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  2. 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.
  3. phb76194d_598

    www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_PSSB2007.pdf
    28 Nov 2007: Nanoruptor ultrasonicator) in presence of sodium dodecylbenzenesulphonate (SDBS) as surfactant [24]. ... 24] M. F. Islam, E. Rojas, D. M. Bergey, A. T.
  4. arX iv:0 711. 4533 v1 [ cond -mat .mtr ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_CM2007.pdf
    10 Dec 2007: In general, lat-tice dynamics is calculated within the Born-Oppenheimeradiabatic framework [24, 25]. ... M. Ziman, Principles of the theory of solids (Cam-. bridge University Press, London, New York, 1964).[24] M.
  5. 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
  6. doi:10.1016/j.physe.2006.06.014

    www-g.eng.cam.ac.uk/nms/publications/pdf/Pisana_PE2007.pdf
    27 Mar 2007: For example, Erlandsson et al. [24,25] reportedsignificant restructuring of 0.5 nm thick Pd films (meltingand Huetting temperatures of 1554 and 275 1C, respec-tively) at 200 1C when subject ... 24] R. Erlandsson, M. Eriksson, L. Olsson, U. Helmersson, I.
  7. Supplementary Information DERIVATION OF EQ. 1 The electronic…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Pisana_NM2007SI.pdf
    2 Mar 2007: Following Ref. 1 (Eq.6 and note 24) and Ref. 2, for.
  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. No Job Name

    www-g.eng.cam.ac.uk/nms/publications/pdf/Pisana_JPCC2007.pdf
    18 Dec 2007: s crystal orienta-tion.24-26 Yu et al. ... R.; Hanein, Y.J. Phys. Chem. B2006, 110, 21419.(24) Ago, H.; Nakamura, K.; Ikeda, K.; Uehara, N.; Ishigami, N.; Tsuji,.
  10. Synthesis and characterization of cluster-assembled carbon thin…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Milani_JAP1997.pdf
    22 Jan 2007: 800 cm21!24 Although the origin of these structures is still amatter of debate, the disorder of as p2 carbon network ismost likely responsible for the observed spectra. ... TaucPle-. num, London, 1974!33D. A. G. Bruggeman, Ann. Phys.Leipzig! 24, 636
  11. doi:10.1016/j.optcom.2007.04.028

    www-g.eng.cam.ac.uk/nms/publications/pdf/King_OC2007.pdf
    21 Jun 2007: The sample absorbed in the UV–Vis range.Absorption shoulders occurred close to the direct band-gap energies of crystalline silicon [24,25]. ... 24] J. Singleton, Band Theory and Electronic Properties of Solids, OxfordUniversity Press, 2001, p.

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