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. Author manuscript; available in PMC: 2009 Oct 30.
Published in final edited form as: J Chem Phys. 2008 Feb 7;128(5):052211. doi: 10.1063/1.2833582

Fig. 3.

Fig. 3

Population distribution at thermal equilibrium for a general three-spin system (a). Saturation of the allowed EPR transitions for one of the dipolar coupled electrons (ω0S1) leads to negative enhancement (b). Saturation of the transition corresponding to the second electron (ω0S2) leads to positive enhancement (c).