We report the synthesis and comprehensive study of the electronic structure of a unique series of dinuclear group 5 cyclo-tetraphosphide inverted sandwich complexes. White phosphorus (P4) reacts with niobium(III) and tantalum(III) β-diketiminate (BDI) tert-butylimido complexes to produce the bridging cyclo-P4 phosphide species {[(BDI)(N(t)Bu)M]2(μ-η(3):η(3)P4)} (1, M = Nb; 2, M = Ta) in fair yields. 1 is alternatively synthesized upon hydrogenolysis of (BDI)Nb(N(t)Bu)Me2 in the presence of P4. The trinuclear side product {[(BDI)NbN(t)Bu]3(μ-P12)} (3) is also identified. Protonation of 1 with [HOEt2][B(C6F5)4] does not occur at the phosphide ring but rather involves the BDI ligand to yield {[(BDI(#))Nb(N(t)Bu)]2(μ-η(3):η(3)P4)}[B(C6F5)4]2 (4). The monocation and dication analogues {[(BDI)(N(t)Bu)Nb]2(μ-η(3):η(3)P4)}{B(Ar(F))4}n (5, n = 1; 6, n = 2) are both synthesized by oxidation of 1 with AgBAr(F). DFT calculations were used in combination with EPR and UV-visible spectroscopies to probe the nature of the metal-phosphorus bonding.
We report the synthesis and comprehensive study of the electronic structure of a unique series of dinuclear group 5 cyclo-tetraphosphide inverted sandwich complexes. White phosphorus (P4) reacts with niobium(III) and tantalum(III) β-diketiminate (BDI) tert-butylimidocomplexes to produce the bridging cyclo-P4 phosphide species {[(BDI)(N(t)Bu)M]2(μ-η(3):η(3)P4)} (1, M = Nb; 2, M = Ta) in fair yields. 1 is alternatively synthesized upon hydrogenolysis of (BDI)Nb(N(t)Bu)Me2 in the presence of P4. The trinuclear side product {[(BDI)NbN(t)Bu]3(μ-P12)} (3) is also identified. Protonation of 1 with [HOEt2][B(C6F5)4] does not occur at the phosphide ring but rather involves the BDI ligand to yield {[(BDI(#))Nb(N(t)Bu)]2(μ-η(3):η(3)P4)}[B(C6F5)4]2 (4). The monocation and dication analogues {[(BDI)(N(t)Bu)Nb]2(μ-η(3):η(3)P4)}{B(Ar(F))4}n (5, n = 1; 6, n = 2) are both synthesized by oxidation of 1 with AgBAr(F). DFT calculations were used in combination with EPR and UV-visible spectroscopies to probe the nature of the metal-phosphorus bonding.
Since its discovery
in the middle of the 17th century, elemental
phosphorus has fascinated chemists. Even still, novel allotropes of
this element continue to be discovered and studied.[1] Among these, white phosphorus (P4) is readily
available as the direct product of reduction of phosphate minerals[2] and could be used directly as a building block
for synthesizing a wide array of phosphorus-containing inorganic and
organic products. Currently, most industrial processes involve molecular
phosphoruschlorination or oxychlorination to PCl and POCl3 before derivatization.[3,4] The
development of environmentally friendly and atom-efficient strategies
for the direct functionalization of P4 to organo-phosphorus
products, polyphosphoruscages, and other P-containing inorganic derivatives
is therefore highly desirable.A classic methodology for activating
white phosphorus involves
using well-identified or in situ generated reduced metalcomplexes.[5−17] Depending on the reducing ability, nature, and coordination environment,
a wide array of metal–phosphide species can be generated.[3,4,18−20] Despite several
recent achievements in the subsequent transformation of these activated
metal–phosphorus species,[7,21−28] direct incorporation of P atoms from P4 under mild conditions
both stoichiometrically and catalytically remains a great challenge
for contemporary main group and transition metal organometallicchemists.
This notably requires a deeper understanding of the nature of the
metal–phosphide interaction and the reaction processes involved.To date, the formation of square-planar cyclo-tetraphosphide
species from P4 has only been observed on rare occasions.[8,29−33] Examples of compounds containing a cyclo-tetraphosphide
motif bridging two metal ions in a symmetrical fashion, also known
as cyclo-P4 inverted sandwiches, remain
extremely limited, and their chemical properties are almost unexplored.
Reported examples of bimetallic inverted sandwiches are neutral and
of general formula [LM]2(μ-P4). They were obtained either from reduction of P4 by low-valent metal species (uranium[32,33] or zirconium[8]) or upon reduction of alkali phosphides[34] and diphosphane[35] by alkali metals dissolved in liquid ammonia (M = K, Rb, Cs). More
recently, Cummins et al. also reported the formation of {[(ODipp)3Nb]2(μ-η3:η3P4)} (Dipp = 2,6-iPr2C6H3) by P abstraction from a niobium triphosphide
precursor.[36] Several tetraphosphane organic
derivatives were also described.[37−39]Recently, we identified
new trivalent group 5 imido complexes supported
by the bulky 2,6-diisopropylphenyl-β-diketiminate (BDI) ligand.[40,41] These species exhibit an extensive and rich reduction chemistry,
including semihydrogenation of alkynes[42] and activation of C–F bonds,[43,44] arenes,[45] and azides[46] through
unusual pathways. In continuation of this work, we targeted the use
of the unsaturated “(BDI)Nb=NtBu”
fragment to achieve early transition metal pnictide complexes. Herein
we investigate the reactivity of these Nb and Ta low-valent precursors
with white phosphorus. The formation and chemistry of rare diniobium
and ditantalum cyclo-P4 inverted sandwich
complexes isolable in three different charge states are described.
Structural, spectroscopic, and density functional theory (DFT) studies
aiming at comparing and determining the precise electronic structure
of this series of molecules are also presented.
Results and Discussion
Reaction of the trivalent [(BDI)(NtBu)M(CO)2] (M = Nb, Ta) dicarbonyl precursors[40,41] with white
phosphorus afforded the dinuclear inverted sandwich complexes {[(BDI)(NtBu)M]2(μ-η3:η3P4)} (1, M = Nb; 2, M = Ta) as bright green (1) and blue (2) crystalline materials in fair yields (Scheme 1). The reaction, performed in benzene at 60 °C, proceeded
faster in the case of niobium (6 vs 24 h, respectively, for M = Nb
vs Ta), which can be attributed to a higher dissociation barrier of
the metal–carbonyl bond in the case of Ta. The reaction proceeded
faster under UV irradiation, with {[(BDI)(NtBu)Ta(CO)2] being converted to 2 in 2 h at room temperature.
However, in that case the isolated yield was decreased to 34% due
to the formation of several byproducts, as gauged by NMR spectroscopy.
