论文标题
超快速光发射后的纳米针尖后几乎没有电子相关性
Few-electron correlations after ultrafast photoemission from nanometric needle tips
论文作者
论文摘要
游离电子在诸如电子显微镜,加速器和光发射光谱等多种应用中至关重要。通常,许多电子的空间电荷效应是令人讨厌的。仅限于极小的时空维度,即使两个电子也可以强烈相互作用。在这种情况下,正如我们在这里所展示的那样,库仑排斥力现在可以非常有利,因为它会导致出人意料的电子电子相关性。我们表明,由于动态的库仑排斥力,纳米针尖的飞秒激光发射的电子在能量上高度相关,可见性为$ 56 \,\%$。我们提取$ 3.3 \,$ ev的平均能量分解和相关衰减时间为$ 82 \,$ fs。重要的是,能量过滤的电子显示出二阶相关函数的次频数分布分布,其小至$ g^{(2)} = 0.34 $,这意味着可以基于简单的能量滤波来实现射击噪声降低噪声的脉冲电子束。甚至预示的电子也可以用于量子增强的电子成像协议。此外,我们还达到了激光驱动电子发射的强场状态。我们深入了解不同电子类别的电子相关性(直接与撤销)如何受到强激光场的影响。我们的工作水平量子电子光学电位,直接对降低降噪和量子电子成像进行直接分析,以及从强相关物质内部的相关电子的直接测量。
Free electrons are essential in such diverse applications as electron microscopes, accelerators, and photo-emission spectroscopy. Often, space charge effects of many electrons are a nuisance. Confined to extremely small space-time dimensions, even two electrons can interact strongly. In this case, the Coulomb repulsion can now be highly advantageous, because it leads to surprisingly powerful electron-electron correlations, as we demonstrate here. We show that femtosecond laser-emitted electrons from nanometric needle tips are highly anti-correlated in energy because of dynamic Coulomb repulsion, with a visibility of $56\,\%$. We extract a mean energy splitting of $3.3\,$eV and a correlation decay time of $82\,$fs. Importantly, the energy-filtered electrons display a sub-Poissonian number distribution with a second order correlation function as small as $g^{(2)} = 0.34$, implying that shot noise-reduced pulsed electron beams can be realized based on simple energy filtering. Even heralded electrons could become available for quantum-enhanced electron imaging protocols. Furthermore, we also reach the strong-field regime of laser-driven electron emission. We gain deep insights into how the electron correlations of the different electron classes (direct vs. rescattered) are influenced by the strong laser fields. Our work levels the field of quantum electron optics, with direct ramifications for shot noise-reduced and quantum electron imaging as well as direct measurements of correlated electrons from inside of strongly correlated matter.