Gao Xin, Min Wei
Department of Chemistry, Columbia University, New York, New York 10027, USA.
Chem Phys Rev. 2025 Jun;6(2):021306. doi: 10.1063/5.0248085. Epub 2025 May 27.
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 (σ), 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 (σ) in the same spirit of Einstein's B coefficient. Unlike σ, σ 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 σ and σ 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.
自17年前问世以来,受激拉曼散射(SRS)显微镜已成为一种变革性的成像方式,能够以高灵敏度、速度、特异性和分辨率可视化化学键。尽管取得了巨大成功,但该领域仍缺乏严格的理论。关于SRS显微镜为何以及在多大程度上能优于传统拉曼显微镜这一基本问题,尚未得到定量解答。传统上通过拉曼截面(σ)来理解的拉曼散射,长期以来因其与线性吸收截面相比极小的值而被认为较弱。然而,这种观点并不完整,甚至具有误导性,因为拉曼散射和线性吸收过程涉及不同阶次的光与物质相互作用。在本综述中,我们总结了最近发展的受激响应公式,该公式以爱因斯坦B系数的精神定义了受激拉曼截面(σ)。与σ不同,σ本质上很强,甚至超过了电子对应物,这得到了实验测量和量子电动力学理论的支持。这个新框架揭示了拉曼散射以前未知的对偶性质,其中对于同一分子,σ和σ可能表现出截然不同的量级,它们通过真空零点涨落的影响相互联系。此外,拉曼对偶性还推广了爱因斯坦系数,从而统一了四个过程(自发和受激发射、自发拉曼和SRS)。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在高时空区域表现出色,解释了其成像化学键无与伦比的能力,而化学键成像本身就需要高空间和时间分辨率。我们期望这一理论能够促进拉曼光谱学的科学理解和技术应用。