Bulletin of the American Physical Society
APS March Meeting 2022
Volume 67, Number 3
Monday–Friday, March 14–18, 2022; Chicago
Session S66: Functional Surfaces, Coatings and Interfaces
8:00 AM–11:00 AM,
Thursday, March 17, 2022
Room: Hyatt Regency Hotel -Grant Park D
Chair: Hao Zeng, SUNY Buffalo
Abstract: S66.00011 : Increasing the Rate of Magnesium Intercalation Underneath Epitaxial Graphene on Silicon Carbide*
10:00 AM–10:12 AM
Presenter:
Jimmy C Kotsakidis
(Monash University)
Authors:
Jimmy C Kotsakidis
(Monash University)
Marc Currie
(U.S. Naval Research Laboratory)
Antonija Grubišić-Čabo
(Monash University)
Anton Tadich
(Australian Synchrotron)
Rachael L Myers-Ward
(U.S. Naval Research Laboratory)
Matthew DeJarld
(U.S. Naval Research Laboratory)
Kevin M Daniels
(University of Maryland)
Chang Liu
(Monash University)
Mark T Edmonds
(Monash University)
Amadeo L Vázquez de Parga
(Autonomous University of Madrid)
Michael S Fuhrer
(Monash University)
D. Kurt Gaskill
(University of Maryland)
Collaborations:
Monash University, U.S. Naval Research Laboratory, University of Maryland, Autonomous University of Madrid, Australian Synchrotron
In this talk, I will briefly overview our recently published works on Mg intercalated graphene, and subsequently, how one can overcome the intercalation challenges posed by Mg. To do this, we laser pattern (ablate) the graphene to form micron-sized discontinuities, and show that this results in a significant increase in the rate of Mg intercalation as observed using low energy electron diffraction and X-ray photoelectron spectroscopy. By modeling Mg intercalation with the Verhulst equation, we are able to empirically compare the intercalation rate between patterned and non-patterned samples. The model implies that the increased intercalation rate is proportional to the increase in edge length from the micron-sized discontinuities. Furthermore, the model and patterning technique we use may be applicable to other intercalated elements or molecules.
*J.C.K. acknowledges the Australian Government Research Training Program and the Monash Centre for Atomically Thin Materials (MCATM) for financial support. J.C.K. and M.S.F. acknowledge funding support from the Australian Research Council (ARC) Laureate Fellowship (FL120100038) and the ARC Centre of Excellence in Future Low-Energy Electronics (CE170100039). A.L.V.P. acknowledges funding support from the Ministerio de Ciencia Innovatión y Universidades project PGC2018-093291-B-I00 and Comunidad de Madrid Project NMAT2D-CM P2018/NMT-4511. D.K.G., R.L.M.-W., M.D., K.M.D., and M.C. acknowledge support by core programs at the U.S. Naval Research Laboratory funded by the Office of Naval Research. This research was undertaken on the soft X-ray beamline at the Australian Synchrotron, part of ANSTO.
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