Scheme 1
Synthesis of Complexes 1 and 2 from the
Dicarbonyl Precursors [(BDI)(NtBu)M(CO)2] (M
= Nb, Ta)
The Nb:P4 ratio had no influence on the reaction, and
similar results were obtained when 2:1 to 1:2 Nb:P4 ratios
were used. Both species are air-stable and were characterized by ES-MS
spectrometry, elemental analysis, UV–vis, and 1H
and 13C NMR spectroscopy. The 1H and 13C NMR patterns for 1 and 2 are consistent
with highly symmetric diamagnetic species in solution. Despite several
attempts performed at various temperatures (−40 to +50 °C),
we were unable to locate 31P NMR resonances in the −1000
to +1500 ppm range for either complex in solution. Gratifyingly, the
solid-state 31P MAS NMR spectrum recorded at 293 K for 1 displayed two sets of signals (δiso = +251(2)
and +84(2) ppm with large chemical shift anisotropy; see Supporting Information (SI)), corresponding to
the two non-equivalent P atoms in the cyclo-P4 ligand, in agreement with the asymmetric μ-η3:η3 coordination mode observed by X-ray crystallography
(see below). In contrast, the previously reported {[(ODipp)3Nb]2(μ-η3:η3P4)} complex featured a sharp singlet resonance
at +124 ppm in its solution 31P{1H} NMR spectrum.[26] Analysis of the solid-state 31P MAS
NMR spectrum for 2 was more difficult because of substantial
line-broadening, and we were only able to identify one type of signal
at δiso = +208(8) ppm (see SI).The solid-state molecular structures of 1 and 2, determined by single-crystal X-ray diffraction, are shown
in Figure 1, and metrical parameters are presented
in Table 1. In both cases, the dimeric {[(BDI)(NtBu)M]2(μ-η3:η3P4)} (M = Nb, Ta) unit lies on a crystallographically
imposed center of symmetry located in the center of the metal–metal
axis. Two independent molecules are found in the asymmetric unit for 1, and the following discussion uses averaged metrical parameters.
The P4core is nearly a perfect square plane with 0°
P–P–P–P torsion angles, P–P–P angles
of 88.86(3)° and 88.83(2)° for 1 and 2, respectively, and almost identical P–P single bonds.
The average P–P bond distances found for 1 and 2 (2.233(3) and 2.248(5) Å, respectively) compare well
with those recently reported for (N2P2Zr)2(P4) (2.240(1) Å)[8] and (DippO3Nb)2(P4) (2.23(2)
Å),[36] formally described as containing cyclo-P44– cores. In contrast,
shorter P–P distances are found in formally dianioniccyclo-P42– rings in Cs or U
complexes (2.14–2.17 Å, see Results and
Discussion below).[32,35] The tetraphosphorus
ring is sandwiched between the two metalcations in an unsymmetrical
fashion, as expressed by the strong dissymmetry between the M–P
distances with, for each metalcenter, one short (Nb1–P1 =
2.511(1) Å in 1; Ta1–P1 = 2.5007(1) Å
in 2) and two average (Nb1–P2 = 2.700(1) Å;
Nb1–P2A = 2.702(2) Å in 1; Ta1–P2
= 2.6918(1) Å; Ta1–P2A = 2.6748(1) Å in 2) metal–phosphorus bond distances. The remaining M–P
interaction, located trans to the metal imido moiety,
is considered as non-bonding with much longer M–P separation
(2.845(1) and 2.8179(1) Å for 1 and 2, respectively), attributed to the trans influence
of the imido ligand. Therefore, the coordination mode of the cyclo-P4 ligand is best described as μ-η3:η3. Interestingly, the metal···metal
separation is shorter in the case of tantalum (4.2993(1) Å in 2) compared to niobium (4.3605(1) Å in 1) and reflects a greater covalent interaction of the tantalum metalcenters with the cyclo-P4core. The metrical
parameters within the (BDI)M(NtBu) unit are unremarkable
and similar to those found in related complexes.[40,41,45,47]
Figure 1
Solid-state
molecular structures of 1 (top) and 2 (bottom).
Hydrogen atoms and diisopropyl aryl groups of
the BDI ligands have been removed, and tBu moieties have
been truncated for clarity. Niobium (light blue), tantalum (green),
phosphorus (orange), nitrogen (blue), and carbon (gray) atoms are
represented with 50% probability ellipsoids. Selected metrical parameters
are reported in Table 1.
Table 1
Selected Metrical Parameters for Compounds 1, 2, and 4–6 Derived
from X-ray Crystallography Data
compd
P–P
[Å]
P–P–P [deg]
M–P
[Å]
M···M
[Å]
Nb=NtBu [Å]
Nb–NBDI [Å]
1
2.233(3)
88.86(3)
2.51–2.85
4.3605(1)
1.779(2)
2.192(6)
2
2.248(5)
88.83(2)
2.50–2.82
4.2993(1)
1.7912(1)
2.177(7)
4
2.235(2)
88.72(8)
2.52–2.79
4.298(1)
1.775(8)
2.265(6)
5
2.209(4)
89.62(6)
2.59–2.87
4.4929(7)
1.774(4)
2.15(2)
6
2.182(5)
88.9(2)
2.69–2.89
4.61(4)
1.768(6)
2.10(1)
Solid-state
molecular structures of 1 (top) and 2 (bottom).
Hydrogen atoms and diisopropyl aryl groups of
the BDI ligands have been removed, and tBu moieties have
been truncated for clarity. Niobium (light blue), tantalum (green),
phosphorus (orange), nitrogen (blue), and carbon (gray) atoms are
represented with 50% probability ellipsoids. Selected metrical parameters
are reported in Table 1.The reaction between [(BDI)(NtBu)M(CO)2]
(M = Nb, Ta) and P4 was also attempted in the presence
of B(C6F5) in an effort to trap intermediate
species, but similar results were obtained.A more convenient
route to 1 involves the hydrogenolysis
of the easily accessed bis-dimethyl precursor (BDI)Nb(NtBu)Me2[47] in the presence of
P4 (Scheme 2). The product precipitated
from n-hexane solvent to afford 1 in
moderate yield after filtration and recrystallization from toluene.
Our group has previously shown that the hydrogenation of (BDI)Nb(NtBu)Me2 reductively eliminates methane and generates
highly reactive low-coordinate Nb(III) intermediates of the general
formula “(BDI)Nb(NtBu)” that can be trapped
in the presence of π-acidic ligands such as CO or arenes.[40,45] Therefore, it is likely that the formation of 1 involves
the reduction of P4 by these low-valent Nb intermediates
generated in situ.
Scheme 2
Formation of 1 and 3 from Hydrogenation
of [(BDI)(NtBu)Nb(Me)2] in the Presence of P4
The moderate yield
of 1 is explained by the formation
of several phosphorus-containing byproducts. However, even if the
reaction does not exclusively yield {[(BDI)(NtBu)M]2(μ-η3:η3P4)}, 1 is the main product of the reaction.
