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  2. USING STANDARD SYSTE

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PRB2000b.pdf
    6 Dec 2006: The p band energies alongGK M innearest-neighbor tight-binding approximation are. E5 6 gu11 2 cos ka!u, 1! ... 11 2 cos ka!5 2a. L a3! or sin(Dka)'a/()La) for small Dk, whereDk is the k dis-.
  3. Resonant Raman spectroscopy of twisted multilayer graphene

    www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6309.pdf
    10 Nov 2014: It comes from TO phononsaround the Brillouin Zone (BZ) edge K16,22, is active by doubleresonance (DR)24, and is strongly dispersive with excitationenergy due to a Kohn Anomaly (KA) at
  4. Light-enhanced liquid-phase exfoliation and current photoswitching in …

    www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms11090.pdf
    11 Apr 2016: The collected precipitate is dried undervacuum for 24 h. The powder X-ray diffraction patterns are obtained using a BrukerAXS D2 Phaser (LYNXEYE detector) with Ni-filtrated Cu-Ka
  5. Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and…

    www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_bookchapter.pdf
    13 Aug 2011: Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and Optoelectronics. T. Hasan, V. Scardaci, P.H. Tan, F. Bonaccorso, A.G. Rozhin, Z. Sun,and A.C. Ferrari. Abstract Polymer composites are an attractive near-term means to exploit

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