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. 2018 Feb 21;9:753. doi: 10.1038/s41467-018-03174-3

Fig. 4.

Fig. 4

Theoretical model and experimental data fitting. a Sample of the experimental data (temperature, T = 2.3 K) and the fitting to the theoretical model. The data is obtained using σ polarized pulsed excitation and σ polarized PL detection. Semi-log plot is used. b, c The two conversion pathways from the WSe2 dark exciton to the interlayer exciton. In the first pathway (A-B-D), the spin flip happens before the interlayer charge transfer while in the second one (A-C-D), the interlayer charge transfer happens before the spin flip. The conversion rate in the first path has an exponential magnetic field dependence while it is constant for the second path. d Scattering rate from dark exciton to interlayer exciton versus magnetic field. The dark-to-interlayer scattering rates in K valley (σ PL) and K′ valley (σ+ PL) are plotted against magnetic field and fitted using exponential function