2023
DOI: 10.1039/d2na00789d
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Chirality variation from self-assembly on Ullmann coupling for the DBCh adsorbate on Au(111) and Ag(111)

Abstract: On-surface Ullmann coupling has been witnessed as an appealing approach for the precise fabrication of carbon-based covalent nanostructures under the solution-free condition. However, chirality has been seldom discussed in Ullmann...

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Cited by 10 publications
(15 citation statements)
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“…Note that because of the shorter fragment, which separates active centres in a molecule of c28 (two segments), and the presence of the protruding side segments, the resulting chains were less winded, as compared to the tetracene unit from Figure 1 . The structures shown in panel B of the figure were in full agreement with the experimental results obtained recently for the Ullmann coupling of 6,12-dibromochrysene on the Au(111) surface [ 48 ]. The average chain length calculated for rac - c28 was equal to 29.46 (see Figure S2 ).…”
Section: Resultssupporting
confidence: 89%
“…Note that because of the shorter fragment, which separates active centres in a molecule of c28 (two segments), and the presence of the protruding side segments, the resulting chains were less winded, as compared to the tetracene unit from Figure 1 . The structures shown in panel B of the figure were in full agreement with the experimental results obtained recently for the Ullmann coupling of 6,12-dibromochrysene on the Au(111) surface [ 48 ]. The average chain length calculated for rac - c28 was equal to 29.46 (see Figure S2 ).…”
Section: Resultssupporting
confidence: 89%
“…In other words, these interactions, which can be weak or strong, were viewed as not affecting the directionality of the intermolecular connections stabilizing the triangular aggregates. However, the above assumption, even though it may seem too far, was proved to be correct for numerous self-assembling systems of surfaces. , For those real systems adsorbed on such substrates, Au(111), Ag(111), and Cu(111), it was observed that the emerging structures were topologically identical to their theoretical counterparts. The only difference was the relative in-plane rotation/shift of the aggregates with respect to the main lattice directions induced by the mismatch of the overlayer and the substrate.…”
Section: Discussionmentioning
confidence: 99%
“…A great number of chiral assemblies have been studied on metal surfaces, including 0D chiral clusters, [24][25][26][27] 1D chiral chains, stripes or lines, filaments, wires [28][29][30][31][32][33][34] and 2D chiral islands, lamellas structures and honeycomb or more complex nontrivial architectures (chiral Kagome networks, quasicrystals, Sierpiński triangle fractals and semi-regular Archimedean tilings) that may possess intriguing physical and chemical properties. Most of these chiral nanostructures are achieved through shortrange chiral recognition induced by non-covalent intermolecular interactions, such as hydrogen bonding, [24,28,30,31,[34][35][36][37][38][39][40][41][42] halogen bonding, [33,[43][44][45][46] van der Waals (vdW) forces, [47] dipoledipole interactions, [48] metal-organic coordination [33,[49][50][51] or cooperative interactions of two or more sorts of intermolecular forces. [27,29,34,40,[52][53][54][55] In addition, the competition between molecule-molecule an...…”
Section: Chiral Assemblies Induced By Short-range Chiral Recognitionmentioning
confidence: 99%