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[
iPr2TpCu]2(m-N2) unit is completed by an inversion center
ꢁ
through the center of the N N bond. A single N2 molecule is
captured in between two CuI centers to give an end-on
ꢁ
binding mode (Molecule A: Cu N 1.829(3); Molecule B:
ꢁ
1.822(3) ꢀ) with a just slightly lengthened N N bond distance
(Molecule A: 1.112(5); Molecule B: 1.110(6) ꢀ) compared to
free dinitrogen (1.0975 ꢀ). Each unique copper center of 3
adopts a pseudo-tetrahedral environment (t = 0.774 and
0.770; idealized tetrahedral geometry t = 1)[18] with three
very similar Cu-NTp bond lengths (Molecule A: 2.026(3),
2.033(3), 2.046(3); Molecule B: 2.016(3), 2.025(3), 2.050-
(3) ꢀ). This pseudo C3 coordination environment at Cu
renders the highest energy Cu d orbitals essentially degener-
ate to maximize their interaction with the degenerate N2 p*
orbitals (Figure 4). This idealized C3 structure is in marked
contrast to many tris(pyrazolyl)borate copper(II) complexes
Figure 2. Tris(pyrazolyl)borate copper dioxygen (a and b) and diaze-
ne (c) adducts along with a tricopper dinitrogen complex (d).
2299 cmꢁ1).[16c] Copper coordination polymers contain parti-
ally reduced N2 supporting ligands (nN2 = 1607 cmꢁ1) have
been prepared recently.[7b] Murray reported a seminal copper
coordination complex featuring N2 as a ligand in 2014
(Figure 2d). It takes advantage of a strongly donating tris(b-
diketiminato) ligand which upon incorporation of three CuI
ions, binds N2 in an unusual trimetallic manner with a reason-
ably activated N2 ligand (nN2 = 1952 cmꢁ1) that is kinetically
stabilized by the cryptophane binding pocket formed by the
linked b-diketiminate ligands.[7a] Herein, we present the
isolation of the first example of an end-on, molecular
dicopper dinitrogen complex [Cu]2(m-1,2-N2) and its forma-
tion from a mixed valence, dicopper monohydride [Cu]2(m-
H).
that often feature two short and one long Cu NTp bonds.[19]
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Although this dicopper dinitrogen complex 3 is stable in the
solid state at ꢁ408C for an extended period, it decays in
solution (CH2Cl2 or toluene) over minutes at room temper-
ature, converting to several untraceable products. Colorless
crystals of 3 slowly crack with gas evolution upon standing at
room temperature.
To unequivocally establish the identity of the trapped
diatomic molecule between the two copper centers in 3,
a solid state sample of 3 was subjected to Raman spectros-
copy. The assignment of the bound dinitrogen stretching
frequency was confirmed through the preparation of 15 N
labelled [iPr2TpCu]2(m-15N2) (3-15N2) under an 15N2 atmos-
phere. Raman difference spectra of 3 (Figure S1B in the
Supporting Information) clearly identify nN2 at 2130 cmꢁ1
(14N2) and 2060 cmꢁ1 (15N2), approximately 200 cmꢁ1 lower
than free 14N2 (2331 cmꢁ1). While the bound N2 ligand in 3 has
a higher nN2 stretching frequency than in Murrayꢁs tricopper
dinitrogen complex Cu3N2L (1952 cmꢁ1),[7a] it is significantly
lower than more weakly bound N2 ligands in copper-
exchanged zeolites such as Cu-ZSM-5 (2295, 2207 cmꢁ1).[16a,e,f]
Simple MO considerations supported by high-level DFT
calculations outline the nature of the [CuI]-N2-[CuI] inter-
action in [iPr2TpCu]2(m-N2) (3). The effective C3 coordination
of the tris(pyrazolyl)borate ligand renders the dyz and dxz
orbitals on the d10 TpCuI fragment degenerate (Figure S22).
This leads to degenerate p-backbonding interactions between
the filled Cu dyz and dxz orbitals and the empty p* levels of the
N2 ligand in the mononuclear TpCu-N2 complex (Figure 4 and
S22). Due to the low energies of the Cu d orbitals, weak p-
backbonding is expected. Interaction with an additional
TpCuI fragment allows for p-backbonding from two trigonal
d10 CuI centers, presumably enhancing the overall copper-
dinitrogen interaction.[4c,5a,6a,20] This simple MO analysis,
however, illustrates that the set of filled dyz/dxz orbitals
brought in by the additional TpCuI fragment is non-bonding
with respect to the N2 p* orbitals. Thus, only modest
enhancement in the copper-dinitrogen interaction is antici-
pated.
The previously reported, blue [iPr2TpCu]2(m-OH)2 was
prepared by mixing a 1m KOH aqueous solution with
iPr2TpCu(NO3) in toluene under an inert atmosphere.[17]
Reaction of [iPr2TpCu]2(m-OH)2 with two equiv Ph3SiH at
ꢁ208C in dichloromethane led to several color changes,
starting from a blue solution that transitioned through purple
and green before becoming colorless with precipitation of
colorless crystals. X-ray crystallography reveals that this
colorless product is [iPr2TpCu]2(m-1,2-N2) (3; Figure 3), iso-
lated in 38% yield. The asymmetric unit of 3 consists of two
crystallographically independent halves in which each
Figure 3. Crystal structure of [iPr2TpCu]2(m-N2) (3), selected bond
lengths [ꢀ] and angles [8] (Molecule A shown). Molecule A: N13-N13’
1.112(5), Cu1-N13 1.829(3), Cu1-N1 2.033(3), Cu1-N3 2.026 (3), Cu1-
N5 2.046(3); N13’-N13-Cu1 177.0(4); Molecule B: N14-N14’ 1.110(6),
Cu2-N14 1.822(3), Cu2-N7 2.050(3), Cu2-N9 2.025(3), Cu2-N11 2.016-
(3); N14’-N14-Cu2 174.7(4). Pink B, dark blue N, light blue Cu.
DFT
[BP86 + GD3BJ/6-311 ++ G(d,p)/SMD-CH2Cl2/
BP86/6-31 + G(d)/gas] calculations on the mono- and dicop-
per adducts iPr2TpCu-N2 (4) and [iPr2TpCu]2(m-N2) (3) support
ꢁ
these simple MO considerations. The calculated N N dis-
2
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2016, 55, 1 – 6
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