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14 Dec 2013: z (nm). DBR. -200 0 2000. 1. 2. 3. 4. abs=0.5. ... Ref. ract. ive. inde. x, |E. |2. z (nm). DBR. -200 0 2000.

30 May 2013: In strained graphene nanobub-bles, it was reported that Bstr can reach 200–400 T [29].In nominally unstrained SLG, the residual strain causedby nm-scale height variations and defects can

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).

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.

25 Mar 2013: Hasan, F. Wang, and A. C. Ferrari, “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. ... The waveguide is inscribed by focusing the pulses, through a 0.4 NA lens, 200 µm below the substrate surface, by a master oscillator

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

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.

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

7 Nov 2013: 3. 4. 5. Dis. tanc. e (μ. m). zx. 0 200 400Force (fN). ... a. Displacement (nm)0 200 400 600 800 1,000 1,200 1,400. Dis.

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.