TY - JOUR
T1 - Monitoring of nonadiabatic effects in individual chromophores by femtosecond double-pump single-molecule spectroscopy
T2 - A model study
AU - Gelin, Maxim F.
AU - Palacino-González, Elisa
AU - Chen, Lipeng
AU - Domcke, Wolfgang
N1 - Publisher Copyright:
© 2019 MDPI AG. All rights reserved.
PY - 2019
Y1 - 2019
N2 - We explore, by theoretical modeling and computer simulations, how nonadiabatic couplings of excited electronic states of a polyatomic chromophore manifest themselves in single-molecule signals on femtosecond timescales. The chromophore is modeled as a system with three electronic states (the ground state and two non-adiabatically coupled excited states) and a Condon-active vibrational mode which, in turn, is coupled to a harmonic oscillator heat bath. For this system, we simulate double-pump single-molecule signals with fluorescence detection for different system-field interaction strengths, from the weak-coupling regime to the strong-coupling regime. While the signals are determined by the coherence of the electronic density matrix in the weak-coupling regime, they are determined by the populations of the electronic density matrix in the strong-coupling regime. As a consequence, the signals in the strong coupling regime allow the monitoring of nonadiabatic electronic population dynamics and are robust with respect to temporal inhomogeneity of the optical gap, while signals in the weak-coupling regime are sensitive to fluctuations of the optical gap and do not contain information on the electronic population dynamics.
AB - We explore, by theoretical modeling and computer simulations, how nonadiabatic couplings of excited electronic states of a polyatomic chromophore manifest themselves in single-molecule signals on femtosecond timescales. The chromophore is modeled as a system with three electronic states (the ground state and two non-adiabatically coupled excited states) and a Condon-active vibrational mode which, in turn, is coupled to a harmonic oscillator heat bath. For this system, we simulate double-pump single-molecule signals with fluorescence detection for different system-field interaction strengths, from the weak-coupling regime to the strong-coupling regime. While the signals are determined by the coherence of the electronic density matrix in the weak-coupling regime, they are determined by the populations of the electronic density matrix in the strong-coupling regime. As a consequence, the signals in the strong coupling regime allow the monitoring of nonadiabatic electronic population dynamics and are robust with respect to temporal inhomogeneity of the optical gap, while signals in the weak-coupling regime are sensitive to fluctuations of the optical gap and do not contain information on the electronic population dynamics.
KW - Nonadiabatic dynamics
KW - Single-molecule spectroscopy
KW - Strong-field regime
KW - Weak-field regime
UR - http://www.scopus.com/inward/record.url?scp=85059883613&partnerID=8YFLogxK
U2 - 10.3390/molecules24020231
DO - 10.3390/molecules24020231
M3 - Article
C2 - 30634541
AN - SCOPUS:85059883613
SN - 1420-3049
VL - 24
JO - Molecules
JF - Molecules
IS - 2
M1 - molecules24020231
ER -