Jonathan M Darmon1, Renyuan Pony Yu1, Scott P Semproni1, Zoë R Turner1, S Chantal E Stieber1, Serena DeBeer2, Paul J Chirik1. 1. Department of Chemistry, Princeton University , Princeton, New Jersey 08544, United States. 2. Max-Planck Institute for Chemical Energy Conversion , Stiftstrasse 34-36, D-45470 Mülheim an der Ruhr, Germany ; Department of Chemistry and Chemical Biology, Cornell University , Ithaca, New York 14835, United States.
Abstract
The electronic structures of pyridine N-heterocyclic dicarbene (iPrCNC) iron complexes have been studied by a combination of spectroscopic and computational methods. The goal of these studies was to determine if this chelate engages in radical chemistry in reduced base metal compounds. The iron dinitrogen example (iPrCNC)Fe(N2)2 and the related pyridine derivative (iPrCNC)Fe(DMAP)(N2) were studied by NMR, Mössbauer, and X-ray absorption spectroscopy and are best described as redox non-innocent compounds with the iPrCNC chelate functioning as a classical π acceptor and the iron being viewed as a hybrid between low-spin Fe(0) and Fe(II) oxidation states. This electronic description has been supported by spectroscopic data and DFT calculations. Addition of N,N-diallyl-tert-butylamine to (iPrCNC)Fe(N2)2 yielded the corresponding iron diene complex. Elucidation of the electronic structure again revealed the CNC chelate acting as a π acceptor with no evidence for ligand-centered radicals. This ground state is in contrast with the case for the analogous bis(imino)pyridine iron complexes and may account for the lack of catalytic [2π + 2π] cycloaddition reactivity.
The electronic structures of pyridineN-heterocyclic dicarbene(iPrCNC)iron complexes have been studied by a combination of spectroscopic and computational methods. The goal of these studies was to determine if this chelate engages in radicalchemistry in reduced base metalcompounds. The iron dinitrogen example (iPrCNC)Fe(N2)2 and the related pyridine derivative (iPrCNC)Fe(DMAP)(N2) were studied by NMR, Mössbauer, and X-ray absorption spectroscopy and are best described as redox non-innocent compounds with the iPrCNCchelate functioning as a classical π acceptor and the iron being viewed as a hybrid between low-spin Fe(0) and Fe(II) oxidation states. This electronic description has been supported by spectroscopic data and DFT calculations. Addition of N,N-diallyl-tert-butylamine to (iPrCNC)Fe(N2)2 yielded the corresponding iron dienecomplex. Elucidation of the electronic structure again revealed the CNCchelate acting as a π acceptor with no evidence for ligand-centered radicals. This ground state is in contrast with the case for the analogous bis(imino)pyridine ironcomplexes and may account for the lack of catalytic [2π + 2π] cycloaddition reactivity.
Iron dinitrogencomplexes
with meridionally coordinating nitrogen-based
pincer-type ligands are of interest due to their activity and versatility
in base-metalcatalysis.[1−3] In 2004, our laboratory reported
the synthesis of (iPrPDI)Fe(N2)2(iPrPDI = 2,6-(2,6-iPr2-C6H3-N=CMe)2C5H3N) and
exploration of its activity in catalytichydrogenation and hydrosilylation
(Scheme 1).[4,5] This iron dinitrogencompound has also proven to be an effective precatalyst for the [2π
+ 2π] cycloaddition of α,ω-dienes[6] with ethylene and butadiene to form vinylcyclobutane[7] and reductive cyclizations involving enynes and
diynes.[8] Modification of the bis(imino)pyridinechelate has resulted in iron dinitrogencomplexes with improved catalytic
performance. Reducing the size of the 2,6-aryl substituents from isopropyl
to ethyl or methyl furnished the dimericiron dinitrogencomplexes
[(RPDI)Fe(N2)]2(μ2-N2) (RPDI = 2,6-(2,6-R2-C6H3-N=CMe)2C5H3N; R = Me, Et), which exhibited dramatically improved activity for
both olefinhydrogenation[9] and hydrosilylation.[10] The hydrosilylation chemistry produced no byproducts
arising from olefin isomerization or dehydrogenative silylation, a
distinct advantage over commercial precious-metalcatalysts.
Scheme 1
Bis(imino)pyridine
and Pyridine N-Heterocyclic Dicarbene Iron Dinitrogen
Complexes That Are Active Precatalysts for Olefin Hydrogenation
The dimers [(RPDI)Fe(N2)]2(μ2-N2) (R = Me,
Et) are depicted as monomers for simplicity.
Bis(imino)pyridine
and Pyridine N-Heterocyclic Dicarbene Iron Dinitrogen
Complexes That Are Active Precatalysts for Olefin Hydrogenation
The dimers [(RPDI)Fe(N2)]2(μ2-N2) (R = Me,
Et) are depicted as monomers for simplicity.Electronic effects on the performance of aryl-substituted bis(imino)pyridineironcatalysts have also been recently evaluated. Introduction of
electron-donating groups into the 4-position of the bis(imino)pyridine
ligand, e.g. (4-Me2N-iPrPDI)Fe(N2)2,[11] increased both hydrogenation[12] and hydrosilylation activity.[5] These findings prompted the study of even more electron
rich iron bis(dinitrogen)complexes. Danopoulos and co-workers reported
the synthesis of (iPrCNC)Fe(N2)2(iPrCNC = 2,6-(2,6-iPr2-C6H3-imidazol-2-ylidene)2-C5H3N)[13] and infrared stretching frequencies
of the symmetric and asymmetricN2 stretching modes, which
established an ironcenter more electron rich than that in the corresponding
bis(imino)pyridinecompounds. Accordingly, (iPrCNC)Fe(N2)2 and its less sterically protected variants (MeCNC)Fe(N2)2 and (MesCNC)Fe(N2)2 are extremely active hydrogenation precatalysts,
with the latter compounds exhibiting rapid turnover for unactivated
tri- and tetrasubstituted alkenes, which are challenging substrates
for even the most active precious-metalcatalysts.[14]The observation of increased catalytichydrogenation
activity with
more electron rich iron dinitrogencomplexes has prompted additional
studies aimed at understanding the origins of this effect. Before
mechanistic studies can be meaningfully interpreted, the electronic
structure of the various iron structural types must be established.
