The ground-state e
lectronic structure of the trinuc
lear co
mp
lex Cu
3(dpa)
4C
l2 (
1), where dpa is the anion of di(2-pyridy
l)a
mine, has been investigated within the fra
mework of density functiona
l theory (DFT) and co
mpared withthat obtained for other known M
3(dpa)
4C
l2 co
mp
lexes (M = Cr, Co, Ni) and for the sti
ll hypothetica
l Ag
3(dpa)
4C
l2co
mpound. Both coinage
meta
l co
mpounds disp
lay three sing
ly occupied
x2-
y2-
like (
mages/gifchars/de
lta.gif" BORDER=0 >) orbita
ls oriented toward thenitrogen environ
ment of each
meta
l ato
m, generating antibonding M-(N
4) interactions. A
ll other
meta
l orbita
lco
mbinations are doub
ly occupied, resu
lting in no de
loca
lized
meta
l-
meta
l bonding. This is at variance with theother known sy
mmetric M
3(dpa)
4C
l2 co
mp
lexes of the first transition series, which a
ll disp
lay so
me de
loca
lizedbonding through the
meta
l backbone, with for
ma
l bond
mu
ltip
licity decreasing in the order Cr > Co > Ni. Anantiferro
magnetic coup
ling deve
lops between the sing
ly occupied MOs via a superexchange
mechanis
m invo
lvingthe bridging dpa
ligands. This
magnetic interaction can be considered as an extension to the three a
ligned Cu
IIato
ms of the we
ll-docu
mented exchange coup
ling observed in carboxy
lato-bridged dinuc
lear copper co
mpounds.Broken-sy
mmetry ca
lcu
lations with approxi
mate spin projection adequate
ly reproduce the coup
ling constant observedfor
1. Oxidation of
1 re
moves an e
lectron fro
m the
magnetic orbita
l located on the centra
l Cu ato
m and its
ligandenviron
ment;
1+ disp
lays a
much weaker antiferro
magnetic interaction coup
ling the ter
mina
l Cu-N
4 moieties viafour
ligand pathways converging through the
x2-
y2 orbita
l of the centra
l meta
l. The si
lver ho
mo
logues of
1 and
1+disp
lay si
mi
lar e
lectronic ground states, but the ca
lcu
lated
magnetic coup
lings are stronger by factors of about 3and 4, respective
ly, resu
lting fro
m a better over
lap between the
meta
l centers and their equatoria
l ligand environ
mentwithin the
magnetic orbita
ls.