Xiao-Ye Wang1,2, Xuelin Yao2, Akimitsu Narita2,3, Klaus Müllen2. 1. State Key Laboratory of Elemento-Organic Chemistry, College of Chemistry , Nankai University , Tianjin 300071 , China. 2. Max Planck Institute for Polymer Research , Ackermannweg 10 , 55128 Mainz , Germany. 3. Organic and Carbon Nanomaterials Unit , Okinawa Institute of Science and Technology Graduate University , Okinawa 904-0495 , Japan.
Abstract
Nanographenes, which are defined as nanoscale (1-100 nm) graphene cutouts, include quasi-one-dimensional graphene nanoribbons (GNRs) and quasi-zero-dimensional graphene quantum dots (GQDs). Polycyclic aromatic hydrocarbons (PAHs) larger than 1 nm can be viewed as GQDs with atomically precise molecular structures and can thus be termed nanographene molecules. As a result of quantum confinement, nanographenes are promising for next-generation semiconductor applications with finite band gaps, a significant advantage compared with gapless two-dimensional graphene. Similar to the atomic doping strategy in inorganic semiconductors, incorporation of heteroatoms into nanographenes is a viable way to tune their optical, electronic, catalytic, and magnetic properties. Such properties are highly dependent not only on the molecular size and edge structure but also on the heteroatom type, doping position, and concentration. Therefore, reliable synthetic methods are required to precisely control these structural features. In this regard, bottom-up organic synthesis provides an indispensable way to achieve structurally well-defined heteroatom-doped nanographenes. Polycyclic heteroaromatic compounds have attracted great attention of organic chemists for decades. Research in this direction has been further promoted by modern interest in supramolecular chemistry and organic electronics. The rise of graphene in the 21st century has endowed large polycyclic heteroaromatic compounds with a new role as model systems for heteroatom-doped graphene. Heteroatom-doped nanographene molecules are in their own right promising materials for photonic, optoelectronic, and spintronic applications because of the extended π conjugation. Despite the significant advances in polycyclic heteroaromatic compounds, heteroatom-doped nanographene molecules with sizes of over 1 nm and their relevant GNRs are still scarce. In this Account, we describe the synthesis and properties of large heteroatom-doped nanographenes, mainly summarizing relevant advances in our group in the past decade. We first present several examples of heteroatom doping based on the prototypical nanographene molecule, i.e., hexa-peri-hexabenzocoronene (HBC), including nitrogen-doped HBC analogues by formal replacement of benzene with other heterocycles (e.g., aromatic pyrimidine and pyrrole and antiaromatic pyrazine) and sulfur-doped nanographene molecules via thiophene annulation. We then introduce heteroatom-doped zigzag edges and a variety of zigzag-edged nanographene molecules incorporating nitrogen, boron, and oxygen atoms. We finally summarize heteroatom-doped GNRs based on the success in the molecular cases. We hope that this Account will further stimulate the synthesis and applications of heteroatom-doped nanographenes with a combined effort from different disciplines.
Nanographenes, which are defined as nanoscale (1-100 nm) graphene cutouts, include quasi-one-dimensional graphene nanoribbons (GNRs) and quasi-zero-dimensional graphene quantum dots (GQDs). Polycyclic aromatic hydrocarbons (PAHs) larger than 1 nm can be viewed as GQDs with atomically precise molecular structures and can thus be termed nanographene molecules. As a result of quantum confinement, nanographenes are promising for next-generation semiconductor applications with finite band gaps, a significant advantage compared with gapless two-dimensional graphene. Similar to the atomic doping strategy in inorganic semiconductors, incorporation of heteroatoms into nanographenes is a viable way to tune their optical, electronic, catalytic, and magnetic properties. Such properties are highly dependent not only on the molecular size and edge structure but also on the heteroatom type, doping position, and concentration. Therefore, reliable synthetic methods are required to precisely control these structural features. In this regard, bottom-up organic synthesis provides an indispensable way to achieve structurally well-defined heteroatom-dopednanographenes. Polycyclic heteroaromaticcompounds have attracted great attention of organic chemists for decades. Research in this direction has been further promoted by modern interest in supramolecular chemistry and organic electronics. The rise of graphene in the 21st century has endowed large polycyclic heteroaromaticcompounds with a new role as model systems for heteroatom-dopedgraphene. Heteroatom-dopednanographene molecules are in their own right promising materials for photonic, optoelectronic, and spintronic applications because of the extended π conjugation. Despite the significant advances in polycyclic heteroaromaticcompounds, heteroatom-dopednanographene molecules with sizes of over 1 nm and their relevant GNRs are still scarce. In this Account, we describe the synthesis and properties of large heteroatom-dopednanographenes, mainly summarizing relevant advances in our group in the past decade. We first present several examples of heteroatom doping based on the prototypical nanographene molecule, i.e., hexa-peri-hexabenzocoronene (HBC), including nitrogen-dopedHBC analogues by formal replacement of benzene with other heterocycles (e.g., aromatic pyrimidine and pyrrole and antiaromaticpyrazine) and sulfur-doped nanographene molecules via thiophene annulation. We then introduce heteroatom-dopedzigzag edges and a variety of zigzag-edged nanographene molecules incorporating nitrogen, boron, and oxygen atoms. We finally summarize heteroatom-doped GNRs based on the success in the molecular cases. We hope that this Account will further stimulate the synthesis and applications of heteroatom-dopednanographenes with a combined effort from different disciplines.