Studies from our laboratory[15,16] and others[17−19] have established the redox activity and noninnocence[20] of bis(imino)pyridine ligands in reduced iron,[21] manganese,[22] and
cobalt[23,24] complexes. Specifically, the five-coordinate
bis(imino)pyridine iron bis(dinitrogen) complex (iPrPDI)Fe(N2)2 is best described as a hybrid structure with
iron(0) and iron(II)canonical forms, where the chelating ligand serves
as a classical π-acid with no evidence for radicalcharacter
on either the ligand or the metal (Scheme 2). Because of the ambiguity in the oxidation state due to the high
covalency in the molecule, we apply the term redox noninnocence in
line with Jørgenson’s original definition.[16,25] The electronic structure of the four-coordinate compound (iPrPDI)FeN2 is distinct from that of the five-coordinate
species and is best described as an intermediate-spin iron(II)compound
antiferromagnetically coupled to a triplet bis(imino)pyridine diradical
dianion (Scheme 2).[21] There is no ambiguity surrounding the oxidation state assignment
of the metal, where the iron is undoubtedly intermediate spin Fe(II),
and hence the bis(imino)pyridine diradical is termed “redox
active”.[16]
Scheme 2
Difference in Electronic
Structures between (iPrPDI)Fe(N2)2 and (iPrPDI)FeN2
The structural similarity between bis(imino)pyridines
and the pyridineN-heterocyclic dicarbenes raised the question if the latter type of
iron dinitrogencomplexes or catalytic intermediates have redox active
chelates with ligand-centered radicals. DFT calculations have been
used to explore the electronic structures of (iPrCNC)Fe(N2)2 and (iPrCNC)Fe(CO)2 and
variants where methyl groups have been introduced into the meta positions
of the centralpyridine ring. Computational studies by Danopoulos
and Sassmannshausen[26] established a classicalFe(0) description for both (iPrCNC)Fe(N2)2 and (iPrCNC)Fe(CO)2 with competitive
iron–pyridine π-back-bonding accounting for the relatively
high carbonyl stretching frequencies in comparison to ironcompounds
with dialkylated phosphine-based [PNP] pincers. Subsequent DFT studies
by Zhang[27] explored the energetics of both
singlet and triplet states for (iPrCNC)Fe(N2)2 and found that the singlet was favored for the five-coordinate
complex. Dissociation of one of the dinitrogen ligands involved singlet–triplet
crossing to produce the high-spin, four-coordinate iron complex(iPrCNC)Fe(N2). Examination of the spin density in
the triplet excited states of (iPrCNC)Fe(N2)2 established radicalcharacter on the [iPrCNC]
ligand, with the principalcomponent in the pyridine ring suggesting
that redox activity is possible. Our laboratory recently described
investigations into the catalyticalkenehydrogenation activity and
electronic structures of (iPrCNC)CoCH3[28] and (iPrCNC)CoH.[29] Both experimental and computational studies supported low-spin
Co(II)complexes and the presence of a ligand-centered, essentially
pyridine localized radical. Support for this view of the electronic
structure was obtained from the observation of Co–H migration
into the 4-position of the pyridine ring under a dinitrogen atmosphere
to yield the modified cobalt dinitrogencomplex. Here we describe
an extension of these studies to the iron bis(dinitrogen) derivative
(iPrCNC)Fe(N2)2 and related neutral
ligand derivatives and report insight into the inability of these
compounds to promote catalytic [2π + 2π] cycloaddition
chemistry with α,ω-dienes.
Results and Discussion
Spectroscopic
Studies on (iPrCNC)Fe(N2)2
Spectroscopic studies were conducted on (iPrCNC)Fe(N2)2 to experimentally establish
the electronic structure of the compound and determine the participation
of the pyridineN-heterocyclic dicarbene. Because monomeric aryl-substituted
bis(imino)pyridine ironcomplexes undergo dissociation of 1 equiv
of N2 upon dissolution in benzene-d6,[4,30] similar behavior was probed for (iPrCNC)Fe(N2)2. As reported previously,[13] the toluene solution infrared spectrum exhibits
two bands for the symmetric and asymmetricdinitrogen stretches centered
at 2112 and 2046 cm–1, respectively. No evidence
was obtained for the putative four-coordinate compound (iPrCNC)FeN2, even after stirring for extended periods in
solution.Budzelaar[31,32] and subsequently our laboratory[15] have
demonstrated the utility of 1HNMR spectroscopy for identifying
redox active chelates in reduced iron and cobaltchemistry. Deviations
of the in-plane chelate hydrogens from their diamagnetic reference
values arise from either thermal population of a triplet excited state
or from temperature-independent paramagnetism and signal participation
of the ligand in the electronic structure. To explore this possibility
with (iPrCNC)Fe(N2)2, the benzene-d61HNMR spectrum of the ironcompound
was compared to that of the free pyridineN-heterocyclic dicarbene
(see Figure S1, Supporting Information).
None of the chemical shifts of (iPrCNC)Fe(N2)2 significantly deviate from those of iPrCNC,
establishing that higher spin states of the ironcompound are sufficiently
energetically separated from the diamagnetic ground state to influence
the 1HNMR spectrum of the compound.The solution behavior of (iPrCNC)Fe(N2)2 was also studied by 15NNMR spectroscopy.
The 15N isotopologue was prepared by exposure of the natural-abundance
iron dinitrogencompound to 15N2 gas. The benzene-d615NNMR spectrum (Figure S2, Supporting Information) exhibits two broad singlets
centered at 323.4 and 348.4 ppm (Δν1/2 = 36
and 33 Hz, respectively). Because the 1HNMR spectrum exhibits
the number of resonances consistent with C2 symmetry and hence rapidly interchanging dinitrogen
ligands, the two peaks observed are likely due to the α and
β nitrogen atoms of a single N2 molecule. The absence
of N≡Ncoupling has been observed previously with iron dinitrogencompounds.[9,33]In addition to
dinitrogencomplexes, four-coordinate bis(imino)pyridineironcompounds with σ-only ligands have also proven useful in
establishing the redox activity of this ligand class in reduced ironchemistry.[34] One illustrative example is
(iPrPDI)Fe(DMAP) (DMAP = 4-N,N-dimethylaminopyridine), an intermediate-spin ferrous compound with
a bis(imino)pyridine triplet diradical dianion. Attempts to synthesize
the CNCiron analogue by addition of DMAP to (iPrCNC)Fe(N2)2 resulted in loss of only 1 equiv of dinitrogen
and furnished a dark crystalline solid identified as (iPrCNC)Fe(DMAP)(N2) in 80% yield as deep red cubes (eq 1).The benzene-d61HNMR spectrum
for (iPrCNC)Fe(DMAP)(N2) exhibits the number
of resonances expected for a C-symmetriciron complex, consistent with coordination of two
different neutral ligands. As with (iPrCNC)Fe(N2)2, the chemical shifts of the in-plane hydrogens do not
significantly deviate from the reference values of the free chelate.
