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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).

7 Apr 2008: new, important parameter to estimate thedoping density.

20 Oct 2008: apparentlylow activation energy.22–24 As nitrogen is preferentially in-corporated into the amorphous carbon phase at the grainboundaries, new electronic states associated with carbon andnitrogen can be produced at and ... Botti, S. Martelli, and E.

25 Jan 2008: Hence, starting from the observation that many features of interestcan be captured by a model that considers only uniform, inextensionally deformedconfigurations of the shell, a new model is presented that expresses ... Section 4 presents this new model,

2 Jul 2008: The presence of a residual D peak in UV Raman spectra of a-C’s is a new finding, which can affect our deriving sp3 content from the T peak, as ... The first UV Raman studies [14,15] found a new peak at 1060 cm-1 labelled T.

25 Jan 2008: 1976. Discrete Field Analysis of Structural Systems. New York:Springer. Deshpande, V.S., Ashby, M.F., & Fleck, N.A.

8 Jan 2008: For example, ferventresearch efforts are focusing on new aircraft concepts in which controlled distortionsof key aerodynamical surfaces tailor the flight envelope. ... nxy. ExZ. nyx. Ey: ð2:2Þ. For straightforwardness, new relationships are defined in

18 Jan 2008: The structure is then deformed plastically to createthe new shape; this deformation will affect the prestresses, but not remove them. ... This gives a new stiffness matrix. D =.  (1 α)D νD 0νD D 00 0 1ν2 D.

25 Jan 2008: Now consider an affine transformation, so that the new structure has nodalcoordinates p̄i. ... p̄j p̄i = UQ(pj pi) (19)and with the infinitesimal relative displacements in the new configurationgiven as.

25 Jan 2008: tures has resulted in a new class of mechanisms: Statically Bal-anced Tensegrity Mechanisms. ... INTRODUCTIONOn the border between structures and mechanisms, we find. a new and special class of structures termedStatically BalancedTensegrity Mechanisms.

29 May 2008: Winterschool/Euroconf. on Electronic Properties ofNovel Materials 2005 (Kirchberg, Austria) (New York:American Institute of Physics) p 114–7. ... walled carbon nanotubes New J.

29 Jan 2008: Finally, Section4 presents conclusions and the new directions which this work provides. ... This gives a new stiffness matrix. D =.  (1 α)D νD 0νD D 00 0 1.

5 Sep 2008: by centrifugation. To do this we dried the sediment and used it to prepare a new dispersion in fresh NMP,. ... Here is the new solvent (outer) surface area, while is the surface area of the voids, which will.

7 Jan 2008: The goal of this contribution is to review the exciting news about theelectronic and phonon states of graphene and to suggest how these discoveries helpunderstand the properties of carbon nanotubes. ... Many of these new ideas proposed for graphene and

28 Apr 2008: Edge-functionalized and substitutionally doped graphene nanoribbons:Electronic and spin properties. F. Cervantes-Sodi, G. Csányi, S. Piscanec, and A. C. FerrariDepartment of Engineering, University of Cambridge, Cambridge CB3 OFA, United Kingdom.