受激拉曼散射显微镜的量子理论。

IF 6.1 Q2 CHEMISTRY, PHYSICAL
Chemical physics reviews Pub Date : 2025-06-01 Epub Date: 2025-05-27 DOI:10.1063/5.0248085
Xin Gao, Wei Min
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引用次数: 0

摘要

自17年前问世以来,受激拉曼散射(SRS)显微镜已经成为一种变革性的成像方式,通过高灵敏度、高速度、高特异性和高分辨率的化学键可视化。尽管它取得了巨大的成功,但在社区中仍缺乏严谨的理论。SRS显微镜为什么以及在多大程度上优于传统的拉曼显微镜的基本问题还没有得到定量的回答。拉曼散射,传统上通过拉曼截面(σ拉曼)来理解,长期以来被认为是弱的,因为与线性吸收截面相比,它的值非常小。然而,这种观点是不完整的,甚至是误导性的,因为拉曼散射和线性吸收过程涉及不同阶次的光-物质相互作用。在本文中,我们总结了最近发展的受激响应公式,该公式与爱因斯坦的B系数相同,定义了受激拉曼截面(σSRS)。与σ拉曼不同,σSRS在本质上是强的,甚至超过了电子拉曼,这得到了实验测量和量子电动力学理论的支持。这个新的框架揭示了拉曼散射的一个以前未知的对偶性质,其中σ拉曼和σSRS在同一分子中可以表现出截然不同的量级,由真空零点波动的影响连接起来。此外,拉曼对偶性还概括了爱因斯坦的系数,使四个过程(自发和受激发射、自发拉曼和SRS)统一起来。最后,该公式提供了SRS显微镜绝对信号和可检测性的定量预测。我们可以证明SRS在高时空状态下表现出色,这解释了其无与伦比的化学键成像能力,而化学键本身就需要高空间和时间分辨率。我们期望这一理论能促进对拉曼光谱的科学认识和技术应用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum theory of stimulated Raman scattering microscopy.

Since its advent 17 years ago, stimulated Raman scattering (SRS) microscopy has emerged as a transformative imaging modality by visualizing chemical bonds with high sensitivity, speed, specificity, and resolution. Despite its enormous success, a rigorous theory is yet lacking in the community. The fundamental question of just why and how much SRS microscopy can outperform conventional Raman microscopy has not been quantitatively answered. Raman scattering, traditionally understood through the Raman cross section (σRaman), has long been believed weak due to its extremely small values when compared to linear absorption cross sections. However, this view is incomplete and even misleading since Raman scattering and linear absorption processes involve different orders of light-matter interaction. In this review, we summarize the recently developed stimulated response formulation, which defines the stimulated Raman cross section (σSRS) in the same spirit of Einstein's B coefficient. Unlike σRaman, σSRS turns out to be intrinsically strong and even exceeding the electronic counterparts, which is supported by experimental measurements and quantum electrodynamic theories. This new framework reveals a previously unknown duality nature of Raman scattering, where both σRaman and σSRS can exhibit vastly different magnitudes for the same molecule, connected by the influence of vacuum zero-point fluctuations. Additionally, the Raman duality also generalizes Einstein's coefficients so that four processes (spontaneous and stimulated emission, spontaneous Raman and SRS) are unified. Finally, the formulation provides quantitative prediction of the absolute signal and detectability of SRS microscopy. We can prove that SRS excels in high spatiotemporal regimes, explaining its unparalleled ability to image chemical bonds, which inherently demand high spatial and temporal resolution. We expect this theory to facilitate both scientific understanding and technological applications of Raman spectroscopy.

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