Imaging electron flow from collimating contacts in graphene
Abstract
The ballistic motion of electrons in graphene opens exciting opportunities for electron-optic devices based on collimated electron beams. We form a collimating contact in a hBN-encapsulated graphene hall bar by adding zigzag contacts on either side of an electron emitter that absorb stray electrons; collimation can be turned off by floating the zig-zag contacts. The electron beam is imaged using a liquid-He cooled scanning gate microscope (SGM). The tip deflects electrons as they pass from the collimating contact to a receiving contact on the opposite side of the channel, and an image of electron flow can be made by displaying the change in transmission as the tip is raster scanned across the sample. The angular half width Δθ of the electron beam is found by applying a perpendicular magnetic field B that bends electron paths into cyclotron orbits. The images reveal that the electron flow from the collimating contact drops quickly at B = 0.05 T when the electron orbits miss the receiving contact. The flow for the non-collimating case persists longer, up to B = 0.19 T, due to the broader range of entry angles. Ray-tracing simulations agree well with the experimental images. By fitting the fields B atmore »
- Authors:
- Publication Date:
- Research Org.:
- Harvard Univ., Cambridge, MA (United States); Pohang Univ. of Science and Technology (POSTECH) (Korea, Republic of); National Institute for Materials Science (NIMS), Tsukuba (Japan)
- Sponsoring Org.:
- USDOE Office of Science (SC), Basic Energy Sciences (BES); National Science Foundation (NSF); National Research Foundation of Korea (NRF); Japan Society for the Promotion of Science (JSPS)
- OSTI Identifier:
- 1437836
- Alternate Identifier(s):
- OSTI ID: 1498664
- Grant/Contract Number:
- FG02-07ER46422; ECCS-1541959; 2015K1A1A2033332
- Resource Type:
- Published Article
- Journal Name:
- 2D Materials
- Additional Journal Information:
- Journal Name: 2D Materials Journal Volume: 5 Journal Issue: 2; Journal ID: ISSN 2053-1583
- Publisher:
- IOP Publishing
- Country of Publication:
- United Kingdom
- Language:
- English
- Subject:
- 36 MATERIALS SCIENCE; graphene; cooled scanning probe microscope; collimation; ballistic electrons; imaging electrons
Citation Formats
Bhandari, S., Lee, G. H., Watanabe, K., Taniguchi, T., Kim, P., and Westervelt, R. M. Imaging electron flow from collimating contacts in graphene. United Kingdom: N. p., 2018.
Web. doi:10.1088/2053-1583/aab38a.
Bhandari, S., Lee, G. H., Watanabe, K., Taniguchi, T., Kim, P., & Westervelt, R. M. Imaging electron flow from collimating contacts in graphene. United Kingdom. https://doi.org/10.1088/2053-1583/aab38a
Bhandari, S., Lee, G. H., Watanabe, K., Taniguchi, T., Kim, P., and Westervelt, R. M. Thu .
"Imaging electron flow from collimating contacts in graphene". United Kingdom. https://doi.org/10.1088/2053-1583/aab38a.
@article{osti_1437836,
title = {Imaging electron flow from collimating contacts in graphene},
author = {Bhandari, S. and Lee, G. H. and Watanabe, K. and Taniguchi, T. and Kim, P. and Westervelt, R. M.},
abstractNote = {The ballistic motion of electrons in graphene opens exciting opportunities for electron-optic devices based on collimated electron beams. We form a collimating contact in a hBN-encapsulated graphene hall bar by adding zigzag contacts on either side of an electron emitter that absorb stray electrons; collimation can be turned off by floating the zig-zag contacts. The electron beam is imaged using a liquid-He cooled scanning gate microscope (SGM). The tip deflects electrons as they pass from the collimating contact to a receiving contact on the opposite side of the channel, and an image of electron flow can be made by displaying the change in transmission as the tip is raster scanned across the sample. The angular half width Δθ of the electron beam is found by applying a perpendicular magnetic field B that bends electron paths into cyclotron orbits. The images reveal that the electron flow from the collimating contact drops quickly at B = 0.05 T when the electron orbits miss the receiving contact. The flow for the non-collimating case persists longer, up to B = 0.19 T, due to the broader range of entry angles. Ray-tracing simulations agree well with the experimental images. By fitting the fields B at which the magnitude of electron flow drops in the experimental SGM images, we find Δθ = 9° for electron flow from the collimating contact, compared with Δθ = 54° for the non-collimating case.},
doi = {10.1088/2053-1583/aab38a},
journal = {2D Materials},
number = 2,
volume = 5,
place = {United Kingdom},
year = {Thu Mar 22 00:00:00 EDT 2018},
month = {Thu Mar 22 00:00:00 EDT 2018}
}
https://doi.org/10.1088/2053-1583/aab38a
Web of Science
Figures / Tables:
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