The most notable feature of the spectrum is the upfield shift of the
ortho and meta hydrogens on the coordinated DMAP to 6.95 and 5.19
ppm, respectively. (iPrCNC)Fe(DMAP)(N2) was
also characterized by a strong N2 absorption at 1998 cm–1 in the pentane solution infrared spectrum. This value
is more reduced by ∼10 cm–1 than values for
other five-coordinate CNCiron dinitrogencomplexes, (iPrCNC)Fe(L)N2 (L = CH2=CH2,
PMe3), reported by Danopoulos.[13]Single crystals of (iPrCNC)Fe(DMAP)(N2) suitable
for X-ray diffraction were obtained from a concentrated diethyl ether
solution at −35 °C. A representation of the molecular
structure is presented in Figure 1 and confirms
the identity of the molecule as a five-coordinate, pseudo-square-pyramidaliron complex with the DMAP ligand occupying the apical position. Selected
bond distances and angles are reported in Table 1. No significant distortions in the chelate are observed in either
the iPrCNC ligand or the coordinated DMAP.
Figure 1
Solid-state structure
of (iPrCNC)Fe(DMAP)(N2) with 30% probability
ellipsoids. Hydrogen atoms are omitted for
clarity.
Table 1
Bond Distances (Å)
and Angles
(deg) for (iPrCNC)Fe(DMAP)(N2)
Fe(1)–N(3)
1.8903(14)
N(1)–C(11)
1.387(2)
Fe(1)–C(10)
1.9156(17)
C(11)–N(2)
1.406(2)
Fe(1)–C(11)
1.9179(17)
N(4)–C(10)
1.405(2)
Fe(1)–N(6)
1.7797(14)
C(10)–N(5)
1.387(2)
Fe(1)–N(8)
2.0467(16)
N(6)–N(7)
1.1323(19)
Solid-state structure
of (iPrCNC)Fe(DMAP)(N2) with 30% probability
ellipsoids. Hydrogen atoms are omitted for
clarity.
Mössbauer, X-ray
Absorption, and DFT Studies
The electronic structures of
a family of pyridineN-heterocyclicdicarbene ironcomplexes were also investigated by zero-field 57Fe Mössbauer spectroscopy at 80 K. Representative
spectra are presented in Figure 2. To our knowledge,
Mössbauer data have not been reported for any ironcompound
in the series. The experimentally determined isomer shifts (δ)
and quadrupole splittings (ΔEQ)
along with those for the corresponding bis(imino)pyridine ironcompound
are reported in Table 2.
Figure 2
Zero-field 57Fe Mössbauer spectra of (iPrCNC)FeBr2 (A), (iPrCNC)Fe(N2)2 (B), (iPrCNC)Fe(DMAP)(N2) (C), and (iPrCNC)Fe(CO)2 (D) recorded at 80 K.
Table 2
Zero-Field 57Fe Mössbauer
Parameters for Pyridine N-Heterocyclic Dicarbene and Pyridine Diimine
Iron Complexesa
compd
δ (mm/s)
|ΔEQ| (mm/s)
(iPrCNC)FeBr2
0.88
1.57
(iPrPDI)FeCl2b
0.89
2.40
(iPrCNC)Fe(N2)2
0.27
0.69
(iPrPDI)Fe(N2)2b
0.39
0.53
(iPrCNC)Fe(DMAP)(N2)
0.24
0.70
(iPrPDI)Fe(DMAP)b
0.31
1.94
(iPrCNC)Fe(CO)2
–0.10
0.62
(iPrPDI)Fe(CO)2b
0.03
1.17
All data were recorded at 80
K, and values are reported relative to α-iron.
Data taken from ref (15).
Zero-field 57Fe Mössbauer spectra of (iPrCNC)FeBr2 (A), (iPrCNC)Fe(N2)2 (B), (iPrCNC)Fe(DMAP)(N2) (C), and (iPrCNC)Fe(CO)2 (D) recorded at 80 K.All data were recorded at 80
K, and values are reported relative to α-iron.Data taken from ref (15).The parameters observed for (iPrCNC)FeBr2 are typical for a high-spin ferrous compound and are similar
to
those observed for the bis(imino)pyridine analogue (iPrPDI)FeCl2. For the reduced compounds, pyridineN-heterocyclicdicarbenecomplexes have isomer shifts consistently lower than those
for the corresponding bis(imino)pyridinecompounds, a result of increased
covalency and relatively short iron–ligand bonds. For (iPrCNC)Fe(N2)2, (iPrCNC)Fe(DMAP)(N2), and (iPrCNC)Fe(CO)2, the data are
consistent with iron(0) compounds with the N-heterocycliccarbenes
serving as π-acids.[35−38]The electronic structures of the pyridineN-heterocyclicdicarbeneiron complexes were also investigated by X-ray absorption spectroscopy
(XAS).[39−41] XAS has proven particularly useful in elucidation
of the electronic structure of bis(imino)pyridine ironcomplexes and
has been able to distinguish between redox non-innocent (iPrPDI)Fe(N2)2 and redox active (iPrPDI)Fe(N2)[21] as well as detect
spin crossover behavior.[42] The normalized
XAS spectra for (iPrCNC)FeBr2, (iPrCNC)Fe(N2)2, (iPrCNC)Fe(DMAP)(N2), and (iPrCNC)Fe(CO)2 are presented
in Figure 3. (iPrCNC)FeBr2 serves as a reference of an established high-spin iron(II)compound,
with a pre-edge energy of 7112.0 eV (Table 3), which is in the range for typicalferrous compounds.[39] The first pre-edge transitions for the other iPrCNCcompounds are shifted by as much as 0.8 eV higher in
energy, with the pre-edge for (iPrCNC)Fe(CO)2 at 7112.8 eV. Both (iPrCNC)Fe(DMAP)(N2) and
(iPrCNC)Fe(N2)2 have similar pre-edge
energies, intensities, and shapes, suggesting that they have similar
oxidation states and hence electronic structures. In XAS, shifts of
both the pre-edge and rising edge (∼7115–7125 eV) to
higher energies are often attributed to a higher metal oxidation state
but can also be influenced by metal back-bonding to ligands, resulting
in the appearance of a more oxidized metalcenter.[43] In the reduced iPrCNC series of compounds, the
rising edge shifts to higher energy as the π-accepting character
of the ligands increases, suggesting that ligand back-bonding is the
primary contribution to the edge shift and is also consistent with
the relatively low isomer shifts observed by Mössbauer spectroscopy.
