Angewandte
Chemie
5.465–5.548 ꢀ, whereas those in 3 are 5.266–5.314 ꢀ; overall,
therefore, the Y3As3 core of 3 is more compact than that of 2.
replacing the para and Cp’ methyl groups with hydrogen
atoms. Geometry optimizations employing two exchange
correlation functionals were carried out in the gas-phase and
using a continuum dielectric, and the results of the calcu-
lations with the hybrid PBE0 functional, including dielectric
effects, are described.
À
Relative to 2, a broader range of Y C bond lengths, that is,
À
2.59(2)–2.731(6) ꢀ, and a greater average Y C bond length
of 2.67 ꢀ, are found in 3. The distortion of the Y3As3 chair
À
conformation in 3 is reflected in the As-Y-As and Y-As Y
À
bond angles of 91.59(2)–94.87(2)8 and 133.59(2)–136.49(2)8,
respectively. The lithium cation in 3 is ligated by three
arsinidene ligands and resides 0.889(8) ꢀ above the mean
Comparing the calculated and experimental Y As bond
lengths, we find good agreement for 1 (3.113 ꢀ vs. 3.095 ꢀ)
but also that the calculations slightly overestimate the average
distance for 2 (3.061 ꢀ vs. 2.998 ꢀ) and for 3 (2.912 ꢀ vs.
2.872 ꢀ). The discrepancies are most likely due to the
inability of the simulations to fully account for solid-state
intermolecular interactions, and also the effects of the counter
cations on 3. Despite this, the overall trend in the decrease of
À
plane of the arsenic atoms. The Li As bond lengths are
2.539(8), 2.563(7) and 2.615(8) ꢀ, and the As-Li-As angles
are 107.2(3), 108.2(3) and 110.0(3)8. An ortho methyl group
on one mesityl substituent is oriented towards Li1, and the
relatively short Li1···C54 distance of 2.777(8) ꢀ may indicate
an agostic interaction similar to that observed in other lithium
complexes containing CH2R substituents (R = H, alkyl,
silyl).[23]
À
the Y As bond length is reproduced. The atomic charges
were calculated by natural bond orbital (NBO) and quantum
theory of atoms in molecules (QTAIM) analyses (Table 1).
The 1H NMR spectrum of [Li(thf)4]2[3]·thf, recorded
30 min after sample preparation in [D8]thf at 298 K (Support-
ing Information, Figure S6), features two resonances at
d(1H) = 6.71 and 6.80 ppm, both of which integrate to three
protons and correspond to two types of mesityl meta CH
environments. The Cp’ CH protons occur as four resonances
at d(1H) = 6.44, 6.15, 5.07, and 4.85 ppm, each of which
integrates to six protons. Distinct singlets for the ortho, para,
and Cp’ CH3 environments were observed in the region
d(1H) = 1.54–2.62 ppm. The appearance of the 1H NMR
spectrum of [Li(thf)4]2[3]·thf is therefore consistent with the
arsinidene complex possessing a C3 symmetry axis coincident
with Li1 and approximately perpendicular to the Y3 plane.
The 7Li NMR spectrum of [Li(thf)4]2[3]·thf features two
resonances, with a sharp peak at d(7 Li) = À1.64 ppm corre-
sponding to the [Li(thf)4]+ cations and a broader peak at
d(1H) = 4.41 ppm corresponding to the {LiAs3} environment
in [Li(thf)4]2[3]·thf (Supporting Information, Figure S8). An
additional feature of the 1H NMR spectrum of [Li-
(thf)4]2[3]·thf is that, over time, additional resonances which
were observed as minor components after 30 min grow in
intensity (Supporting Information, Figure S7). After a period
of only two hours, the additional resonances account for
a significant component of the NMR spectrum. It was not
possible to identify the decomposition products; however, this
unexpected feature suggests that the arsinidene ligands in
[Li(thf)4]2[3]·thf react with the thf solvent.
À
Table 1: Experimental and calculated Y As bond lengths, atomic charges
(q) for 1–3, and QTAIM-derived topological parameters at the bond
critical points.
1
2
3
[a]
[b]
À
Y As [ꢀ]
3.0945(6)
3.113
+1.09, +0.42
+1.89, +0.86
35.86, 30.36
0.024
2.998[c]
3.061[c]
2.8722[c]
2.912[c]
+1.13, À0.53
+1.82, À0.81
35.89, 32.20
0.038
À
Y As [ꢀ]
qNBO (Y/As)
+1.26, À0.10
+1.85, +0.03
35.89, 31.30
0.030
q
QTAIM (Y/As)
lQTAIM
1
H
d(Y,As)
À0.00577
À0.0338
À0.0592
0.200
0.302
0.438
[a] Experimental. [b] PBE0+COSMO. [c] Average length.
lQTAIM =localization index, 1=electron density (e bohrÀ3), H=energy
density (a.u.), d=delocalization index.
Both types of analysis show an increasing negative charge on
the arsenic donor atom on moving from 1 to 2 to 3. The
QTAIM-derived localization index, l, which provides a mea-
sure of the number of electrons localized on a given atom,
increases by 0.94 from 1 to 2, and again by 0.90 from 2 to 3.
The analogous parameters for yttrium are essentially constant
across the three complexes, which indicates that the observed
À
decrease in Y As bond lengths is due to stronger ionic
interactions. However, the fact that the calculations produce
Dl < 1 implies a small-but-increasing non-ionic contribution
as the negative charge on arsenic increases.
To the best of our knowledge, complex 3 is the first rare-
earth metal complex of an arsinidene ligand, which is
surprising given that arsinidene ligands are well-known in
transition-metal chemistry.[24] Several alkali metal complexes
of arsinidene ligands have also been structurally character-
ized.[25] Complex 3 is related to the rare-earth metal
phosphinidene complexes, particularly the heterobimetallic
À
The Y As bonding was investigated further by a topolog-
ical analysis of the electron density. The parameter 1, which
describes the electron density at the QTAIM-derived bond
critical point (BCP), increases from 1 to 2 to 3, as expected
based on the decreasing Y As bond lengths, and which is
consistent with the change in l. The 1 values indicate an
À
lithium–scandium
complex
[(PNP)Sc(m-dmp)(m-Br)Li]
À
(PNP = N(2-iPr2PC6H3-4-Me)2, 2,6-Mes2C6H3, dme = dime-
thoxyethane).[10] Notably, the arsinidene ligands in 3 adopt
a m-bridging coordination mode, which is an obvious parallel
with rare-earth metal phosphinidene complexes.
The variation in the character of the yttrium–arsenic
bonding in complexes 1, 2, and 3 was investigated using
density functional theory: the calculations were simplified by
enhancement in the non-ionic contribution to the Y As
bonding in the arsinidene complex 3; however, the values are
still markedly less than expected for a typical covalent bond
(1 > 0.2). The values of the energy density (H) at the BCP, and
the values of the delocalization indices (d), which provides
a measure of the number of electrons shared between yttrium
and arsenic, are indicative of considerable ionic bonding
Angew. Chem. Int. Ed. 2015, 54, 1 – 5
ꢀ 2015 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
3
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