April 22 - 26, 2024
Seattle, Washington
May 7 - 9, 2024 (Virtual)
Symposium Supporters
2024 MRS Spring Meeting
QT05.06.02

Spatially Structuring The Surface Energy of Monolayer Graphene through Selective Heterointerface Engineering

When and Where

Apr 25, 2024
2:00pm - 2:30pm
Room 446, Level 4, Summit

Presenter(s)

Co-Author(s)

Zakaria Al Balushi1,2

University of California, Berkeley1,Lawrence Berkeley National Laboratory2

Abstract

Zakaria Al Balushi1,2

University of California, Berkeley1,Lawrence Berkeley National Laboratory2
Selective bottom-up chemical synthesis of low dimensional quantum materials with high spatial resolution has long been a goal of crystal growers. The challenge, however, lies in the spatial modification of the surface energy landscape of a substrate, a crucial factor that promotes the diffusion and accumulation of adatoms and/or molecules along the surface energy gradient, consequently facilitating nucleation in regions of reduced surface energy. Herein, we demonstrate the achievement of a highly controllable surface energy landscape of monolayer graphene on diamond like carbon (DLC) substrate through a heterointerface containing trapped gallium in a uniquely designed spatial structure. The process involves three steps: (i) spatial-selectively Ga<sup>+</sup> ion implantation into DLC substrate to create “hill” features with a step height of 4 nm; (ii) polymer-free transfer of monolayer graphene on top of Ga<sup>+</sup>-implanted DLC; (iii) <i>in-situ</i> high-vacuum annealing process above 300°C for gallium precipitation at the graphene-DLC heterointerface with low energy electron microscope (LEEM). During the annealing process, both gallium precipitation and gallium-catalyzed reconstruction of the DLC structure contribute to a shift in the local surface work function of graphene, resulting in a decrease in the surface energy of graphene compared to that of pristine graphene. At 300°C, the surface work function difference ( between graphene residing on the “hill” features and unmodulated region is -142 meV, corresponding to a surface energy difference ( between the modulated graphene region and unmodulated region of -0.23 mN/mm. However, at 500°C, is 240 meV with a of -14.5 mN/mm. Notably, this difference remains consistent even upon cooling down to 300°C due to the irreversibility of gallium precipitation. In summary, a surface energy landscape of graphene with a high level of complexity can be realized by carefully tuning annealing conditions and the spatial arrangement of “hill” features, facilitating the selective area growth of materials in various nanofabrication processes.

Keywords

atom probe tomography | neutron scattering | x-ray tomography

Symposium Organizers

Jessica Boland, University of Manchester
Shelly Michele Conroy, Imperial College London
Ismail El Baggari, Harvard University
Juan Carlos Idrobo, University of Washington

Session Chairs

Shelly Michele Conroy
Juan Carlos Idrobo
Suk Hyun Sung

In this Session