Figure 3
Normalized
Fe K-edge XAS spectra of [(iPrCNC)Fe] complexes.
Data were collected at 10 K.
Table 3
Experimentally Fit XAS Pre-Edge Positions
and Areasa
compd
peak 1 (eV);
area
peak 2 (eV);
area
(iPrCNC)FeBr2
7112.0; 11.9(9)
NA
(iPrPDI)FeCl2b
7111.8; 8(3)
7113.5(3); 8(4)
(iPrCNC)Fe(N2)2
7112.4; 13(1)
7113.8; 8.1(7)
(iPrPDI)Fe(N2)2b
7111.9; 6.4(1)
7114.0; 19.8(4)
(iPrCNC)Fe(DMAP)(N2)
7112.0; 2.4(5)
7113.3; 14(1)
(iPrPDI)Fe(DMAP)b
7111.1; 13.3(3)
7115.0; 20.2(1)
(iPrCNC)Fe(CO)2
7112.8; 13.5(1)
7114.5; 8.0(1)
(iPrPDI)Fe(CO)2b
7112.4; 10.2(1)
7114.5; 16.6(2)
All intensities are calculated using
the Simpson rule method described in ref (21) and are multiplied by 100. Errors are given
in parentheses, and those that are less than <1 are below the resolution
of the experimental technique and are omitted.
Data taken from ref (21).
Normalized
Fe K-edge XAS spectra of [(iPrCNC)Fe] complexes.
Data were collected at 10 K.All intensities are calculated using
the Simpson rule method described in ref (21) and are multiplied by 100. Errors are given
in parentheses, and those that are less than <1 are below the resolution
of the experimental technique and are omitted.Data taken from ref (21).The
XAS data for (iPrCNC)Fe(N2)2 and
(iPrCNC)Fe(CO)2 were compared to those
for the structurally similar bis(imino)pyridinecompounds in an attempt
to delineate the relative contributions from π-back-bonding
of the CNC versus PDI chelate from the CO or N2 supporting
ligands (Figure 4, Table 3).[21] The overall spectral shapes for the
[(iPrPDI)Fe] and [(iPrCNC)Fe] compounds are
similar but the edges for the iPrCNC examples are generally
shifted to higher energies. As with the [iPrPDI] compounds,
the pre-edges of (iPrCNC)Fe(N2)2 and
(iPrCNC)Fe(CO)2 exhibit two features. On the
basis of previous assignments for [iPrPDI] compounds,[21] it is likely the lower energy pre-edge feature
corresponds to a metal 1s to 3d transition with strong contributions
from the chelate π* orbital. The first pre-edge feature is shifted
0.5 eV higher in energy for (iPrCNC)Fe(N2)2 in comparison to (iPrPDI)Fe(N2)2 and 0.4 eV to higher energy for (iPrCNC)Fe(CO)2 in comparison to (iPrPDI)Fe(CO)2, suggesting
that the iPrCNC ligand affects a 0.4–0.5 eV shift
to higher energy in the first pre-edge feature in comparison to iPrPDI. Therefore, the high pre-edge energy of 7112.8 eV for
(iPrCNC)Fe(CO)2 is best attributed to increased
chelate π-back-bonding and not a higher metal oxidation state.
The second pre-edge feature in the iPrPDI compounds results
from transitions to N2 or CO π* orbitals.[21] For (iPrCNC)Fe(CO)2, the
second pre-edge feature at 7114.5 eV is the same as that of the iPrPDI analogue, supporting the assignment as a predominantly
CO π* transition. The 0.9 eV pre-edge shift to higher energy
of (iPrCNC)Fe(DMAP)(N2) versus (iPrPDI)Fe(DMAP) may be rationalized by combined contributions from the iPrCNC ligand and the coordinated N2 ligand. The
similarities of the iPrCNCiron XAS spectra to those of
the [(iPrPDI)Fe] compounds support that the main contributions
to spectral energy and shape result from back-bonding to the N2 and CO ligands. While the spectra for the iPrCNC
ligand are shifted 0.4–0.5 eV to higher energies than those
for iPrPDI, the overall electronic structural descriptions
for (iPrCNC)Fe(N2)2 and (iPrCNC)Fe(CO)2 appear similar to those for the [(iPrPDI)Fe] compounds.
Figure 4
Normalized Fe K-edge XAS spectra of [(iPrCNC)Fe]
complexes
and comparison to the bis(imino)pyridine analogues. Data were collected
at 10 K.
