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Thermal conductivity of ultrathin tetrahedral amorphous carbon…
www-g.eng.cam.ac.uk/nms/publications/pdf/Balandin_APL2008.pdf4 Aug 2008: and density, compared with those by S-bend ca-thodic vacuum arc.5,16,20,24 The thickest ta-C measured herehas a density of 2.6 g / -
Self-assembled nanotube field-effect transistors for label-free…
www-g.eng.cam.ac.uk/nms/publications/pdf/Hu_JAP2008.pdf6 Oct 2008: P. Herman, J. Vac. Sci. Technol. B 24, 3173 2006.35A. Vijayaraghavan, S. -
A MODEL TO INTERPRET THE RAMAN SPECTRA OF DISORDERED, ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_MRSSP2001.pdf2 Jul 2008: shown. 600 0C is the onset of major H effusion and sp3 to sp2 conversion in ta-C:H [23,24]. ... Milne, A. Tagliaferro, W. Beyer, Diam. Relat. Mater. 9, 765 (2000) 24. -
Characterization of carbon nanotube--thermotropic nematic liquid…
www-g.eng.cam.ac.uk/nms/publications/pdf/Trushkevych_JPD2008.pdf29 May 2008: are the catalyst metals(metal impurities in the studied CNT material are estimatedto be 4%wt by the manufacturer [24]). ... 23] www.merck.de[24] http://www.sigma-aldrich.com[25] Rugar D and Hansma P 1990 Atomic force microscopy. -
Supporting Online Material
www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008SI.pdf5 Sep 2008: Physical Review Letters 85 (24), 5214 (2000). 9 Tuinstra, F. and Koenig, J. -
nnano.2008.215 563..568
www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008.pdf5 Sep 2008: based sheets. Nano Lett. 7, 3569 – 3575 (2007).24. Dresselhaus, M. -
Edge-functionalized and substitutionally doped graphene…
www-g.eng.cam.ac.uk/nms/publications/pdf/Cervantes-Sodi_PRB2008.pdf28 Apr 2008: spectroscopy also allows monitoringof doping and defects.24,26,31,32 Once identified, graphene lay-ers can be processed into nanoribbons by lithography.9,12,17,33. ... carbon nanotubes70–73 and bulksemiconductors, or if it would rather cause a shift of -
Electron and Phonon Properties of Graphene:Their Relationship with…
www-g.eng.cam.ac.uk/nms/publications/pdf/Charlier_BOOK2008.pdf7 Jan 2008: 1c. The linear dispersion given by (2) is the solution to the following effectiveHamiltonian at the K(K′) point [24]:.
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