Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations
Most of spectroscopic signals are specified by the nonlinear laser-induced polarization. In recent years, population-detection of signals becomes a trend in femtosecond spectroscopy. Polarization-detected (PD) and population-detected signals are fundamentally different, because they are determined b...
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sg-ntu-dr.10356-1808442024-10-29T06:33:34Z Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations Sun, Kewei Vasquez, Luis Borrelli, Raffaele Chen, Lipeng Zhao, Yang Gelin, Maxim F. School of Materials Science and Engineering Chemistry Fluorescence Polarization Most of spectroscopic signals are specified by the nonlinear laser-induced polarization. In recent years, population-detection of signals becomes a trend in femtosecond spectroscopy. Polarization-detected (PD) and population-detected signals are fundamentally different, because they are determined by photoinduced processes acting on disparate time scales. In this work, we consider the fluorescence-detected (FD) N-wave-mixing (NWM) signal as a representative example of population-detected signals, derive a rigorous expression for this signal, and discuss its approximate variants suitable for numerical simulations. This leads us to the definition of the phenomenological FD (PFD) signal, which contains as a special case all definitions of FD signals available in the literature. Then we formulate and prove the population-polarization equivalence (PPE) theorem, which states that PFD NWM signals produced by (possibly strong) laser pulses can be evaluated as conventional PD signals in which the effective polarization is determined by the PFD transition dipole moment operator. We use the PPE theorem for the construction of the ab initio protocol for the simulation of PFD 4WM signals. As an example, we calculate electronic two-dimensional (2D) PFD spectra of the gas-phase pyrazine and compare them with the corresponding PD 2D spectra. M.F.G. acknowledges the support from the National Natural Science Foundation of China (Grant No. 22373028). L.P.C. acknowledges support from the starting grant of research center of new materials computing of Zhejiang Lab (No. 3700-32601). R.B. acknowledge the research project “nuovi Concetti, mAteriali e tecnologie per l’iNtegrazione del fotoVoltAico negli edifici in uno scenario di generazione diffuSa” [CANVAS], funded by the Italian Ministry of the Environment and the Energy Security, through the Research Fund for the Italian Electrical System (type-A call, published on G.U.R.I. n. 192 on18-08-2022). 2024-10-29T06:33:34Z 2024-10-29T06:33:34Z 2024 Journal Article Sun, K., Vasquez, L., Borrelli, R., Chen, L., Zhao, Y. & Gelin, M. F. (2024). Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations. Journal of Chemical Theory and Computation, 20(17), 7560-7573. https://dx.doi.org/10.1021/acs.jctc.4c00592 1549-9618 https://hdl.handle.net/10356/180844 10.1021/acs.jctc.4c00592 39185737 2-s2.0-85202673346 17 20 7560 7573 en Journal of Chemical Theory and Computation © 2024 American Chemical Society. All rights reserved. |
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Chemistry Fluorescence Polarization Sun, Kewei Vasquez, Luis Borrelli, Raffaele Chen, Lipeng Zhao, Yang Gelin, Maxim F. Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
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Most of spectroscopic signals are specified by the nonlinear laser-induced polarization. In recent years, population-detection of signals becomes a trend in femtosecond spectroscopy. Polarization-detected (PD) and population-detected signals are fundamentally different, because they are determined by photoinduced processes acting on disparate time scales. In this work, we consider the fluorescence-detected (FD) N-wave-mixing (NWM) signal as a representative example of population-detected signals, derive a rigorous expression for this signal, and discuss its approximate variants suitable for numerical simulations. This leads us to the definition of the phenomenological FD (PFD) signal, which contains as a special case all definitions of FD signals available in the literature. Then we formulate and prove the population-polarization equivalence (PPE) theorem, which states that PFD NWM signals produced by (possibly strong) laser pulses can be evaluated as conventional PD signals in which the effective polarization is determined by the PFD transition dipole moment operator. We use the PPE theorem for the construction of the ab initio protocol for the simulation of PFD 4WM signals. As an example, we calculate electronic two-dimensional (2D) PFD spectra of the gas-phase pyrazine and compare them with the corresponding PD 2D spectra. |
author2 |
School of Materials Science and Engineering |
author_facet |
School of Materials Science and Engineering Sun, Kewei Vasquez, Luis Borrelli, Raffaele Chen, Lipeng Zhao, Yang Gelin, Maxim F. |
format |
Article |
author |
Sun, Kewei Vasquez, Luis Borrelli, Raffaele Chen, Lipeng Zhao, Yang Gelin, Maxim F. |
author_sort |
Sun, Kewei |
title |
Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
title_short |
Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
title_full |
Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
title_fullStr |
Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
title_full_unstemmed |
Interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
title_sort |
interconnection between polarization-detected and population-detected signals: theoretical results and ab initio simulations |
publishDate |
2024 |
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https://hdl.handle.net/10356/180844 |
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1814777765280350208 |