Normalized Fe K-edge XAS spectra of [(iPrCNC)Fe]
complexes
and comparison to the bis(imino)pyridine analogues. Data were collected
at 10 K.Although (iPrCNC)Fe(N2)2 has been
the subject of previous computational studies, to our knowledge broken-symmetry
solutions corresponding to redox active ligand radical electronic
structures have not been investigated. The acquisition of 57Fe Mössbauer and XAS spectral data provides experimental parameters
from which to calibrate the computational results. Broken-symmetry
possibilities[44] were explored for (iPrCNC)Fe(N2)2 at the B3LYP level of
DFT. In the broken symmetry notation BS(m,n) describes a state in which there are m unpaired spin-up electrons and n unpaired spin-down
electrons on separate fragments.[44−46]Full-molecule
calculations were performed on three models for (iPrCNC)Fe(N2)2: a spin-restricted RKS
and spin unrestricted BS(2,2) and BS(1,1). The two broken-symmetry
calculations converged to the same BS(1,1) description with an overlap
of S = 0.75, which was 2.2 kcal/mol lower in energy
than the RKS solution. Molecular orbital diagrams from both the RKS
and BS(1,1) outputs are presented in Figure 5. Also presented in Figure 5 is the spin density
plot generated from the BS(1,1) solution. The calculated geometric
parameters from both the BS(1,1) and RKS solutions (Table S1, Supporting Information) are in excellent agreement
with the experimental data and are within experimentalerror from
each other. The 57Fe Mössbauer parameters were also
computed from the two solutions but the values (RKS, δ = 0.26
mm/s, ΔEQ = +0.74 mm/s; BS(1,1),
δ = 0.34 mm/s, ΔEQ = +0.61
mm/s) are indistinguishable on the basis of the error in the calculations
(δ = ±0.1 mm/s; ΔEQ =
±0.5 mm/s)[47] and the experimental
values (δ = 0.27 mm/s; |ΔEQ| = 0.69 mm/s). On the basis of energetic, structural, and spectroscopic
parameters, DFT calculations are unable to distinguish the classical
π-back-bonding description versus the redox active alternative.
Analogous calculations were performed on (iPrCNC)Fe(DMAP)(N2), and the results are presented in the Supporting Information. As with (iPrCNC)Fe(N2)2, the energetics of the RKS and BS(1,1) solutions
were indistinguishable, with the broken-symmetry solution being 3
kcal/mol lower in energy. However, the computed 57Fe Mössbauer
parameters (RKS, δ = 0.28 mm/s, ΔEQ = +0.73 mm/s; BS(1,1), δ = 0.36 mm/s; ΔEQ = +0.50 mm/s) favor the RKS description.
Figure 5
(top)
Qualitative MO diagrams for (iPrCNC)Fe(N2)2 obtained from RKS (left) and BS(1,1) (right) DFT calculations
at the B3LYP level . (bottom) Spin density plot for (iPrCNC)Fe(N2)2 obtained from the BS(1,1) solution.
(top)
Qualitative MO diagrams for (iPrCNC)Fe(N2)2 obtained from RKS (left) and BS(1,1) (right) DFT calculations
at the B3LYP level . (bottom) Spin density plot for (iPrCNC)Fe(N2)2 obtained from the BS(1,1) solution.As an additionalcomparison for
the calculated electronic structure
descriptions, the XAS spectra were calculated using TD-DFT methods.
In both coordination compounds and enzymes, calculated TD-DFT XAS
spectra have shown good agreement with experiment.[21,48] However, the calculated XAS spectra for this series were plagued
by charge transfer transitions. This is a limitation of DFT that has
been previously described due to the strong dependence of calculated
charge transfer bands on the degree of Hartree–Fock mixing.[21,49] A full examination of Hartree–Fock mixing in these compounds
is beyond the scope of this study. Most notably, the combined computational
and experimental results for both (iPrCNC)Fe(N2)2 and (iPrCNC)Fe(DMAP)(N2) provide
no definitive evidence for a redox active pyridineN-heterocyclicdicarbene with ligand-centered radicals. On the basis of the spectroscopic
studies, the computational data, and previous studies on (iPrPDI)Fe(N2)2,[21] we
favor a more classical, redox non-innocent description for both reduced
compounds where the iPrCNC ligand acts as a π-acceptor.
Thus, both (iPrCNC)Fe(N2)2 and (iPrCNC)Fe(DMAP)(N2) are best considered iron(0)
compounds with contribution from an iron(II) resonance structure where
the chelate has been reduced by two electrons and is in its closed-shell
form.
Insights into Iron-Catalyzed [2π + 2π] α,ω-Diene
Cycloaddition
Aryl-substituted bis(imino)pyridine iron dinitrogencomplexes are known to catalyze the [2π + 2π] cycloaddition
of α,ω-dienes to yield the corresponding bicycloheptane
derivatives.[6,7,50] Because
(iPrPDI)Fe(N2)2 and (iPrCNC)Fe(N2)2 have similar ground states, the
catalyticcycloaddition chemistry of the latter was studied. Monitoring
a benzene-d6 solution of N,N-diallyl-tert-butylamine in the
presence of 10 mol % of (iPrCNC)Fe(N2)2 by 1HNMR spectroscopy revealed minimalolefin isomerization
along with cyclization to the 3-exo-substituted pyrrolidine rather
than cycloaddition (Scheme 3).
Scheme 3
Reaction
of N,N-Diallyl-tert-butylamine in the Presence of 10 mol % of (iPrCNC)Fe(N2)2
Partial (∼30%) consumption of the starting material
was
observed over the course of 22 h at 23 °C, and the two products,
designated A and B, were formed in an approximate
1:1 ratio. For A, the NMR data are consistent with exclusive
formation of the trans isomer of the internalalkene. By comparison,
[2π + 2π] cycloaddition promoted by (iPrPDI)Fe(N2)2 is complete in less than 15 min under identicalconditions. Repeating the catalytic experiment under 1 atm of H2 at 23 °C resulted in formation of three new products,
cis and trans isomers of C as well as D,
in a 3:3:4 ratio on the basis of integration of the tert-butyl resonances. Additional analysis by GC-MS established that C was a 1:1 mixture of the diastereomers cis- and trans-3,4-dimethylpyrrolidine. Product D was identified as the open-chain hydrogenation product N-(tert-butyl)-N-propylpropan-1-amine
(Scheme 3).Repeating the hydrogenation
experiment with 1 atm of D2 gas placed deuterium exclusively
in the methyl positions of the
cis isomer of C, suggesting hydrogenation of a putative
ironmetallacycle (Scheme 4).[50] For trans-C, deuterium was
located in a 1:1 ratio in both the methyl and methine positions, likely
arising from hydrogenation (deuteration) of the 3-exo-substituted pyrrolidine rather than the ironmetallacycle. The open-chain
product D also contained a 1:1 ratio of deuterium in
the methyl and methylene positions, consistent with hydrogenation
of the diene substrate and the known performance of (iPrCNC)Fe(N2)2 as an olefinhydrogenation catalyst.[12]
Scheme 4
Catalytic Deuteration of N,N-diallyl-tert-butylamine in the
Presence of (iPrCNC)Fe(N2)2
Additional insight into the
catalytic results was provided by the
stoichiometric reaction of N,N-diallyl-tert-butylamine with (iPrCNC)Fe(N2)2. Recrystallization from pentane following addition
of the diene to the iron complex yielded brown shards identified as
the iron dienecomplex (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu). Danopoulos and co-workers have previously reported that
addition of ethylene to (iPrCNC)Fe(N2)2 resulted in loss of 1 equiv of dinitrogen and yielded the characterized
iron ethylene dinitrogencomplex (iPrCNC)Fe(CH2=CH2)(N2).[13] Crystallographiccharacterization established a near-square-pyramidal
geometry, with the ethylene ligand occupying the apical position.The benzene-d61HNMR spectrum
of diamagnetic(iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) exhibited the number of resonances consistent with a compound
with C2 symmetry. Diagnostic upfield-shifted
resonances for coordination of the diene were observed, with the most
extreme case being located at 0.69 ppm. Similar NMR behavior was reported
by Danopoulos for (iPrCNC)Fe(CH2=CH2)(N2).[13] The solid-state
structure of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) was determined by X-ray diffraction, and a representation
of the molecular structure is presented in Figure 6. Selected metrical parameters are reported in Table 4. The allyl and tert-butyl groups
of the diene were disordered over two positions.
