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www-g.eng.cam.ac.uk/nms/publications/pdf/Scheel_PSSb2008.pdf2 Oct 2008: 3. Theinitial room temperature Raman intensity can be regainedapproximately by refocusing the laser spot on the new sam-ple surface. ... References. [1] S. Reich, C. Thomsen, and J. Maultzsch, Carbon Nan-otubes: Basic Concepts and Physical Properties -
doi:10.1016/j.physe.2007.11.034
www-g.eng.cam.ac.uk/nms/publications/pdf/Hu_PE2007.pdf27 May 2008: In this work, we demonstrate a new technique forhysteresis suppression by chemically functionalizing thesurfaces where the SWNTs are deposited. ... Dekker, New York, 1967. [27] L.T. Zhuravlev, Colloids Surf. A 173 (2000), 1–38.0. -
PII: S0022-5096(02)00107-2
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2003.pdf25 Jan 2008: 6. A similarcalculation for a structure that satis0es the static condition yields no new information,as the ability to carry all average stresses is equivalent to saying that the unit cell ... W.H. Freeman, New York.Hyun, S., Torquato, S., 2002. Optimal -
Carbon Nanotube Polycarbonate Composites for Ultrafast Lasers
www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_AM2008.pdf5 Nov 2008: tions.[22–25] Here, we use PC as a new optical polymer matrix, in. ... In summary, we demonstrated polycarbonate as a new. photonic polymer host, where SWNTs were homogeneously. -
Kohn Anomalies in Graphite and Nanotubes S. Piscanec1, M. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_MRSSP2005.pdf2 Jul 2008: We thus developed a new adaptive k-point sampling approach. 0.00 0.04 0.08 0.12 0.16 0.201560. -
PRL 95, 036101 (2005) P H Y S I ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Hofmann_PRL2005.pdf26 Jun 2008: In PECVD, the plasma creates new and more reactivespecies, such as radicals, in the gas phase and/or thecatalyst surface [35– 37]. ... of Carbon (Marcel Dekker, New York, 1978), Vol. 14,p. 83. [11] C. -
doi:10.1016/j.physe.2007.10.088
www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_PE2007.pdf27 May 2008: Available online 12 November 2007. Abstract. Optical trapping is a new tool for the manipulation and deposition of single wall carbon nanotube (SWNT) bundles. ... Jackson, Classical Electrodynamics, second ed., Wiley, New. York, 1975. [31] R. -
Using APL format
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_APL1999.pdf20 Feb 2008: Besides the usual Rayleigh surface mode, we also observe a new pseudosurface acousticmode of longitudinal polarization, which is a modified version of the longitudinal guided modeusually found in slow-on-fast -
Elastic Constants of Nanometer Thick Diamond-like Carbon Films Marco…
www-g.eng.cam.ac.uk/nms/publications/pdf/Beghi_MRSSP2001.pdf2 Jul 2008: N. Thurston, Academic, New York, 1972, p.35 17. R. Pastorelli, S. -
Thermal conductivity of ultrathin tetrahedral amorphous carbon…
www-g.eng.cam.ac.uk/nms/publications/pdf/Balandin_APL2008.pdf4 Aug 2008: metal-oxide-semiconductortechnology, stimulate the search for new materials.1 Carbonhas a variety of allotropes, including graphene, carbon nano-tubes, diamond, and diamondlike carbons DLC. ... Seitz and D. TurnbullAcademic, New York, 1958, Vol. 7, p. 1. -
doi:10.1016/j.physe.2008.01.007
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PE2008.pdf28 May 2008: The symposia covered the progressin design, manufacturing and characterization of nano-tubes, nanowires and graphene, and new developmentsleading to possible commercial applications of thesematerials. ... Krenn 2517. New dimensionality classifications of -
doi:10.1016/j.physe.2007.10.024
www-g.eng.cam.ac.uk/nms/publications/pdf/Mattevi_PE2007.pdf27 May 2008: New York, 1988. [17] R. Seidel, G.S. Duesberg, E. Unger, A.P. -
doi:10.1016/j.physe.2007.09.161
www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_PE2007.pdf27 May 2008: Sakano, Organic Solvents, Physical. Properties and Methods of Purification, Wiley, New York, 1986. -
doi:10.1016/j.scriptamat.2006.03.028
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/seffen2006.pdf2 Jan 2008: 2] P. Weiss, Wings of change. Science News Online, Decem-ber, 2003. -
Room temperature single electron charging in single silicon…
www-g.eng.cam.ac.uk/nms/publications/pdf/Rafiq_JAP2008.pdf13 Mar 2008: Grabert and M. H. Devoret Plenum, New York, 1991. 8Y. Takahashi, M. -
Nanowire Lithography on SiliconAlan Colli,† Andrea Fasoli,‡ Simone…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NL2008.pdf21 May 2008: the macroscale, NWsrepresent a new class of materials for thin-film-transistors(TFTs),5,6 sensors,7,8 and transparent flexible electronics.6,9,10. -
doi:10.1016/j.physe.2007.10.058
www-g.eng.cam.ac.uk/nms/publications/pdf/Tan_PE2007.pdf27 May 2008: The new features observedin PLE can be explained by EET and are assigned indetail. ... Crosses indicate the. lipses show the new PLE features assigned to EET [7]. -
Ion Beam Doping of Silicon NanowiresAlan Colli,*,† Andrea Fasoli,‡ ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NL2008b.pdf20 Aug 2008: F., Ed.; North-Holland:Amsterdam, 1992. (9) Sze, S. M. Physics of Semiconductor DeVices; Wiley: New York, 1981.(10) Pelaz, L; Marqués, L. ... 17) Ziegler, J. F.; Biersack, J. P.; Littmark, U. The Stopping and Rangesof Ions in Solids; Pergamon: New York, -
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: 5. Conclusions. A new system for ultrafast spectroscopy based on an amplified Er-doped fiber laser is presented and characterized. -
nnano.2008.215 563..568
www-g.eng.cam.ac.uk/nms/publications/pdf/Hernandez_NN2008.pdf5 Sep 2008: New J. Phys.023034 (2008). 13. Zhou, S. Y. et al. Origin of the energy bandgap in epitaxial graphene—Reply. ... M. & Scott, R. L. Regular and related solutions 1st edn (Van NostrandReinhold Company, New York, 1970).
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