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. 2016 May 10;113(21):E2916–E2924. doi: 10.1073/pnas.1524720113

Fig. S2.

Fig. S2.

(A) Fittings by two- and three-state HMMs. (B) Dwell time analysis by the three-state HMM. (Left) The dwell time of the highest FRET state among the three states was fitted by single-exponential function of which the rate constant was 1.8 s−1, which was consistent with 2.1 s−1 for the high FRET state in the two-state HMM (main text). (Right) The combined dwell time of the remaining two FRET states was fitted by a convolution of two exponential functions of which the rate constant was 2.5 s−1, which is consistent with 2.4 s−1 for the middle FRET state in the two-state HMM (main text). AIC, Akaike Information Criterion.