By Edwin Bidwell Wilson
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A. Sanchez-Garcia, E. Calleja, E. Monroy, F. J. Sanchez, F. Calle, E. Muñoz, R. com/science/article/B6TJ6-3W8STD4-4/ 1/ceb4d2577504cc8815a0de8507ed2712 32. L. Cerutti, J. Ristić, S. Fernández-Garrido, E. Calleja, A. Trampert, K. H. Ploog, S. Lazic, J. M. APL/88/213114/1 33. Y. Cui, X. Duan, J. Hu, C. 1021/ jp0009305 34. -K. Lew, L. Pan, T. E. Bogart, S. M. Dilts, E. C. Dickey, J. M. Redwing, Y. Wang, M. Cabassi, T. S. Mayer, S. W. APL/85/3101/1 35. S. Bae, C. Na, J. Kang, J. 1021/ jp0458708 36.
Without covering, the polymer will charge up and the e-beam will be partially deﬂected, causing an intensity increase. This can be observed in Fig. 3b. Between two wires, a broad area of enhanced intensity shows the charging and thus the isolation between the wires. Directly next to the wire, no charging can be observed, meaning a suﬃcient amount of electrons will be able to reach the wire before they charge the material signiﬁcantly. In contrast, Fig. 3c shows a grid of unorganized, crossing wires, which are able to provide conductivity in both directions and contain insulated islands instead 32 M.
Mayers, T. Herricks, and Y. Xia: Chem. Mater. 14, 4736 (2002) 32. K. K. Caswell, C. M. Bender, and C. J. Murphy: Nano Lett. 3, 667 (2003) 33. J. Jhu, S. Liu, O. Palchik, Y. Koltypin, and A. Gedanken: Langumir 16, 6396 (2000) 34. Y. Sun, Y. Yin, B. Gates, B. T. Mayers and Y. Xia: Nano Lett. 2, 165 (2002) 35. C. S. Ah, S. D. Hong, and D. J. Jang: J. Phys. Chem. B 103, 3073 (1999) ZnO Nanostructures: Optical Resonators and Lasing Klaus Thonke1 , Anton Reiser1 , Martin Schirra1 , Martin Feneberg1 , Günther M.
A Statistical Discussion of Sets of Precise Astronomical Measurements IV by Edwin Bidwell Wilson