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Why Infrared sSNOM at the Nanoscale?Characterization and IdentificationPolymersSemiconductors7.5um x 7.5um7.5umM. Raschke et. al. ChemPhysChem 2005 A.J. Huber et. al. NanoLett 200850nm x 50nmBiology: Tobacco Mosaic Virus50nm x 50nmBiology: Human Tooth Dentin100nm50nm x 50nmM. Brehm et. al. NanoLett 2006G.O. Andreev – 2011, unpublished6/27/13 Bruker Nano Surfaces 4a
Why Infrared sSNOM at the Nanoscale?Characterization and IdentificationPolymersSemiconductors50nm x 50nmBiology: Tobacco Mosaic Virus~2um Spot7.5um x 7.5um50nm x 50nm7.5umM. Raschke et. al. ChemPhysChem 2005 A.J. Huber et. al. NanoLett 2008Biology: Human Tooth Dentin100nm50nm x 50nmM. Brehm et. al. NanoLett 20066/27/13 Bruker Nano SurfacesG.O. Andreev – 2011, unpublished4b
Page 1: Beating the Diffraction limit by 10
Page 6 and 7: Just how big is a 1000X improvement
Page 8 and 9: Resolution limit in near field opti
Page 10 and 11: Optical contrast in sSNOM for 3D an
Page 12 and 13: How the near field light (E nf ) is
Page 14 and 15: sSNOM results from customers:implem
Page 16 and 17: University of Toronto - Prof. Walke
Page 18 and 19: IntroductionGraphene Discovery, wit
Page 20 and 21: Infrared study of Graphene: rich sp
Page 22 and 23: Let’s probe Graphene’s universa
Page 24 and 25: Colocalized SPM investigation ofGra
Page 26 and 27: sSNOM in universal conductivity reg
Page 28 and 29: Now let’s switch to the plasmonic
Page 30 and 31: sSNOM of Graphene: fast imaging ofp
Page 32: Conclusion• Near field imaging wi

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