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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.