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Sub 200 fs pulse generation from a graphene mode-locked ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Popa_APL_2010_20.pdf18 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. -
Charles Oatley: pioneer of scanning electron microscopy
www-g.eng.cam.ac.uk/125/achievements/oatley/cwo1.htm14 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. -
Interim Report
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Murat%27s%20publication/Interim%20Report.pdf1 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. -
Graphene speeds pair to Sto...
www-g.eng.cam.ac.uk/nms/highlights-press/Nature_Nobel.pdf6 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 -
graphane-suppFFMF.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/graphane-suppFFMF.pdf20 Jul 2010: 2% -0.18 70 200 200 1 0.21 58 1.263 697 85.3. ... 5. Γ M K Γ0. 200. 400. 600. 800. 1000. 1200. -
Innoglast report_090710mo
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/Innoglast%20report_090710mo_%28low%20res%29.pdf12 Jul 2010: Table 4.2 Mesh density of the adhesive layer. DC993 SikaForce Holdtite 3M Bohle SLS 6 25 6 25 4 200 4 100 4 200 No. ... of. Elements T-peel 6 20 6 20 4 200 4 100 4 200 The differences between the numerical solutions (elastic and visco-elasto-plastic) and -
JWA96 - Characterization of Dynamic Nonlinear Absorption of Carbon…
www-g.eng.cam.ac.uk/nms/publications/pdf/CLEO2010_JWA96.pdf29 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 -
First-Principles Prediction of Doped Graphaneas a High-Temperature…
www-g.eng.cam.ac.uk/nms/publications/pdf/Savini_PRL2010.pdf15 Jul 2010: 0 200 400 600 800 1000 1200 1400. Phonon Frequency (cm ). 0. 0.002. 0.004. 0.006. 0.008. α F. ( ω)/. ω (. cm. ). -1. 8 % doping4 % doping. 2 % doping. ... 2 1 % doping. -1. TO CC stretching modes. 0 200 400 600 800 1000 1200 1400. -
Graphene Grows Up | SPIE Newsroom: SPIE
www-g.eng.cam.ac.uk/nms/highlights-press/Graphene%20Grows%20Up.pdf2 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 -
SE14 paper Dev of design methods of glass structures:Layout 3
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/SE14%20paper%20%20Dev%20of%20design%20methods%20of%20glass%20structures.pdf26 Jul 2010: interlayer. At roomtemperature, PVB is comparatively soft with an elongation atbreakage of more than 200%. ... Vertical Sloping or Horizontal. Annealed glass 150 100. Fully tempered glass 200 150. -
Making Graphene Luminescent by Oxygen Plasma Treatment
www-g.eng.cam.ac.uk/nms/publications/pdf/Gokus_ACSNANO2009.pdf14 Jan 2010: The dynamics can be described by a triple-exponential with decay times40, 200, and 1000 ps. ... Two Dimensional Gas of Massless. Dirac Fermions in Graphene. Nature 2005, 438, 197–200.3. -
320 fs pulse generation from an ultrafast laser inscribed ...
www-g.eng.cam.ac.uk/nms/publications/pdf/beecher_apl2010.pdf20 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 -
arX iv:1 003. 4714 v1 [ cond -mat .oth ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_Arxiv2010_graphene.pdf25 Mar 2010: 4: (Circles) Output pulse duration; (squares) time-bandwidth product. 0 200 400 600 8000.0. -
Nano Res (2010) 3: 404–411 404 Ultrafast Stretched-Pulse Fiber ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010.pdf21 Jun 2010: AntiAliasColorImages false /CropColorImages true /ColorImageMinResolution 150 /ColorImageMinResolutionPolicy /Warning /DownsampleColorImages true /ColorImageDownsampleType /Average /ColorImageResolution 200 /ColorImageDepth -1 ... Quality 10 >> -
Surface-Enhanced Raman Spectroscopyof GrapheneFred Schedin,†…
www-g.eng.cam.ac.uk/nms/publications/pdf/nn1010842.pdf28 Oct 2010: V.; Firsov,A. A. Two-Dimensional Gas of Massless Dirac Fermions inGraphene. Nature (London) 2005, 438, 197–200. -
Graphene Mode-Locked Ultrafast LaserZhipei Sun,† Tawfique Hasan,†…
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_ACSNANO_2010.pdf23 Feb 2010: Sub-200-fs Pulsed Erbium-Doped Fiber LaserUsing a Carbon Nanotube-Polyvinylalcohol Mode Locker.Appl. Phys. -
Graphene photonics and optoelectronics
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_naturephoto_2010.pdf31 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. -
Density Gradient Ultracentrifugation of Nanotubes: Interplay of…
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_JPCh_2010.pdf15 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,†.
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