Since the isolation of single graphene layers by Geim and Novoselov,[1] graphene has opened up tremendous opportunities
for materials science because of its extraordinary properties and
broad applications.[2−5] In particular, the ultrahigh charge-carrier mobility of graphene
is extremely appealing for electronic devices; however, the use of
graphene as the active layer in field-effect transistors (FETs) is
hindered by the lack of an electronic band gap because the devices
cannot be switched off.[6] This disadvantage
can be overcome by reduction in the dimensionality of graphene, generating
quasi-zero-dimensional graphene quantum dots (GQDs) and quasi-one-dimensional
graphene nanoribbons (GNRs) (Figure ).[5,7] Because of quantum confinement,
these nanoscale graphenes (nanographenes) are promising for next-generation
semiconductor applications with finite band gaps.[8,9] The
fabrication of nanographenes is often accomplished through top-down
methods such as “cutting” of graphene and carbon nanotubes.[5] The applications of nanographenes, for example,
in electronic devices, catalysis, bioimaging and sensing, have also
been demonstrated.[8,10] However, the top-down approach
cannot accurately control the size and edge structure, which are highly
relevant to the physical and chemical properties of nanographenes.
Therefore, control of the nanographene structure at the atomic level
is required to achieve reliable structure–property correlations
and desired functions.[5] This goal can be
realized through bottom-up syntheses starting with molecular precursors,
and this approach illustrates how organic chemists can contribute
to the materials science of nanographenes, providing atomically precise
GQDs (e.g., nanographene molecules) and GNRs.[11,12] The capability to precisely control nanographene structures further
promotes the creation of emergent materials such as magnetic GNRs
and topological insulators by rational molecular design.[13−15]
Figure 1
Schematic
illustration of graphene and its nanoscale subunits (i.e.,
nanographenes), including nanographene molecules (atomically precise
graphene quantum dots) and graphene nanoribbons.
Schematic
illustration of graphene and its nanoscale subunits (i.e.,
nanographenes), including nanographene molecules (atomically precise
graphene quantum dots) and graphene nanoribbons.Atomic doping is a common strategy to tune the properties of inorganic
materials, for instance, in silicon-based semiconductor industry:
doping of silicon with group III or group V elements can achieve p-doped
or n-doped semiconductors, respectively. The atomic doping strategy
is also essential to nanographene materials through incorporation
of heteroatoms into the graphenic carbon network, effectively modulating
the electronic, magnetic, and catalytic properties.[16] Again, the bottom-up method is indispensable to achieve
atomic precision not only in terms of the size and edge structure
but also with regard to the heteroatom type, doping position, and
concentration. This accuracy is an indispensable tool for controlling
the physical properties and revealing structure–property relationships.[11,12] In addition, structurally well-defined heteroatom-dopednanographenes
are intriguing semiconducting materials. The heteroatoms in the nanographene
framework provide more opportunities for materials development (i)
by modulating the band gap and thus the photophysical properties,
(ii) by offering rich electrochemical activities, (iii) by installing
coordinating sites for metals, and (iv) by stabilizing charges and
spins in the carbon skeleton.[16] Nevertheless,
large nanographene molecules and GNRs incorporating various heteroatoms
(e.g., B,[17] N,[18,19] O,[20] S,[21] and
P[22]) are still scarce.[16]Our group has been working on the synthesis, characterization,
and application of nanographenes during the past decades. In 1995
we reported the synthesis of alkyl-substituted hexa-peri-hexabenzocoronene (HBC) 1b,[23] which has a diameter of over 1 nm and can thus be regarded as a
nanographene molecule (Figure a).[5,7] Since this seminal work, we have synthesized
various HBC derivatives and other larger nanographene molecules by
means of a general synthetic strategy, namely, cyclodehydrogenation
of polyphenylene precursors (e.g., hexaphenylbenzene 2, Figure a) to afford
planarized products.[24] The alkyl substituents
not only impart solubility and solution processability to the disc-shaped
nanographene molecules but also induce the formation of columnar liquid-crystalline
mesophases (Figure b).[24] Charges can therefore be transported
through the columnar π–π stacking channel, which
is a special concept for FETs and photovoltaic devices.[25−27] We have further extended the synthetic strategy to achieve atomically
precise GNRs through conventional solution chemistry and modern on-surface
syntheses.[28] These advances have been reviewed
in our previous contributions.[5,7,11,12,24,28] In this Account, we focus on our works toward
heteroatom-dopednanographenes, which have yet been comprehensively
summarized. In the following, we will discuss the design, synthesis,
properties, and future opportunities of the research on heteroatom-dopednanographene molecules and GNRs.
Figure 2
(a) Synthesis of HBCs from the corresponding
hexaphenylbenzene
precursors via cyclodehydrogenation. (b) Columnar self-assembly of
disc-shaped nanographene molecules. Reproduced from ref (24). Copyright 2007 American
Chemical Society.
(a) Synthesis of HBCs from the corresponding
hexaphenylbenzene
precursors via cyclodehydrogenation. (b) Columnar self-assembly of
disc-shaped nanographene molecules. Reproduced from ref (24). Copyright 2007 American
Chemical Society.
From HBC
to Heteroatom-Doped HBC Derivatives
Nitrogen-Doped
Nanographene Molecules
Following the synthetic strategy of
HBCs, it is easy to imagine the
possibility of incorporating heteroatoms into the HBC skeleton by
replacing the outer phenyl groups with other heteroaromatic rings
in the hexaarylbenzene precursor (Figure a). Indeed, Draper et al. synthesized the
first N-dopedHBC 4 in 2002 through cyclodehydrogenation
of the corresponding pyrimidine-substituted precursor 3 (Figure b).[29] The incorporation of pyrimidine rings endowed
the nanographene molecule with electron-accepting properties compared
with the parent HBC. Furthermore, the N atoms in the bay region served
as a coordinating site with transition metals (e.g., PdII and RuII).[30] Not surprisingly,
such metal complexes displayed profoundly changed absorption and emission
features.
Figure 3
(a) General synthetic route to heteroatom-doped HBC analogues.