Figure 6
Representation of the
molecular structure of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) with 30% probability ellipsoids. Hydrogen
atoms are omitted for clarity. The allyl and tert-butyl groups of the diene were disordered over two positions and
successfully modeled.
Table 4
Bond Distances (Å) and Angles
(deg) for (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu)
Fe(1)–N(3)
1.9008(16)
N(1)–C(1)
1.398(3)
Fe(1)–C(1)
1.972(2)
C(1)–N(2)
1.406(2)
Fe(1)–C(11)
1.990(2)
N(4)–C(11)
1.404(3)
Fe(1)–C(36)
2.079(2)
C(11)–N(5)
1.400(3)
Fe(1)–C(37)
2.135(4)
C(36)–C(37)
1.315(5)
Fe(1)–C(40)
2.087(4)
C(40)–C(41)
1.413(5)
Fe(1)–C(41)
2.076(2)
Representation of the
molecular structure of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) with 30% probability ellipsoids. Hydrogen
atoms are omitted for clarity. The allyl and tert-butyl groups of the diene were disordered over two positions and
successfully modeled.The electronic structure
of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu was investigated
by zero-field 57Fe Mössbauer spectroscopy and broken-symmetry
DFT calculations.[51] The Mössbauer
spectrum (Figure 7) exhibits a doublet with
an isomer shift of 0.31
mm/s and a quadrupole splitting of 0.60 mm/s. These parameters are
indistinguishable from the values for (iPrCNC)Fe(N2)2 and (iPrCNC)Fe(DMAP)(N2) (Table 1) and suggest a high degree of covalency
and similar electronic structures among the three reduced compounds.
DFT calculations performed at the B3LYP level successfully reproduced
the experimental Mössbauer parameters (RKS, δ(calcd)
= 0.35 mm/s, ΔEQ(calcd) = 0.18 mm/s)
and support a classicalclosed-shell ironcompound with no evidence
for ligand-centered radicals. Notably, the electronic structure observed
for (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) differs
from that reported for (iPr(TB)PDI)Fe(η2,η2-(CH2=CHCH2)2NTs) (iPr(TB)PDI = 2,6-(2,6-iPr2-C6H3-N=C-(CH2)3)2(C5HN)), a molecule with an S = 1 ground state (δ = 0.63 mm/s, ΔEQ = 2.47 mm/s).[50]
Figure 7
Zero-field 57Fe Mössbauer spectrum of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) at 80 K.
Zero-field 57Fe Mössbauer spectrum of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) at 80 K.The reactivity of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) with dihydrogen was explored to correlate
the intermediacy
of the dienecomplex with the observed hydrogenative cyclization chemistry.
Exposure of a benzene-d6 solution of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu) to 1 atm of
H2 resulted in rapid and selective formation of cis-C. Repeating the experiment with D2 gas and analysis of the products by 1H and 2HNMR spectroscopy revealed formation of the d2 isotopologue of cis-C,
where the isotopic label was located 1:1 in the 3,4-methyl groups.
Re-exposure of the reaction mixture to 1 atm of dinitrogen resulted
in re-formation of (iPrCNC)Fe(N2)2. These results are consistent with previous observations in bis(imino)pyridineironchemistry where, even if the catalyst resting state is the metaldienecomplex, the corresponding metallacycle is kinetically accessible
and gives rise to cyclization products under catalyticconditions.
Concluding Remarks
The electronic structures of reduced
pyridineN-heterocyclic dicarbeneiron complexes have been investigated by a combination of structural,
spectroscopic, and computational studies. In all cases examined, the
[(iPrCNC)Fe] motif prefers five-coordinate bis(neutral)
ligand complexes with no experimental evidence for four-coordinate
alternatives arising from ligand dissociation. Among these compounds,
the tridentate pyridineN-heterocyclic dicarbenechelate acts as a
classical π-acceptor with no evidence for ligand-centered radicals,
suggesting that an iron(0) oxidation state is the most appropriate
description for this family of molecules. Attempts to promote the
catalytic [2π + 2π] cyclization of N,N-diallyl-tert-butylamine with (iPrCNC)Fe(N2)2 were unsuccessful, instead producing
exo-methylene pyrrolidine and olefin isomerization products in low
yield. These results, along with hydrogenation and isotopic labeling
experiments, demonstrate that the requisite ironmetallacycles for
[2π + 2π] cycloaddition are kinetically accessible but,
in the absence of ligand radicals and higher oxidation state iron,
C–C bond formation via reductive elimination is not observed,
highlighting the importance of redox active bis(imino)pyridine ligands
for this type of catalysis.
Experimental Section
General
Considerations
All air- and moisture-sensitive
manipulations were carried out using standard vacuum line, Schlenk,
and cannula techniques or in an MBraun inert-atmosphere drybox containing
an atmosphere of purified nitrogen. Solvents for air- and moisture-sensitive
manipulations were initially dried and deoxygenated using literature
procedures.[52] Benzene-d6 was purchased from Cambridge Isotope Laboratories and
dried over 4 Å molecular sieves. The following compounds were
prepared as described previously: (iPrCNC)FeBr2,[53] (iPrCNC)Fe(N2)2,[13] and (iPrCNC)Fe(CO)2.[13]1HNMR spectra
were recorded on Varian Mercury 300 and Inova 400, 500, and 600 spectrometers
operating at 299.76, 399.78, 500.62, and 599.78 MHz, respectively. 13CNMR spectra were recorded either on an Inova or on a Bruker
500 spectrometer operating at 125.893 and 125.853 MHz, respectively.
