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DOI: 10.1039/C7CC06372E
COMMUNICATION
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value agrees better with the range from experiment (79 to 87
Hz, sign not determined).
This CTP geometry explains why the complex
±
MoH(PMePh2)(SAr)3, Ar = 2,4,6-iPr3C6H2 readily reacts with
pyridine to give the complex MoH(PMePh2)(py)(SAr)3, Ar =
2,4,6-iPr3C6H2,7 now known to have
a capped trigonal
bipyramidal (CTB) geometry9 with the pyridine across from the
hydride and the phosphorus at a small angle to the hydride,
producing a 2JHP of 87 Hz (eq 1).
Figure 2. The structure of MoH(PMe3)(SAr)3 with all of the hydrogens on the ligands
and all of the carbons apart from the ipso carbons removed. Selected bond distances
(Å) and angles (°): Mo(1)-H(12) 1.65, Mo(1)-P(6) 2.37, Mo(1)-S(2) 2.34, Mo(1)-S(4) 2.36,
Mo(1)-S(8) 2.33; H(12)-Mo(1)-P(6) 54.1, H(12)-Mo(1)-S(2) 73.5, H(12)-Mo(1)-S(8) 84.6,
P(6)-Mo(1)-S(2) 115.0, P(6)-Mo(1)-S(4) 84.6, P(6)-Mo(1)-S(8) 91.3, S(2)-Mo(1)-S(4)
112.9, S(4)-Mo(1)-S(8) 121.1, S(8)-Mo(1)-S(2) 121.6.
The original proposal for the sulfur-carbon bond cleavage of
Figure 1 was that the hydride would attack the carbon;8
however this would involve isotope exchange with the hydride
The molybdenum in MoH(SAr)3(PRPh2) was proposed to be
in a trigonal bipyramidal geometry with the hydride trans to
the phosphine ligand on the basis of the observation in the
2
NMR spectra of a large JHP coupling constant ranging from 79
to 87 Hz between the hydride, detected at 3.3 ppm for one of
the compounds, and the phosphorus nuclei.7, 8 However DFT
calculations
using
a
slightly
simplified
structure
(Mo(PMe3)(H)(SAr)3, Ar = 2,6-Me2C6H3) now provide strong
evidence that the most stable isomer of these complexes has
molybdenum in an unprecedented distorted capped trigonal
pyramidal (CTP) geometry (Figure 2).
In this diamagnetic, five coordinate complex the
molybdenum sits 0.3 Å above the middle of a distorted triangle
defined by the three sulfur atoms (Figure 2). The phosphorus
is at the vertex of the distorted S3P trigonal pyramid with the
short Mo-P bond (2.37 Å) at a 78° angle to the S3 basal plane.
The hydride ligand caps one PS2 face of this CTP with a small
2
HMoP angle of 54.1°. Thus the large JHP is associated with this
small angle between these nuclei. There are no distortions of
the PMe3 ligand that would indicate bonding favouring 5-
coordinate phosphorus. The HOMO is a lone pair with
approximately (dxz)2(Mo) character, out of phase with a (pz)2
lone pair on S8 (see the SI) where the x direction is along the
Mo-S8 bond and the z direction is between the Mo-H and Mo-
P
bonds. None of the 620 five-coordinate complexes
containing a terminal hydride found in the Cambridge
Structural Database has such a CTP geometry. Two isomers
with the hydride approximately trans to the phosphorus in a
distorted trigonal bipyramidal (TBP) geometry were located as
stable minima at 10 and 13 kcal/mol higher in energy and a
distorted trigonal bipyramidal complex in the triplet state was
located at 5 kcal/mol higher in energy. Even the model
complex Mo(PMe3)(H)(SMe)3 with much smaller substituents
that was not observed and our DFT studies could not find a
suitable transition state for the hydride attack. The methanol
that is needed to trigger this cleavage reaction (Figure 1) can
easily coordinate to give a formally Mo(IV) methanol complex
as shown in eq 1. From this experimentally unobserved
methanol adduct, the C-S bond is readily cleaved in an
on the sulfurs adopts this CTP geometry.
Apparently
molybdenum is large enough to accommodate ligands cis to
each other, thus avoiding trans H-Mo-P and H-Mo-S bond
2
weakening. The JHP (unscaled) were calculated using the
Figure 3. (a) The methanol adduct MoH(PR3)(OHMe)(SAr)3 (Mo(1)-H(22) 1.66, Mo(1)-
P(13) 2.39, Mo(1)-O(15) 2.21, Mo(1)-S(2) 2.36, Mo(1)-S(4) 2.33, Mo(1)-S(17) 2.36,
O(15)-H(16) 0.97, S(4)-C(5) 1.78 Å; H(22)-Mo(1)-P(13) 52.1, H(22)-Mo(1)-O(15) 148.5,
P(13)-Mo(1)-O(15) 158.7, Mo(1)-S(4)-C(5) 113.0°); (b) the hydrogen transfer transition
state (OH…CSMo) (1635i cm-1; Mo(1)-H(22) 1.66, Mo(1)-P(13) 2.45, Mo(1)-O(15) 2.07,
Mo(1)-S(2) 2.37, Mo(1)-S(4) 2.20, Mo(1)-S(17) 2.38, O(15)-H(16) 1.21, S(4)-C(5) 2.14,
gauge-independent atomic orbital method as -70 Hz for the
CTP geometry and -31 Hz for the TBP geometry. The former
H(16)-C(5) 1.33 Å; H(22)-Mo(1)-P(13) 54.3, H(22)-Mo(1)-O(15) 146.7, P(13)-Mo(1)-O(15)
157.7, Mo(1)-S(4)-C(5) 107.1°); (c) the sulfido product MoH(S)(PR3)(OMe)(SAr)2.HAr
This journal is © The Royal Society of Chemistry 20xx
2 | J. Name., 2012, 00, 1-3
(Mo(1)-H(22) 1.65, Mo(1)-P(13) 2.56, Mo(1)-O(15) 1.93, Mo(1)-S(2) 2.40, Mo(1)-S(4)
2.14, Mo(1)-S(17) 2.42 Å; H(22)-Mo(1)-P(13) 54.8, H(22)-Mo(1)-O(15) 145.6, P(13)-
Mo(1)-O(15) 155.7° plus HAr (C(5)-H(16) 1.10 Å).
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