(b) Synthesis of N-doped HBC 4 incorporating pyrimidine
rings. (c) Synthesis of hexapyrrolohexaazacoronenes 6 incorporating pyrrole rings. (d) Several N-doped HBC analogues with
a mixture of benzene and pyrrole rings. (e, f) Extensions of the hexapyrrolohexaazacoronene
family, as exemplified by compounds 10–14.
(a) General synthetic route to heteroatom-dopedHBC analogues.
(b) Synthesis of N-dopedHBC 4 incorporating pyrimidine
rings. (c) Synthesis of hexapyrrolohexaazacoronenes 6 incorporating pyrrole rings. (d) Several N-dopedHBC analogues with
a mixture of benzene and pyrrole rings. (e, f) Extensions of the hexapyrrolohexaazacoronene
family, as exemplified by compounds 10–14.To develop electron-donating HBC
analogues, in 2007 our group reported
the synthesis and properties of hexapyrrolohexaazacoronenes 6 through oxidative cyclodehydrogenation of hexapyrrolylbenzene
precursors 5 (Figure c).[31] The peripheral benzene
rings were formally replaced with six pyrroles, providing a π
skeleton isoelectronic to that of HBC. The interior nitrogens played
an important role in stabilizing the oxidation states, and thereby,
the dication of 6c was generated by chemical oxidation
and isolated under ambient conditions. Later on, together with Takase,
Nishinaga, and co-workers, we extended the family of pyrrole-fused
HBC analogues by incorporating a mixture of phenyl and pyrrolyl groups
in the hexaarylbenzene precursors (Figure d).[32] This unique
class of molecules has attracted great interest from other groups.
For example, Takase, Uno, and co-workers made further modifications
by changing the peripheral aryl moieties (compounds 10 and 11) or by extending the benzenecore to naphthalene
(compound 12) (Figure e).[33−35] Stępień et al. reported disc-shaped
naphthalene monoimide-fused hexapyrrolohexaazacoronene 13 as well as an interesting derivative 14 containing
five-, six-, and seven-membered rings, obtained from an indole-containing
precursor (Figure f).[36,37]As pyrimidine and pyrrole are both
6π aromatic heterocycles,
incorporation of these rings into nanographene molecules does not
change the aromatic nature because the number of π electrons
is unchanged. From a chemistry perspective, we were interested in
designing a new class of nanographene molecules involving antiaromatic
rings that would lead to low energy gaps between the highest occupied
molecular orbital (HOMO) and the lowest unoccupied molecular
orbital (LUMO) as well as excellent redox properties.[38] In 2017, together with Auwärter, Barth,
Palma, and co-workers, we conceived an azomethine ylide homocoupling
strategy to achieve the synthesis of pyrazine-embedded HBC 15, which possessed an 8π central ring through the introduction
of a pyrazinecore instead of a benzenecore (Figure a).[39] After deprotonation
of dibenzo-9a-azaphenalene salts 16, polycyclic azomethine ylides (PAMYs) 17 were generated
in situ with several existing resonance structures, including the
zwitterionic and diradical forms (Figure d). The PAMYs were highly reactive and underwent
dimerization in solution upon heating to afford “dimers” 18. Oxidative dehydrogenation of 18b in a sealed
NMR tube under exclusion of air gave N-dopedhexabenzoperylene 19, but further cyclodehydrogenation in solution was unsuccessful.
Nevertheless, the on-surface method enabled the synthesis of the fully
fused N-dopedHBC 15 through dimerization and concomitant
cyclodehydrogenation on Ag(111) under ultrahigh vacuum (UHV) using
dibenzo-9a-azaphenalene salt 16a as
the precursor. The chemical structure of 15 was unambiguously
characterized by high-resolution scanning tunneling microscopy (STM)
and noncontact atomic force microscopy (nc-AFM) with a CO-functionalized
tip (Figure b,c).
Density functional theory (DFT) calculations at the B3LYP/6-311G(d,p)
level revealed a significantly narrowed HOMO–LUMO gap of 15 (2.06 eV) compared with that of the pristine HBC 1a (3.57 eV), suggesting that the introduction of antiaromatic
rings could be an effective way to tune the HOMO–LUMO gap and
develop low-energy-gap nanographene materials.
Figure 4
(a) Chemical structures
of aromatic HBC 1a and antiaromatic
pyrazine-embedded HBC 15. (b) STM and (c) nc-AFM images
of 15. Scale bars: 2 Å. A molecular model is partially
superimposed on the STM image, and a white arrow pointing to the N
atoms indicates the molecular symmetry axis. Reproduced with permission
from ref (39). Published
by Springer Nature. (d) Synthetic route to 15. TBA, tri-n-butylamine; DMSO, dimethyl sulfoxide; DDQ, 2,3-dichloro-5,6-dicyano-1,4-benzoquinone.
(a) Chemical structures
of aromaticHBC 1a and antiaromaticpyrazine-embedded HBC 15. (b) STM and (c) nc-AFM images
of 15. Scale bars: 2 Å. A molecular model is partially
superimposed on the STM image, and a white arrow pointing to the N
atoms indicates the molecular symmetry axis. Reproduced with permission
from ref (39). Published
by Springer Nature. (d) Synthetic route to 15. TBA, tri-n-butylamine; DMSO, dimethyl sulfoxide; DDQ, 2,3-dichloro-5,6-dicyano-1,4-benzoquinone.
Sulfur-Doped Nanographene
Molecules
Incorporation of thiophene rings into the polyphenylene
precursors
results in S-dopednanographene molecules after cyclodehydrogenation.
