4914
Inorg. Chem. 1997, 36, 4914-4915
Synthesis and X-ray Crystal Structure Determination of the First Lanthanide Complexes Containing
Primary Phosphide Ligands: Ln[P(H)Mes*]2(thf)4 (Ln ) Yb, Eu)
Gerd W. Rabe,*,† Ilia A. Guzei,‡ and Arnold L. Rheingold‡
Anorganisch-chemisches Institut, Technische Universita¨t Mu¨nchen, Lichtenbergstrasse 4, 85747 Garching, Germany,
and Department of Chemistry, University of Delaware, Newark, Delaware 19716
ReceiVed April 11, 1997
As part of an effort to investigate the coordination chemistry
of the lanthanides with phosphide ligand systems as well as
the corresponding bonding aspects, we now extended our
systematic studies toward the reactivity of divalent lanthanide
iodide1 complexes of the general formula LnI2(thf)2 (Ln ) Yb,
Eu) with the potassium salt of a primary phosphane, namely
KP(H)Mes* (Mes* ) 2,4,6-tBu3C6H2).2 Earlier work has
demonstrated that different structural types of secondary phos-
phide derivatives of the lanthanides3,4 can be prepared and
structurally characterized.
We now report the synthesis and crystal structure determi-
nation of two novel phosphide derivatives of the lanthanides of
the general formula Ln[P(H)Mes*]2(thf)4 (Ln ) Yb (1), Eu (2)).
LnI2(thf)2 (Ln ) Yb, Eu) reacts immediately with 2 equiv of
KP(H)Mes* in tetrahydrofuran at room temperature to give
complexes 1 and 2, respectively, in 60% yield. Interestingly,
1 and 2 are formed using both a 1:1 and a 1:2 ratio of reagents.
Crystals of both orange-yellow 1 and bright yellow 2 were
obtained from toluene/thf/pyridine at -30 °C.
in 1 range from 76.3(2) to 108.5(1)° (76.0(3) to 111.2(2)° for
the corresponding angles in 2). The molecular structures of
complexes 1 and 2 resemble the structural motif that we
observed earlier in lanthanide bis(phosphido) complexes of the
general formula Ln[PR2]2(L)4 (L ) thf, N-methylimidazole).3g-i
The Yb-P distance in the molecular structure of 1 is 3.025
(2) Å. It can be compared, e.g., with the Yb-P distances in
Yb[PPh2]2(thf)4 (2.991(2) Å)3g and in bis(η5-2,5-diphenylphos-
pholyl)Yb(thf)2 (2.959(1) Å)4b and also with the corresponding
distances reported for the divalent ytterbium phosphinomethanide
complex {(thf)Li[C(PMe2)2(SiMe3)]}2‚YbI2(thf) (2.96(1)-
3.08(1) Å)6 and the tertiary phosphane adducts of divalent
Yb[N(SiMe3)2]2[Me2PCH2CH2PMe2] (3.012(4) Å)7 and trivalent
Yb(C5Me5)2Cl[Me2PCH2PMe2] (2.941(3) Å).8
(5) Crystal data for 1‚2thf: C60H108O6P2Yb, Mr ) 1160.44, monoclinic,
C2/c, a ) 22.4646(3) Å, b ) 19.2702(1) Å, c ) 18.7672(3) Å, â )
126.325(1)°, V ) 6545.5(1) Å3, Z ) 4, Fcalc ) 1.178 g cm -3, F(000)
) 2464, Mo KR radiation (λ ) 0.710 73 Å), T ) 222(2) K, µ(Mo
KR) ) 1.520 mm-1. A total of 11 459 reflections were collected on
a Siemens P4/CCD diffractometer for a yellow crystal with ap-
proximate dimensions 0.55 × 0.10 × 0.10 mm3 in the range 3.1° e
2θ e 56.3°; 6920 reflections were independent, and 5927 reflections
were considered observed. The structure was solved by direct methods
and refined by full-matrix least-squares calculations based on F2 to
final residuals of R1 ) 0.0447 and wR2 ) 0.1308 for 5927 observed
data (I > 2σ(I)) and GOF ) 1.036. Minimal/maximal residual electron
density: 0.888/ -0.692 e Å-3. Crystal data for 2‚2thf: C60H108EuO6P2,
Mr ) 1139.36, monoclinic, C2/c, a ) 22.2985(3) Å, b ) 19.2553(4)
Å, c ) 18.7396(4) Å, â ) 126.290(1)°, V ) 6485.4(2) Å3, Z ) 4,
The molecular structures of 1 and 2 were determined
crystallographically5 as formally hexacoordinated Ln[P(H)-
Mes*]2(thf)4 (Figure 1, Ln ) Yb). Additionally, two tetrahy-
drofuran solvent molecules are present in both crystal lattices.
It is interesting to note that the presence of pyridine is essential
for a successful induction of crystal growth of 1 and 2.
