4.5 Article

Facile characterization of ripple domains on exfoliated graphene

Journal

REVIEW OF SCIENTIFIC INSTRUMENTS
Volume 83, Issue 7, Pages -

Publisher

AMER INST PHYSICS
DOI: 10.1063/1.4737428

Keywords

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Funding

  1. National Research Laboratory (NRL) Program [2008-0060004]
  2. World Class University (WCU) Program [R31-2008-000-10057-0, R-31-2008-000-10055-0]
  3. Nano-Material Technology Development Program [2011-0030228]
  4. Quantum Metamaterials Research Center through the NRF [R11-2008-053-03002-0]
  5. Korea government Ministry of Education, Science and Technology (MEST)
  6. Seoul RBD Program [WR090671]
  7. SRC Centre for Topological Matter through the National Research Foundation (NRF) of Korea [2011-0030787]
  8. Ministry of Education, Science and Technology (MEST) of Korea
  9. Office of Basic Energy Sciences, Division of Materials Sciences and Engineering of the U.S. Department of Energy [DE-AC02-05CH11231]
  10. [KRF-2010-0005390]
  11. Ministry of Education, Science & Technology (MoST), Republic of Korea [KAIST_HR_2012_5] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)
  12. National Research Foundation of Korea [2010-0005390, 2011-0030228, 2011-0030787, 2008-0060004, R31-2012-000-10057-0, 2008-0062164] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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Ripples in graphene monolayers deposited on SiO2/Si wafer substrates were recently shown to give rise to friction anisotropy. High friction appears when the AFM tip slides in a direction perpendicular to the ripple crests and low friction when parallel. The direction of the ripple crest is, however, hard to determine as it is not visible in topographic images and requires elaborate measurements of friction as a function of angle. Here we report a simple method to characterize ripple crests by measuring the cantilever torsion signal while scanning in the non-conventional longitudinal direction (i.e., along the cantilever axis, as opposed to the usual friction measurement). The longitudinal torsion signal provides a much clearer ripple domain contrast than the conventional friction signal, while both signals show respective rotation angle dependences that can be explained using the torsion component of the normal reaction force exerted by the graphene ripples. We can also determine the ripple direction by comparing the contrast in torsion images obtained in longitudinal and lateral scans without sample rotation or complicated normalization. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4737428]

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