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4 Feb 2014: Bandgap engineering is usually attempted by patterning into graphene nanoribbons (GNRs) (24,11), but GNRs tend to have low mobilities (<200 cm2V1s1) (27) as a consequence of carrier scattering on disordered ... Although these inverters pave the way to

22 Aug 2014: Hasan, F. Wang, and A. C. Ferrari, "Sub 200 fs pulse generation from a graphene mode-locked fiber.

6 Feb 2014: Math. 18, 169–200. (doi:10.4153/CJM-1966-021-8). Kavicky, S. 2004 Anatomy of an exhibition.

5 Jun 2014: C.Sub 200 fs Pulse Generation from a Graphene Mode-Locked Fiber Laser.

15 Jul 2014: BRUNA ET AL. VOL. XXX ’ NO. XX ’ 000–000 ’ XXXX. www.acsnano.org. A. C XXXX American Chemical Society. Doping Dependence of the RamanSpectrum of Defected GrapheneMatteo Bruna, Anna K. Ott, Mari Ijäs, Duhee Yoon, Ugo Sassi, and Andrea C.

5 Jun 2014: 7b. These aggregates having a height rangingfrom 60 to 200 nm and a width spanning from 0.6 to 2 mm, werefound to be randomly distributed within the polymer matrix.Their ... Experimental sectionMaterials. Poly(3-hexylthiophene) (P3HT) (Fig. 1b)

6 Feb 2014: P. W. Fowler et al.3242. on February 6, 2014rspa.royalsocietypublishing.orgDownloaded from. (Tarnai & Gáspár 1983a) is 5185025.200. ... The edge length is 49833021.200, intermediate between the Kólya–Goldbergand Tarnai–Gáspár arrangements.

14 Mar 2014: organic vapor phase epitaxy (MOVPE, AIXTRON AIX 200/4) as described in [47]. ... The pump laser is coupled into a 200 µm fiber. Fig.

14 Mar 2014: W- 3XU). -0C. a)> 2ÚNU). cebs 1.3 1. 400 0 -400 -200 0 200 400z(nm). ... 400 -200 0 200z(nm). DBR. 2.0. C0 1.5E4)UCÇ 1.0a). 0.5ü=. I I ' I.

14 Feb 2014: High performance bilayer-graphene terahertz detectors. Davide Spirito,1 Dominique Coquillat,2 Sergio L. De Bonis,1 Antonio Lombardo,3. Matteo Bruna,3 Andrea C. Ferrari,3 Vittorio Pellegrini,1,4 Alessandro Tredicucci,1. Wojciech Knap,2 and Miriam S.