Twisting Between Topological Phases in 1D Conjugated Polymers via a Multiradical Transition State

Author:

Alcón Isaac1ORCID,Canonico Luis Manuel1ORCID,Papior Nick2ORCID,Garcia Jose‐Hugo1ORCID,Cummings Aron W.1ORCID,Tremblay Jean‐Christophe3ORCID,Pruneda Miguel14ORCID,Brandbyge Mads5ORCID,Paulus Beate6ORCID,Roche Stephan17ORCID

Affiliation:

1. Catalan Institute of Nanoscience and Nanotechnology (ICN2) CSIC and BIST Campus UAB Bellaterra Barcelona 08193 Spain

2. Computing Center Technical University of Denmark Kongens Lyngby DK‐2800 Denmark

3. Laboratoire de Physique et Chimie Théoriques CNRS‐Université de Lorraine UMR 7019, ICPM Metz 57070 France

4. Nanomaterials and Nanotechnology Research Centre (CINN) CSIC Avenida de la Vega 4‐6 El Entrego 33940 Spain

5. Department of Physics Technical University of Denmark Kongens Lyngby DK‐2800 Denmark

6. Institut für Chemie und Biochemie Physikalische und Theoretische Chemie Freie Universität Berlin Arnimallee 22 14195 Berlin Germany

7. ICREA Institució Catalana de Recerca i Estudis Avançats Barcelona 08070 Spain

Abstract

AbstractIn recent years, it has become possible via on‐surface bottom‐up synthesis to engineer the topological character of carbon nanostructures. Graphene nanoribbons and 1D conjugated polymers (1DCPs) have thus tailored so as to host either topologically trivial or non‐trivial phases. Molecular design is the primary means to set the topological class of these nanomaterials. However, external control over topology is also demonstrated via electric fields or top‐down hydrogenation. Inspired by the connection between topology and π‐conjugation, here it is demonstrated via first‐principles calculations that aryl ring twist angles also serve as topological knobs. Focusing on rationally designed 1DCPs composed of triarylmethyl (TAM) units, it is shown that rotation of certain aryl rings enables a transition from the trivial to the topologically non‐trivial phase. Accordingly, fixing a particular twist angle configuration (e.g., via chemical functionalization) is equivalent to robustly setting a targeted topological phase. It is also found that in considered 1DCPs, the quantum phase transition occurs without the electronic band gap closing, due to a multiradical antiferromagnetic phase emerging at the transition point. All in all, this study highlights the potential of aryl ring twisting for engineering topological properties in carbon nanomaterials and establishes TAM 1DCPs as exotic topological 1D systems.

Funder

Ministerio de Ciencia e Innovación

Publisher

Wiley

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