This work reports Mössbauer and DFT studies of the diiron-N
2 complex L
MeFeNNFeL
Me (L =
![](/im<font color=)
ages/gifchars/beta2.gif" BORDER=0 ALIGN="middle">-diketiminate),
1a. Complex
1a, formally diiron(I), has a system spin
S = 3 with an isolated
MS = ±3quasi-doublet as a ground state; the
MS = ±2 doublet is >100 cm
-1 higher in energy. Complex
1a exhibitsat 4.2 K a large, positive m
agnetic hyperfine field,
Bint = +68.1 T, and an effective
g value of 16 ± 2 alongthe easy m
agneti
zation axis of the ground doublet; this value is significantly larger than the spin-only value(
g = 12). These results have been rationali
zed by DFT calculations, which show that each Fe site donatessignificant electron density into the
![](/im<font color=)
ages/gifchars/pi.gif" BORDER=0 >* orbitals of dinitrogen, resulting in a configuration best described astwo high-spin Fe
II (
Sa =
Sb = 2) bridged by triplet N
22- (
Sc = 1). In this description the minority spin electronof each iron is accommodated by two nonbonding, closely spaced 3d orbitals,
z2 and
yz (
z is perpendicularto the diketiminate planes,
x is along the Fe···Fe vector). Spin-orbit coupling between these orbital statesgenerates a large unquenched orbital momentum along the iron-iron vector. The
S = 3 ground state of
1a results from strong antiferrom
agnetic direct exchange couplings of the Fe spins (
Sa =
Sb = 2) to theN
22- spin (
Sc = 1) and can be formulated as
![](/im<font color=)
ages/entities/verbar.gif">((
Sa,
Sb)
Sab = 4,
Sc = 1),
S = 3>;
H =
J(
Sa +
Sb)·
Sc with
J ![](/im<font color=)
ages/entities/ap.gif">3500 cm
-1.