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. 2012 May 23;109(23):8850-8855. doi: 10.1073/pnas.1111582109

Fig. 2.

Fig. 2.

Configurational entropy for the REM as a function of E for c = 0,c = cK,c > cK (from top to bottom). The equilibrium energy is stuck at the value Eeq(β). For c < cK the partition function is dominated by configurations with energy Eeq(β) (the straight line has a slope β). For c > cK the partition function is dominated by the contribution from the reference configuration; higher states lead to a subleading contribution.