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Proceedings - Interdisciplinary Center for Nanotoxicity

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144<br />

Conference on Current Trends in Computational Chemistry 2009<br />

Figure 2. Representations of the linear spin density <strong>for</strong> the truncated L = 11 SWNT (a)<br />

and the capped L = 10 (b) with CH adsorbed at selected sites, versus the tube length.<br />

In all calculation, a plane wave basis was used in conjunction with three‐dimensional<br />

periodic boundary conditions [1]. From our results, the SWNT spin density distributions largely<br />

govern the adsorption energy variations at non‐equivalent sites of attachment and are<br />

there<strong>for</strong>e of crucial importance <strong>for</strong> the correct representation of the interaction between finite<br />

SWNT substrates and hydrocarbon radical adsorbates.<br />

[1] J.Furthmueller, J.Hafner, G.Kresse, Phys. Rev. B50, 15606 (1993).

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