This selectivity may be partially driven by the relative inertness
of compound 1 (see below), which, together with its poorer
solubility, facilitates its isolation.The remaining dark green
filtrate contained several byproducts,
as gauged by NMR spectroscopy. Notably, the 1H NMR spectrum
exhibited several signals in the 4.8–5.4 ppm range, corresponding
to the HC(C(Me)NAr)2 protons of several
BDI-Nb species. The 31P NMR spectrum displayed a complicated
pattern of resonances between −162 and +184 ppm, attesting
that several phosphorus-containing species are formed. Unfortunately,
these species exhibited similar solubility and co-crystallized in
common solvents (n-hexane, benzene, toluene, HMDSO,
OEt2); despite several attempts, their separation in preparative
scale was unsuccessful, preventing their full analysis.Even
so, fractional recrystallization of the n-hexane
reaction mixture at −40 °C produced a microcrystalline
material whose analysis by ES-MS spectroscopy indicated the presence
of a high-nuclearity species, 3, with a molecular peak
at m/z = 1698.2800 corresponding
to [{[(BDI)NbNtBu]3(P12)}-BDI]+. The formation of a trinuclear species was corroborated by
the 1H NMR spectrum, which displayed three resonances integrating
for one proton each at 5.36, 5.30, and 4.96 ppm and corresponding
to three independent BDI ligands within the same molecule.Analysis
by X-ray diffraction revealed a system composed of 12
phosphorus atomscapped by three (BDI)Nb=NtBu fragments
(Figure 2) of the general overall formula {[(BDI)NbNtBu]3(μ-P12)} (3). The architecture of the P12 core is unprecedented
and can be seen as a P7 cage featuring a nortricyclane-type
structure, reminiscent of the well-documented heptaphosphide Zintl
anion [P73–],[48−51] connected to a five-membered cyclo-P5 ring. The P–P bond distances
vary between 2.146(1) and 2.290(1) Å. These metric values are
comparable to those of other known phosphidecages and are in agreement
with simple P–P bonds.[51−53] The Nb–P bond lengths
range between 2.560(1) and 2.648(1) Å and are shorter in the
case of Nb3 (mean Nb–P distance value for Nb3 = 2.564(6) vs
2.62(2) Å for Nb1 and Nb2), which is expected given a lower coordination
number for Nb3compared to those of Nb1 and Nb2.
Figure 2
Solid-state molecular
structure of 3. Hydrogen atoms
and methyl groups from the tBu and iPr moieties
are omitted for clarity. Niobium (light blue), phosphorus (orange),
nitrogen (blue), and carbon (gray) atoms are represented with 50%
probability ellipsoids. Selected bond distances [Å] and angles
[°]: Nb1–P1 2.622(1), Nb1–P2 2.623(1), Nb1–P3
2.648(1), Nb2–P1 2.623(1), Nb1–P3 2.575(1), Nb1–P4
2.622(1), Nb3–P11 2.569(1), Nb3–P9 2.560(1), Nb1–N1
1.747(3), Nb1–N2 2.206(3), Nb1–N3 2.182(3), Nb2–N4
1.763(3), Nb2–N5 2.188(3), Nb2–N6 2.198(3), Nb3–N7
1.754(3), Nb3–N8 2.234(3), Nb3–N9 2.220(3), P–P
bond length range 2.146(1)–2.290(1).
Solid-state molecular
structure of 3. Hydrogen atoms
and methyl groups from the tBu and iPr moieties
are omitted for clarity. Niobium (light blue), phosphorus (orange),
nitrogen (blue), and carbon (gray) atoms are represented with 50%
probability ellipsoids. Selected bond distances [Å] and angles
[°]: Nb1–P1 2.622(1), Nb1–P2 2.623(1), Nb1–P3
2.648(1), Nb2–P1 2.623(1), Nb1–P3 2.575(1), Nb1–P4
2.622(1), Nb3–P11 2.569(1), Nb3–P9 2.560(1), Nb1–N1
1.747(3), Nb1–N2 2.206(3), Nb1–N3 2.182(3), Nb2–N4
1.763(3), Nb2–N5 2.188(3), Nb2–N6 2.198(3), Nb3–N7
1.754(3), Nb3–N8 2.234(3), Nb3–N9 2.220(3), P–P
bond length range 2.146(1)–2.290(1).Phosphorus has a proclivity for homoatomic bonding,[51−54] and activation of P4 by transition metal species can
lead to various P (n > 4) species upon aggregation of smaller fragments. However,
clusters
of nuclearity above n = 7 are obtained only on very
rare occasions.[4,18] To date, only two other P12 clusters possessing different topologies have been described.
Bertrand reported the high-yield synthesis of a HNC-capped P12 cluster from P4,[55] and the
structure of the trinuclear cobalt {(Cp′)Co]3(μ-P12)} (Cp′ = 1,2,4-tBuC5H2) complex was elucidated from 31P NMR spectroscopy by
Scherer et al.[56] In the present case, 1 was found unreactive toward P4, and 3 is therefore not the result of P4 incorporation into 1. Unfortunately, separation of 3 from the other
reaction byproducts failed in our hands, preventing further analysis
of this compound.In an attempt to find a more efficient method
for the preparation
of compound 2, we investigated the hydrogenolysis of
the tantalum dimethyl complex (BDI)Ta(NtBu)Me2 in the presence of P4. However, the outcome was quite
different from that observed for its Nb counterpart. Indeed, the major
product of the reaction was the cyclometalated tantalum hydride species
{ArNC(Me)CHC(Me)N-[2-(CHMeCH2)-6-Pr-C6H3]}Ta(NBu)H, as assayed by NMR spectroscopy, similar to what we previously
reported for the same reaction performed in the absence of white phosphorus.[41]
Reactivity Studies
Compound 1 is fairly
robust and can be handled in air either in the solid state or in solution.
The cyclo-P4 ring was not hydrogenated
in the presence of H2 and was not displaced by strong π-acidic
ligands such as CO.In order to determine if the coordinated cyclo-P4 exhibited basic properties, we explored
the reaction of 1 with 2 equiv of [HOEt2][B(C6F5)4]. The reaction produced a new compound
formulated as {[(BDI#)Nb(NtBu)]2(μ-η3:η3P4)}[B(C6F5)4]2 (4), in which the BDI backbone
has been protonated (Scheme 3, BDI# = [ArNC-(Me)]2CH2). Compound 4 can be isolated in high yields as pink crystals. Because of its
ion-pair formulation, 4 has poor solubility in hydrocarbon
solvents, Et2O, CH2Cl2, and CHCl3, but is fairly soluble and stable in (CH2Cl)2. In addition, 4 was found to decompose in polar
coordinating solvents such as THF or pyridine to yield a complex mixture
of unidentified products. Protonation of the BDI ligand was confirmed
by the 1H NMR spectrum for 4, which displays
two doublets at 5.44 and 4.68 ppm (2JHH = 16.7 Hz) that couple in the 1H–1HCOSY NMR spectrum, corresponding to the two diastereotopicCH2 protons in H2C(C(Me)NAr)2.
