Angewandte
Communications
Chemie
sharp shape of 1H- and 19F-NMR-signal sets for [HB(C6F5)3]À
are indicative of complete consumption of B(C6F5)3 in these
mixtures.
First, a phosphine adduct to the SnIV dihydrostannyl
cation [Ar*SnH2(PtBu3)]+ (1) is formed. Only a few phos-
phine adducts to stannylium ions are known.[12] The NMR
spectra characteristically feature a doublet signal at dH =
5.90 ppm for the two Sn-bonded hydrides. These split up to
2
a doublet arising from a JP-H coupling of 40 Hz and further
1
reveal 119/117Sn satellites with a JSn-H coupling constant of
2100/2008 Hz. This coupling constant is almost 180 Hz greater
than that observed for the parent neutral Ar*SnH3; an
Figure 1. ORTEP of [Ar*Sn(PtBu3)]+ (2). Thermal ellipsoids are set at
50% probability and protons, the counteranion, and lattice benzene
are omitted for clarity. Canonical frontier molecular orbitals at an
isodensity value of. 0.05 are shown. Selected distances [ꢂ] and
angles [8]: Sn–P 2.7071(3), Sn–C1 2.1876(12); closest Sn-ortho-CTrip of
the two Trip groups 3.27/3.35; P-Sn-C1 113.38(3), C4-C1-Sn 158.0(1).
HOMO–LUMO gap: 5.610 eV.
increase that may be rationalized by a higher Sn s-orbital
1
share in the Sn H bonding. The H-coupled 119Sn NMR signal
À
appears at dSn = À340 ppm as a triplet, corroborating the
constitution of a Sn atom with two hydrogen atoms attached
(further splitting from a small 1JSn-P coupling is not resolved).
The shift is in the range of tetra-substituted stannanes and the
predicted 119Sn chemical shift for a computationally deter-
mined structure of this cation is in reasonable agreement
(dSn,calcd = À382 ppm). The 31P NMR signal for [Ar*SnH2-
(PtBu3)]+ (1) is observed at dP = 72.1 ppm with tin satellites
revealing a very small 1JSn-P coupling of only 32 Hz which is an
order of magnitude smaller than in [Me3PSnMe3]+.[12c] The
formation process of 1 resembles Burfordꢀs approach to
stannylphosphonium cations.[12c]
phenomenon for ArSnX and usually rationalized by steric
effects.[16] The P-Sn-C angle amounts to 113.38(3)8. From the
combination of a large R-E-(L) angle for a cationic [RE(L)]+
species we anticipate further interesting reactivity.[14a,17] The
flanking Trip groups mildly tilt over towards the cationic tin
center indicating weak arene interactions. The Sn–arene
distances are comparable to those computationally predicted
for [Ar’Sn(MeNHC)]+ (Ar’ = 2,6-Mes2C6H3-, Mes = 2,4,6-
Me3C6H2-).[18] However, computational probing reveals a sig-
nificant impact on the 119Sn NMR shift (Figure 2) and there-
The second compound formed in the reaction is assigned
to the phosphine adduct to the SnII cation [Ar*Sn(PtBu3)]+
(2). It reveals a 119Sn NMR resonance at dSn = 1420 ppm as
a doublet due to strong 1JSn-P coupling of about 1990 Hz, in the
range known for P–SnII compounds.[13] The downfield shift is
indicative of dicoordinate SnII compounds and the computa-
tionally predicted 119Sn NMR shift (dSn,calcd = 1387 ppm) is in
excellent agreement with the experimental data. No further
splitting of the signal is observed in 1H-coupled spectra,
confirming that all hydrogen atoms have been removed from
the Sn. 31P NMR spectroscopy reveals a signal at dP =
95.0 ppm with the respective tin satellites. The drastic increase
1
of JSn-P coupling constants upon reductive dehydrogenation
from [Ar*SnH2(PtBu3)]+ (1) to [Ar*Sn(PtBu3)]+ (2) by almost
two orders of magnitude may mark the differing nature of the
Figure 2. Computational examination of the arene interaction on the
119Sn NMR shift on hypothetical [ArSn(PtBu3)]+ derivatives. Structural
modifications have been made to the optimized [Ar*Sn(PtBu3)]+
structure and the shifts were directly computed on the basis of these
structures without further re-optimization. Shifts dSn are given in parts
per million, relative to tetramethylstannane.
À
P Sn bond in these species. The Sn–P coupling behaves invers
1
À
to couplings of the Sn H moiety where JSnIV-H is often one
order of magnitude bigger than 1JSnII-H. For neutral phosphinyl
1
stannylenes a JSn-P coupling of around 1450 Hz was repor-
ted.[13a]
A
31P-EXSY-NMR experiment only revealed chem-
ical exchange of the free phosphine with [Ar*Sn(PtBu3)]+ (2),
but not with [Ar*SnH2(PtBu3)]+ (1) on the examined NMR
time scale.
fore strongly indicates an electronic interaction.[18] Flanking
arene interactions in Group 14 cations have been observed
previously.[19] Attempts to obtain crystals of [Ar*SnH2-
(PtBu3)]+ (1) from the reaction mixtures only yielded color-
less needles of phosphonium hydridoborate [HP(tBu)3][HB-
(C6F5)3].[1c]
X-ray diffraction studies revealed the molecular structure
of 2 with the phosphine being arranged almost symmetrically
between the two flanking Trip-groups (Trip = 2,4,6-iPr3C6H2-;
Figure 1). Compound 2 represents an example of the rare
structural motif of cationic, dicoordinate tetrylenes.[14] An
example of phosphine adducts to cationic SnII transition metal
According to 31P NMR spectroscopy, the initial integra-
tion ratio of 2/1/PtBu3/[HPtBu3]+ is (roughly) 1.3:2:1:2.[20]
These mixtures were formed within a couple of minutes and
only slowly showed some further conversions and partial
decomposition over several days. Small amounts of dehydro-
coupling product Ar*H2SnSnH2Ar* were formed under
complexes is known.[15] The Sn P bond of 2.7071(3) ꢁ is fairly
À
long compared to a neutral phosphino stannylene Ar*SnP-
(SiMe3)2 (2.527(1) ꢁ).[13a] The tin atom strongly deviates (ca.
228) from the central phenyl plane, which is an established
2
ꢀ 2017 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2017, 56, 1 – 6
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