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. Author manuscript; available in PMC: 2010 Aug 6.
Published in final edited form as: J Phys Chem B. 2009 Aug 6;113(31):10923–10933. doi: 10.1021/jp9031805

Figure 5.

Figure 5

(A) Recombination kinetics of ferric HRP-NO as a function of magnetic field. The sample was stabilized for 30 minutes after each field intensity change. The pump and probe wavelengths were 403nm and 420nm, respectively. Black solid lines are the MEM fits and the insert shows the MEM rate distributions as a function of magnetic field. (B) Comparison of the ferrous MbNO rebinding kinetics with (H=10 T) and without application of a magnetic field. No difference outside of experimental error is observed. The inset shows the MEM rate distributions, which contain differences due to experimental noise and finite data truncation effects (see ref. 58).