Scheme 3
Formation of 4 (Ar = 2,6-Diisopropylphenyl; ArF = Pentafluorophenyl)
Further confirmation of the molecular structure of 4 was obtained by single-crystal X-ray crystallography. The
structure
consists of ion pairs with two BArF counteranions balancing
the charge of the {[(BDI#)(NtBu)Nb]2(μ-η3:η3P4)}2+ dicationiccomplex shown in Figure 3. Selected metrical parameters are given in Table 1. The CH2 protons in H2C(C(Me)NAr)2 were located from the Fourier
difference map and refined isotropically. The H2C(C(Me)NAr)2 ligand core is no longer planar, with
the sp3-hybridized methylene carbon lying at 0.51(1) Å
below the plane defined by the two C=N imino moieties. The
C=N bond lengths are short (1.286(6) Å), in agreement
with localized double imine bonds. As a consequence of the β-diketiminate
protonation, the interaction between the niobiumcenter and the neutral
BDI# ligand is weakened compared to that found in 1, with longer Nb–N bond distances in 4 (2.265(6) Å) than in 1 (2.192(6) Å). This
results in a stronger Nb-cyclo-P4 interaction
in 4, as shown by the shorter Nb···Nb
separation (4.298(1) Å in 5 vs 4.3605(1) Å
in 1), while the geometry of the tetraphosphoruscore
is essentially unchanged, with similar phosphorus–phosphorus
bond distances and angles in 1 and 4 (see
Table 1). The average Nb=NtBu imido bond length in 5 (1.775(8) Å) is similar
to that found for 1.
Figure 3
Solid-state molecular structures of 4 (top), 5 (middle), and 6 (bottom).
Hydrogen atoms are
not shown except for those of the methylene group of the protonated
BDI# ligand in 4, diisopropyl aryl groups
of the BDI ligands and B(C6F5)4 counteranions
have been removed, and tBu moieties have been truncated
for clarity. Niobium (light blue), phosphorus (orange), nitrogen (blue),
hydrogen (white), and carbon (gray) atoms are represented with 50%
probability ellipsoids. Selected metrical parameters are reported
in Table 1.
Solid-state molecular structures of 4 (top), 5 (middle), and 6 (bottom).
Hydrogen atoms are
not shown except for those of the methylene group of the protonated
BDI# ligand in 4, diisopropyl aryl groups
of the BDI ligands and B(C6F5)4counteranions
have been removed, and tBu moieties have been truncated
for clarity. Niobium (light blue), phosphorus (orange), nitrogen (blue),
hydrogen (white), and carbon (gray) atoms are represented with 50%
probability ellipsoids. Selected metrical parameters are reported
in Table 1.To probe possible nucleophilicity, 1 was treated
with
acyl chlorides but did not react and was not affected by the strong
Lewis acid B(C6F5)3. Overall, the
lack of reactivity of the cyclo-P4 unit
with Brønsted and Lewis acids might reflect the poor basicity/nucleophilicity
of the tetraphosphide in 1, but this may as well be a
kinetic effect due to the steric protection provided by the bulky
BDI ligands; note that we previously reported analogous behavior with
the arene inverted sandwich complex {[(BDI)Nb(NtBu)]2(μ-η6:η6C6H6)}.[45]Although the niobiumcenters in 1 can formally be described as d0 metalcenters, the overall molecule
should be considered electron-rich and can therefore be easily oxidized.The reaction between 1 and 1 equiv of Ag[B(C6F5)4] proceeded quickly at room temperature
in toluene and afforded an insoluble dark green material. Complex
{[(BDI)(NtBu)Nb]2(μ-η3:η3P4)}{B(C6F5)4} (5) was isolated in 77% yield upon extraction
of the solid residue with α,α,α-trifluorotoluene
and crystallization by n-hexane layering. In return, 5 could be quantitatively reduced back to 1 using
1 equiv of bis(cyclopentadienyl)cobalt(II) (as assayed by 1H NMR spectroscopy, Scheme 4). The 1H NMR spectrum for 5 displays several broad, unassignable
features from −0.8 to +8.9 ppm that remain broad over the −50
to +60 °C temperature range, and no 31P NMR signals
could be located. This is attributed to the paramagnetic nature of
this S = 1/2 radical species
(see EPR study below).
Scheme 4
Redox Chemistry of 1
The two-electron oxidation
product, {[(BDI)(NtBu)Nb]2(μ-η3:η3P4)}{B(C6F5)4}2 (6), was isolated in 64%
yield from an analogous reaction
performed with greater than 2 equiv of the silver oxidizing agent.
This ion-pair compound is insoluble in most conventional solvents. 6 is either poorly soluble or reactive with most solvents,
but it is sufficiently stable in α,α,α-trifluorotoluene
to obtain 1H and 31P NMR spectra. The 1H NMR spectrum for 6 features the expected BDI resonances
for a symmetric diamagnetic species in solution. Contrary to 1, 6 displays a sharp singlet resonance in its 31P NMR spectrum at +516 ppm, which indicates that all the
phosphorus atoms of the cyclo-P42– moiety are equivalent on the NMR time scale. This resonance is shifted
significantly downfield compared to that of the previously reported
M2P4 species (δ = +331–348 ppm
for M = K, Rb, Cs).Interestingly, the choice of the counteranion
of the Ag(I) salt
turned out to be crucial: use of Ag[BF4] in place of Ag[B(C6F5)4] resulted in a complex mixture
of products, as gauged by 1H NMR spectroscopy. Analysis
of the reaction mixture by 19F NMR showed a broad resonance
centered at +83 ppm which corresponds to the previously reported Nb(V)
difluoride species [(BDI)(NtBu)NbF2].[47] This likely arises from fluoride abstraction
from tetrafluoroborate by a cationic Nb species. Alternatively, when
triflate was used in place of the non-coordinating tris-pentafluoroborate
anion, the pentavalent niobium triflate species [(BDI)(NtBu)Nb(OTf)2] (7) was isolated as yellow crystals
in 24% yield. Compound 7 was fully characterized by multinuclear
NMR spectroscopy, elemental analysis, IR, and X-ray diffraction (see SI). The formation of 7 most likely
involves a reactive intermediate which undergoes ligand exchange in
the presence of coordinating triflate anions. However, attempts to
isolate or characterize by 31P NMR the byproduct(s) were
unsuccessful.Here we consider it appropriate to draw a parallel
between the
present cyclo-P4 inverted sandwich species
and the related benzene inverted sandwich species {[(BDI)Nb(NtBu)]2(μ-η6:η6-C6H6)}, which is best described as
a diniobium(III) complex with strong Nb–arene back-donation.[45] In the latter case, and contrary to what is
observed for 2, we observed that the two-electron oxidation
is irreversible and the arene-bridged complex decomposes.[57] This difference in reactivity can be ascribed
to a stronger interaction and stronger orbital overlap with the cyclo-P4 ring vs C6H6.
This is also consistent with the fact that benzene does not displace
CO in the dicarbonyls [(BDI)(NtBu)M(CO)2] (M
= Nb, Ta), while P4 does.
