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3 Feb 2014: 5. 6. 7. θ [rad]. m/D. κ T0. φ = 43o, t = 0.2 mmL = 200 mmL = 300 mmL = 400 mmL = 500 mm. ... Gentilini C. et al./ Physics Engineering 01 (2009) 000–000. 200 250 300 350 400 450 500.

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

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.

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

6 Feb 2014: Higher-Order Rigidity – What Is the Proper Definition. Discrete & Computational Geometry 11, 193–200.Connelly, R., Terrell, M., 1995.

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.

5 Mar 2014: In the 1,200–1,350 nm emission range, exciton-exciton resonances of SWNTs such as (13,2), (12,4), (10,5), (9,7), (10,6), (8,7), (11,4), ... 6.4a) with respect to other tubes. The strong PL emission in the 1,080–1,200 nm range.

6 Mar 2014: 200 K. 230 K260 K. 1300120011001000. Raman Shift (cm-1. ). 30 T(b) (1,1). ... Vunit. l3B. 2B. γ 21. 2v. V1B 4.1 106 cm1. This value leads to W (kz) 104 cm1 at 30 T and 200 K,too small to explain the observed

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 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.