In 2007 we synthesized tribenzothiophene-fused HBC 21a as the first example of S-dopednanographene molecules through cyclodehydrogenation
of the C3-symmetric precursor 20a (Figure a).[40] Recently, the tribenzothiophene-fused HBCcore
of 21a was derivatized by attaching alkoxy and alkyl
chains (21b and 21c) to ensure good solubility
and to tune their HOMO and LUMO levels.[41] Remarkably, the electron-rich thiophene rings in the alkyl-substituted
tribenzothiophene-fused HBC 21c could be oxidized into
electron-deficient thiophene-S,S-dioxide moieties, greatly lowering both the HOMO and LUMO levels
by about 0.5 eV and representing an appealing feature of thiophene
incorporation. In 2011, Draper et al. described another way of introducing
thiophene rings in S-dopedHBC analogue 24 (Figure b).[42] During the oxidative cyclodehydrogenation, dimerization
of 24 was also observed via intermolecular oxidative
coupling at the thiophene α-position.
Figure 5
Syntheses of S-doped
nanographene molecules. m-CPBA, m-chloroperoxybenzoic acid.
Syntheses of S-dopednanographene molecules. m-CPBA, m-chloroperoxybenzoic acid.Apart from the above-mentioned
method through cyclodehydrogenation
of suitable precursors to incorporate thiophene rings, we have also
developed a postfunctionalization strategy to fuse thiophenes onto
the HBCcore based on edge-perchlorinated HBC 26.[43] A thiolation reaction was performed to provide
trithiophene-annelated HBCs 27 in 35–50% yield
and dithiophene-annelated products 28 in 1.5–3%
yield (Figure ).[44] Furthermore, Tan, Zheng, and co-workers employed 27a as hole-transporting material (HTM) in perovskite solar
cells, providing the best efficiency of 12.8%, which could be improved
to 14.0% through further device optimization.[45] Further studies indicated that 27a endowed the devices
with enhanced stability compared with the well-established HTM 2,2′,7,7′-tetrakis[N,N-bis(4-methoxyphenyl)amino]-9,9′-spirobifluorene
(Spiro-OMeTAD). In addition, together with Wu, Feng, and co-workers,
we used nanographene molecule 27a as a precursor to fabricate
ultrathin S-dopedgraphene films, which were found to be applicable
to ultrahigh-rate microsupercapacitors.[46]
Figure 6
Synthesis
of S-doped nanographene molecules 27 and 28 via postfunctionalization of perchlorinated HBC 26.
DMI, 1,3-dimethyl-2-imidazolidinone. The single-crystal structure
of perchlorinated HBC 26 was reproduced with permission
from ref (43). Copyright
2013 Macmillan Publishers Ltd.
Synthesis
of S-dopednanographene molecules 27 and 28 via postfunctionalization of perchlorinated HBC 26.
DMI, 1,3-dimethyl-2-imidazolidinone. The single-crystal structure
of perchlorinated HBC 26 was reproduced with permission
from ref (43). Copyright
2013 Macmillan Publishers Ltd.Intrigued by the beautiful structure of contorted hexa-cata-hexabenzocoronene (29) (Figure a)[47] as well as
its partially thiophene-substituted analogues such as
dibenzotetrathienocoronenes 30 (Figure b) reported by Nuckolls et al.,[48] we synthesized two fully thiophene-fused coronenes,
that is, hexathienocoronenes (HTCs) 31 and 32a–c (Figure c,d).[49] HTCs 31 and 32a–c exhibited almost identical
absorption features and a highly electron-rich nature with higher
HOMO levels compared with 30. Single-crystal X-ray analysis
revealed a columnar π-stacking structure of HTC 32b. A discotic liquid-crystalline phase was observed for HTC 32c with longer dodecyl chains. Together with Chen et al.,
we employed the backbone of HTC 32a to form a gemini-type
amphiphile by attaching hydrophobic and hydrophilic side chains on
opposite sides of the aromaticcore.[50] The
obtained amphiphilic molecule 32d self-assembled into
nanofibers in solution. After chemical oxidation with nitrosonium
tetrafluoroborate (NOBF4), the nanofibers became electroconductive
with a resistivity of 1.1 MΩ, which is lower than the value
for the amphiphilic HBC nanotubes (2.5 MΩ).[51]
Figure 7
Chemical structures of (a, b) hexa-cata-hexabenzocoronene
(29) and dibenzotetrathienocoronenes 30 as
well as (c, d) hexathienocoronenes 31 and 32.
Chemical structures of (a, b) hexa-cata-hexabenzocoronene
(29) and dibenzotetrathienocoronenes 30 as
well as (c, d) hexathienocoronenes 31 and 32.
Heteroatom
Doping on the Zigzag Edges
The edge topologies of nanographene
molecules, such as armchair
and zigzag structures (Figure ), are essential to their chemical and physical properties.[12] The majority of bottom-up-synthesized nanographene
molecules have armchair edges, as represented by HBC and its derivatives.
Although relatively rare, zigzag-edged nanographene molecules are
particularly appealing, as they often have low HOMO–LUMO gaps
and an open-shell ground state with long zigzagperipheries.[52] Despite the appealing characteristics of zigzag-edged
nanographene molecules, their syntheses and characterizations are
largely hampered by their instability under ambient conditions. On
the one hand, replacement of the all-carbonzigzag edges with isostructural
heteroatoms provides new access to stable nanographene molecules featuring
zigzag architectures. On the other hand, heteroatom-dopedzigzag edges
are often theoretically considered as active sites in electrochemical
catalysts for the oxygen reduction and hydrogen evolution reactions.[53,54] The synthesis of nanographene molecules having such edge structures
can thus provide atomically precise models for investigating the electrocatalytic
mechanism.
Figure 8
Schematic illustration of armchair and zigzag edge structures of
nanographene molecules.
