The properties of graphene nanoribbons (GNRs)1,2,3,4,5—such as conductivity or semiconductivity, charge mobility and on/off ratio—depend greatly on their width, length and edge structure. Existing bottom–up methods used to synthesize GNRs cannot achieve control over all three of these parameters simultaneously, and length control is particularly challenging because of the nature of step-growth polymerization6,7,8,9,10,11,12,13,14,15,16,17,18. Here we describe a living annulative π-extension (APEX)19 polymerization technique that enables rapid and modular synthesis of GNRs, as well as control over their width, edge structure and length. In the presence of palladium/silver salts, o-chloranil and an initiator (phenanthrene or diphenylacetylene), the benzonaphthosilole monomer polymerizes in an annulative manner to furnish fjord-type GNRs. The length of these GNRs can be controlled by simply changing the initiator-to-monomer ratio, achieving the synthesis of GNR block copolymers. This method represents a type of direct C–H arylation polymerization20 and ladder polymerization21, activating two C–H bonds of polycyclic aromatic hydrocarbons and constructing one fused aromatic ring per chain propagation step.
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This work was supported by the ERATO programme from JST (JPMJER1302 to K.I.), the JSPS KAKENHI (grants JP26810057, JP16H00907, JP17K1955 and JP18H02019 to H.I.), the SUMITOMO Foundation (141495 to H.I.) and the DAIKO Foundation (H.I.). We acknowledge Taoka Chemical Co., Ltd for providing samples. We thank K. Kuwata (Nagoya University) for MALDI–TOF mass measurements; M. Kamigaito and M. Uchiyama (Nagoya University) for measurements of molecular weight by size-exclusion chromatography multi-angle light scattering (SEC-MALS); T. Hashizume (Hitachi Ltd and Tokyo Institute of Technology) for advice on the STM and AFM measurements; C. M. Crudden (Queen’s University and Nagoya University), G. J. P. Perry (Nagoya University) and A. Miyazaki (Nagoya University) for comments and proofreading. Computations were performed at the Research Center for Computational Science, Okazaki, Japan. ITbM is supported by the World Premier International Research Center (WPI) Initiative, Japan.
Nature thanks Lawrence T. Scott and the other anonymous reviewer(s) for their contribution to the peer review of this work.
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Extended data figures and tables
Extended Data Fig. 1 Mass spectroscopy analysis and confirmation of livingness of APEX polymerization.
a, MALDI–TOF mass spectrum (reflection mode) of fjord-type GNR 2 (M n = 1.3 × 104, Đ = 1.23) with trans-2-[3-(4-tert-butylphenyl)-2-methyl-2-propenylidene]malononitrile (DCTB) as the matrix. b, Summary of observed and calculated molecular ion peaks. c, Confirmation of livingness of APEX polymerization by one-pot SEC analyses. d, SEC charts of the reaction progress after 1 h, 3 h and 12 h.
a, Raman spectra of fjord-type GNR 2, obtained with a 532-nm excitation laser. b, Synthesis of model dimer 3b by step-by-step APEX reaction of phenanthrene. c, Synthesis of model dimer 3a by APEX reaction.
Observed 1H NMR spectra of GNR 2 (in Cl2CDCDCl2 at 120 °C) and dimer 3a (in CD2Cl2 at 22 °C). All of the peaks of 3a range from 7.2 to 7.9 p.p.m. Two doublet-of-doublet peaks appear at a higher magnetic field (chemical shift δ = 7.2–7.3 p.p.m.), which are attributed to the most shielded aromatic hydrogen atoms, in the orange-coloured fjord regions. Other aromatic hydrogen atoms in the fjord regions next to the alkyl substituents (red circle) are found as a singlet peak at 7.32 p.p.m. On the other hand, the most deshielded aromatic hydrogen atoms in the bay and cove regions appear at 7.8–7.9 p.p.m. The 1H NMR spectrum of fjord-type GNR 2 shows broadened peaks at 7.0–8.3 p.p.m., which is expected to reflect the repeating helicene structure.
a, Observed IR spectra of GNRs 2 and 5 (blue and red lines) and IR spectrum of tetramer 10 (black line) predicted by DFT calculations at the B3LYP/6-31G(d) level of theory. b, UV-vis absorption spectra of GNRs 2 and 5 (blue and red lines). c, Emission spectra of GNRs 2 and 5 (blue and red lines) excited at 320 nm. d, Raman spectra of GNR 5, obtained by excitation by a 532-nm laser.