Structural Comparisons
The isolation of a family of
closely related systems in several charge states provides a rare opportunity
for comparing their structures and physicochemical properties. Both 5 and 6 were structurally characterized by single-crystal
X-ray diffraction (Figure 3). As in the structure
of 1, each niobium atom in 5 and 6 is coordinated by a bidentate (BDI) ligand, a (NtBu)
imido fragment bound in a terminal fashion, and a planar η3:η3-bridging cyclo-P4 ring perpendicular to the Nb–Nb axis. The three structures
differ in their charge state, resulting in the presence of one and
two BArF counterions in the structures of complexes 5 and 6, respectively.In Table 1, the most relevant structural parameters for the cyclo-P4 species 1, 2, and 4–6 are reported. The geometry
of the P4 motif is an almost perfect square plane across
the series, with P–P–P angles close to 90 °C (see
Table 1). The P–P bond lengths within
each P4core show very little deviation, and therefore
the discussion is based on an averaged value for each species. Comparison
of the P–P distances shows very significant differences: specifically,
the average P–P bond length is almost identical (within esd’s)
in 1 and 4 (2.234 Å), both containing
a formally cyclo-P44– core, but is shortened by around 0.03 Å in 5 (2.209(4)
Å) and by another 0.03 Å in 6 (2.182(5) Å).
Such distances compare well to those found in other systems containing
the reduced cyclo-P4 motif and seem diagnostic
of its formal charge state, with values ranging from 2.22 to 2.25
Å for tetraanionic rings[8,36] and from 2.14 to 2.20
Å for dianionic rings.[32,33,35] The degree of interaction between the metalcenter and the bridging
tetraphosphide is also very dependent on the oxidation state. Overall,
shorter Nb–P bond distances are found in the reduced species 1 compared to 6, although these span an extended
range because of the asymmetriccoordination mode of the P4core. This is best seen when comparing the Nb···Nb
separation, which increases significantly from 4.3605(1) Å in 1 to 4.4929(7) Å in 5 and 4.61(4) Å
in 6. This is compensated by a stronger donation from
the BDI backbone and, to a lesser extent, from the imido ligand to
the d0 metalcenters, as expressed by a shortening of the
Nb–NBDI distances (2.192(6) Å in 1 vs 2.10(1) Å in 6). Hence, as expected, the data
show that increasing the charge on the central cyclo-P4 ring results in a more contracted [Nb2P4] core.
Computational Analysis
Although
it is convenient to
refer to formal charges when describing these systems, the nature
of metal–phosphorus bonding is essentially covalent. We thus
turned to DFT calculations to get a better comprehension of their
electronic structure.Geometry optimizations were carried out
without any symmetry constraints on complexes 1, 2, 4–6 using the B3PW91 functional
(see SI for computational details). This
functional is found to correctly account for the structural features
of the five investigated complexes (see SI for metriccomparison with X-ray data). The maximum deviation of
the P–P bonds is around 0.04 Å, whereas the P–P–P
angles are perfectly reproduced. The unsymmetrical coordination of
P4 to the two metalcenters is also reproduced computationally.
Thus, these computational methods appear to be well suited to further
study the electronic and spectroscopic properties of these complexes
(see below). Since an unsymmetrical coordination of P4 to
the two Nb centers is found in 1, any attempt to analyze
atomiccharges is questionable. Thus, a NBO analysis was carried out.
Analysis of the Wiberg bond indexes (WBO) points in the direction
of formally Nb(V) metalcenters and a P44– ligand. Indeed, for one Nb center, two interactions with the BDI
ligand (WBO = 0.51), one interaction with the imido (WBO = 1.93),
and four interactions with the four phosphorus (WBO = 0.88, 0.64,
0.64, and 0.37) are found, as well as a weak Nb–Nb interaction
(WBO = 0.23).The analysis of the molecular orbitals in 1, 2, and 4 shows that the HOMO
is a δ-bonding
orbital involved in the covalent bonding between the metalcenters
and the P4 ring, while the electron density in the non-bonding
LUMO is essentially localized on metal d-orbitals. (See Figure 4 for a representation of the HOMO and LUMO orbitals
in 1.)
Figure 4
HOMO (left) and LUMO (right) orbitals of complex 1.
HOMO (left) and LUMO (right) orbitals of complex 1.In 5, the coordination
is slightly less strong, in
line with longer Nb–P bond distances. Indeed, for one Nb center,
the two interactions with the BDI ligand (WBO = 0.57) and the one
with the imido (WBO = 1.95) are equivalent (even slightly stronger)
to those in complex 1, but the four interactions with
the four phosphorus (WBO = 0.71, 0.52, 0.52, and 0.36) as well as
the Nb–Nb one (WBO = 0.12) are weakened.
EPR Spectroscopy
The room-temperature X-band EPR spectrum
of 5 was nicely resolved and could be satisfactorily
simulated: both experimental and simulated spectra are presented in
Figure 5. The spectrum is isotropic and is
defined by a single g value, giso = 2.041. The 19 equally spaced lines and splitting pattern
suggest that the spin is delocalized onto two equivalent Nb centers.
Accordingly, the spectrum was modeled with a hyperfine interaction
of 41.5 G, with two equivalent 93Nb nuclei (100% natural
abundance, I = 9/2). No evidence
for superhyperfine couplings with the I = 1/231P nuclei could be detected.
Figure 5
Room-temperature
liquid-solution (CF3C6H5) X-band
EPR spectrum of 5 (black line) and simulation
(red line). Hyperfine coupling constant: Aiso = 41.5 G (93Nb, 100% natural abundance, I = 9/2); giso =
2.041.
Room-temperature
liquid-solution (CF3C6H5) X-band
EPR spectrum of 5 (black line) and simulation
(red line). Hyperfine coupling constant: Aiso = 41.5 G (93Nb, 100% natural abundance, I = 9/2); giso =
2.041.Using DFT methods, it has been
possible to derive the spin density
of complex 5, which was computed as a doublet spin state,
yielding an extra α spin. The spin density is found to be mainly
located on the two Nb centers (more than 0.6 electron), with the remaining
0.4 electron delocalized over the different ligands. The spin density
is symmetrically distributed over the two Nb centers, in agreement
with the EPR experiment. This observation is in stark contrast to
that of {[(BDI)(NtBu)Nb]2(μ-C6H6)}{BArF}, where the single electron
is not delocalized equally onto both niobiums, resulting in a more
complex EPR signal.[57] The more isotropic
and equal distribution of the spin density in 5 suggests
better orbital overlap.
Optical Spectra
The optical spectra
of the formally cyclo-P44– species 1, 2 (recorded in toluene solution),
and 4 (recorded in dichloroethane) feature two types
of intense absorptions
(Figure 6). High-intensity (20 000 <
ε < 37 000 L·cm–1·mol–1) bands are observed in the UV region around 320 nm
that we attribute to intraligand π→π* transitions.
Additionally, 1, 2, and 4 display
strong absorption bands (29 000 < ε < 42 000
L·cm–1·mol–1) in the
visible region (λ = 645, 603, and 694 nm for 1, 2, and 4, respectively) responsible for the bright
colors of these molecules. Given their high intensities, it is unlikely
that these correspond to Laporte-forbidden d→d transitions.
Instead, we attribute these processes to phosphorus-to-metalcharge-transfer
transitions. The energy for this transition is strongly affected both
by the nature of the metalcenter (Ta vs Nb) and by the supporting
ligand (BDI vs BDI#) and is therefore a useful tool to
probe the nature of the metal–cyclo-P4 interaction.
