Superconductivity of K‐Intercalated Epitaxial Bilayer Graphene

ORCID
0000-0001-8365-5472
Affiliation
Institute of Solid State Physics Friedrich‐Schiller‐Universität Jena Helmholtzweg 5 07743 Jena Germany
Huempfner, Tobias;
GND
1216348588
ORCID
0000-0002-2327-5950
Affiliation
Institute of Solid State Physics Friedrich‐Schiller‐Universität Jena Helmholtzweg 5 07743 Jena Germany
Otto, Felix;
GND
140645977
ORCID
0000-0003-0969-9180
Affiliation
Institute of Solid State Physics Friedrich‐Schiller‐Universität Jena Helmholtzweg 5 07743 Jena Germany
Forker, Roman;
ORCID
0000-0002-5790-7653
Affiliation
Department of Physics Friedrich‐Alexander‐Universität Erlangen‐Nürnberg Erwin‐Rommel‐Str. 1 91058 Erlangen Germany
Müller, Paul;
GND
1201693934
ORCID
0000-0001-6904-1909
Affiliation
Institute of Solid State Physics Friedrich‐Schiller‐Universität Jena Helmholtzweg 5 07743 Jena Germany
Fritz, Torsten

Graphene‐based materials are among the most promising candidates for studying superconductivity arising from reduced dimensionality. Apart from doping by twisted stacking, superconductivity can also be achieved by metal‐intercalation of stacked graphene sheets, where the properties depend on the choice of the metal atoms and the number of graphene layers. Many different and even unconventional pairing mechanisms and symmetries are predicted in the literature for graphene monolayers and few‐layers. However, those theoretical predictions have yet to be verified experimentally. Here, it is shown that potassium‐intercalated epitaxial bilayer graphene is a superconductor with a critical temperature of T c  = 3.6 ± 0.1 K. By scanning‐tunneling microscopy and angle‐resolved photoelectron spectroscopy, the physical mechanisms are analyzed in great detail, using laboratory equipment. The data demonstrate that electron–phonon coupling is the driving force enabling superconductivity. Although the consideration of an s‐wave pairing symmetry is sufficient to explain the experimental data, evidence is found for the existence of multiple energy gaps. Furthermore, it is shown that low‐dimensional effects are most likely the cause of a gap ratio of 6.1 ± 0.2 that strongly exceeds the Bardeen‐Cooper‐Schrieffer (BCS) value of 3.52 for conventional superconductors. These results highlight the importance of reduced dimensionality yielding unusual superconducting properties of K‐intercalated epitaxial bilayer graphene.

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