a, SEC charts of the crude product of reactions with various I′/M ratios. b, c, M n and M w profiles versus M/I′ and conversion of the monomer in the living APEX polymerization. d, Observed IR spectra of GNR 7 with different polymer lengths (blue, green, yellow and red lines) and IR spectrum of dimer 11 (black line) predicted by DFT calculations at the B3LYP/6-31G(d) level of theory. e, Raman spectra of GNR 7 with different polymer lengths (blue, green, yellow and red lines), obtained with excitation by a 532 nm laser.
a, MALDI–TOF mass spectrum (reflection mode) of fjord-type GNR 7 (M n = 1.2 × 104 Da, Đ = 1.04) with DCTB as the matrix. b, Summary of observed and calculated molecular ion peaks.
a–d, MALDI–TOF mass spectra (reflection mode) of armchair-type GNR 8 (M n = 8.3 × 103 Da, Đ = 1.31) with 7,7,8,8-tetracyanoquinodimethane as the matrix and AgOCOCF3 as an additive. e, Summary of observed and calculated molecular ion peaks. The formation of GNR 8 with M n = 2.4 × 104 Da (Đ = 1.32) was confirmed by MALDI–TOF mass spectroscopy analysis, where 11 distinct mass peaks, each with gaps of m/z = 378 (DP(n) = 21–31), were observed. Around the [M+Ag]+ peaks with n = 25 and 27, mass peaks derived from two additional hydrogen atoms ([M+Ag+2H]+) were clearly observed, which indicates partial completion of the Scholl reaction. f, Efficiency of the transformation reaction to the armchair-type GNR 8 10. According to the literature10, we also estimated the efficiency of cyclodehydrogenation at each observed mass peak by using the theoretical number of lost hydrogen atoms during cyclodehydrogenation (N H(T.)) and the number of lost hydrogen atoms derived from MALDI–TOF mass measurements (N H(R.)) As a result, 96%–100% efficiencies (N H(T.)/N H(R.)) were confirmed at each m/z peak. The highest peak was found at m/z = 10,121.3213 (DP(n) = 26, [M+107Ag]+), which is higher than the PS-based M n, but the top peak DP (DPtop) and the dispersity pattern were almost identical to those of the starting fjord-type GNR 2. No peak corresponding to shorter oligomers or fragments was observed in the full-scale MALDI–TOF mass spectrum (Supplementary Fig. 19). The detection of larger GNRs with a molecular weight of over 20,000 Da appeared to be difficult owing to limitations in the measurement of the highly aggregating flat armchair GNR in the MALDI–TOF mass instrument.
Extended Data Fig. 8 Analytical SEC, UV-vis absorption, emission, IR and Raman spectroscopy data for armchair-type GNR 8.
a, SEC charts of armchair-type GNR 8 obtained by the Scholl reaction of fjord-type GNR 2 with different polymer lengths. b, UV-vis absorption spectra of 8. c, Emission spectra of 8. d, Observed IR spectra of GNR 8 with different polymer lengths (red, yellow, blue and purple lines) and IR spectrum of dimer 11 (black line) predicted by DFT calculations at the B3LYP/6-31G(d) level of theory. e, Raman spectra of GNR 8 with different polymer lengths (red, yellow, blue and purple lines), obtained by excitation by a 532-nm laser.
a, STM image of armchair-type GNR 8 (M n = 2.4 × 104 Da, Đ = 1.32) deposited on HOPG (U = 1.0 V, I = 250 pA, T = 78 K). b, Dimeric assembly model of GNR 8. c, d, Cross-sectional height profile taken perpendicularly (i) and horizontally (ii) with respect to the wire shown in a. The observed substance had about 0.4 nm thickness and 3 nm width, and the repeating peripheral stripes had 0.4–0.5 nm intervals ((i) and (ii)). The existence of this substance was considered as the assembly of two molecules of 8, as depicted in b, and the observed periodicity of 0.4–0.5 nm corresponds to the longitudinal length between the alkyl side chains ((ii) in d). e, AFM phase image of self-assembling GNR 8 (M n = 2.4 × 104 Da, Đ = 1.32) on graphene cleaved on SiO2. f, Magnified AFM phase image of e. g, Cross-sectional height profile taken along the white line in f, perpendicularly to the observed stripe.
This file contains preparation methods for all compounds, methods for spectroscopic analysis and microscopic observations, DFT calculations, Supplementary Figures 1–42, Supplementary Tables 1 and 2, Supplementary Discussion for IR spectra and Supplementary References.
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Yano, Y., Mitoma, N., Matsushima, K. et al. RETRACTED ARTICLE: Living annulative π-extension polymerization for graphene nanoribbon synthesis. Nature 571, 387–392 (2019). https://doi.org/10.1038/s41586-019-1331-z
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