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24 May 2013: II). We find that the Raman scat-tering efficiency of the G peak [dS/d(G)] is 200 105m1 Sr1 at 2.41 eV. ... Eq. (12) we get dS/d(G)SLG 200 105 m1Sr1 anddS/d(G)(2D)SLG 1580 105 m1Sr1.

14 Mar 2013: In the high-frequency region above 200 cm1, theE12g (384 cm1), A1g (409 cm1), 2LA(M) (453 cm1),. ... Although the in-plane modes in 5 and 6L-MoS2above 200 cm1 are almost identical, the C and LB modepositions below 100 cm1 are different.

4 Apr 2013: 6. 0 50 100 150 200 250 300 3500.0. 0.2. 0.4. ... G). 200. (a) (b) (c). φ φ. Figure S2. Polarization.(a) Geometry for polarized measurements.

16 Jul 2013: The second stage, t 200 fs, isdominated by the emission of optical phonons,98 which ingraphene are associated with an unusually large energy scale(200 meV)88,99 and are moderately ... which act on a much longer time scale(200 fs).

25 Sep 2013: 200 -100 0 100 2000.0. 0.2. 0.4. 0.6. 0.8. 1.0 Data Fit.

16 Jan 2013: 1b), and the glass substrate is then heated (200 C for 10 – 20 mins)49,50. ... On the C-face, larger domains (200 nm) of multilayered, rotationally disordered graphene are produced198,199.

4 Apr 2013: NATURE NANOTECHNOLOGY | VOL 8 | APRIL 2013 | www.nature.com/naturenanotechnology 235. Graphene is the two-dimensional building block for sp2 carbon allotropes of every other dimensionality. It can be stacked into three-dimensional graphite, rolled