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High pressure Raman scattering of silicon nanowires
www-g.eng.cam.ac.uk/nms/publications/pdf/0957-4484_22_19_195707.pdf30 Mar 2011: Raman spectroscopy has proven to be an effective andnondestructive characterization technique to understand thelattice dynamics of SiNWs [14–20]. ... Si–SiO2 nanochains, i.e., filamentary nanostructures wherecrystalline Si spheres are connected by -
PHYSICAL REVIEW B 83, 115441 (2011) Tilted potential induced ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Connolly_PRB_2011.pdf25 Mar 2011: 1(a)]. Atlarger source-drain voltage (VSD ), the conductance betweenthe resonances increases, leading to diamond-shaped regionswith VSD of 15–20 mV where the current is blockaded[Fig. ... We findthat dch 675 10 nm and w 805 20 nm for thirty-sixcurves -
Brownian Motion of GrapheneOnofrio M. Maragó,†,* Francesco…
www-g.eng.cam.ac.uk/nms/publications/pdf/nn1018126.pdf3 May 2011: For Ty and Tz, no data is shownfor , 20 because the flake is expelled from the trap by radiation pressure above this critical value. ... C. GraphenePhotonics and Optoelectronics. Nat. Photonics 2010, 4,611–622. 20. Perrin, F. -
Development of a universal stress sensor for graphene and carbon…
www-g.eng.cam.ac.uk/nms/publications/pdf/NatComm_2011.pdf29 Mar 2011: and. (11)(11). 1,0009008007006005004003002001000. –10. –15. –20. –25. –30. –35. –40. –5. 0. ... Carbon 29, 1267–1279 (1991). 20. Casiraghi, C. et al. Rayleigh imaging of graphene and graphene layers. -
Dynamic Catalyst Restructuring during Carbon Nanotube Growth
www-g.eng.cam.ac.uk/nms/publications/pdf/nn102118y.pdf6 Jan 2011: The blue atoms in a cylindrical region of 1 nm di-ameter and length are fixed to avoid tail slip during the 20 nsMD. ... 20. Harutyunyan, A. R.; Tokune, T.; Mora, E. Liquid as aRequired Catalyst Phase for Carbon Single-WalledNanotube Growth. -
acs_NL_nl-2011-01432g 1..7
www-g.eng.cam.ac.uk/nms/publications/pdf/cancado_2011_NL.pdf14 Aug 2011: Phys. Rev. B 1979,20, 392–401.(13) Lespade, P.; Marchard, A.; Couzi, M.; Cruege, F. ... disordered, amorphous, and diamondlike carbon. Phys. Rev. B 2001,64, 075414–075426.(20) Ferrari, A. -
acs_JA_ja-2010-10939a 1..6
www-g.eng.cam.ac.uk/nms/publications/pdf/Zhao_JACS_2011.pdf3 May 2011: arXiv:1010.4679v1,2010.(20) Gunes, F.; Shin, H. J.; Biswas, C.; Han, G. H.; Kim, E. ... M.; Huang, W.; Shen, Z. X. Adv. Funct. Mater. 2010, 20, 3504.(27) Zhao, W. -
Nano Res. 2011, 4(4): 343–359 343 Photoluminescence of CdSe ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_NanoRes_2011.pdf3 May 2011: A FEI Philips XL-30 sFEG SEM and a FEI Philips Tecnai 20 TEM are used. ... Furthermore, the peak position blue-shifts 20 meV/decade, drifting from 1.64 to 1.73 eV in Fig. -
Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and…
www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_bookchapter.pdf13 Aug 2011: This is typically attained by functionalization [20, 23, 75,105–107, 172, 486] and/or in-situ polymerization [117, 237, 281, 327, 349, 449,475]. ... Covalent functionalization of SWNTs disrupts the extended π -network,hence changes their
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