However, pyridine molecules are neither coordinated to the
metal center nor incorporated in the crystal lattice. This
observation is certainly surprising in light of the fact that
pyridine is a stronger base than tetrahydrofuran. Additional
confirmation for the absence of pyridine was obtained from both
F
calc ) 1.169 g cm -3, F(000) ) 2436, Mo KR radiation (λ ) 0.710 73
Å), T ) 222(2) K, µ(Mo KR) ) 1.061 mm-1. A total of 10 619
reflections were collected on a Siemens P4/CCD diffractometer for a
yellow crystal with approximate dimensions 0.55 × 0.40 × 0.40 mm3
in the range 3.1° e 2θ e 56.6°; 5966 reflections were independent,
and 3648 reflections were considered observed. The structure was
solved by direct methods and refined by full-matrix least-squares
calculations based on F2 to final residuals of R1 ) 0.0816 and wR2 )
0.2002 for 3648 observed data (I > 2σ(I)) and GOF ) 1.024. Minimal/
maximal residual electron density: 1.308/-1.453 e Å-3. The function
1
the H NMR and the 13C NMR spectra of crystals of 1 in
tetrahydrofuran-d8.
The isomorphous molecular structures of 1 and 2 display
distorted octahedral environments around the lanthanide cation,
situated at an inversion center, with the two -[P(H)Mes*]
ligands in trans positions (with a P-Yb-P angle of
162.54(6)° and a P-Eu-P angle of 160.5(1)°, respectively).
The deviation from ideal octahedral geometry can best be seen
by examing the interligand angles. The L-Yb-(cis L) angles
minimized was R(wF2) ) ∑[w(Fo - Fc )2]/∑[(wFo )2]1/2, R ) ∑∆/
∑(Fo), ∆ ) |(Fo - Fc)|. The systematic absences in the diffraction
data were consistent for space groups C2/c and Cc. E statistics
suggested the centrosymmetric space group, C2/c, which yielded
chemically reasonable and computationally stable results of refinement.
The structures were solved using direct methods, completed by
subsequent difference Fourier syntheses and refined by full-matrix
least-squares procedures. Structures 1 and 2 are isomorphous. The
complex molecules are each located on a 2-fold axis. The asymmetric
unit also contains a solvent molecule of tetrahydrofuran. In order to
model disorder in the free molecule of THF, it was constrained to the
same geometry as one of the coordinated tetrahydrofuran ligands. One
2
2
2
† Technische Universita¨t Mu¨nchen.
‡ University of Delaware.
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1999.
(2) Rabe, G. W.; Yap, G. P. A.; Rheingold, A. L. Inorg. Chem. 1997, 36,
1990 and references cited therein.
(3) (a) Rabe, G. W.; Riede, J.; Schier, A. J. Chem. Soc., Chem. Commun.
1995, 577. (b) Rabe, G. W.; Ziller, J. W. Inorg. Chem. 1995, 34, 5378.
(c) Rabe, G. W.; Riede, J.; Schier, A. Organometallics 1996, 15, 439.
(d) Rabe, G. W.; Riede, J.; Schier, A. Inorg. Chem. 1996, 35, 40. (e)
Rabe, G. W.; Riede, J.; Schier, A. Inorg. Chem. 1996, 35, 2680. (f)
Rabe, G. W.; Yap, G. P. A.; Rheingold, A. L. Inorg. Chem. 1997, 36,
3212. (g) Rabe, G. W.; Yap, G. P. A.; Rheingold, A. L. Inorg. Chem.
1995, 34, 4521. (h) Rabe, G. W.; Riede, J.; Schier, A. Main Group
Chem. 1996, 1, 273. (i) Rabe, G. W.; Yap, G. P. A.; Rheingold, A. L.
Inorg. Chim. Acta, in press.
peak from the final difference map of 2 that remained, 1.22 e Å-3
,
was 0.63 Å from the metal and was considered noise. All non-hydrogen
atoms were refined with anisotropic displacement coefficients. The
hydrogen atom on phosphorus was located, and its thermal parameter
was refined while the P-H distance was constrained to 1.400(2) Å.
All other hydrogen atoms were treated as idealized contributions. All
software and sources of scattering factors are contained in the
SHELXTL (5.3) program library (G. Sheldrick, Siemens, XRD,
Madison, WI). Atomic coordinates, bond distances and angles, and
thermal parameters of 1 and 2 have been deposited at the Cambridge
Crystallographic Data Centre (Depository No. CSD-100132).
(6) Karsch, H. H.; Ferazin, G.; Steigelmann, O.; Kooijman, H.; Hiller,
W. Angew. Chem., Int. Ed. Engl. 1993, 32, 1739.
(4) (a) Nief, F.; Ricard, L. J. Organomet. Chem. 1994, 464, 149. (b) Nief,
F.; Ricard, L.; Mathey, F. Polyhedron 1993, 12, 19. (c) Atlan, S.;
Nief, F.; Ricard, L. Bull. Soc. Chim. Fr. 1995, 132, 649.
(7) Tilley, T. D.; Andersen, R. A.; Zalkin, A. J. Am. Chem. Soc. 1982,
104, 3725.
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