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1 - 10 of 23 search results for KaKaoTalk:vb20 200 |u:www-g.eng.cam.ac.uk where 0 match all words and 23 match some words.
  1. Results that match 1 of 2 words

  2. OE_revised.dvi

    www-g.eng.cam.ac.uk/nms/publications/pdf/oe-20-22-25077.pdf
    18 Oct 2012: Hasan, F. Wang, and A. C. Ferrari, “Sub 200 fs pulse generation from a graphenemode-locked fiber laser,” Appl. ... 10-3. 10-2. 10-1. 100. -20 -10 0 10 200.0. 0.2. 0.4.
  3. Light–matter interaction in a microcavity-controlled…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Michael_NatComm2012.pdf
    20 Jun 2012: p (kW cm–2). 100 150 200. Figure 3 | Electrically excited microcavity-controlled graphene thermal emitter. ... 200. 300. 0. 0. 1.0. 3. 2. 20. 15. 0.5. 0.
  4. acs_nn_nn-2011-044609 1..15

    www-g.eng.cam.ac.uk/nms/publications/pdf/ACSNano2012_felice.pdf
    3 May 2012: Drops of inks are dispensed on holey carbon trans-mission electron microscopy (TEM) grids for TEM anal-ysis, using a Tecnai T20 high-resolution electronmicroscope with an acceleration voltage of 200 ... The O2 plasma is generated at 200 Wand 4 101 Torr
  5. Graphene field-effect transistors as room-temperature terahertz…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nmat3417.pdf
    28 Sep 2012: The channellength is between 7 and 10µm, while the gate width is LG =200 or300 nm, depending on the device. ... Figure 4a,bplots our measured NEPs as functions of VG. The minimumRT NEP is 200 nW Hz1/2 for SLG and almost one order ofmagnitude lower (30
  6. 49 Zammit_rev3

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Kenneth%20Publications/49%20Zammit.pdf
    15 Oct 2012: This study uses a relatively large model in a scale of 1:10, in contrast to common wind tunnel scales of 1:200 to 1:400.
  7. Hindawi Publishing CorporationJournal of NanomaterialsVolume 2012,…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cole_JNanoMater2012.pdf
    9 May 2012: c). (d). Fe (1 nm)(10 nm). Vertical CNT forest. SiOx (200 nm). ... 200. 0. 0 200 400 600 800. 0.02. 0.015. 0.01. 0.005.
  8. 17th Microoptics Conference (MOC' II), Sendai, Japan, Oct. 30 ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/graphene_composites_for_ultrafast_photonics.pdf
    12 Jan 2012: z -400 -200 0 200 400. Time delay (fs). 1575. Fig.3.
  9. sample.tex

    www-g.eng.cam.ac.uk/nms/publications/pdf/Pedersen_IEEEPhotonics2012.pdf
    20 Jun 2012: We considera pulse centred at 1060 nm with a time window of 200 ps divided into 212 points and a dopedfibre with length 0.9 m, dispersion β2 = 0.018. ... 0. 2. 4. 6. 8. 10. 12. 14. 0 100 200 300 400 500 600 700.
  10. (Chancellor's \24322m boost for Britain's wonder stuff:…

    www-g.eng.cam.ac.uk/nms/highlights-press/mail_online.pdf
    27 Dec 2012: Despite this, it is 200 times stronger than steel and several times tougher than diamond. ... Comments (47). NewestOldest. Best ratedWorst rated. View all. £200 Million (200,000,000) for nanotechnology, but £2 Billion (2,000,000,000) the government
  11. Mode-locking by nanotubes of a Raman laser based on a highly doped…

    www-g.eng.cam.ac.uk/nms/publications/pdf/CTu1I4.pdf
    30 May 2012: 15] D. Popa et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.

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