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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.

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.

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.

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

20 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.

12 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

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

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

15 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.

14 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.