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Atomic transient recorder

机译:原子瞬态记录仪

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In Bohr's model of the hydrogen atom, the electron takes about 150 attoseconds (1 as = 10~(-18)) to orbit around the proton, defining the characteristic timescale for dynamics in the electronic shell of atoms. Recording atomic transients in real time requires excitation and probing on this scale. The recent observation of single sub-femtosecond (1 fs = 10~(-15)s) extreme ultraviolet (XUV) light pulses has stimulated the extension of techniques of femtochemistry into the attosecond regime. Here we demonstrate the generation and measurement of single 250-attosecond XUV pulses. We use these pulses to excite atoms, which in turn emit electrons. An intense, waveform-controlled, few cycle laser pulse obtains 'tomographic images' of the time-momentum distribution of the ejected electrons. Tomographic images of primary (photo)electrons yield accurate information of the duration and frequency sweep of the excitation pulse, whereas the same measurements on secondary (Auger) electrons will provide insight into the relaxation dynamics of the electronic shell following excitation. With the current ~750-nm laser probe and ~100-eV excitation, our transient recorder is capable of resolving atomic electron dynamics within the Bohr orbit time.
机译:在玻尔的氢原子模型中,电子大约需要150阿秒(1 as = 10〜(-18))在质子周围旋转,从而定义了原子电子壳中动力学的特征时标。实时记录原子瞬态需要这种规模的激发和探测。最近对单个亚飞秒(1 fs = 10〜(-15)s)极紫外(XUV)光脉冲的观察刺激了飞化学技术向阿秒范围的扩展。在这里,我们演示了单个250阿秒XUV脉冲的产生和测量。我们使用这些脉冲来激发原子,原子继而发射电子。强烈的,波形控制的,很少周期的激光脉冲可获取所喷射电子的时间动量分布的“断层图像”。一次(光)电子的断层图像可产生有关激励脉冲的持续时间和频率扫描的准确信息,而对二次(Auger)电子的相同测量将提供对激发后电子壳弛豫动力学的了解。利用电流〜750 nm的激光探针和〜100 eV的激发,我们的瞬态记录仪能够解析玻尔轨道时间内的原子电子动力学。

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