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. 2021 Jul 6;12(27):6341–6347. doi: 10.1021/acs.jpclett.1c01447

Figure 4.

Figure 4

TR-EPR on a randomly oriented ensemble of D-χ-A molecules. Parameters: Δg = 0.002, rDA = 25 Å, = 9.8 GHz. (a) and (b) Two-dimensional maps of ⟨Sy(t, B)⟩ for an initial singlet or polarized state, respectively. (c) Field dependence of the absorption TR-EPR spectrum, integrated in the time-window corresponding to the first maxima-minima in the maps of panels (a) and (b), for the states Inline graphic, ρp (with either p = −1 or p = 1, leading to the same result in solution). (d) Time dependence around B ≈ 349.5 mT, highlighting the opposite behavior at short times for polarized and unpolarized states. Simulations include relaxation, dephasing, and recombination of the radical pair, with T1 = 2 μs, T2 = 0.5 μs, TR = 10 μs (in the singlet–triplet RP basis, see the Supporting Information), and Gaussian broadening with fwhm = 0.15 mT.36 Inset: schematic energy-level diagram, with states practically corresponding to eigenstates of Szi. Allowed EPR transitions of D (A) are indicated by blue (purple) dashed lines.