All 1H and 13CNMR chemical shifts are reported
relative to SiMe4 using the 1H (residual) and 13Cchemical shifts of the solvent as a secondary standard.
For diamagneticcomplexes, many assignments were made on the basis
of COSY, HSQC, and HMBCNMR experiments. Infrared spectra were collected
on a Thermo Nicolet spectrometer. Elemental analyses were performed
at Robertson Microlit Laboratories, Inc., in Ledgewood, NJ.Single crystals suitable for X-ray diffraction were coated with
polyisobutylene oil in a drybox, transferred to a nylon loop, and
then quickly transferred to the goniometer head. A Bruker APEX2 Duo
diffractometer equipped with molybdenum and copper X-ray tubes (λ
= 0.71073 and 1.54178 Å, respectively) was used to collect data
for (CNC)Fe(DMAP)(N2) (Cu
source) and (iPrCNC)Fe(η2,η2-(CH2CHCH2)2NtBu) (Mo source). The space group was identified, and the data were
processed using the Bruker SAINT+ program and corrected for absorption
using SADABS. The structures were solved using direct methods (SIR92)
completed by subsequent Fourier synthesis and refined by full-matrix
least-squares procedures.57Fe Mössbauer spectra
were recorded on a SEE
Co. Mössbauer spectrometer (MS4) at 80 K in constant acceleration
mode. 57Co/Rh was used as the radiation source. WMOSS software
was used for the quantitative evaluation of the spectral parameters
(least-squares fitting to Lorentzian peaks).[54] The temperature of the samples was controlled by a Janis Research
Co. CCS-850 He/N2cryostat within an accuracy of ±1
K. Isomer shifts were determined relative to α-iron at 298 K.For X-ray absorption spectroscopy, samples were prepared in an
inert-atmosphere nitrogen glovebox as finely ground dilutions in boron
nitride pressed into 1 mm Al spacers and shipped to the experimental
site in a liquid nitrogen Dewar. X-ray absorption spectra were recorded
at the Stanford Synchrotron Radiation Lightsource (SSRL) on beamline
BL7-3 under standard ring conditions. The beamline optics were optimized,
and the monochromator was fully tuned at 7500 eV. The incident energy
was calibrated by setting the first inflection of an iron foil to
7111.2 eV. Data were measured in transmission mode. Data were processed
using EXAFSPAK[55] and pictured using Kaleidagraph.[56]All DFT calculations were performed with
the ORCA program package.[51] The geometry
optimizations of the complexes
and single-point calculations on the optimized geometries were carried
out at the B3LYP level of DFT.[57] The all-electron
Gaussian basis sets were those developed by Ahlrichs’ group.[58] Triple-ζ-quality basis sets def2-TZVP
with one set of polarization functions on the metals and on the atoms
directly coordinated to the metalcenter were used. For the carbon
and hydrogen atoms, slightly smaller polarized split-valence def2-SV(P)
basis sets were used that were of double-ζ quality in the valence
region and contained a polarizing set of d functions on the non-hydrogen
atoms. Auxiliary basis sets were chosen to match the orbital basis.[59] The RIJCOSX[60] approximation
was used to accelerate the calculations.Throughout this paper,
computational results are described using
the BS approach by Ginsberg[61] and Noodleman
et al.[62] Because several BS solutions to
the spin-unrestricted Kohn–Sham equations may be obtained,
the general notation BS(m,n)[63] has been adopted, where m (n) denotes the number of spin-up (spin-down) electrons at
the two interacting fragments. Canonical and corresponding[64] orbitals, as well as spin density plots, were
generated with the program Chimera.[65] Nonrelativistic
single-point calculations employed the CP(PPP) basis set for iron.[66] The Mössbauer isomer shifts were calculated
from the computed electron densities at the ironcenters as previously
described.[67] TD-DFT calculations were calculated
as previously described.[21,48]
Preparation of (iPrCNC)Fe(DMAP)(N2)
A 20 mL scintillation vial was
charged with 0.100 g (0.155 mmol)
of (iPrCNC)Fe(N2)2 in approximately
10 mL of diethyl ether. With stirring, 0.019 g (0.16 mmol) of 4-N,N-dimethylaminopyridine was added and
a color change to red-orange was observed. After it was stirred for
30 min, the solution was concentrated and layered with approximately
5 mL of pentane. Storing the solution at −35 °C resulted
in crystallization of 0.092 g (80%) of an analytically pure, dark
solid identified as (iPrCNC)Fe(DMAP)(N2). Anal.
Calcd for C42H51N9Fe: C, 68.38; H,
6.97; N, 17.09. Found: C, 67.98; H, 6.76; N, 16.81. 1HNMR (benzene-d6, 23 °C): δ
1.00 (d, 6 Hz, 6H, CH(CH3)2), 1.05 (d, 6 Hz, 6H, CH(CH3)2), 1.11 (d, 6 Hz, 6H, CH(CH3)2), 1.19 (d, 6 Hz, 6H, CH(CH3)2), 1.93 (s, 6H, N(CH3)2),
3.00 (spt, 6 Hz, 2H, CH(CH3)2), 3.12 (spt, 6 Hz, 2H, CH(CH3)2), 5.19 (d, 6 Hz, 2H, 3-DMAP), 6.83 (s, 2H, imidazolylidene
backbone), 6.95 (d, 6 Hz, 2H, 2-DMAP), 7.20–7.33
(m, 6H, m-aryl and 3-pyr), 7.38 (t, 7 Hz, 2H, p-aryl), 7.59–7.70 (m, 3H, imidazolylidene backbone
and 4-pyr). 13CNMR {1H} (benzene-d6, 23 °C): δ 23.1 (CH(CH3)2), 23.3 (CH(CH3)2), 25.6 (CH(CH3)2),
26.7 (CH(CH3)2), 28.4 (CH(CH3)2), 28.5 (CH(CH3)2), 38.2 (N(CH3)2), 98.6 (pyr), 106.9 (DMAP), 109.8
(imidazolylidene backbone), 122.9 (aryl), 123.9 (pyr), 124.4 (aryl),
126.2 (imidazolylidene backbone), 129.1 (aryl), 139.0 (aryl), 140.9
(pyr), 146.7 (aryl), 148.8 (aryl), 151.8 (DMAP), 152.0 (DMAP), 203.6
(carbene). IR (pentane, 22 °C): ν(N2) 1998 cm–1. IR (KBr): ν(N2) 1987 cm–1.
