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  2. 24.4 res highs MH SA

    www-g.eng.cam.ac.uk/nms/highlights-press/NanotechnologyStencilissimoNat.pdf
    27 Apr 2008: Vol 452|24 April 2008. parts contain 11 protofilaments in all other bacteria studied so far. ... Discuss this paper at http://blogs.nature.com/nature/journalclub. JOURNAL CLUB. NATURE|Vol 452|24 April 2008. <<
  3. www-g.eng.cam.ac.uk/smirt/literature/smirtateng.pdf

    www-g.eng.cam.ac.uk/smirt/literature/smirtateng.pdf
    14 May 2008:
  4. PII: S0022-5096(02)00107-2

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2003.pdf
    25 Jan 2008: Received 5 June 2002; accepted 24 September 2002. Abstract. This paper shows that repetitive, in0nite structures cannot be simultaneously statically, andkinematically, determinate?
  5. (Noticias da Europa \253 Bem Comum)

    www-g.eng.cam.ac.uk/nms/highlights-press/Noticias%20da%20Europa.pdf
    13 Mar 2008: Noticias da Europa « Bem Comum http://bemcomum.wordpress.com/2008/03/12/noticias-da-europa-8/. 1 of 2 13/03/2008 14:24. « ... Noticias da Europa « Bem Comum http://bemcomum.wordpress.com/2008/03/12/noticias-da-europa-8/. 2 of 2 13/03/2008 14:24.
  6. doi:10.1098/rspa.2005.1598

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2006.pdf
    25 Jan 2008: 24. 35 dq. dĈ. " #C/:. ð4:3ÞTo find equilibrium configurations of the structure, we look for points where. ... K̂ Zv2Û=vq2 v2Û=vq vĈ. v2Û=vq vĈ v2Û=vĈ2. 24. 35; ð4:5Þ. is positive definite.
  7. SESTO POTERE - Infomedia italia

    www-g.eng.cam.ac.uk/nms/highlights-press/SESTO%20POTERE.pdf
    13 Mar 2008: APPELLO. ANIMALISTI AGLI USA E ALL'UE. (12/3/2008 11:24) IL PRESIDENTE DEL PARTITO DEI CACCIATORI PROTESTA.
  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. phb79632d_580

    www-g.eng.cam.ac.uk/nms/publications/pdf/Wang_PSSb2008.pdf
    2 Oct 2008: Received 2 May 2008, revised 24 June 2008, accepted 25 June 2008Published online 29 August 2008. ... Such wavelength tuning in passivelymode-locked fiber ring lasers was observed before in non-nanotube systems, and is usually attributed to
  11. C:/Documents and Settings/Administrator/My Documents/afstuderen/asme…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/schenk2006.pdf
    25 Jan 2008: 1.14. 1.16. 1.18. 1.2. 1.22. 1.24. 1.26. h/r. norm. aliz. ed.
  12. Delivered by Ingenta to:Dublin City University IP : 136.206.1.20Thu,…

    www-g.eng.cam.ac.uk/nms/publications/pdf/King_JNN2008.pdf
    17 Jul 2008: Delivered by Ingenta to:Dublin City University. IP : 136.206.1.20Thu, 17 Jul 2008 13:44:24. ... IP : 136.206.1.20Thu, 17 Jul 2008 13:44:24. RESEARCHARTICLE. King et al.
  13. L-band ultrafast fiber laser mode locked by carbon nanotubesZ. ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_APL2008.pdf
    20 Aug 2008: and mechanical and environ-mental robustness.11–24 To date, SWNT-based saturable ab-sorbers have been used to mode-lock fiber,12–21 waveguide,22. ... solid-state,23 and semiconductor lasers.24 These cover abroad range from 1 to 1.6 m.12–24
  14. zerostiffness_paper.dvi

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/schenk2007.pdf
    25 Jan 2008: C = {v Ed | vT Qv = 0} (24). forms a projective conic.
  15. doi:10.1016/j.physe.2007.11.034

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hu_PE2007.pdf
    27 May 2008: Previous studies showed that SWNTs tend todeposit in areas covered with polar chemicals when thewafer is dipped in a SWNT solution [23,24]. ... Lett. 303 (1999) 125. [24] S.G. Rao, L. Huang, W. Setyawan, S.
  16. 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
  17. 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.
  18. doi:10.1016/j.physe.2007.09.161