Figure 6
Solution UV–visible absorption spectra (298 K)
of complexes 1 (bright green line, toluene), 2 (blue line,
toluene), 4 (fuchsia line, DCE), 5 (dark
green line, CF3C6H5), and 6 (purple line, CF3C6H5).
Solution UV–visible absorption spectra (298 K)
of complexes 1 (bright green line, toluene), 2 (blue line,
toluene), 4 (fuchsia line, DCE), 5 (dark
green line, CF3C6H5), and 6 (purple line, CF3C6H5).Time-dependent density functional theory (TD-DFT)
calculations
were carried out to further probe the nature of these transitions.
The calculated λmax values (see table in SI) are in good agreement with the experimental
values and correspond to a HOMO–LUMO excitation. Upon analysis
of the nature of the HOMO and LUMO orbitals involved in the excitation,
it appears that the transition can be described as a pseudo-charge
transfer between the cyclo-P4 ligand (HOMO)
and the metalcenters (LUMO). While 1 and 2 exhibit similar electron configurations, this transition for 2 is radically blue-shifted in comparison with that for 1. DFT shows an increased stabilization of the HOMO δ-bonding
orbital in the case of tantalum due to increased covalency, resulting
in a larger HOMO–LUMO gap in 2, as observed by
UV–visible spectroscopy. This is also in agreement with the
X-ray structural data, which show shorter Ta–P bonds in 2 than Nb–P bonds in 1 (see above).The optical spectrum for the radical cation species 5 features ligand π→π* transitions in the UV region
as well as a broad and intense (ε = 22 750 L·cm–1·mol–1) absorption band at
low energy (λ = 921 nm, Figure 6). The
nature of the frontier orbitals involved in this transition indicates
that there is an electronic rearrangement between the SOMO (mainly
based on a bonding Nb–P–P–Nb interaction) and
the LUMO (non-bonding interaction between the two Nb centers). As
a consequence of the depopulation of the Nb–P4–Nb
δ-bonding orbital, no such intense transition is observed in
the symmetric fully oxidized dication complex 6. Instead,
the absorption spectrum for 6 shows a broad feature centered
at λ = 522 nm (ε = 6160 L·cm–1·mol–1), corresponding to a transition from BDI-Nb bonding
orbitals (HOMO–10, HOMO–8) to the LUMO (non-bonding
interaction between one d-orbital located on each Nb).
Conclusions
We have shown that low-coordinate d2 Nb and Ta complexes
supported by a combination of imido and β-diketiminate ligands
result in a strong activation of P4 to yield unusual cyclo-tetraphosphide-bridged inverted sandwich complexes.
The structure of an unprecedented P12 cluster byproduct
was also determined. Interestingly, the reaction of [(BDI)Nb(NtBu)]2(μ-η3:η3P4) with [HOEt2][B(C6F5)4] was found to result in the protonation
of the BDI ligand rather than the phosphide ring.We have demonstrated
for the first time that the cyclo-P4 motif
can exist in various oxidation states within
the same system. Specifically, salts of the {[(BDI)(NtBu)Nb]2(μ-η3:η3P4)} (n = 1, 2) mono- and dication were isolated. This offered us the rare
opportunity to compare the physicochemical properties of a family
of structurally related compounds. The combined chemical, structural,
spectroscopic, and density functional theory analyses suggest that
the best description for these complexes is as high-valent Nb centers
with substantial covalent bonding with the cyclo-P4core. They also revealed that the metal–phosphorus
interaction was stronger for Ta than for Nb, and that it was weakened
upon oxidation. An increased reactivity is thus expected for the cationic
species reported in this work; studies aimed at determining the full
scope of reactivity of these species are currently being pursued.
In addition, future work will be directed toward the expansion of
these studies to encompass niobium imido systems supported by sterically
modified BDI as well as other bidentate ligands in order to elucidate
the role played by steric and electronic factors in the formation
and the kinetic stability of these species.
Experimental
Section
General Considerations
Unless otherwise noted, all
reactions were performed either using standard Schlenk line techniques
or in an MBraun inert atmosphere glovebox under an atmosphere of purified
nitrogen (<1 ppm of O2/H2O). Glassware and
cannulae were stored in an oven at ∼160 °C for at least
12 h prior to use. Toluene, n-hexane, THF, and benzene
were purified by passage through a column of activated alumina, stored
over 3 or 4 Å molecular sieves, and degassed prior to use. α,α,α-Trifluorotoluene
and dichloroethane were dried over P2O5, distilled
under reduced pressure, degassed, and stored over 4 Å molecular
sieves. C6D6 was dried over sodium/benzophenone,
and CDCl3 was dried over CaH2. The deuterated
solvents were then vacuum-transferred to a storage flask and degassed
before being stored over activated molecular sieves in a drybox. (BDI)(CO)2Nb(NtBu),[40] (BDI)(CO)2Ta(NtBu),[41] and (BDI)(Me)2Nb(NtBu)[47] were prepared
using literature procedures. White phosphorus (P4) was
prepared from red phosphorus thermolysis under vacuum.[58] All other reagents were acquired from commercial
sources and used as received. NMR spectra were recorded on Bruker
AV-300, AVQ-400, AVB-400, DRX-500, AV-500, and AV-600 spectrometers.
Chemical shifts were measured relative to residual solvent peaks,
which were assigned relative to an external TMS standard set at 0.00
ppm. 31P and 19F chemical shifts were referenced
to an external standard (Ph3PO for 31P set at
23 ppm and BF3·OEt2 for 19F
set at 0.00 ppm). 1H and 13C NMR assignments
were routinely confirmed by 1H–1HCOSY
and 1H–13C HSQC experiments. Samples
for UV–vis–NIR spectroscopy were prepared in a Schlenk-adapted
quartz cuvette and analyzed on a Varian Cary 50 scanning spectrophotometer.
The uncorrected melting points were determined using sealed capillaries
prepared under nitrogen on an Optmelt SRS. Elemental analyses were
performed either at the School of Human Sciences, Science Center,
London Metropolitan University, or at the College of Chemistry, University
of California, Berkeley. The X-ray structural determinations were
performed at CHEXRAY, University of California, Berkeley, on a Bruker
SMART APEX II QUAZAR diffractometer. Solution EPR spectra were collected
at 9.251 GHz (X-band) frequency at room temperature in CF3C6H5 using a Varian E-109 spectrometer equipped
with an E-102 microwave bridge. The EPR spectra were simulated and
optimized using WinSim.[59] Mass spectra
were acquired on a Finnigan LTQ FT mass spectrometer equipped with
an ESI source. THF and n-hexane solutions were prepared
and filtered in the glovebox and maintained under a nitrogen atmosphere
until injection in the spectrometer through a syringe pump. Mass spectra
were recorded over a mass range (m/z) of 400–2000 with a Fourier transform ion cyclotron resonance
(FT-ICR) MS detector, while MS/MS data were obtained with a linear
ion trap (LTQ) analyzer. The exact mass and experimental isotopic
profiles were compared in each case to the theoretical ones. Details
concerning X-ray diffraction analyses and DFT computational studies
are provided in the SI.
