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ULTIMATE COMPUTING - Quantum Consciousness Studies

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NanoTechnology 193<br />

Figure 10.2: Nanoscale view of substrate to STM tip electron tunneling. By Paul<br />

Jablonka (Schneiker and Hameroff, 1987).<br />

Mode Number I II III IV<br />

Quantity held constant i, v h, v h, i h, i, v<br />

Quantity measured h i v i/v<br />

Table 10-1: STM operating modes; i, v, h are tunneling current, voltage, and<br />

height (tip to sample surface distance) respectively (Schneiker, 1986).<br />

The 1986 Nobel Prize for Physics was split between the 50 year old<br />

cornucopia of microknowledge, the electron microscope, and a brand new,<br />

unfulfilled technology, scanning tunneling microscopy (STM). The STM half of<br />

the Prize was awarded to Gerd Binnig and Heinrich Rohrer of the IBM Zurich<br />

Research Laboratories where STM was invented in 1981 (Binnig, Rohrer, Gerber<br />

and Weibel, 1982). The principle used in STM is extremely simple (Figure 10.1).<br />

Piezoceramic materials expand or shrink extremely small distances (i.e.<br />

angstroms, or tenth nanometers) in response to applied voltage. In STM,<br />

piezoceramic holders scan an ultrasharp conducting tip (such as tungsten) over a<br />

conducting or semiconducting surface (Figure 10.1). When the STM tip is within<br />

a few angstroms of a surface, a small voltage applied between the two gives rise

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