(b) Constant height mode Measure the tunneling current while scanning on a given, smooth x-y-z contour. The z-position (output of feedback loop) is measured.

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Presentation transcript:

(b) Constant height mode Measure the tunneling current while scanning on a given, smooth x-y-z contour. The z-position (output of feedback loop) is measured at discrete (x, y)-positions. line-scan image, grey-scale image or color encoded image. Observe dynamical processes, but increase the risk of crashing the tip

3. STM application & extension (a) Reconstruction in Si(111) The rhombohedral surface unit cell are the corner hole and the 12 maxima, the adatoms. G. Binnig, H. Rohrer, Ch. Gerber, and E. Weibel, Phys. Rev. Lett. 50, 120 (1983)

Si(111) surface-7x7 reconstruction

(b) DNA Fig. a, Unsmoothed, unfiltered plane-subtracted STM image of DNA ~80x120 Å b. Model of the Van der Waals surface of A-DNA derived from X-ray crystallographic data, scaled to a. Robert J. Driscoll, Michael G. Youngquist & John D. Baldeschwieler Nature (1990)

Quantum Corral of 48 iron atoms on copper surface positioned one at a time with an STM tip (corral diameter 14 nm) (c) Atom Manipulation and Surface Standing Wave G. Binnig, H. Rohrer Rev. Mod. Phys. 71, 324 (1999)

(d) STM extension scanning near-field optical microscope (SNOM), atomic force microscope (AFM), Maxwell stress microscopy, scanning electrochemical microscopy et. al.

4.STM in our group Recent work: Surface reconstruction of TiO2 (110) by Ti interstitials STM image of a strand (1.2V; 0.5nA) with the height profiles across (left, dotted line) and along (right) the line defect. K. T. Park, M. H. Pan, V. Meunier, and E. W. Plummer, Phys. Rev. Lett. 96, (2006)

Sr2RuO4: layered perovskite without copper that exhibits superconductivity (A)STM image of a 4 by 4 surface area showing extremely large terraces and steps. (B)Height along the line scan shown in the STM image. (C)Ball model of the bulk unit cell of Sr2RuO4. Red, strontium; blue, oxygen; and green, ruthenium (in the center of the octahedron). R. Matzdorf, Z. Fang, Ismail, Jiandi Zhang, T. Kimura, Y. Tokura, K. Terakura, and E. W. Plummer, Science 289, 746 (2000)

UT STM (SERF 101-E) Frontview Scan range: xy :12 x12 z: 1.5 Resolution: xy: 0.1nm z: 0.01nm

Sample stage

Electronics

STM scanner Applications  Single atom or molecule spectroscopy.  Atomic resolved spectroscopy maps.  The temperature and magnetic field range to study the quantum response of nano-objects.  Optical access to the sample in the magnetic field for probing and exciting atoms or molecules. Low Temperature, High Field STM Scanning Tunneling Microscope with extreme stability under extreme conditions Nature 415, 412 (2002)– Lang and Davis Bi 2 Sr 2 CaCu 2 O 8+  Electronic inhomogeneity: Bi 2 Sr 2 CaCu 2 O 8+  Isolated concrete block with pit Acoustic isolation room Dewar / Magnet Active vibration isolation Growth Chamber Manipulator Analysis chamber Transfer Chamber C 2 H 2, C 2 D 2 Single molecule vibrational spectroscopy: C 2 H 2, C 2 D Science 280, 1732 (1998)---Stipe and Ho 1 K Stage 300 mK Stage Sample Cleaver STM Head Rotation Stage He3 Pot He3 Condensor He4 Pot Heat Switches Tip Triangular sapphire rod Sample Holder Tube scanner Shear stacks Sample A CNMS partner instrument built by ORNL, The University of Tennessee, and The University of Houston Transfer chamber 300 mK stage 1 K stage Rotating STM Sample cleaver Scientific Drivers  Atomically-resolved topography and spectroscopy maps  Quantum response at low T and High B  Real Space---K space Capabilities  Low T mK  High B - 9 Tesla  STM rotates in magnetic field  Cryogenic UHV cleaving  Sample Fabrication in UHV

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