Research paperAbsorptive and dispersive responses in a two-level molecule with vibronic coupling: Permanent dipole moments effects
Graphical abstract
Introduction
The dynamic behavior of a molecular system interacting with strong electromagnetic fields in the presence of a thermal reservoir has been the subject of several studies [1], [2], [3], [4], [5]. Four-wave-mixing spectroscopy (FWM) and polarization have been used to determine the parameters associated with the dissipation mechanisms in such molecular systems. These parameters, controlled by the longitudinal and transversal relaxation times T1 and T2, have also been validated with experiments and theoretical developments in nonlinear optical. Theoretical and experimental developments in resonant processes of Rayleigh-type Optical Mixing (RTOM) signals, proposed by Yajima and Souma [6], [7]. In another study, Boyd et al [8] characterized a two-level system through the study of parametric interactions in Four-wave Mixing (FWM). Souma et al [9] later performed experiments in resonant wave mixing on Rhodamine 6G, DQCI and Cresyl-violet dyes in ethanol using phase-conjugate configuration. Erskine et al [10] proposed femtosecond studies of the recovery dynamics of Malachite Green in solution. In aqueous solutions, Marcano and García-Golding [11] studied the power effects using polarization spectroscopy. To include phenomenological dephasing constants, these works introduced stochastic modulations of the levels, harmonic oscillators models, or microscopic models of non-Born-Oppenheimer dynamics on multidimensional excited state potential energy surfaces [12]. For pure and mixed states [13], vibronic coupling constants (VCC) and coupling densities (VCD) have been successfully applied as reactivity indices of fullerenes and nanographene. Also, newly emerging vibrational progressions due Herzberg-Teller vibronic coupling that show up in absorption spectra and quantum beats in photon echo signals have been rigorously studied [14].
The presence of intramolecular coupling is of great importance in various physical and chemical processes. Some examples include i) weak transition probabilities forbidden by symmetry in absorption and emission [15], ii) relaxation rates of internal conversion [16], iii) harmonic diabatic potentials studied by femtosecond spectroscopy [17], iv) optical absorption band shape of dimmers [18], and v) resonances in a scattering process [19]. Curve-crossing problems have received special attention in recent years, and they have found applications in various fields of physics, chemistry, and biology [20]. The introduction of a residual perturbation, which may arise from a residual electron–electron correlation and/or spin–orbit coupling terms in the Hamiltonian of the system, may couple the above electronic states, causing a separation of the two curves in agreement with the avoided-crossing rule. The insertion of residual terms allows us to generate a new adiabatic basis, which gives a functional account of the original diabatic states [21], [22]. We evaluate the density matrix elements for both coherence and population difference descriptions, which allows us to express the macroscopic polarization in the FWM spectroscopy. We evaluate the dispersive and absorptive optical properties as a function of the parameters governing the coupling. Our results show the sensitivity of these optical properties with respect to the adiabatic dipole moments. We also demonstrate that at certain frequency detuning regions, the absorption curves display radical changes showing the possibility of generating parametric amplifications tunable to the organic dyes used.
Section snippets
Vibronic coupling
We take a two-level vibronic model to study the simplest molecular system based on harmonic potential curves. The Hamiltonian that describes the molecule is given by:
where where and are the nuclear and electronic kinetic energy operators, is the potential energy term, is a spin–orbit residual term. The total wavefunction is given by:
which represents a linear combination of two Born-Oppenheimer (BO)
Bloch́s optical equations and nonlinear optical properties
To describe the temporal evolution of the system, we start with the Liouville equation . In this case: , where ; S, F, TR represent the system, field, and thermal reservoir, respectively. The remaining Hamiltonians correspond to the interactions between them.
The dynamic of the density matrix of the system (S) is given by:
with being a relaxation matrix. The density matrix elements
Theoretical results
The influence of permanent dipole moments on the nonlinear absorption coefficient and refractive index of a two-level molecular system (Malachite Green) with vibronic coupling, is studied. Its characteristics parameters are and , and . It should be noted that the proposed model of radiation-matter interaction is completely general. It is important to point out that the parameters we are using in this work, related to the Malachite Green,
Final comments
The transition and permanent dipole moments are strongly influenced by intramolecular coupling. Of particular importance is the case when non-zero permanent dipole moments from coupled states are obtained and compared to those from uncoupled states. Also, we have found, in the opposite direction, cancellation of the transition dipole moment of the coupled states, starting from non-zero permanent and transition dipole moments for the uncoupled states. The effective susceptibility at the field
CRediT authorship contribution statement
J.L. Paz: Conceptualization, Formal analysis, Investigation, Supervision, Writing - review & editing. Marcos Loroño: Software. Alberto Garrido Schaeffer: Validation. Lenin A. González-Paz: Validation. Edgar Marquez: Software. Joan Vera-Villalobos: Validation. José R. Mora: Software. Ysaias J. Alvarado: Validation, Conceptualization, Writing - review & editing.
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
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