| Literature DB >> 29791082 |
Rafal Zuzak1, Ruth Dorel2, Marek Kolmer1, Marek Szymonski1, Szymon Godlewski1, Antonio M Echavarren2,3.
Abstract
A unified approach to the synthesis of the series of higher acenes up to previously unreported undecacene has been developed through the on-surface dehydrogenation of partially saturated precursors. These molecules could be converted into the parent acenes by both atomic manipulation with the tip of a scanning tunneling and atomic force microscope (STM/AFM) as well as by on-surface annealing. The structure of the generated acenes has been visualized by high-resolution non-contact AFM imaging and the evolution of the transport gap with the increase of the number of fused benzene rings has been determined on the basis of scanning tunneling spectroscopy (STS) measurements.Entities:
Keywords: acenes; atomic force microscopy; dehydrogenation; surface chemistry; undecacene
Year: 2018 PMID: 29791082 PMCID: PMC6099251 DOI: 10.1002/anie.201802040
Source DB: PubMed Journal: Angew Chem Int Ed Engl ISSN: 1433-7851 Impact factor: 15.336
Scheme 1Unified approach to higher acenes by on‐surface dehydrogenation of hydroacenes.
Scheme 2Synthesis of tetrahydroacenes 1.
Figure 1On‐surface generation of higher acenes. a,b) Empty state STM images of the Au(111) surface partially covered with a) hydrogen‐protected acene precursors 1 a, 1 b, and 1 d, and kinked isomer 1 d′, and b) heptacene (2), octacene (3), decacene (5) and kinked decacene isomer (5′). Precursor molecules are easily discernible by the presence of two pronounced lobes corresponding to two non‐aromatic rings each containing two methylene groups, exemplary precursors are marked by rectangles: 1 a—violet, 1 b—green, 1 d—blue. Parent acenes in (b) are indicated by rectangles: 2—purple, 3—gray, 5—yellow. Dashed lines in (a) and (b) indicate directions of profile lines shown in (c). After deposition a small fraction of molecules could be found already partially (white contour) or very rarely completely dehydrogenated (red rectangle). White and yellow arrows in (a) and (b) indicate the typical displacement of precursors and frustrated motion of acenes during STM imaging, respectively. Tunneling current 30 pA, bias voltage +2.0 V. c) Profile lines along precursor molecules and parent acenes showing a difference in their STM appearance and evidencing the presence of two pronounced lobes in the topographies of the precursors. d–h) Laplace filtered constant height, frequency shift nc‐AFM images of 2 (d), 3 (e), 4 (f),27 5 (g), and 5′ (h) generated by annealing, scale bar: 5 Å. i) Structural scheme of 5′.
Figure 2On‐surface generation of undecacene (6). Empty state STM images of the Au(111) surface a) with the mixture of undecacene precursors 1 e and 1 e′ and b) subsequently thermally generated parent 6 and kinked undecacene isomer 6′. Tunneling current: a,b) 30 pA, c) 150 pA, bias voltage +2.0 V. c) High‐resolution filled state STM image of 6 with eleven lobes visible along the molecule, tunneling current 30 pA, bias voltage −1.0 V. d–e) Present Laplace filtered constant height, frequency shift nc‐AFM images of 6 (d) and 6′ (e); scale bar: 5 Å.
Figure 3STS measured transport gap for long acenes on Au(111). a) Dependence of the gap on the number of fused benzene rings with the inverse proportionality fit (red curve) and exponential decay (blue curve) for pentacene–decacene data. Values recorded for kinked isomers are displayed by orange triangles.28 b) Transport gap drawn as a function of the inversed number of rings with the linear fit for pentacene–decacene data. Gap values for pentacene29 and hexacene23 are taken from the literature.