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2 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

27 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.

25 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

5 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.

2 Jul 2008: We thus developed a new adaptive k-point sampling approach. 0.00 0.04 0.08 0.12 0.16 0.201560.

26 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.

27 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.

20 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

2 Jul 2008: N. Thurston, Academic, New York, 1972, p.35 17. R. Pastorelli, S.

4 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.

28 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

27 May 2008: New York, 1988. [17] R. Seidel, G.S. Duesberg, E. Unger, A.P.

27 May 2008: Sakano, Organic Solvents, Physical. Properties and Methods of Purification, Wiley, New York, 1986.

2 Jan 2008: 2] P. Weiss, Wings of change. Science News Online, Decem-ber, 2003.

13 Mar 2008: Grabert and M. H. Devoret Plenum, New York, 1991. 8Y. Takahashi, M.

21 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.

27 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].

20 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,

15 Aug 2008: 5. Conclusions. A new system for ultrafast spectroscopy based on an amplified Er-doped fiber laser is presented and characterized.

5 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).