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15 Jul 2014: Ref 9measured I(D)/I(G) for irradiated single layer. Address correspondence toacf26@eng.cam.ac.uk. Received for review May 16, 2014and accepted June 24, 2014. ... Lett. 2010, 104, 227401. 24. Kalbac, M.; Reina-Cecco, A.; Farhat, H.; Kong, J.; Kavan,

5 Jun 2014: 3HT and (b) 24% GNR with P3HT. The insets show the scan at a larger. ... 23 V, for 0%, 11%, and 24% blends. However, itwas slightly higher, ca.

3 Feb 2014: CB. [C2. B2 C. A. ]0.5(24). nserting the smallest root back into Eq. ... The corresponding F/V ratios are giveny Eq. (24) and, after some manipulation, it can be shown that:.

22 Aug 2014: locked pulses has potential applications in nonlinear frequency. conversion [23] and surgery [24]. ... 24 cm-1. larger than in individual flakes [2]. Thus, even if the.

7 Aug 2014: The new symmetry theorem for equiauxetics gives an opportunity to look back at some frameworksthat were first discussed [20–23] before the term “auxetic” came into use [24] and to see ... 23. Tarnai, T. Folded Structures. Symmetry Art Sci. 2002, 2,

6 Mar 2014: B dependence can beexplained through the Slonczewski-Weiss-McClure (SWM)model [22–24]. ... q̃ = 2mlB V1. kzmV1. cos θ. sin2 θ V 24/V 21 cos.

7 Aug 2014: 24].The polyhedral homotopy algorithm is based largely on workpublished by Li [19], while the path following algorithm waswritten specifically for this application. ... 

14 Feb 2014: reports.10,20,24 This is interpreted as due to the larger gate. length, as predicted by the photo-induced voltage equation:15. ... Teppe, A. Tredicucci, and T. Nagatsuma,. Nanotechnology 24, 214002 (2013).11A. Lisauskas, S.

6 Feb 2014: Figure 8 shows cubewrappings with (b, c) = (1, 0), (1, 1), (2, 0), (2, 1), which are derived from 6-, 12-,24- and 30-vertex octahedrites, respectively. ... Figure 8. Wrappings of the cube. The tiling T in each case is the dual of an octahedrite

10 Nov 2014: ARTICLE. Received 24 Jan 2014 | Accepted 19 Sep 2014 | Published 10 Nov 2014. ... The G peakcorresponds to the high-frequency E2g phonon at G. The Dpeak is due to the breathing modes of six-atom rings and requiresa defect for its activation16,22–24.