H2 (1 atm) was added to a 250 mL n-hexane
solution of [(BDI)(CH3)2Nb(NtBu)]
(2.28 g, 3.73 mmol, 1 equiv) and P4 (0.28
g, 2.23 mmol, 0.6 equiv). The reaction mixture immediately turned
green and then was stirred at room temperature for 12 h to give a
dark green suspension. The n-hexane fraction was
filtered, and the solid residue was recrystallized from toluene, giving 1 as a dark green crystalline solid (1.33 g, 1.03 mmol, 55%).
The dark green n-hexane solution was left to stand
at −40 °C overnight, producing a green microcrystalline
material. Analysis by 1H NMR (500 MHz, C6D6, 293 K) showed the formation of several byproducts and notably
three resonances at δ = 5.36 (s, 1H, HC(C(Me)NAr)2), 5.30 (s, 1H, HC(C(Me)NAr)2),
and 4.96 (s, 1H, HC(C(Me)NAr)2), attributed
to 4. Fractional recrystallization from n-hexane at −40 °C afforded dark green crystals of 4 suitable for X-ray diffraction. ES-MS: m/z = 1698.2800 [{[(BDI)NbNtBu]3(P12)}-BDI]+ (calcd for C70H109N7Nb3P12: 1698.2787). Successive
recrystallizations failed to separate 4 from co-crystallized
byproducts, preventing full analysis.
[HOEt2][B(C6F5)4] (117 mg, 0.155
mmol, 2 equiv) was added to an 8 mL α,α,α-trifluorotoluene
suspension of 1 (100 mg, 0.078 mmol, 1 equiv). The reaction
mixture was stirred for 1 h at room temperature and turned from turquoise
green to dark green. The mixture was then filtered to give a green
filtrate that was cooled at −40 °C and left standing overnight
in the freezer. This afforded pink crystals that were recovered, washed
with 2 × 1 mL of Et2O, and dried in vacuo to give 4 as a pink crystalline material (168 mg, 0.064
mmol, 82%). Single crystals suitable for X-ray diffraction were obtained
similarly. 1H NMR (400 MHz, C2H4Cl2:CDCl3 95:5, 293 K): δ = 7.05 (t, 4H, CHAr, 3JHH = 7.9 Hz), 6.90 (d, 4H, CHAr, 3JHH = 8.0 Hz), 6.79 (d, 4H, CHAr, 3JHH = 7.9 Hz), 5.44 (d, 2H, H2C(C(Me)NAr)2, 2JHH = 16.7 Hz),
4.68 (d, 2H, H2C(C(Me)NAr)2, 2JHH = 16.7 Hz), 2.80 (sept,
4H, CHMe2, 3JHH = 6.6 Hz), 2.71 (sept, 4H, CHMe2, 3JHH = 6.6 Hz), 2.29
(s, 12H, HC(C(Me)NAr)2), 1.57 (s, 18H,
NBu), 1.00 (dd, 24H,
CHMeMe, 3JHH = 6.6 Hz), 0.93 (d, 12H, CHMeMe, 3JHH = 6.6 Hz), 0.36 (d, 12H, CHMeMe, 3JHH = 6.6 Hz). 19F NMR (376 MHz, THF-d8, 293 K): δ
= −132.1, −162.6, and −166.5 (B(C6F5)4). FT-IR (cm–1): 2970
(w), 2847 (w), 1643 (w), 1620 (w), 1513 (m), 1455 (s), 1372 (m), 1322
(m), 1273 (m), 1204 (m), 1172 (m), 1132 (m), 1086 (s), 975 (s), 933
(w), 842 (w), 798 (m), 773 (m), 755 (m), 702 (m), 683 (m), 659 (m).
UV–vis (C2H4Cl2): λ1 = 694 nm (ε = 29 900 L·cm–1·mol–1), λ2 = 515 nm (ε
= 4250 L·cm–1·mol–1),
λ3 = 325 nm (ε = 19 900 L·cm–1·mol–1). Anal. Calcd for C114H102F40B2N6Nb2P4: C, 51.72; H, 3.88; N, 3.17. Found: C, 51.56;
H, 3.94; N, 3.11. mp: 221–223 °C.
{[(BDI)Nb(NtBu)]2(μ-η3:η3P4)}[B(C6F5)4]
(5)
A 3 mL THF solution of AgB(C6F5)4 (122 mg, 0.155 mmol, 1 equiv) was
added to a 20 mL toluene solution of 1 (200 mg, 0.155
mmol, 1 equiv). The reaction mixture was stirred for 1 h at room temperature.
The solids were recovered by filtration, washed with 1 mL of toluene,
and extracted with 3 × 2 mL of α,α,α-trifluorotoluene.
The dark green suspension was filtered, layered with 12 mL of n-hexane, and left standing at room temperature for 3 days.
This gave dark green crystals of 5 that were recovered,
washed with n-hexane, and dried in vacuo (236 mg, 0.120 mmol, 77%). Dark green block-shaped single crystals
suitable for X-ray diffraction were obtained similarly. The 1H NMR spectrum (600 MHz, CDCl3, 223 to 333 K) recorded
for this paramagnetic radical species features uninformative broad
signals in the −0.5 to +8.9 ppm range. FT-IR (cm–1): 2970 (w), 2882 (w), 1643 (w), 1514 (m), 1455 (s), 1352 (m), 1315
(m), 1258 (m), 1210 (m), 1178 (w), 1125 (w), 1085 (s), 1022 (w), 978
(s), 932 (m), 856 (s), 795 (s), 771 (s), 755 (s), 697 (m), 683 (m),
659 (m). UV–vis (CF3C6H5):
λ1 = 921 nm (ε = 22 750 L·cm–1·mol–1), λ2 = 655 nm (ε = 7060 L·cm–1·mol–1), λ3 = 435 nm (ε = 7100 L·cm–1·mol–1), λ4 = 372 nm (ε = 17 600 L·cm–1·mol–1), λ5 = 330 nm (ε = 31 500
L·cm–1·mol–1), λ6 = 296 nm (ε = 35 300 L·cm–1·mol–1). ES-MS: m/z = 1286.5074 [[(BDI)Nb(NtBu)]2(μ-η3:η3P4)]+ (calcd for
C66H100N6Nb2P4: 1286.5093). Anal. Calcd for C90H100F20BN6Nb2P4: C, 54.98; H, 5.13;
N, 4.27. Found: C, 55.08; H, 5.43; N, 4.06. mp: (decomp) 279–281
°C.
{[(BDI)Nb(NtBu)]2(μ-η3:η3P4)}[B(C6F5)4]2 (6)
A 2 mL THF solution
of AgB(C6F5)4 (92 mg, 0.117 mmol,
3 equiv) was added to a 20 mL toluene solution of 1 (50
mg, 0.039 mmol, 1 equiv). The reaction mixture was stirred for 1 h
at room temperature. The solids were recovered by filtration, washed
with 1 mL of toluene, and extracted with 24 mL of α,α,α-trifluorotoluene.
The dark purple suspension was filtered, layered with 50 mL of n-hexane, and left standing at room temperature for 2 days.
