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1 - 10 of 38 search results for katalk:za31 24 / / / / / |u:www-g.eng.cam.ac.uk where 0 match all words and 38 match some words.

  1. Results that match 1 of 2 words

  2. Ion Beam Doping of Silicon NanowiresAlan Colli,*,† Andrea Fasoli,‡ ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NL2008b.pdf
    20 Aug 2008: The hysteresis observed in Figure 3a when reversing thegate sweeping direction is generally thought to arise fromcharge trapping at surface states or defects in the oxide.14,23,24. ... E.; Johnson, A. T. Appl. Phys. Lett. 2005, 87, 193104.(24) Weber, W.

  3. Vapor-phase nucleation of individual CdSe nanostructuresfrom…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_APL2008.pdf
    21 Jan 2008: on functionalized substrates;22,24 and c they canbe made of the same material of the final NWs, thus, mini-mizing chemical contaminations.20. ... Although nanocrystal-seeded growth has proven viablefor NWs synthesis,10,20,21,24 many fundamental

  4. Nanowire Lithography on SiliconAlan Colli,† Andrea Fasoli,‡ Simone…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NL2008.pdf
    21 May 2008: Also, a precise control overthe doping concentration and crystallographic direction ofCS-NWs is still lacking,24 while for SOI-NWs these param-eters would be accurately determined by the initial propertiesof ... M. Nano Lett. 2005, 5, 2287.(24) Wu, Y.;

  5. nnano.2008.312 738..742

    www-g.eng.cam.ac.uk/nms/publications/pdf/Wang_NNANO2008.pdf
    8 Dec 2008: From the average output power andrepetition rate, the energy per pulse is 24 pJ. ... Received 19 May 2008; accepted 24 September 2008;. published 2 November 2008.

  6. Self-assembled nanotube field-effect transistors for label-free…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hu_JAP2008.pdf
    6 Oct 2008: P. Herman, J. Vac. Sci. Technol. B 24, 3173 2006.35A. Vijayaraghavan, S.

  7. Using APL format

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_APL1999.pdf
    20 Feb 2008: density of 3.24 g/cm3.15 The dispersionrelations depend on the elastic constants of both the olayer (E,G) surf and the inner layer (E,G) bulk. ... Knapp and co-workers3,24 proposed a finite-element modelovercome the limitations of the Oliver–Pharr1,2

  8. doi:10.1016/j.ijsolstr.2003.09.029

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/wicks2004.pdf
    25 Jan 2008: 24. 35 dðn 1ÞdðnÞ. dðn þ 1Þ. 24. 35 fðn 1ÞfðnÞ. ... fðn þ 1Þ. 24. 35 ðA:1Þ. The individual matrices K0 and K1 can be found by standard methods (Livesley, 1964).

  9. SUPPLEMENTARY INFORMATION Hydrodynamics of a carbon nanotube For…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_NL2008si.pdf
    4 Sep 2008: 2z〈Z(t)Z(t τ )〉 (24). where we assume center-of-mass and angular uctuations to be uncorrelated,so that we can neglect cross terms of type ... Using Eqs.22-24 we are able to t well our experimental data (seeFig.

  10. doi:10.1016/j.physe.2007.10.088

    www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_PE2007.pdf
    27 May 2008: References. [1] A. Ashkin, Phys. Rev. Lett. 24 (1970) 156. [2] A. ... Gittes, C.F. Schmidt, Opt. Lett. 23 (1998) 7. [24] A. Rohrbach, Phys.

  11. doi:10.1016/j.physe.2007.10.044

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hsieh_PE2007.pdf
    27 May 2008: eXerox Research Centre of Canada, Mississauga, Ont., Canada L5K 2L1. Available online 24 October 2007. ... Several groups haverecently considered CNTs for fabrication of TFTs, usingvarious fabrication methods, including spin coating, dropcasting, and

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