We re
port a new theoretical
model that accounts for the unusual
magnetic
pro
perties of thecyanide cluster {[Mn
II(t
mphen)
2]
3[Mn
III(CN)
6]
2} (t
mphen = 3,4,7,8-tetra
methyl-1,10-
phenanthroline). The
model takes into account (1) the s
pin-orbit interaction, (2) the trigonal co
mponent of the crystal field actingon the ground-state cubic
3T1(
![](/isubscribe/journals/jacsat/126/i51/eqn/ja046771ae10001.gif)
) ter
ms of the a
pical Mn(III) ions, and (3) the isotro
pic contribution to theexchange interaction between Mn(III) and Mn(II) ions. The ground state of the cluster was shown to be thestate with the total angular
mo
mentu
m projection
![](/i<font color=)
mages/entities/verbar.gif">
MJ![](/i<font color=)
mages/entities/verbar.gif"> = 15/2; the energies of the low-lying levels obtainedfro
m this treat
ment increase with decreasing
![](/i<font color=)
mages/entities/verbar.gif">
MJ![](/i<font color=)
mages/entities/verbar.gif"> values, a situation that leads to a barrier for the reversalof
magnetization (
Ueff ![](/i<font color=)
mages/entities/a
p.gif"> 30 c
m-1). The new
model ex
plains the recently discovered single-
molecule
magnetbehavior of the {[Mn
II(t
mphen)
2]
3[Mn
III(CN)
6]
2} in contrast to the traditional a
pproach that takes into accountonly the ground-state s
pin (S) and a negative zero-field s
plitting
para
meter (
DS < 0).