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_PE2007.pdf
    27 May 2008: Inaddition to dielectric screening [24,25], the presence ofbundles [20,21] contributes to the red shift in theabsorption spectrum compared to sample C1. ... Werecently reported that addition of PVP in a freshlyprepared SWNT dispersion increases the PL
  19. Femtonewton Force Sensing withOptically Trapped NanotubesO. M.…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_NL2008.pdf
    8 Oct 2008: Phys. ReV. Lett. 1970, 24, 156–159.(2) Ashkin, A.; Dziedzic, J. M.; Bjorkholm, J.E.; Chu, S. ... Phys. ReV.Lett. 2008, 100, 163903. (24) Rohrbach, A. Stiffness of optical traps: Quantitative agreement betweenexperiment and electromagnetic theory.
  20. 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
  21. doi:10.1016/j.physe.2007.10.024

    www-g.eng.cam.ac.uk/nms/publications/pdf/Mattevi_PE2007.pdf
    27 May 2008: re-organization of the C atoms in a sp2 network (284.5 eV,CNT growth) [21,24]. ... 24] J.C. Lascovich, R. Giorgi, S. Scaglione, Appl. Surf. Sci. 47 (1991) 17.
  22. Carbon Nanotube Polycarbonate Composites for Ultrafast Lasers

    www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_AM2008.pdf
    5 Nov 2008: Published online: September 24, 2008. [1] Y.-C. Chen, N. R. Raravikar, L. ... Appl. Phys. A 2003, 76, 111. [24] S. Singh, Y. Pei, R.
  23. 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
  24. Effect of the sp2 carbon phase on n-type conduction ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ikeda_JAP2008.pdf
    20 Oct 2008: for further N2 addi-tion up to 20%;22,24 ii electron mobility increases slightlywith N2 10%–20%;. ... 0 TM1/2, following Ref. 24, with VRH0 independent of TM. However, the slopes for.
  25. PRL 95, 036101 (2005) P H Y S I ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hofmann_PRL2005.pdf
    26 Jun 2008: In order to getaccurate growth rate measurements, we prepattern thecatalyst by e-beam lithography to get free standing verti-cally aligned CNFs [2], rather than rely on weight gainmeasurements [24] or ... B. K. Teo et al., Nano Lett. 4, 921 (2004).[24] L.
  26. Sub-100 fs two-color pump-probe spectroscopy of Single Wall Carbon ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Gambetta_OE2008.pdf
    15 Aug 2008: Ghislanzoni, 24, 23900 Lecco, Italy 2Engineering Department, Cambridge University, 9 JJ Thompson Avenue, Cambridge CB3 0FA United Kingdom. ... Rev. B 70, 241403 (2004). 24. J. Lefebvre, S. Maruyama, and P.
  27. 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.;
  28. Elastic Constants of Nanometer Thick Diamond-like Carbon Films Marco…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Beghi_MRSSP2001.pdf
    2 Jul 2008: 12 14 16 18 20 22 24. 20. 40. 60. 80.
  29. 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.
  30. 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.
  31. Thermal conductivity of ultrathin tetrahedral amorphous carbon…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Balandin_APL2008.pdf
    4 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 /
  32. nnano.2008.67 210..215

    www-g.eng.cam.ac.uk/nms/publications/pdf/Das_NN2008.pdf
    7 Apr 2008: A similar behaviour isobserved for the longitudinal optic (LO) G2 peak of dopedmetallic nanotubes8,9,24, for exactly the same reasons. ... Phys. Rev. B 73, 155426 (2006). 24. Tsang, J. C., Freitag, M., Perebeinos, V., Liu, J. &
  33. 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.
  34. A MODEL TO INTERPRET THE RAMAN SPECTRA OF DISORDERED, ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_MRSSP2001.pdf
    2 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.
  35. Characterization of carbon nanotube--thermotropic nematic liquid…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Trushkevych_JPD2008.pdf
    29 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.
  36. nnano.2008.215 563..568

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008.pdf
    5 Sep 2008: based sheets. Nano Lett. 7, 3569 – 3575 (2007).24. Dresselhaus, M.
  37. Supporting Online Material

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008SI.pdf
    5 Sep 2008: Physical Review Letters 85 (24), 5214 (2000). 9 Tuinstra, F. and Koenig, J.
  38. Edge-functionalized and substitutionally doped graphene…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cervantes-Sodi_PRB2008.pdf
    28 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
  39. Electron and Phonon Properties of Graphene:Their Relationship with…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Charlier_BOOK2008.pdf
    7 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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