Abstract

A major goal of heterogeneous catalysis is to optimize catalytic selectivity. Selectivity is often limited by the fact that most heterogeneous catalysts possess sites with a range of reactivities, resulting in the formation of unwanted by‐products. The construction of surface‐confined covalent organic frameworks (sCOFs) on catalytically active surfaces is a desirable strategy, as pores can be tailored to operate as catalytic nanoreactors. Direct modification of reactive surfaces is impractical, because the strong molecule–surface interaction precludes monomer diffusion and formation of extended architectures. Herein, we describe a protocol for the formation of a high‐quality sCOF on a Pd‐rich surface by first fabricating a porous sCOF through Ullmann coupling on a Au‐rich bimetallic surface on Pd(111). Once the sCOF has formed, thermal processing induces a Pd‐rich surface while preserving the integrity of the sCOF architecture, as evidenced by scanning tunneling microscopy and titration of Pd sites through CO adsorption.

Highlights

  • A major goal of heterogeneous catalysis is to optimize catalytic selectivity

  • This paper describes the construction of surface-confined covalent organic framework scaffolding on a reactive metal surface

  • As we found that the network presents remarkable thermal stability on Au(111), we conjectured that palladium enrichment of the surface could be prompted by thermal annealing whilst preserving the integrity of the surface-confined covalent organic frameworks (sCOFs)

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Summary

The percentage of hexagonal pores is close to that found on

Au(111) by Blunt et al.[2] (50 %) and we can, conclude that the morphology of the sCOF on the alloy is very similar to the one obtained on the Au(111) surface. Islands of periodically arranged close-packed protrusions on top of a MoirØ background were imaged. We interpret these features as bromine adatoms, which are the by-product of the on-surface reaction. The apparent Br–Br interspacing distance is 6.8 Æ 0.1 Š, and the superstructure is rotated approximately 208 from the direction of the MoirØ paptternp These dimensions are consistent with a commensurate ( 7 ” 7)R 19.18 superlattice (see Figure S3 in the Supporting Information). It was not possible to image individual atoms by contrast to the atomically resolved Br island within

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Findings
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