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24 May 2013: As a consequence,. 205435-11098-0121/2013/87(20)/205435(12) 2013 American Physical Society. ... Lett. 51, 1355 (1987).56C. Casiraghi, Diamond Relat. Mater. 20, 120 (2011).57S.

11 Nov 2013: lization of the hybrids using high-resolutionmicroscopic techniques.16,20,21 This requiresdeposition and fixing of the hybrids on asurface. ... 5%) and 1.5d-AC-6hr (50%) spectra with respect tothe 1.5d (fwhm(G) = 20.7 cm1).

4 Apr 2013: For triple-resonant processes with γ  = 20  meV, we have ħvF/γ  35  nm; for double-resonant processes, vF/Ω  3.5  nm (for ħΩ  = 0.2  eV). ... However even in SLG with very few defects, FWHM(D) is 20 cm–1, thus larger than this splitting.

4 Apr 2013: Thus, A(2D) decreases as EF movesaway from the Dirac point79,80. From the measureddependence, the two contributions to γ could be sepa-rated, giving an estimate for γeph 20 30

16 Jul 2013: We stress that in Eq. (20) we introduced an infinitesimalquantity η in the argument of one of the delta distributions. ... Carrying out algebraic manipulations, we rewrite Eq. (20) in the following simplified manner:.

7 Nov 2013: Both Au nan-oparticles (AuNPs, diameters 9.5–254  nm)20 and Ag nanoparticles (AgNPs, diameters 20–275  nm)21 have been optically trapped in three dimensions.

16 Jan 2013: on current-annealed suspended SLGs43, while room temperature (RT) mobilities up to 20 000 cm2 V1 s1 were measured in as-prepared SLGs44. ... 1b), and the glass substrate is then heated (200 C for 10 – 20 mins)49,50.