Schematic illustration of armchair and zigzag edge structures of
nanographene molecules.Inspired by the high
performance of N-dopedgraphene-based materials
for electrocatalysis, we synthesized dibenzo-9a-azaphenalene 35 as a model compound to study the catalytic activity of
N-dopedzigzag edges. Although we could not demonstrate a reasonable
activity of 35 in electrocatalysis, we further achieved
the synthesis of the linearly extended “dimer” 38 (Figure ), indicating the potential of further extension toward the corresponding
GNRs.[55] The PAMY unit in 35 was highly reactive, stemming from its diradical and zwitterionic
resonance structures (Figure d). Therefore, compounds 35 and 38 were generated only under inert conditions by deprotonation of their
charged precursors 34 and 37. In addition,
because of the extremely high chemical reactivity of the N-dopedzigzag
edges, the dibenzo-9a-azaphenalene-based PAMY offered
a new entry to internally N-dopednanographene molecules through 1,3-dipolar
cycloaddition with dipolarophiles.[56] This
chemical reactivity was also independently exploited by Ito, Tokimaru,
and Nozaki[57] and used for syntheses of
azapentabenzocorannulene derivatives.[58,59]
Figure 9
Synthesis of
N-doped zigzag peripheries 35 and 38.
Synthesis of
N-dopedzigzagperipheries 35 and 38.We have also considered the incorporation of multiple
heteroatoms
to obtain stable heteroatom-dopedzigzag edges and deeper insights
into the effects of doping on the chemical and physical properties.
Together with Zhang, Feng, and co-workers, we conceived nitrogen–boron–nitrogen
(NBN)-dopedzigzagperipheries based on 1,9-diaza-9a-boraphenalene as the next structural motif.[60] Both monomers 40 and the linearly fused “dimer” 45 were synthesized through electrophilic borylation (Figure ). The NBN-dopedzigzag edges exhibited high chemical stability, allowing for electrophilic
bromination of 40b and further modifications through
cross-coupling reactions to give 42 (Figure a). Furthermore, chemical
oxidation of monomers 40 led to σ dimers 43 connected at the positions para to the
N atoms. To avoid such a dimerization reaction during oxidation, the
active positions were protected by additional phenyl substituents
(i.e., compound 42). Clean single-electron oxidation
of the NBN-dopedzigzagperipheries to afford radical cation 42•+ was demonstrated by in situ spectroelectrochemistry,
shedding light on the photophysical perperties of its isoelectronic
dibenzophenalenyl radical.
Figure 10
Synthesis of NBN-doped zigzag peripheries based
on the 1,9-diaza-9a-boraphenalene motif. (a) Synthetic
route to monomers 40 and further derivatizations.
(b) Synthetic route to “dimer” 45.
NBS, N-bromosuccinimide; o-DCB, o-dichlorobenzene.
Synthesis of NBN-dopedzigzagperipheries based
on the 1,9-diaza-9a-boraphenalene motif. (a) Synthetic
route to monomers 40 and further derivatizations.
(b) Synthetic route to “dimer” 45.
NBS, N-bromosuccinimide; o-DCB, o-dichlorobenzene.In parallel to the studies on heteroatom-dopednanographene molecules,
we also tried to tackle the syntheses of peri-acenes (e.g., peri-tetracene[61,62] and peri-pentacene[63]), which comprise two acenes laterally fused at all of the peri positions and can be viewed as segments of full zigzag
GNRs (Figure ).
It was thus a logical extension to consider the synthesis of heteroatom-dopedperi-acenes as the next targets. Our initial attempts to
make NBN-dopedperi-tetracene turned out to be challenging,
and we are still working on different routes to synthesize it, but
we were successful in installing oxygen–boron–oxygen
(OBO) segments on the zigzagperipheries of peri-acenes.
More specifically, we developed a tandem demethylation–borylation
method to construct OBO-fused tetrabenzo[a,f,j,o]perylenes 48 by simple heating of precursors 47 with BBr3 in o-dichlorobenzene (Figure a).[64] Further cyclodehydrogenation of 48 provided the first
heteroatom-dopedperi-tetracenes 49 in
2016, before the all-carbonperi-tetracenes were
achieved in 2018.[65,66] The OBO-dopedperi-tetracene exhibited excellent ambient stability, blue fluorescence,
and a large HOMO–LUMO gap with a low-lying HOMO level compared
with pristine peri-tetracene. The incorporation of
OBO units drastically changed the properties of peri-tetracene, and therefore, isoelectronic heteroatom doping would
be important to maintain the open-shell character of peri-tetracene while improving its stability for potential applications.
It is noteworthy that Hatakeyama et al. independently reported compound 48a obtaind by a different method (Figure b), in which a precursor containing two
extra iodo groups was used to generate 48a in 55% yield.[67] Our method gives higher yields (>90%) and
is
simpler since it is based on direct C–H borylation without
the need for iodo groups in the precursor. It must be noted that Hatakeyama
et al. also independently reported the use of the direct C–H
borylation method to synthesize heteroatom-dopedbenzo[fg]tetracene structures with OBO, NBN, and SBS substitution on the
zigzagperipheries.[68]
Figure 11
Schematic representations
of peri-acenes and heteroatom-doped peri-acene-type nanographene molecules as a segment of full
zigzag GNRs.
Figure 12
(a) Synthesis of OBO-doped peri-tetracenes 49. (b) Another method to synthesize the
uncyclized precursor 48a and an isomer of 48b with different substituent
positions (compound 51). TfOH, trifluoromethanesulfonic
acid.
Schematic representations
of peri-acenes and heteroatom-dopedperi-acene-type nanographene molecules as a segment of full
zigzag GNRs.(a) Synthesis of OBO-dopedperi-tetracenes 49. (b) Another method to synthesize the
uncyclized precursor 48a and an isomer of 48b with different substituent
positions (compound 51). TfOH, trifluoromethanesulfonic
acid.In our pursuit of longer peri-acene-type nanographene
molecules, we synthesized OBO-dopedperi-hexacene
as the longest peri-acene analogue.[69] We first tried to furnish the OBO-fused precursor 54 by our tandem demethylation–borylation method from
1,2,4,5-tetrakis(3-methoxynaphthalen-2-yl)benzene (52) (Figure a), but
the reaction was not successful, probably because of the high reactivity
of naphthalene α-positions during the electrophilic borylation.
