论文标题
原子自旋波控制和旋转依赖性踢,带状次秒脉冲
Atomic spin-wave control and spin-dependent kicks with shaped subnanosecond pulses
论文作者
论文摘要
与原子气体的电偶极转变相连的旅行光子的吸收自然会导致电偶极旋转波兴奋。对于许多应用,在可能发生自发发射之前,高度希望形成并连贯控制自旋波的空间波形。本文详细介绍了一种最近开发的光学控制技术,以实现此目标,在此过程中,反向传播的,次纳秒脉冲通过周期性驱动辅助转变,将次波长几何阶段赋予自旋波。特别是,我们将此技术应用于激光冷却的$^{87} $ rb原子上的旋转波的波向量,通过驱动带有形状优化的脉冲的辅助$ d1 $过渡,以使需求关闭并回忆起超级超级超级。我们在自旋波控制过程中研究了自旋依赖性动量转移,这导致了瞬态光学力量,高达$ \ sim 1 \ hbar k $/ns,并通过共同表征旋转波控制和Mate-Wave Controls Acceleration来研究获得$ 75 \%SIM 75 \%SIM 75 \%$ Spin Wave控制效率的局限性。在数值建模的帮助下,我们将控制保真度的未来改善投射到$ 99 \%$级别时,当原子状态得到更好的准备并通过为更快,更强大的脉搏塑形器配备。我们的技术还可以对超级发射进行无背景测量,以揭示出光学深度的发射强度和衰减速率的精确缩放。
The absorption of traveling photons resonant with electric dipole transitions of an atomic gas naturally leads to electric dipole spin wave excitations. For a number of applications, it would be highly desirable to shape and coherently control the spatial waveform of the spin waves before spontaneous emission can occur. This paper details a recently developed optical control technique to achieve this goal, where counter-propagating, shaped sub-nanosecond pulses impart sub-wavelength geometric phases to the spin waves by cyclically driving an auxiliary transition. In particular, we apply this technique to reversibly shift the wave vector of a spin wave on the $D2$ line of laser-cooled $^{87}$Rb atoms, by driving an auxiliary $D1$ transition with shape-optimized pulses, so as to shut off and recall superradiance on demand. We investigate a spin-dependent momentum transfer during the spin-wave control process, which leads to a transient optical force as large as $\sim 1\hbar k$/ns, and study the limitations to the achieved $70\sim 75\%$ spin wave control efficiency by jointly characterizing the spin-wave control and matterwave acceleration. Aided by numerical modeling, we project potential future improvements of the control fidelity to the $99\%$ level when the atomic states are better prepared and by equipping a faster and more powerful pulse shaper. Our technique also enables a background-free measurement of the superradiant emission to unveil the precise scaling of the emission intensity and decay rate with optical depth.