Abstract

Coherent anti-Stokes Raman spectroscopy (CARS) and Ccherent anti-Stokes hyper-Raman spectroscopy (CAHRS), as other high-order nonlinear spectroscopy techniques, are widely exploited in many research fields, such as dynamic processes, gene expression spectrum screening, high-resolution spectroscopy, and nonlinear high-resolution imaging. However, it is difficult to make a quantitative analysis of the spectral signals that involve a large number of high-order micropolarizability tensors. It is reported that the CARS and CAHRS microscopic hyperpolarizability tensor elements can be decomposed into the product of the differentiation of Raman microscopic polarizability tensor α′i′j′ and hyper-Raman microscopic polarizability tensor β′i′j′k′ so that the high-order spectra can be simplified to the analysis of low-order spectra. In this paper, we use the bond additivity model (BAM) combined with experimental corrections to address the carbon dioxide (CO2) molecule and present the simplified scheme for differentiation of hyper-Raman microscopic polarizability tensor elements β′i′j′k′. Taking advantage of this approach, combined with the experimental correction, the differentiation of Hyper-Raman microscopic polarizability tensor elements β′i′j′k′ of the CO2 is obtained and the expressions of β′i′j′k′ for antisymmetric vibrations of CO2 are deduced. Finally, substituting the differentiation of Raman microscopic polarizability tensor elements α′i′j′ reported in the literature into the ratio above can obtain the proportional relationship between the microscopic polarizability tensor elements of CARS and CAHRS of the CO2. This method can provide the basis for the quantitative analysis of high-order nonlinear spectral profiles.

Highlights

  • In the past ten years, as a high-order nonlinear spectroscopy technique, coherent anti-Stokes Raman spectroscopy (CARS) and its surface enhancement methods [1–6] and coherent anti-Stokes hyper-Raman spectroscopy (CAHRS) [7–9] have gained important applications in kinetic processes, gene expression profile screening, high-resolution spectroscopy, nonlinear high-resolution imaging technology, and so on

  • Based on the second-order nonlinear optical process of the sum frequency generation vibrational spectroscopy (SFG-VS) quantitative analysis method [11–13], we propose a method to simplify the high-order microscopic polarizability tensor elements of CARS and CAHRS [10, 14]

  • By using the bond additivity model (BAM) and its experimental modification, a simplified scheme is proposed to calculate the hyperRaman microscopic polarizability tensor differential β′i′j′k′ of the carbon dioxide (CO2) molecule. is approach is quite general, and it can be extended to other nonlinear coherent Raman spectroscopic techniques to simplify the relationship between the microscopic polarizability tensor elements and quantitative analysis of the experimental signal, such as time-domain Raman spectroscopy [18, 19], stimulated Raman scattering [20, 21], and nonlinear high-resolution microscopy [5, 6]

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Summary

Introduction

In the past ten years, as a high-order nonlinear spectroscopy technique, coherent anti-Stokes Raman spectroscopy (CARS) and its surface enhancement methods [1–6] and coherent anti-Stokes hyper-Raman spectroscopy (CAHRS) [7–9] have gained important applications in kinetic processes, gene expression profile screening, high-resolution spectroscopy, nonlinear high-resolution imaging technology, and so on. As a high-order nonlinear coherent optical process, the spectral signals of CARS and CAHRS are contributed by the third and fourth-order microscopic polarizability tensor elements of molecular groups [10]. Based on the second-order nonlinear optical process of the sum frequency generation vibrational spectroscopy (SFG-VS) quantitative analysis method [11–13], we propose a method to simplify the high-order microscopic polarizability tensor elements of CARS and CAHRS [10, 14]. Is approach is quite general, and it can be extended to other nonlinear coherent Raman spectroscopic techniques to simplify the relationship between the microscopic polarizability tensor elements and quantitative analysis of the experimental signal, such as time-domain Raman spectroscopy [18, 19], stimulated Raman scattering [20, 21], and nonlinear high-resolution microscopy [5, 6].

BAM Solves β9i9j9k9 of CO2
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