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Silicon Substitution in Nanotubes and Graphene via Intermittent Vacancies

  • Heena Inani
  • , Kimmo Mustonen*
  • , Alexander Markevich
  • , Er Xiong Ding
  • , Mukesh Tripathi
  • , Aqeel Hussain
  • , Clemens Mangler
  • , Esko I. Kauppinen
  • , Toma Susi
  • , Jani Kotakoski
  • *Corresponding author for this work
  • University of Vienna

Research output: Contribution to journalArticleScientificpeer-review

32 Citations (Scopus)
236 Downloads (Pure)

Abstract

The chemical and electrical properties of single-walled carbon nanotubes (SWCNTs) and graphene can be modified by the presence of covalently bound impurities. Although this can be achieved by introducing chemical additives during synthesis, it often hinders growth and leads to limited crystallite size and quality. Here, through the simultaneous formation of vacancies with low-energy argon plasma and the thermal activation of adatom diffusion by laser irradiation, silicon impurities are incorporated into the lattice of both materials. After an exposure of ∼1 ion/nm2, we find Si-substitution densities of 0.15 nm-2 in graphene and 0.05 nm-2 in nanotubes, as revealed by atomically resolved scanning transmission electron microscopy. In good agreement with predictions of Ar irradiation effects in SWCNTs, we find Si incorporated in both mono- and divacancies, with ∼2/3 being of the first type. Controlled inclusion of impurities in the quasi-1D and -2D carbon lattices may prove useful for applications such as gas sensing, and a similar approach might also be used to substitute other elements with migration barriers lower than that of carbon.

Original languageEnglish
Pages (from-to)13136-13140
Number of pages5
JournalJournal of Physical Chemistry C
Volume123
Issue number20
DOIs
Publication statusPublished - 23 May 2019
MoE publication typeA1 Journal article-refereed

Funding

M.T. and T.S. acknowledge the Austrian Science Fund (FWF) project P 28322-N36 for funding, and T.S. and A.M. also the European Research Council (ERC) grant no. 756277-ATMEN. E.I.K., E.D., and A.H. acknowledge the support from the Academy of Finland via projects 286546-DEMEC and 292600-SUPER, from TEKES Finland via projects 3303/ 31/2015 (CNT-PV) and 1882/31/2016 (FEDOC), and the Aalto Energy Efficiency (AEF) Research Program through the MOPPI project. A.M. and T.S. acknowledge the Vienna Scientific Cluster for computer time. J.K., H.I., and K.M. were supported by the FWF project I3181 and the Wiener Wissenschafts-, Forschungs-und Technologiefonds (WWTF) project MA14-009, and K.M. further by the Finnish Cultural Foundation through a grant from the Finnish Postdoc Pool and J.K. through FWF project P31605. H.I. further acknowledges support from the Vienna Doctoral School in Physics.

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