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  2. phb76154d_590

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_PSSB2007.pdf
    28 Nov 2007: Ferrari. Engineering Department, Cambridge University, Cambridge CB3 0FA, UK. Received 24 May 2007, accepted 18 June 2007. ... and annealing treatment on device resistance. Curves correspond to devices with 10, 11 and 24 SiNWs.
  3. Non-destructive Characterisation of Carbon Films Andrea C. Ferrari…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_BOOK2008.pdf
    18 Dec 2007: Figure 1b and c shows the ternary phase diagrams which summarise the compositions of carbon nitrides with increasing N content [24]:. ... Higher N contents cause a transition to a lower sp3 fraction and give softer films similar to PLCHN [24].
  4. Raman fingerprint of charged impurities in grapheneC. Casiraghia� and …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_APL2007.pdf
    10 Dec 2007: neutrality point away from zero gatevoltage.12–14,19,23,24 However, it is quite remarkable that“pristine” samples, with no contacts, exhibit almost an orderof magnitude doping variation, with a
  5. doi:10.1016/j.ijsolstr.2004.02.037

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/galletly2004b.pdf
    27 Dec 2007: It was generated using Abaqus. (2002). A length of tube was modelled with a 48 by 48 mesh (24 by 24 for the a 90 case) using S4R.
  6. No Job Name

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_NL2007.pdf
    18 Sep 2007: carbon nanotubes, and viruses.24-28 Rayleigh scatteringexperiments can be performed by using two differentstrategies. ... K.;Ferrari, A. C.; Mauri, F.Nat. Mater.2007, 6, 198. (24) Ignatovich, F.
  7. Optical phonons in carbon nanotubes: Kohn anomalies, Peierls…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_PRB2007.pdf
    12 Feb 2007: In metallic SWNTs theEPC strongly affects the phonon frequencies, giving rise toKohn anomalies KA12–16 and Peierls distortionsPD.15,17–24 A correct understanding and a quantitativelyprecise description of electron-phonon ... It was proposed thatthey
  8. LETTERS Breakdown of the adiabaticBorn–Oppenheimer approximationin…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Pisana_NM2007.pdf
    2 Mar 2007: Thedependence of the electronic bands on u can be obtained from theDFT electron–phonon coupling matrix elements (see equation (6)and note 24 of ref. ... Phys. Rev. Lett. 96,. 136806 (2006).24. Moos, G., Gahl, C., Fasel, R., Wolf, M. &
  9. ISSN:1369 7021 © Elsevier Ltd 2007JAN-FEB 2007 | VOLUME ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_MT2007.pdf
    8 Jan 2007: These films are usually deposited by plasma-enhanced. chemical vapor deposition (PECVD) at low bias voltage22-24. ... For a 100 nm a-C:H-coated bottle, the OTR is reduced. to 0.0008 cc/package/24 hours from the 0.04 cc/package/24 hours of.
  10. Thermal and chemical vapor deposition of Si nanowires:Shape control,…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_JAP2007.pdf
    18 Dec 2007: 12b correspond to deviceswith 7, 24, and 10 SiNWs for types I, II, and III, respec-tively. ... Curvescorrespond to devices with 7, 24, and 10 SiNWs for types I, II, and III,respectively.
  11. Photoluminescence Spectroscopy of Carbon Nanotube Bundles:Evidence…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Tan_PRL2007.pdf
    27 Sep 2007: due toits much lower position than previous investigations ofthese tubes [18,19,24,25]. ... 24] H. Htoon et al., Phys. Rev. Lett. 94, 127403 (2005).[25] S.

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