳定六边形[2]。数值模拟也发现了这一点。相反,对于小信号和大泵浦失谐,SHE被附加非线性张力的出现所修正,这表明存在非线性共振(NLR)。然而,DOPO和DFWM的这些附加条件是不同的,限制了这两个系统之间存在的相似性。
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引用次数: 0
Spectral Dynomics of Multi-Mode Dye Lasers and Single-Atom Absorption 多模染料激光器的光谱动力学与单原子吸收
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561680
J. Sierks, T. Latz, V. M. Baev, P. Toschek
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引用次数: 11
Quasi-Probability Distribution for Photon Number Operator and Quadrature Operator in Coherent State 相干态光子数算子和正交算子的准概率分布
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561847
V. Peřinová, A. Luks
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引用次数: 0
Temporal Atom Optics with a Gravitational Cavity 具有引力腔的时间原子光学
Pub Date : 1996-01-01 DOI: 10.1109/EQEC.1996.561746
P. Szriftgiser, M. Arndt, J. Dalibard, P. Desbiolles, D. Guéry-Odelin, A. Steane
In thc optical rcgimc, multiplc hcanm interference is a pcrpular method to drastically cnhiincc the resolution of i i n intcrfcrnmctcr. Wc rcport hcrc on the rcalixition of ii multiple bem intcrfcrometcr with niiittcr W;IVCS. An atom is cohcrcntly split into morc than two aloniic wavcpackcts hy optical pumping into a vclocity dcpcndcnt inultilcvcl dark superposition state. The monienta o f two ad.jacent paths diffcr by two photon niomcnta. Whcn the atom is spatially recombined, wc ohscrvc an intcrfercncc signal that shows ;in Airy-function likc pattern characteristic for multiplc hcani interference. This method offers thc prospect o f achieving a very high resolution, since the enclosed arca is larger than that of the corresponding conventional two-beam intcrfcrometcr. For our experimcnt, we usc a cesium atomic beam and two counterpropagating optical hcams in a e-0polarization configuration tuncd to the 6Sln(F=4)-6Pln(F=4) transition of the cesium DI -line. In a first laser pulse, ccsium atonis are optically pumped into a dark superposition of thc five even magnetic ground state sublevels (mr; = -4, -2, .... 4). The momenta of the atoms in these sublevels are 0,2hk, ... ,8hk relative to the momentum of the mF = -4 sublevel (Fig. I ) . The paths spatially separate for a time T, after which a second laser pulse splits each of the five paths further into five. A third pulse at time T after the second pulse closes all partial interferometers. To read out the interferometer, we detect the fluorescence emitted during the final pulse. Typical interferometer signals for T = 5 ps are shown in Fig. 2 as a function of the phase of the final pulse. With no additional phase, the atoms are already in a dark state at this time and no fluorescence is emitted. When the phase is varied, fluorescence can be observed since the atom is not dark any more for the light field. The experimental width of the dip presently is 0.32.2~. which is broader than the theoretical value of 0.18.2~. but clearly narrower than the value 0 . 5 2 ~ observed in a two-beam interferometer. With the use of colder atoms and magnetic shielding a fringe width close to the theoretical value should be possible. For much longer interaction times we expect a washing out of the fringes caused by a recoil phase shift that increases quadratically with the path number. When the total interaction time 2T is an integer multiple of the two-photon recoil energy, a revival of the original fringe pattem OCCUIS.
在光学系统中,多波段干涉是一种常用的大幅度提高光学系统分辨率的方法。本文报道了用小W - IVCS校准2个多波长干涉计的研究进展。一个原子通过光泵浦进入一个速度相关的多周期暗叠加态,同时分裂成两个以上的孤子波包。两个人的钱。相邻路径相差两个光子。当原子在空间上重组时,会产生一个干扰信号,该信号显示出类似于多波段干扰的y函数模式特征。这种方法提供了实现非常高分辨率的前景,因为封闭的弧线比相应的传统双光束干涉计的弧线要大。在我们的实验中,我们使用了一个铯原子束和两个在e-0偏振配置下的反传播光学凸透镜来调谐铯DI线的6Sln(F=4)-6Pln(F=4)跃迁。在第一个激光脉冲中,原子铯被光泵送到五个均匀磁基态亚能级(mr;= -4, -2, ....这些亚能级中原子的动量为0,2hk,…,相对于mF = -4亚能级的动量为8hk(图1)。这些路径在空间上分离一段时间T,之后第二个激光脉冲将这五条路径进一步分成五条。在第二个脉冲之后的T时刻,第三个脉冲关闭所有的部分干涉仪。为了读出干涉仪,我们检测在最后一个脉冲中发出的荧光。图2显示了T = 5ps时典型干涉仪信号作为最终脉冲相位的函数。由于没有额外的相位,此时原子已经处于暗态,不会发出荧光。当相位变化时,可以观察到荧光,因为原子在光场中不再是暗的。目前试验的倾角宽度为0.32.2~。这比理论值0.18.2~要宽。但明显比0窄。在双光束干涉仪中观测到。利用较冷的原子和磁屏蔽,条纹宽度接近理论值应该是可能的。对于更长的相互作用时间,我们预计由于后坐力相移引起的条纹洗出,该相移随路径数呈二次增长。当总相互作用时间2T是双光子反冲能量的整数倍时,原始条纹模式就会恢复。
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引用次数: 0
期刊
EQEC'96. 1996 European Quantum Electronic Conference
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