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24 May 2012: 1 of 2 24/05/2012 11:27. conversion efficiency, with a consequent reduction of the pump threshold. ... 2 of 2 24/05/2012 11:27.

19 Jun 2012: IASS Annual Symposium - IASS-APCS 2012. Seoul, South Korea, 21-24 May 2012. ... Seoul, South Korea, 21-24 May 2012. 3. Analysis of the double-skin tensegrity glass façade.

27 Dec 2012: BBC News - Graphene research gets £21.5m investment fund http://www.bbc.co.uk/news/science-environment-20846282. 1 of 2 27/12/2012 13:24. ... 2 of 2 27/12/2012 13:24.

30 May 2012: Award. 6. References [1] S.V. Chernikov et al., “Raman fibre laser operating at 1.24 μm.” Electronics Letters 34, 680 (1998).

28 Sep 2012: We also note a further sign switch around VG =0 in all curves.This suggests a contribution to the photoresponse of thermoelectricorigin23,24, arising from the presence of the ungated ... 24. Gabor, N. M. et al. Hot-carrier-assisted intrinsic

4 Dec 2012: Phys. Lett. 95 111108. [24] Özgören K and Ilday F Ö 2010 Opt.

3 Dec 2012: 03/12/2012 It's not exactly HARDware. Nokia and Samsung in race to launch 'flexible' mobile phones during 2013 - News - Gadgets & Tech - The Independent.

2 May 2012: April 24, 2012. C 2012 American Chemical Society. Graphene Electronics, Fresh from the Printer.

12 Jan 2012: LPE graphene is exfoliated by ultrasonication (see Fig.2a), either in water [25-28] or in organic solvents [24,28,30]. ... To prepare environmentally stable polymer composites, in particular, against humidity and temperature, graphene can be directly

19 Jun 2012: IASS Annual Symposium - IASS-APCS 2012. Seoul, South Korea, 21-24 May 2012. ... Seoul, South Korea, 21-24 May 2012. A specially constructed C++ application performs the manufacturability analysis.

12 Sep 2012: field measurements. 0. 20. 40. 60. 80. 0 4 8 12 16 20 24. ... S_Fr 28 404 431 24 576 24.3. S_Fl 28 305 333 122 1090 8.9.

13 Mar 2012: DecoupledSLG may exist on the surface of bulk graphite.23,24 To avoidcontributions from such SLGs, we recorded the spectra ofseveral locations to select a region with a bulk graphitelikeRaman spectrum, ... 080(5) 0.041(10) 0.08(3) 0.044(5) 0.044(24) 2γ5

15 Oct 2012: UK. [3] Wellershoff F. & Hortmanns M. (1999). “Wind Loads on Double Façade Systems with Gaps Greater than 15cm”, Proceedings of the 10th International Conference on Wind Engineering, Copenhagen, Denmark, 21-24

3 May 2012: thus affecting the homogeneityofthefinalprintedfeatures.89 Thefinalassemblyofprintednanoparticleinksdependsonthesubstratesurfaceenergy(SE),22,24 as well as ink viscosity and surface tension.22. ... Figure 5c is thedrop ejection sequence for the pristine

18 Oct 2012: 24. S. Y. Set, H. Yaguchi, Y. Tanaka, and M. Jablonski, “Ultrafast fiber pulsed lasers incorporating carbon nanotubes,”IEEE J. ... Nanotubes have mode-lockedfiber [18, 24–29], waveguide [30, 31], solid-state [32–34] and semiconductor lasers [35],

20 Jun 2012: 0.16. 0.18. 0.2. 0.22. 0.24. 0.26. 0.28. 0.3. 0.32. 1000 1020 1040 1060 1080 1100 1120 1140. ... Mater. 21, 3874-3899 (2009). [24] Z. Sun,T. Hasan and A. C.

9 May 2012: alignment. The films demonstrated optoelectroniccharacteristics nearing the ITO benchmark and superiorcharacteristics to competing organic technologies such asTDA and PEG-enhanced PEDOT:PSS [24, 25]. ... 45, no. 5, pp. 913–921,2007. [24] B. D. Martin, N

20 Jun 2012: Further data analysis reveals that microcavity-controlled thermal radiation is emitted into a narrow lobe with a total angular width of 24 (FWHM) only (see Supplementary Methods and Supplementary Fig. ... 24. Casiraghi, C. et al. Rayleigh imaging of

2 Apr 2012: The easiest way to get high-quality FLG is by graphiteexfoliation22 on SiO2/Si, to enhance visibility23,24. ... 91, 063124 (2007).24. Casiraghi, C. et al. Rayleigh imaging of graphene and graphene layers.

30 May 2012: that this result is in contrast to previous models where thecapacitance of a similar size dot was lower than anticipatedtheoretically,24 demonstrating the sensitivity of such estimatesto screening effects.