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Comment on “Nonlinear current-voltage curves of gold quantum point contacts” [Appl. Phys. Lett.87, 103104 (2005)]
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1.
1.M. Yoshida, Y. Oshima, and K. Takayanagi, Appl. Phys. Lett. 87, 103104 (2005).
http://dx.doi.org/10.1063/1.2037874
2.
2.J. Bürki and C. A. Stafford, Appl. Phys. A: Mater. Sci. Process. 81, 1519 (2005), and references therein.
http://dx.doi.org/10.1007/s00339-005-3389-8
3.
3.J. Bürki, C. A. Stafford, and D. L. Stein, Phys. Rev. Lett. 95, 090601 (2005).
http://dx.doi.org/10.1103/PhysRevLett.95.090601
4.
4.J. Bürki, R. E. Goldstein, and C. A. Stafford, Phys. Rev. Lett. 91, 254501 (2003).
http://dx.doi.org/10.1103/PhysRevLett.91.254501
5.
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FIG. 1.

The activation energy as a function of wire length for a magic Au nanocylinder with . The vertical dashed line indicates the critical length at which the transition in activation behavior takes place.

Image of FIG. 2.

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FIG. 2.

Conductance vs length change , during compression of short ( , solid line) and long ( , dashed line) Au wires, both with initial conductance . Inset (a) shows the long wire before (left) and after (right) expansion of the leads. The corresponding shapes for the short wire are shown in inset (b).

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2006-04-18
2014-04-17

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Scitation: Comment on “Nonlinear current-voltage curves of gold quantum point contacts” [Appl. Phys. Lett.87, 103104 (2005)]
http://aip.metastore.ingenta.com/content/aip/journal/apl/88/16/10.1063/1.2195895
10.1063/1.2195895
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