Here we report the molecular structures and reactivities of the two co
mplexes [{Cu(O2CPh)dppm}2] (A) and [{Cu(O2CPh)dppm}2].H2O (B), contain
ing isomeric dibenzoato copper(I) moieties doubly bridged by dppm liga
nds (dppm=bis(diphenylphosphino)methane). In the isomeric unit [{Cu(O2
CPh)dppm}2] of B, the two metal atoms are also bridged by one of the t
wo benzoato ligands and a significant shortening of the transannular C
u ... Cu distance (2.994(2) angstrom in B versus 3.359(2) angstrom in
A) is observed. The eight-membered Cu2P4C2 ring adopts an approximate
chair conformation in A and a saddle conformation in B. The structures
of A and B have been determined by single crystal X-ray diffraction m
ethod. The crystals of A are triclinic, space group P1BAR, with Z = 1
in a unit cell of dimensions a = 11.841(2), b = 11.366(2), c = 10.769(
2) angstrom, a = 100.68(2), beta = 101.45(2) and gamma = 93.37(2)-degr
ees. The crystals of B are monoclinic, space group P2(1)/a, with Z=4 i
n a unit cell of dimensions a=21.295(3), b = 13.295(2), c = 22.068(3)
angstrom and beta = 114.72(2)-degrees. Final R was 0.032 (2553 reflect
ions) for A and 0.058 (3909 reflections) for B. Bulky anions react wit
h A and B metathetically removing one of the benzoato groups or, when
coordinating, both of them. The characteristics of the new anions modu
late the conformation of the Cu2(dppm)2 unit. Thermally stimulated dep
olarization current (TSDC) measurements have also been performed on B
to study the electric polarization phenomena induced by reorientation
of dipole moments of the crystallization water molecules in the temper
ature range 100 less-than-or-equal-to T less-than-or-equal-to 350 K. T
he reorientation ability of the dipole water molecules is probably fav
oured by the dynamic disorder of the atoms, which surround the water m
olecules in the crystal lattice.