Therefore, we adopted Hatakeyama’s method by introducing iodo
groups on the central benzene to synthesize 1,4-diiodo-2,3,5,6-tetrakis(3-methoxynaphthalen-2-yl)benzene
(53). After lithiation and reaction with BBr3, the OBO-fused precursor 54 was obtained in 43% yield
(Figure a). However,
oxidative cyclodehydrogenation of 54 in solution did
not provide the planarized product after attempts under different
conditions. We thus employed on-surface synthesis in collaboration
with Fasel et al. and achieved the OBO-dopedperihexacene 55 on Au(111) by heating precursor 54 at 380 °C under
UHV (Figure a).
The structure of 55 was unambiguously characterized by
STM and nc-AFM (Figure b,c). Furthermore, OBO-dopedperi-hexacene 55 formed two kinds of 1D superstructures via intermolecular
hydrogen bonding and metal coordination with the OBO segments on the
zigzag edges (Figure b,d), demonstrating a potential edge-doping strategy for engineering
self-assembled structures of graphene nanoarchitectures.
Figure 13
(a) Synthetic
route to OBO-doped peri-hexacene 55.
(b) STM and (c) nc-AFM images of 55 on a
Au(111) surface. (d) Schematic illustration of molecular assembly
via metal coordination and O···H hydrogen bonding.
Reproduced from ref (69). Copyright 2017 American Chemical Society.
(a) Synthetic
route to OBO-dopedperi-hexacene 55.
(b) STM and (c) nc-AFM images of 55 on a
Au(111) surface. (d) Schematic illustration of molecular assembly
via metal coordination and O···H hydrogen bonding.
Reproduced from ref (69). Copyright 2017 American Chemical Society.The OBO-fused precursor 54 featured a double [5]helicene
substructure, which underwent a conformational change upon interactions
with the surface.[69] On the other hand,
in the crystal structure of double [5]helicene 48a, we
observed a pair of (P,P) and (M,M) enantiomers in one unit cell.[64] Hatakeyama et al. separated the enantiomers
of such a double [5]helicene through the incorporation of bulky tert-butyl groups (compound 51) to increase
the isomerization energy barrier.[67] The
interesting properties of double helicenes inspired us to further
push the limit of double helicene synthesis and to explore their chiroptical
properties. By adjusting the connectivity of the naphthalene rings,
we synthesized the first double [7]helicene 57 (Figure a),[70] which is an isomer of the π-extended OBO-fused
double [5]helicene 54. Compound 57 was obtained
in 7% yield through a tandem demethylation–borylation reaction
of 1,2,4,5-tetrakis(2-methoxynaphthalen-1-yl)benzene (56). The isolated yield is apparently lower than those of compounds 48 (over 90%), presumably because of the high strain built
up during the ring closure. Single-crystal X-ray diffraction revealed
substantial π overlap between the terminal benzene rings (Figure b). Compound 57 exhibited excellent chiral stability, which facilitated
the optical resolution of the enantiomers by chiral HPLC. The separated
(P,P) and (M,M) isomers displayed opposite responses in circular dichroism
spectra (Figure c). The successful synthesis of the first double [7]helicene with
OBO incorporation demonstrated the efficacy of the tandem demethylation–borylation
method in the synthesis of even strained architectures, stimulating
more efforts toward longer double helicenes and opening up a new avenue
to chiral synthetic nanographenes.
Figure 14
(a) Synthetic route to OBO-fused double
[7]helicene 57. (b) Single-crystal structures of the
(M,M) and (P,P) isomers.
(c) Circular dichroism spectra of the (M,M) and (P,P) isomers.
Reproduced from ref (70). Copyright 2016 American Chemical Society.
(a) Synthetic route to OBO-fused double
[7]helicene 57. (b) Single-crystal structures of the
(M,M) and (P,P) isomers.
(c) Circular dichroism spectra of the (M,M) and (P,P) isomers.
Reproduced from ref (70). Copyright 2016 American Chemical Society.To examine the scope of the tandem demethylation–borylation
reaction, we tested the direct C–H borylation reactivity toward
the chemically inert 2- and 7-positions of pyrene (Figure ).[71] We found that the tandem reaction readily occurred under typical
conditions, generating a new kind of oxaborin-annelated pyrene-based
chromophores (60 and 63) in excellent yields
(>95%). The singly annelated compound 60 displayed
strong
blue fluorescence (λmax = 442 nm, ΦF = 70%), whereas the doubly annelated product 63b resembled
perylene diimide (PDI) dyes in terms of bright green fluorescence
(λmax = 525 nm, ΦF = 84%) and strong
aggregation tendency in solution. The tandem demethylation–borylation
reaction thus provided a new method for π extension of pyrene
to obtain novel photonic and optoelectronic materials.
Figure 15
Synthetic
routes to oxaborin-annelated pyrene derivatives 60 and 63 and their solutions in CHCl3 under UV light
(365 nm). Images were reproduced with permission
from ref (71). Copyright
2018 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.
Synthetic
routes to oxaborin-annelated pyrene derivatives 60 and 63 and their solutions in CHCl3 under UV light
(365 nm). Images were reproduced with permission
from ref (71). Copyright
2018 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.
