Lectures 19: Scanning Tunneling Microscopy

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Lectures 19: Scanning Tunneling Microscopy 1 STM Scanning Tunneling Microscope e2 I = GV G = w h 12 Scanning Tunneling Microscope Heinrich Rohrer Tunneling current starts to flow Gerd Binnig when a sharp tip approaches Nobel Prize 1986 a conducting surface at a distance of approximately 1nm (10Angstrom). The tip is mounted on a piezoelectric tube, which allows tiny movements by applying a voltage at its electrodes. The electronics control the tip position to keep tunneling current and, hence, the tip-surface distance constant, while at the same time scanning a small area of the sample surface. This movement is recorded and can be displayed as an image of the surface topography. Under ideal circumstances, the individual atoms of a surface can be resolved and displayed. 2 Example: fcc and bcc Iron in Films Xe atom on (100)Ni Surface Reconstruction Rearrangement of Atoms at a Surface NiPt The (100)-oriented surface of Ni is a simple square lattice of atoms, Pt atoms form layer on top of the square lattice of the unreconstructed second layer. And this is what the (100) surface of a PtNi alloy looks like at approx. 68% Pt concentration in the first monolayer. What you see in the image is a single bright row of atoms shifted by half an interatomic distance in the direction of the rows (red arrow). These atoms have a hexagonal environment (6 nearest neighbours) in the first monolayer, which is already the same local structure as in the 'hex' reconstruction of pure Pt. 3 Electron Waves and Interference Phenomena of de Broglie waves of electrons Corrals for surface state electrons DoS in the surface band iron atoms on a copper surface. Density Electrons from the tip tunnel of states empty states in the surface band inside (which better coupled to it) metal Quantum 'Mirage' Group of Don Eigler at IBM Almaden Research Center 4.

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