论文标题
光发射从根本上与发射粒子的量子相干性息息相关
Light emission is fundamentally tied to the quantum coherence of the emitting particle
论文作者
论文摘要
在物理和工程的许多领域中,通过自由电荷颗粒对光的相干发射是无处不在的,并且在所有相关的实验环境中,光线的特性被经典电磁势能成功捕获。光和自由量子问题波之间的相互作用的出现带来了有关粒子波函数的基本问题。在这里,我们表明,即使在看似古典的实验机制中,光发射从根本上讲与发射颗粒的量子特性(例如它们的量子相干性和相关性)相关。通过采用量子电动力学,我们揭示了粒子相干动量不确定性的作用,没有哪种光的发光将成为主导。例如,我们将Cherenkov辐射(Cherenkov Radiation)视为光线的冲击波。相反,我们发现冲击波的持续时间从下面结合了粒子的连贯动量不确定性,这是由于粒子和光之间的基本纠缠而导致的。这种量子光学范式在分析电子显微镜中打开了新的能力,从而实现了形状电子波袋的量子相关性的测量。我们的发现还针对Cherenkov探测器在粒子物理学中的应用。例如,通过测量光谱光子自相关,可以揭示粒子的波函数大小,形状和相干性。对于许多其他技术,此类方案对于许多高能颗粒特别有趣。
Coherent emission of light by free charged particles is ubiquitous in many areas of physics and engineering, with the light's properties believed to be successfully captured by classical electromagnetism in all relevant experimental settings. The advent of interactions between light and free quantum matter waves brought about fundamental questions regarding the role of the particle wavefunction. Here we show that even in seemingly classical experimental regimes, light emission is fundamentally tied to quantum properties of the emitting particles, such as their quantum coherence and correlations. By employing quantum electrodynamics, we unveil the role of the particle's coherent momentum uncertainty, without which decoherence of light becomes dominant. As an example, we consider Cherenkov radiation, envisioned for almost a century as a shockwave of light. We find instead that the shockwave's duration is fundamentally bound from below by the particle's coherent momentum uncertainty due to the underlying entanglement between the particle and light. This quantum optical paradigm opens new capabilities in analytical electron microscopy, enabling the measurement of quantum correlations of shaped electron wavepackets. Our findings also have applications for Cherenkov detectors in particle physics. For example, by measuring spectral photon autocorrelations, one can unveil the particle's wavefunction size, shape and coherence. Such schemes are especially intriguing for many high-energy particles, where other techniques are not available.