Toward Heteroatom-Doped Graphene Nanoribbons
The studies of the nanographene molecules have paved the way to
heteroatom-doped GNRs by offering model cases. For example, when we
established the surface-assisted synthesis of atomically precise GNRs
together with Fasel et al. in 2010, we fabricated chevron-type GNR 65 from 6,11-dibromo-1,2,3,4-tetraphenyltriphenylene precursor 64 (Figure a,b).[72] The chevron-type GNR comprises
HBC units that are fused side by side. Therefore, considering the
many heteroatom-dopedHBC analogues as described previously, one could
easily imagine synthesizing heteroatom-doped chevron-type GNRs by
modifying the triphenylene-based molecular precursors. Among the various
possibilities, N doping is particularly interesting, as it can effectively
lower the valence and conduction bands to afford n-type semiconductors.
In 2013, Bronner, Hecht, Tegeder, and co-workers synthesized N-doped
chevron-type GNRs 67 by replacing one or two phenyl rings
with 4-pyridinyl groups in the monomers (Figure c).[73] Compared
with the pristine chevron-type GNR 65, the introduction
of N atoms simultaneously lowered the valence and conduction bands,
leaving the band gaps nearly unchanged. In 2014, together with Du,
Gao, and co-workers, our group reported N-doped GNR 67b fabricated on Au(111) under UHV and investigated its structure by
high-resolution STM.[74] Different from its
all-carboncounterpart 65, the N-doped GNR 67b exhibited a side-by-side alignment due to the inter-ribbon N···H
interactions (Figure d). In the same year, together with Fasel et al., we reported the
on-surface synthesis of GNR heterojunction 69 comprising
alternating pristine and N-doped GNR segments (Figure e–g).[75] The incorporation of N atoms was accomplished by replacing two phenyl
groups with 5-pyrimidinyl rings in the triphenylene-based precursor
to give monomer 68. The resulting GNR heterojunction 69 displayed a band offset of about 0.5 eV, representing the
first GNR-based p–n junction and indicating great potential
for future applications in nanoelectronics.
Figure 16
(a) Surface-assisted
synthesis of chevron-type GNR 65. (b) STM image of GNR 65 on a Au(111) surface. Reproduced
with permission from ref (72). Copyright 2010 Macmillan Publishers Ltd. (c) Surface-assisted
synthesis of N-doped chevron-type GNRs 67. (d) High-resolution
STM image of GNR 67b, displaying a side-by-side alignment
due to inter-ribbon N···H interactions. Reproduced
with permission from ref (74). Copyright 2014 AIP Publishing LLC. (e) Surface-assisted
synthesis of GNR heterojunction 69. (f, g) STM images
of GNR heterojuction 69, with N-doped and pristine GNR
segments highlighted in blue and light-gray dashed lines, respectively.
Reproduced with permission from ref (75). Copyright 2014 Macmillan Publishers Ltd.
(a) Surface-assisted
synthesis of chevron-type GNR 65. (b) STM image of GNR 65 on a Au(111) surface. Reproduced
with permission from ref (72). Copyright 2010 Macmillan Publishers Ltd. (c) Surface-assisted
synthesis of N-doped chevron-type GNRs 67. (d) High-resolution
STM image of GNR 67b, displaying a side-by-side alignment
due to inter-ribbon N···H interactions. Reproduced
with permission from ref (74). Copyright 2014 AIP Publishing LLC. (e) Surface-assisted
synthesis of GNR heterojunction 69. (f, g) STM images
of GNR heterojuction 69, with N-doped and pristine GNR
segments highlighted in blue and light-gray dashed lines, respectively.
Reproduced with permission from ref (75). Copyright 2014 Macmillan Publishers Ltd.N-doping of GNRs in the form of pyridine and pyrimidine
rings lowers
the energies of the valence and conduction bands, whereas the band
gap is nearly unaffected because the lone pair of N atoms is not conjugated
with the GNR π system. In this regard, S doping in the form
of thiophene incorporation is supposed to involve the lone pair in
the π conjugation of GNRs and thus can effectively modulate
the electronic structures and band gaps. Recently, together with Du,
Gao, and co-workers, our group described the on-surface synthesis
of S-doped GNR 71 by employing 6,11-dibromo-1,4-diphenyl-2,3-bis(thien-3-yl)triphenylene
(70) as the monomer (Figure a), that is, by replacing two phenyl rings
with 3-thienyl groups in the typical triphenylene-based monomer.[76] Different from the N-doped chevron-type GNRs,
the rotation of the single bonds connecting thienyl rings and the
triphenylenecore led to different isomers when the precursor was
deposited on the Au(111) surface (Figure b). After polymerization and cyclodehydrogenation
at 450 °C, different S-doped GNR segments were obtained (Figure c–e), giving
rise to a sequence of tunable band gaps (1.28–1.78 eV), as
confirmed by experimental STM and scanning tunneling spectroscopy
(STS) as well as theoretical calculations. Through molecular engineering
of the triphenylene-based monomers, Fischer et al. further achieved
heteroatom-doped chevron-type GNRs with trigonal-planar S-, N-, and
O-dopant atoms.[77]
Figure 17
(a) Surface-assisted
synthesis of S-doped GNR 71.
(b) Distinct isomers of 70 due to restriction of thienyl
group rotation on Au(111). (c) Schematic illustration of GNR 71 on Au(111). (d) Large-area STM image of GNR 71. (e) High-resolution STM image of GNR 71 with an overlaid
chemical structure. Reproduced with permission from ref (76). Copyright 2017 Tsinghua
University Press and Springer-Verlag GmbH Germany.
(a) Surface-assisted
synthesis of S-doped GNR 71.
(b) Distinct isomers of 70 due to restriction of thienyl
group rotation on Au(111). (c) Schematic illustration of GNR 71 on Au(111). (d) Large-area STM image of GNR 71. (e) High-resolution STM image of GNR 71 with an overlaid
chemical structure. Reproduced with permission from ref (76). Copyright 2017 Tsinghua
University Press and Springer-Verlag GmbH Germany.As we had developed heteroatom-dopedzigzag-edged nanographene
molecules, we subsequently aimed at synthesizing GNRs with heteroatom-dopedzigzag edge topologies. During the past years, although armchair GNRs
have been extensively investigated,[79] zigzag
GNRs have very rarely been achieved (Figure ).[13] Chiral GNRs
with a mixture of armchair and zigzag edges have also attracted great
attention, but the bottom-up-synthesized structures have been limited
only to (3,1)-GNRs (for the definition of the chiral index, see Figure ) obtained from
9,9′-bianthracene-based monomers,[80] calling for further variations of the chiral edge configurations.
