Skip to main content
. 2023 Mar 7;4(7):1720–1730. doi: 10.1039/d2ma00136e

Fig. 4. (a) Differential transmission spectrum upon non-resonant pumping (Epump = 3.1 eV), for T = 5 K, τ = 0.5 ps (red dots) and the corresponding fit (dashed line). The model used for fitting contains the PB of Γ1 and Inline graphic (positive Gaussian features), the energy shift of the excitonic state (derivative Gaussian shape Inline graphic) and an associated excited state PA Π1 (negative Gaussian feature). (b) Widths of the fit components for Γ1 (triangles) and Inline graphic (circles). A fit with the dispersion relation of optical phonons (dashed red line) gives an estimate of the LO phonon energy of 14.7 meV. (c) Two dimensional map showing the time resolved coherent oscillations upon hot carrier excitation pumping at 3.1 eV, as a function of pump delay time and detection energy. The observed oscillations persist for longer than 20 ps. The nodal point at E = 1.927 eV marks the position of the exciton coupled to the observed coherent phonons. (d) Fourier transform spectrum of the oscillatory dynamics displayed in (c), and integrated over all the probe energies. This corresponds to the resonant impulsive stimulated Raman spectrum of (PEA)2SnI4 at 5 K.

Fig. 4