This produced dark purple needle-shaped crystals of 6 that were recovered, washed with n-hexane, and
dried in vacuo (66 mg, 0.025 mmol, 64%). Dark purple
needle-shaped single crystals suitable for X-ray diffraction were
obtained similarly. 1H NMR (600 MHz, CF3C6H5:C6D6 95:5, 293 K): resonances of aromatic protons could not be detected because of overlap
with solvent, δ = 6.90 (s, 2H, HC(C(Me)NAr)2), 2.96–2.88 (sept, 4H, CHMe2, 3JHH = 6.6 Hz), 2.68–2.61
(sept, 4H, CHMe2, 3JHH = 6.6 Hz), 2.18 (s, 12H, HC(C(Me)NAr)2), 1.26 (s, 18H, NBu), 1.10 (d, 24H, CHMeMe, 3JHH = 6.5 Hz), 1.05 (d, 12H, CHMeMe, 3JHH = 6.6 Hz),
0.62 (d, 12H, CHMeMe, 3JHH = 6.6 Hz). 19F NMR (376 MHz, CF3C6H5:C6D6 95:5, 293 K):
δ = −131.4, −162.8, and −166.5 (B(C6F5)4). 31P NMR (243 MHz,
CF3C6H5:C6D6 95:5, 293 K): δ = 516 (s, P4). FT-IR (cm–1): 2971 (w), 2862 (w), 1644 (w), 1513 (m), 1456 (s), 1373 (m), 1321
(m), 1272 (m), 1203 (m), 1174 (m), 1132 (m), 1085 (s), 976 (s), 931
(m), 801 (m), 773 (m), 755 (m), 702 (m), 683 (m), 659 (m). UV–vis
(CF3C6H5): λ1 =
527 nm (ε = 6150 L·cm–1·mol–1), λ2 = 325 nm (ε = 21 350
L·cm–1·mol–1). Anal.
Calcd for C114H100F40B2N6Nb2P4: C, 51.76; H, 3.81; N, 3.18.
Found: C, 51.77; H, 3.70; N, 3.12. mp: (decomp) 229–232 °C.
Reduction of 5 into 1
A 0.5
mL α,α,α-trifluorotoluene solution of CoCp2 (1.4 mg, 0.008 mmol, 1 equiv) was added to a 4 mL α,α,α-trifluorotoluene
solution of 5 (15 mg, 0.008 mmol, 1 equiv). The reaction
was stirred for 1 h at room temperature, and the color turned from
dark green to turquoise green. The solvent was removed in
vacuo, the residue was extracted with CDCl3, and
the green solution was analyzed by 1H NMR, showing the
characteristic resonances for 1.
[(BDI)Nb(NtBu)(OTf)2] (7)
A 2 mL toluene
solution of AgOTf (40 mg, 0.155 mmol, 2 equiv) was
added to an 8 mL toluene solution of 1 (100 mg, 0.078
mmol, 1 equiv). The reaction mixture was stirred overnight at room
temperature before filtration. The resulting pale, bright lime green
solution was concentrated and stored at −40 °C overnight.
This produced yellow crystals of 7 that were collected
and dried in vacuo (33.0 mg, 0.038 mmol, 24%). Single
crystals suitable for X-ray diffraction were grown similarly. 1H NMR (500 MHz, C6D6, 293 K): δ
= 7.03 (m, 4H, C–HAr), 6.94 (m, 2H, C–HAr), 6.24 (s, 1H, HC(C(Me)NAr)2), 2.59–2.48
(m, 4H, CHMe2), 1.90 (s, 6H, HC(C(Me)NAr)2),
1.66 (d, 6H, CHMe2, 3JHH = 6.4 Hz), 1.28 (d, 6H, CHMe2, 3JHH = 6.4 Hz), 1.07 (d, 6H, CHMe2, 3JHH = 6.7 Hz), 0.83 (d, 6H, CHMe2, 3JHH = 6.7 Hz), 0.75
(s, 9H, NtBu). 13C{1H} NMR (125.8
MHz, C6D6, 293 K): δ = 173.53 (C, HC(C(Me)NAr)2), 144.83 (C, Ar), 144.28 (C, Ar), 139.93 (C, Ar), 129.19
(CH, Ar), 125.07 (CH, Ar), 125.04 (CH, Ar), 113.69 (CH, HC(C(Me)NAr)2), 69.89 (C(Me)3), 33.89 (CH, iPr),
30.26 (CH3, Nb=NtBu), 28.32 (CH, iPr), 26.13 (CH3, HC(C(Me)NAr)2), 25.67
(CH3, iPr), 24.99 (CH3, iPr), 24.85 (CH3, iPr), 24.71 (CH3, iPr). 19F NMR (376 MHz, C6D6, 293 K): δ = −75.37 (q, 3F, CF3, JFF = 4.9 Hz), −77.12 ppm (q, 3F, CF3, JFF = 4.9 Hz). FT-IR (cm–1): 2970 (w), 2936 (w), 2874 (w), 1532 (w), 1462 (w),
1432 (w), 1372 (w), 1335 (m), 1231 (m), 1187 (s), 1173 (s), 1020 (s),
987 (s), 932 (m), 887 (w), 852 (w), 801 (m), 759 (w), 731 (m), 631
(s), 566 (m). Anal. Calcd for C35H50F6N3NbO6S2 C, 47.78 ; H, 5.73 ; N,
4.78. Found: C, 47.75 ; H, 5.79; N, 4.67. mp: (decomp) 258–260
°C.
Authors: Ba L Tran; Madhavi Singhal; Hyunsoo Park; Oanh P Lam; Maren Pink; J Krzystek; Andrew Ozarowski; Joshua Telser; Karsten Meyer; Daniel J Mindiola Journal: Angew Chem Int Ed Engl Date: 2010-12-17 Impact factor: 15.336
Authors: Christoph Schwarzmaier; Awal Noor; Germund Glatz; Manfred Zabel; Alexey Y Timoshkin; Brandi M Cossairt; Christopher C Cummins; Rhett Kempe; Manfred Scheer Journal: Angew Chem Int Ed Engl Date: 2011-06-22 Impact factor: 15.336
Authors: Rhett C Smith; Eugenijus Urnezius; Kin-Chung Lam; Arnold L Rheingold; John D Protasiewicz Journal: Inorg Chem Date: 2002-10-07 Impact factor: 5.165
Authors: Fabian Spitzer; Christian Graßl; Gábor Balázs; Eva M Zolnhofer; Karsten Meyer; Manfred Scheer Journal: Angew Chem Int Ed Engl Date: 2016-02-29 Impact factor: 15.336
Authors: Merle Arrowsmith; Michael S Hill; Andrew L Johnson; Gabriele Kociok-Köhn; Mary F Mahon Journal: Angew Chem Int Ed Engl Date: 2015-05-27 Impact factor: 15.336
Authors: Fabian Spitzer; Christian Graßl; Gábor Balázs; Eric Mädl; Martin Keilwerth; Eva M Zolnhofer; Karsten Meyer; Manfred Scheer Journal: Chemistry Date: 2017-01-25 Impact factor: 5.236