Preparation of (iPrCNC)Fe(η2,η2-(CH2=CHCH2)2NtBu)
A 20 mL scintillation vial was charged with a
solution of 0.075 g (0.12 mmol) of (CNC)Fe(N2)2 in approximately 5 mL of diethyl
ether. With stirring, approximately 0.020 g (0.13 mmol) of N,N-diallyl-tert-butylamine
was added, causing an immediate color change to brown. After it was
stirred for 30 min, the solution was concentrated and layered with
approximately 5 mL of pentane. Storing the solution at −35
°C resulted in crystallization of a brown solid (0.030 g, 35%)
identified as (iPrCNC)Fe(η2,η2-(CH2CHCH2)2NtBu). Anal. Calcd for C45H60FeN6:
C, 72.95; H, 8.16; N, 11.34. Found, C, 72.81; H, 7.91; N, 11.47. 1HNMR (benzene-d6, 23 °C):
δ 0.69 (t, 11 Hz, 2H, N(CH2CHCH2)2), 0.78 (d, 7 Hz, 6H, CH(CH3)2), 0.89 (d, 7 Hz, 6H, CH(CH3)2), 0.94 (s, 9H, NC(CH3)3), 1.20 (d, 7 Hz, 6H, CH(CH3)2), 1.53 (d, 7 Hz, 6H, CH(CH3)2), 2.03 (d, 12 Hz, 2H, N(CH2CHCH2)2), 2.13 (d, 8 Hz, 2H, N(CH2CHCH2)2), 2.42 (spt, 7 Hz, 2H,
CH(CH3)2), 2.47 (spt, 7 Hz,
2H, CH(CH3)2), 3.93 (dd, 12
Hz, 3 Hz, 2H, N(CH2CHCH2)2), 4.70–4.76 (m, 2H, N(CH2CHCH2)2), 6.20 (d, 2 Hz, 2H, imidazolylidene
backbone), 6.93 (d, 8 Hz, 2H, m-aryl), 6.98 (d, 8
Hz, 1H, 3-pyr), 7.04 (t, 8 Hz, 1H, p-aryl), 7.12
(d, 2 Hz, 1H, imidazolylidene backbone), 7.23 (d, 8 Hz, m-aryl), 7.30 (d, 8 Hz, 1H, 3-pyr), 7.37 (t, 8 Hz, 1H, 4-pyr), 7.40
(t, 8 Hz, 1H, p-aryl), 7.46 (d, 2 Hz, 1H, imidazolylidene
backbone). 13C{1H} NMR (benzene-d6, 23 °C): δ 21.6 (CH(CH3)2), 22.2 (CH(CH3)2), 26.8 (CH(CH3)2),
27.0 (CH(CH3)2), 28.4 (CH(CH3)2 or C(CH3)3), 28.5 (CH(CH3)2 or C(CH3)3), 28.6
(N(CH2CHCH2)2),
28.8 (CH(CH3)2 or C(CH3)3), 52.4 (C(CH3)3), 54.0 (N(CH2CHCH2)2), 61.4 (N(CH2CHCH2)2), 99.4 (3-pyr), 100.4 (3-pyr), 110.2 (imidazolylidene
backbone), 113.0 (imidazolylidene backbone), 114.8 (4-pyr), 123.2
(m-aryl), 124.1 (m-aryl), 127.0
(imidazolylidene backbone), 127.0 (imidazolylidene backbone), 129.5
(p-aryl), 130.3 (p-aryl), 138.4
(aryl), 139.1 (aryl), 146.2 (pyr), 146.5 (aryl), 147.6 (aryl), 152.4
(pyr), 195.8 (carbene), 208.8 (carbene).
General Procedure for Catalytic
Experiments
A 20 mL
scintillation vial was charged with 0.010 g (16 μmol) of (iPrCNC)Fe(N2)2 and 0.65 g of benzene-d6. N,N-Diallyl-tert-butylamine (0.024 g, 0.16 mmol) was added, which caused
an immediate color change from green to brown. The solution was transferred
to a J. Young tube, which was stored in a 23 °Cwater bath. The
reaction was monitored by 1HNMR spectroscopy. For experiments
where the solution was exposed to 1 atm of H2 or D2, after transfer to a J. Young tube, the solution was immediately
submerged in liquid nitrogen. The headspace was evacuated on a high-vacuum
line, and 1 atm of H2 or D2 was introduced.
The sample was thawed in a 23 °Cwater bath.
Authors: Amanda C Bowman; Carsten Milsmann; Crisita Carmen Hojilla Atienza; Emil Lobkovsky; Karl Wieghardt; Paul J Chirik Journal: J Am Chem Soc Date: 2010-02-10 Impact factor: 15.419
Authors: Stephan M Rummelt; Jonathan M Darmon; Renyuan Pony Yu; Peter Viereck; Tyler P Pabst; Zoë R Turner; Grant W Margulieux; Shunlin Gu; Paul J Chirik Journal: Organometallics Date: 2019-08-09 Impact factor: 3.876
Authors: Deidra L Gerlach; Sopheavy Siek; Dalton B Burks; Jamie M Tesh; Courtney R Thompson; Robert M Vasquez; Nicholas J White; Matthias Zeller; Douglas B Grotjahn; Elizabeth T Papish Journal: Inorganica Chim Acta Date: 2017-07-01 Impact factor: 2.545
Authors: Michael L Baker; Michael W Mara; James J Yan; Keith O Hodgson; Britt Hedman; Edward I Solomon Journal: Coord Chem Rev Date: 2017-02-09 Impact factor: 22.315
Authors: Megan Mohadjer Beromi; C Rose Kennedy; Jarod M Younker; Alex E Carpenter; Sarah J Mattler; Joseph A Throckmorton; Paul J Chirik Journal: Nat Chem Date: 2021-01-25 Impact factor: 24.427