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  2. Nanosecond-pulse fiber lasers mode-locked with nanotubesE. J. R.…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Kelleher_APL_2009.pdf
    16 Sep 2009: W a v e l e n g t h ( μ m ). 2 0. 1 0. 0. SpectralPower(d. B) ( b ). FIG. ... 5. RF spectrum a and pulse train b of the 1200 m laser.
  3. Hasan_JPCC2008

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_JPCC2008.pdf
    21 Jan 2009: E.; Avouris, P. Phys. ReV. B 1998, 58, 13870.(6) O’Connell, M. ... G.; Vamivakas, A. N.; Yin, Y.; Ünlü, M. S.; Goldberg,B. B.; Swan, A.
  4. Uniaxial strain in graphene by Raman spectroscopy: G peak ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Mohiuddin_PRB_2009.pdf
    1 Jun 2009: Po. s(2. D). (cm. -1). Strain(%). B. ω2D/ε - 64cm-1/%. FIG. ... K. Swan, M. S. Unlu, B. B. Goldberg, M. A. Pimenta, J.
  5. Nanotube-Polymer Composites for Ultrafast Photonics

    www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_ADVMAT09.pdf
    20 Oct 2009: Polystyrene-block-polyacrilic acid(PS-b-PAA) forms micelles around SWNTs due to the gradualaddition of water. ... Figure 4a and b schematically describeEET from a donor to an acceptor SWNT.

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