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24.4 res highs MH SA
www-g.eng.cam.ac.uk/nms/highlights-press/NanotechnologyStencilissimoNat.pdf27 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. << -
www-g.eng.cam.ac.uk/smirt/literature/smirtateng.pdf
www-g.eng.cam.ac.uk/smirt/literature/smirtateng.pdf14 May 2008: -
PII: S0022-5096(02)00107-2
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2003.pdf25 Jan 2008: Received 5 June 2002; accepted 24 September 2002. Abstract. This paper shows that repetitive, in0nite structures cannot be simultaneously statically, andkinematically, determinate? -
(Noticias da Europa \253 Bem Comum)
www-g.eng.cam.ac.uk/nms/highlights-press/Noticias%20da%20Europa.pdf13 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. -
doi:10.1098/rspa.2005.1598
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2006.pdf25 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. -
SESTO POTERE - Infomedia italia
www-g.eng.cam.ac.uk/nms/highlights-press/SESTO%20POTERE.pdf13 Mar 2008: APPELLO. ANIMALISTI AGLI USA E ALL'UE. (12/3/2008 11:24) IL PRESIDENTE DEL PARTITO DEI CACCIATORI PROTESTA. -
doi:10.1016/j.ijsolstr.2003.09.029
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/wicks2004.pdf25 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). -
SUPPLEMENTARY INFORMATION Hydrodynamics of a carbon nanotube For…
www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_NL2008si.pdf4 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. -
phb79632d_580
www-g.eng.cam.ac.uk/nms/publications/pdf/Wang_PSSb2008.pdf2 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 -
C:/Documents and Settings/Administrator/My Documents/afstuderen/asme…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/schenk2006.pdf25 Jan 2008: 1.14. 1.16. 1.18. 1.2. 1.22. 1.24. 1.26. h/r. norm. aliz. ed. -
Delivered by Ingenta to:Dublin City University IP : 136.206.1.20Thu,…
www-g.eng.cam.ac.uk/nms/publications/pdf/King_JNN2008.pdf17 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. -
L-band ultrafast fiber laser mode locked by carbon nanotubesZ. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_APL2008.pdf20 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 -
zerostiffness_paper.dvi
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/schenk2007.pdf25 Jan 2008: C = {v Ed | vT Qv = 0} (24). forms a projective conic. -
doi:10.1016/j.physe.2007.11.034
www-g.eng.cam.ac.uk/nms/publications/pdf/Hu_PE2007.pdf27 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. -
doi:10.1016/j.physe.2007.09.161
www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_PE2007.pdf27 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 -
Vapor-phase nucleation of individual CdSe nanostructuresfrom…
www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_APL2008.pdf21 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 -
doi:10.1016/j.physe.2007.10.088
www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_PE2007.pdf27 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. -
Femtonewton Force Sensing withOptically Trapped NanotubesO. M.…
www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_NL2008.pdf8 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. -
Using APL format
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_APL1999.pdf20 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 -
doi:10.1016/j.physe.2007.10.024
www-g.eng.cam.ac.uk/nms/publications/pdf/Mattevi_PE2007.pdf27 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. -
Carbon Nanotube Polycarbonate Composites for Ultrafast Lasers
www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_AM2008.pdf5 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. -
Effect of the sp2 carbon phase on n-type conduction ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ikeda_JAP2008.pdf20 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. -
doi:10.1016/j.physe.2007.10.044
www-g.eng.cam.ac.uk/nms/publications/pdf/Hsieh_PE2007.pdf27 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 -
PRL 95, 036101 (2005) P H Y S I ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Hofmann_PRL2005.pdf26 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. -
Sub-100 fs two-color pump-probe spectroscopy of Single Wall Carbon ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Gambetta_OE2008.pdf15 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. -
Nanowire Lithography on SiliconAlan Colli,† Andrea Fasoli,‡ Simone…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NL2008.pdf21 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.; -
Elastic Constants of Nanometer Thick Diamond-like Carbon Films Marco…
www-g.eng.cam.ac.uk/nms/publications/pdf/Beghi_MRSSP2001.pdf2 Jul 2008: 12 14 16 18 20 22 24. 20. 40. 60. 80. -
nnano.2008.312 738..742
www-g.eng.cam.ac.uk/nms/publications/pdf/Wang_NNANO2008.pdf8 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. -
Ion Beam Doping of Silicon NanowiresAlan Colli,*,† Andrea Fasoli,‡ ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NL2008b.pdf20 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. -
Thermal conductivity of ultrathin tetrahedral amorphous carbon…
www-g.eng.cam.ac.uk/nms/publications/pdf/Balandin_APL2008.pdf4 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 / -
nnano.2008.67 210..215
www-g.eng.cam.ac.uk/nms/publications/pdf/Das_NN2008.pdf7 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. & -
Self-assembled nanotube field-effect transistors for label-free…
www-g.eng.cam.ac.uk/nms/publications/pdf/Hu_JAP2008.pdf6 Oct 2008: P. Herman, J. Vac. Sci. Technol. B 24, 3173 2006.35A. Vijayaraghavan, S. -
A MODEL TO INTERPRET THE RAMAN SPECTRA OF DISORDERED, ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_MRSSP2001.pdf2 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. -
Characterization of carbon nanotube--thermotropic nematic liquid…
www-g.eng.cam.ac.uk/nms/publications/pdf/Trushkevych_JPD2008.pdf29 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. -
nnano.2008.215 563..568
www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008.pdf5 Sep 2008: based sheets. Nano Lett. 7, 3569 – 3575 (2007).24. Dresselhaus, M. -
Supporting Online Material
www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008SI.pdf5 Sep 2008: Physical Review Letters 85 (24), 5214 (2000). 9 Tuinstra, F. and Koenig, J. -
Edge-functionalized and substitutionally doped graphene…
www-g.eng.cam.ac.uk/nms/publications/pdf/Cervantes-Sodi_PRB2008.pdf28 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 -
Electron and Phonon Properties of Graphene:Their Relationship with…
www-g.eng.cam.ac.uk/nms/publications/pdf/Charlier_BOOK2008.pdf7 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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