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  2. nnano.2008.67 210..215

    www-g.eng.cam.ac.uk/nms/publications/pdf/Das_NN2008.pdf
    7 Apr 2008: new, important parameter to estimate thedoping density.
  3. Effect of the sp2 carbon phase on n-type conduction ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ikeda_JAP2008.pdf
    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.
  4. doi:10.1098/rspa.2005.1598

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2006.pdf
    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,
  5. A MODEL TO INTERPRET THE RAMAN SPECTRA OF DISORDERED, ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_MRSSP2001.pdf
    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.
  6. doi:10.1098/rspa.2006.1750

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/seffen2007b.pdf
    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
  7. 48th AIAA/ASME/ASCE/AHS/ASC Structures, Structural Dynamics and…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/norman2007.pdf
    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.
  8. Single member actuation of kagome lattice structures A.C.H. Leung, ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/leung2007.pdf
    25 Jan 2008: 1976. Discrete Field Analysis of Structural Systems. New York:Springer. Deshpande, V.S., Ashby, M.F., & Fleck, N.A.
  9. zerostiffness_paper.dvi

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/schenk2007.pdf
    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.
  10. C:/Documents and Settings/Administrator/My Documents/afstuderen/asme…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/schenk2006.pdf
    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.
  11. Characterization of carbon nanotube--thermotropic nematic liquid…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Trushkevych_JPD2008.pdf
    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.

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