Figure 18
Schematic
representation of (a) armchair GNRs, (b) zigzag GNRs,
and (c) chiral GNRs. The edge configuration of chiral GNRs in (c)
is defined by the translation vector C, described as C = na1 + ma2 = (n, m), where a1 and a2 represent the
unit vectors of the graphene lattice. Reproduced from ref (78). Copyright 2018 American
Chemical Society.
Schematic
representation of (a) armchair GNRs, (b) zigzag GNRs,
and (c) chiral GNRs. The edge configuration of chiral GNRs in (c)
is defined by the translation vector C, described as C = na1 + ma2 = (n, m), where a1 and a2 represent the
unit vectors of the graphene lattice. Reproduced from ref (78). Copyright 2018 American
Chemical Society.In 2018, together with
Fasel et al., we reported the surface-assisted
synthesis of the first heteroatom-doped chiral (4,1)-GNR 74 from the rationally designed monomer 6,16-dibromo-9,10,19,20-tetraoxa-9a,19a-diboratetrabenzo[a,f,j,o]perylene (73) containing both boron and oxygen (Figure a). It should be
noted that bottom-up-synthesized GNRs with multiple heteroatom substitution
are still scarce.[81] Monomer 73 was synthesized through tandem demethylation–borylation of
1,4-bis(5′-bromo-2′-methoxyphenyl)-2,5-bis(2′-methoxyphenyl)benzene
(72) bearing two bromo groups. The structure of the chiral
GNRs was characterized by STM and nc-AFM (Figure b–d) as well as Raman spectroscopy.
STS studies and theoretical calculations revealed a larger band gap
of the OBO-doped (4,1)-GNRs compared with the pristine (4,1)-GNRs.
As a result of the OBO units on the edges, lateral assembly of the
chiral GNRs was observed, achieving aligned GNR arrays with different
homochiral and heterochiral inter-ribbon assembly modes (Figure e,f). The first
OBO-doped GNRs suggested that the OBO structures on the edges facilitated
lateral alignment of GNRs, which would be of importance for future
GNR-based devices.
Figure 19
(a) Surface-assisted synthesis of OBO-doped (4,1)-GNR 74. (b) Large-area STM image and (c) high-resolution STM image
of GNR 74 on Au(111). (d) nc-AFM image of GNR 74. (e,
f) Theoretically calculated models of inter-ribbon interactions for
heterochiral and homochiral assemblies of GNR 74, respectively.
Reproduced from ref (78). Copyright 2018 American Chemical Society.
(a) Surface-assisted synthesis of OBO-doped (4,1)-GNR 74. (b) Large-area STM image and (c) high-resolution STM image
of GNR 74 on Au(111). (d) nc-AFM image of GNR 74. (e,
f) Theoretically calculated models of inter-ribbon interactions for
heterochiral and homochiral assemblies of GNR 74, respectively.
Reproduced from ref (78). Copyright 2018 American Chemical Society.
Conclusions and Outlook
We have summarized our works
on heteroatom-dopednanographene molecules
and GNRs during the past decade. On the basis of the prototypical
nanographene molecule HBC, we have explored N doping through the incorporation
of aromatic pyrrole and antiaromaticpyrazine rings. We have also
developed a series of thiophene-annelated HBC derivatives as S-dopednanographene molecules. These results have promoted heteroatom doping
as a powerful method for modulating the energy levels, band gaps,
aromaticity, electron densities, and magnetic properties of nanographene
molecules. Moreover, being aware of the importance of zigzag-edged
nanographene molecules, we have explored heteroatom doping on zigzag
edge structures, including generation of the PAMY as well as NBN and
OBO incorporation. In particular, the OBO-dopedcompounds are easy
to synthesize and are stable under ambient conditions, thereby representing
a new class of nanographene molecules, including stable peri-tetracene and peri-hexacene analogues displaying
intermolecular self-assembly tendency on the surface and double [7]helicene
with high chiral stability as well as new pyrene-based chromophores.
All of these achievements in nanographene molecules have paved the
way to heteroatom-doped GNRs, such as N-doped and S-doped chevron-type
GNRs with tunable band gaps and OBO-doped chiral (4,1)-GNRs with lateral
alignment.Nanocarbon science has attracted increasing interest
in recent
years, giving rise to a variety of carbon nanostructures. The incorporation
of heteroatoms into the carbon frameworks provides a number of new
opportunities to fine-tune the molecular properties. Certainly this
process defines grand challenges in synthesis, thereby requesting
the development of new and efficient synthetic methods. Convincing
cases have been demonstrated in the PAMY chemistry and the tandem
demethylation–borylation reaction, both of which have opened
up new avenues to various heteroatom-dopednanographenes. Furthermore,
the synthesis of heteroatom-doped GNRs is lagging behind that of nanographene
molecules. There is much room to explore new structures such as pyrrole-
and pyrazine-incorporated GNRs and heteroatom-doped full zigzag GNRs.
In any case, close collaborations among chemists, physicists, and
engineers are required to realize the applications of GNRs in future
nanoelectronic and spintronic devices.
Authors: Kang Yuan; Daniel Volland; Sven Kirschner; Marina Uzelac; Gary S Nichol; Agnieszka Nowak-Król; Michael J Ingleson Journal: Chem Sci Date: 2022-01-04 Impact factor: 9.825