Md. Fryzuk et al., MAGNETIC EXCHANGE IN DINUCLEAR CHROMIUM(II) COMPLEXES - EFFECT OF BRIDGING CHLORIDES AND BRIDGING HYDRIDES IN ANTIFERROMAGNETIC COUPLING, Inorganic chemistry, 33(24), 1994, pp. 5528-5534
The preparation, solid-state structures, and magnetic properties of tw
o new Cr(II) amido diphosphine complexes are described. Reaction of th
e lithium salt LiN(SiMe(2)CH(2)PPh(2))(2) with CrCl2.THF results in th
e formation of the dinuclear chloride-bridged species {[(Ph(2)PCH(2)Si
Me(2))(2)N]Cr}(2)(mu-Cl)(2), 1. This complex is paramagnetic at room t
emperature with a magnetic moment corresponding to four unpaired elect
rons per chromium; however, as the temperature is lowered, magnetic su
sceptibility measurements show that 1 exhibits antiferromagnetic behav
ior with J = -12.4 cm(-1) and g = 1.99. Chloride 1 can be converted to
the mononuclear methyl complex CrMe[N(SiMe(2)CH(2)PPh(2))(2)] by reac
tion with MeLi. Under a hydrogen atmosphere, the methyl complex is con
verted to the dinuclear hydride derivative {[(Ph(2)PCH(2)SiMe(2))(2)N]
Cr}(2)(mu-H)(2), 3. A variable temperature magnetic susceptibility stu
dy shows that this species is very strongly antiferromagnetically coup
led with J = -139 cm(-1) and g = 1.98. The magnetic coupling correlate
s with the Cr-Cr distances observed in the solid state for these compl
exes: for 1, the Cr-Cr distance is 3.64 while for the hydride 3 a much
shorter distance of 2.641 Angstrom is found. Crystals of {[(Ph(2)PCH(
2)SiMe(2))(2)N]Cr}(2)(mu-Cl)(2), 1, are triclinic, a = 11.508(2) Angst
rom, b = 12.267(3) Angstrom, c = 13.096(2) Angstrom, alpha = 90.80(2)d
egrees, beta = 112.91(1)degrees, gamma = 109.52(2)degrees, Z = 1, and
space group P $($) over bar$$ 1; those of {[(Ph(2)PCH(2)SiMe(2))(2)N]C
r}(2)(mu-H)(2), 3, are monoclinic, a = 11.776(1) Angstrom, b = 19.061(
2) Angstrom, c = 13.990(2) Angstrom, beta = 103.153(10)degrees, Z = 2,
and space group P2(1)/n. The structures were solved by direct (chlori
de) and Patterson (hydride) methods and were refined by full-matrix le
ast-squares procedures to R = 0.064 and 0.038 (R(w) = 0.037 and 0.039)
for 1832 and 3617 reflections with I greater than or equal to 3 sigma
(I), respectively.