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1 - 10 of 30 search results for katalk:za33 24 |u:www-g.eng.cam.ac.uk where 0 match all words and 30 match some words.

  1. Results that match 1 of 2 words

  2. Hasan_JPCC2008

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_JPCC2008.pdf
    21 Jan 2009: either due to the dispersant molecules surroundingthe SWNTs8,9,11,24 or to the presence of SWNT bundles.41-44. ... L.; Heinz, T. F. Phys. ReV. Lett. 2006, 96,167401. (24) Walsh, A.

  3. was estimated to be 5 × 1016 m−2 on ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Elias_Science2009.pdf
    1 Feb 2009: Y. S. Li, N. R. Tao, K. Lu, Acta Mater. 56, 230 (2008).24. ... state by annealing (we used 450C in Ar atmo-sphere for 24 hours; higher annealing T dam-aged graphene).

  4. /home/journal/dvi/EPJD013-EPJD-final-print.dvi

    www-g.eng.cam.ac.uk/nms/publications/pdf/Milani_1999_EurPJD.pdf
    2 Feb 2009: All these parameters arein agreement with a more pronounced graphitic ordering ofthe sample [24]. ... Opt. 23, 3806 (1984)24. J. Robertson: Prog. Solid State Chem. 21, 199 (1991)25.

  5. Exp Astron (2009) 23:809–847DOI 10.1007/s10686-008-9115-8 O R I G ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Kuppers_EA2008.pdf
    23 Feb 2009: Exp Astron (2009) 23:809–847DOI 10.1007/s10686-008-9115-8. O R I G I N A L A R T I C L E. Triple F—a comet nucleus sample return mission. Michael Küppers H. U. Keller E. Kührt M. F. A’Hearn K. Altwegg R. Bertrand H. Busemann M. T. Capria L.

  6. Small Diameter Membrane Reflector Structures M. Santer∗ Imperial…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009ConfAIAAb.pdf
    9 Mar 2009: d2sb =. 4λψ2δ5tD3. π2n. (EmEs. )(24). and hence the mass msb of the offset struts to provide adequate resistance against buckling is.

  7. Plasma restructuring of catalysts for chemical vapor deposition of ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cantoro_JAP2009.pdf
    24 Mar 2009: 064304-2 Cantoro et al. J. Appl. Phys. 105, 064304 2009. Downloaded 24 Mar 2009 to 129.169.178.169. ... J. Appl. Phys. 105, 064304 2009. Downloaded 24 Mar 2009 to 129.169.178.169.

  8. Raman Spectroscopy of GrapheneEdgesC. Casiraghi,†,⊥ A. Hartschuh,‡ H. …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_NanoLett2009.pdf
    8 Apr 2009: Thisis not due to increasing disorder, since in this case we expectFWHM(G) to increase,15 but it could be related to a dopingvariation,15,18,24 that is, this edge ... C. Solid State Commun. 2007, 143, 47.(24) Das, A.; Pisana, S.; Piscanec, S.; Chakraborty

  9. Phonon renormalization in doped bilayer graphene A. Das,1 B. ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Das_PRB2009.pdf
    14 Apr 2009: D peak: the 2Dpeak.18 This lies at 2690 cm1 and involves phonons atK q.18,24 q depends on the excitation energy, due todouble resonance, and the linear dispersion of ... Lett. 91, 233108 2007.24 A. C. Ferrari, Solid State Commun. 143, 47 2007.25 A.

  10. CNT arrays for photonics - nanotechweb.org

    www-g.eng.cam.ac.uk/nms/highlights-press/cnt_photonics.pdf
    24 Apr 2009: CNT arrays for photonics - nanotechweb.org http://nanotechweb.org/cws/article/tech/38812. 1 of 2 2009/4/24 15:27. ... nanotechweb.org. TECHNOLOGY UPDATE. Apr 24, 2009. Carbon nanotube arrays could be employed in photonic devices like deep-UV photonic

  11. Uniaxial strain in graphene by Raman spectroscopy: G peak ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Mohiuddin_PRB_2009.pdf
    1 Jun 2009: Moreover, no G peak splitting was observed foruniaxial strain,20,24 again in contrast with both our observa-tion and general expectations. ... Z. X. Shen, Phys. Rev. B 77, 115416 2008.24 T. Yu, Z.

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