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Observed data were well reproduced when five magnetic pathways were assumed on the basis of the Hamiltonian, H, 2J1( SMn1·SMn1, S Mn1″·SMn1T, 2J 2(SMn1·SMn2″ +SMn1*·SMn2″ +SMn2·SMn1″ +S Mn2·SMn1T, 2J 3(SMn1·SMn2, SMn1′·SMn2, S Mn2″·SMn1″, S Mn2″·SMn1T, 2J 4-(SMn2·SMn2″, 2J5SMn1·S Mn2″, SMn1′
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-1. Five parameters would be overparametric; however, attempts to fit with two or three averaged exchange parameters failed.
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