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		    |  | Scanning Probe Microscopy (SPM) | SPM includes a number of techniques for determining physical, electronic, and chemical properties
			of nanomaterials and nanodevices.  In our lab, we focus on developing new SPM modes that can be
			combined with electronic transport measurements to explain the operation of electrical devices. 
 Kelvin probe force microscopy (KPFM) directly images the surface potentials in a device,
			with minimal sample perturbation. KPFM allows us to determine how and where resistance manifests
			itself within a nanoscale device.  We use this technique to spatially resolve electronic dissipation
			due to contact resistances, defect scattering, and electron-phonon interactions.
 
 Scanning gate microscopy (SGM) is a complementary technique that provides additional information
			about the localized sensitivity of nanocircuit to electric fields.  Using the scanning tip, the
			transconductance of a device can be probed to observe inhomogeneities, locally deplete or saturate
			the carrier density in specific regions, and isolate the effect of defects or contact barriers.
			The Collins group has extended SGM into a spectroscopic tool that we use for identifying specific
			electronic states associated with different types of SWNT defects.
 
 
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		    |  | Publications | Mean free paths in single-walled carbon nanotubes measured by Kelvin probe force microscopy E.J. Fuller, D. Pan, B.L. Corso, O.T. Gül & P.G. Collins
			Phys. Rev. B 89, 245450 (2014).
 
 Quantitative Kelvin Probe Force Microscopy of Current-Carrying Devices
 E.J. Fuller, D. Pan, B.L. Corso, O.T. Gul, J.R. Gomez & P.G. Collins,
			Appl. Phys. Lett. 102, 083503-5 (2013).
 
 Distinguishing Carbon Nanotube Defect Chemistry Using Scanning Gate Spectroscopy
 S.R. Hunt, E.J. Fuller, B.L. Corso & P.G. Collins
			Phys. Rev. B 85, 235418 (2012).
 
 Scanning Gate Spectroscopy and Its Application to Carbon Nanotube Defects
 S.R. Hunt, D. Wan, V.R. Khalap, B.L. Corso & P.G. Collins,
			Nano Lett. 11, 1055-60 (2011).
 
 
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		    |  | Acknowledgements | 
			| This research is financially supported by the NSF. |  | 
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  AFM and KPFM images along a SWNT at three different biases.
 
  
    Composite images of topography (grey) and SGM (red), showing that semiconducting SWNTs can have
			uniform transconductance due to bandstructure, or concentrated transconductance due to
			Schottky barriers.
 
  
  When defects are present, they provide a third, localized type of transconductance.
 
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