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  2. Sub 200 fs pulse generation from a graphene mode-locked ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Popa_APL_2010_20.pdf
    18 Nov 2010: Sub 200 fs pulse generation from a graphene mode-locked fiber laserD. ... In conclusion, we demonstrated a graphene-based SAmode-locker for generation of pulses shorter than 200 fs.
  3. Interim Report

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Murat%27s%20publication/Interim%20Report.pdf
    1 Nov 2010: 100 110 120 130 140 150 160 170 180 190 200 210 220 230 240 250. ... Linear(Closed. Door). 70 80 90. 100 110 120 130 140 150 160 170 180 190 200 210 220 230 240 250.
  4. Surface-Enhanced Raman Spectroscopyof GrapheneFred Schedin,†…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn1010842.pdf
    28 Oct 2010: V.; Firsov,A. A. Two-Dimensional Gas of Massless Dirac Fermions inGraphene. Nature (London) 2005, 438, 197–200.
  5. Density Gradient Ultracentrifugation of Nanotubes: Interplay of…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_JPCh_2010.pdf
    15 Oct 2010: Density Gradient Ultracentrifugation of Nanotubes: Interplay of Bundling and SurfactantsEncapsulation. F. Bonaccorso,† T. Hasan,† P. H. Tan,†,‡ C. Sciascia,† G. Privitera,† G. Di Marco,. P. G. Gucciardi, and A. C. Ferrari,†.
  6. Charles Oatley: pioneer of scanning electron microscopy

    www-g.eng.cam.ac.uk/125/achievements/oatley/cwo1.htm
    14 Oct 2010: Oatley's first task at ADRDE was to investigate ways of improving the receivers used in the CD sets which operated at the then relatively high frequency of 200 MHz.
  7. Graphene speeds pair to Sto...

    www-g.eng.cam.ac.uk/nms/highlights-press/Nature_Nobel.pdf
    6 Oct 2010: 2. Novoselov, K. S. et al. Nature 438, 197-200. (2005). | Article | PubMed | ISI | OpenURL | | ChemPort |. 3. Kim, K. S. et al. Nature 457, 706-710 (2009). | Article | PubMed | OpenURL | | ChemPort
  8. 320 fs pulse generation from an ultrafast laser inscribed ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/beecher_apl2010.pdf
    20 Sep 2010: 320 fs pulse generation from an ultrafast laser inscribed waveguide lasermode-locked by a nanotube saturable absorber. S. J. Beecher,1,a R. R. Thomson,1 N. D. Psaila,1 Z. Sun,2 T. Hasan,2 A. G. Rozhin,2. A. C. Ferrari,2 and A. K. Kar11Department of
  9. Graphene photonics and optoelectronics

    www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_naturephoto_2010.pdf
    31 Aug 2010: a. Graphene. ITO. Arc discharge SWNTs. TiO2/Ag/TiO2. ZnO/Ag/ZnO. 200 400 600 800. ... Th is is mainly due to limited optical absorption when only one SLG is used, short photocarrier lifetimes and small eff ective photodetection areas (200 nm in ref.
  10. Graphene Grows Up | SPIE Newsroom: SPIE

    www-g.eng.cam.ac.uk/nms/highlights-press/Graphene%20Grows%20Up.pdf
    2 Aug 2010: We first created a laserworking at the telecom window at 1550 nm and now we have lasers based ongraphene saturable absorbers that can produce 200-fs pulses as well as workover
  11. JWA96 - Characterization of Dynamic Nonlinear Absorption of Carbon…

    www-g.eng.cam.ac.uk/nms/publications/pdf/CLEO2010_JWA96.pdf
    29 Jul 2010: a). 0 5 10 15 200.0. 0.2. 0.4. 0.6. 0.8. 1.0 τp=0.25 ps τp=0.5 ps τp=0.75 ps τp=1

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