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  2. Sub-100fs pulse generation from a fiber oscillator mode-locked by…

    www-g.eng.cam.ac.uk/nms/publications/pdf/2011_CLEO_CMK6.pdf
    7 Apr 2011: 20. Inte. nsity (. dB. m). Wavelength (nm). nm. -400 -200 0 200 400. ... 3, 653 (2010). [19] D. Popa et al., "Sub 200 fs pulse generation from a graphene mode-locked fiber laser," Appl.
  3. OPTIMISING CINNECTIONS IN STRUCTURAL GLASS v7

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/OPTIMISING%20CINNECTIONS%20IN%20STRUCTURAL%20GLASS.pdf
    6 Jul 2011: 0.8. 0. 100. 200. 300. 400. 500. 600. 700. 800. Maxim. ... 300-400. 200-300. 100-200. Application of computer algorithm The comparisons carried out so far are based on the comparison of the maximum principal tensile stress.
  4. Nonlinear optics: Fibre sources in the deep ultraviolet

    www-g.eng.cam.ac.uk/nms/publications/pdf/nphoton.2011.166.pdf
    29 Jul 2011: news & views. Wavelength-tunable deep-ultraviolet (DUV; 200–300 nm) and vacuum-ultraviolet (VUV; 100–200 nm) lasers are needed in fields such as lithography1, medicine1 and spectroscopy2. ... cascaded second-harmonic converters to change 800 nm light
  5. James_Watson.indd

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/James%27%20publications/GPD.pdf
    24 Jun 2011: 1GLASS PERFORMANCE DAYS 2011 | www.gpd.fi. Novel Connections for Steel-Glassand Glass-Glass StructuresJames Watson 1, Mauro Overend 21 University of Cambridge, U.K.2 University of Cambridge, U.K. Keywords. 1 = Low temperature brazing 2 = Connections
  6. BBC News - Is graphene a miracle material?

    www-g.eng.cam.ac.uk/nms/highlights-press/bbc_graphene_2011.pdf
    26 May 2011: About 200 companies and start-ups are now involved in research around graphene.In 2010, it was the subject of about 3,000 research papers.
  7. Graphene Q-switched, tunable fiber laserD. Popa, Z. Sun, T. ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Popa_APL2011.pdf
    15 Feb 2011: The repetition rate ispump-dependent up to 200 mW Fig. 4b, a typical sig-nature of Q-switching.1 The output spectrum is tunable from1522 to 1555 nm. ... 80 100 120 140 160 180 200. 1.21.82.43.03.6. 80 100 120 140 160 180 200.
  8. A WHOLE-LIFE VALUE BASED ASSESSMENT AND OPTIMISATION MODEL FOR ...

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Qian%27s%20publication/BS2011.pdf
    24 Nov 2011: 11 ; (200 1600)1 exp( 1.017 0.00558 ). (6) where 4 denotes the illumination (lux) at working plane. ... coating. 175-200 187.5. Triple glazing. unit. Clear 180-195 187.5 Clear with low-e.
  9. Atomic force microscope nanolithography of graphene: Cuts,…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Puddy_APL_2011.pdf
    4 Apr 2011: b) (d). 200 nm 70 nm. pre-modificationpost-modification. G(μS). Vbg (V) Vbg (V)20 40 60 80 20 40 60 80. ... 200. 40. 60. 80100. 10. 0. 20. 30. (a) (c). FIG.
  10. THE CARBON NEGATIVE BUILDING FAÇADE R. Boyd1; M. Overend1; ...

    www-g.eng.cam.ac.uk/gft/media/UG%20projects/papers/The%20carbon%20negative%20building%20facade.pdf
    17 Sep 2011: O2/. m2). West. South. East. North. 0. 200. 400North. East. South.
  11. acs_nn_nn-2011-01203s 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn201203s.pdf
    5 Oct 2011: SOI areas are removed (Figure 6h).21 The following conditionsare used: main rf power: 400 W; bias power: 50 W; gases cycled:SF6 (250 sccm)/C4F8 (200 sccm)/O2(100 sccm); ... Deposition conditions are asfollows: temperature: 200 C; deposition cycle: 250 ms
  12. Strong plasmonic enhancement of photovoltage in graphene

    www-g.eng.cam.ac.uk/nms/publications/pdf/2011Etchermeyer_ncomms.pdf
    30 Aug 2011: 150. 200. 250. 300. 350. 8. 8. 6 80 2 4 6 80. ... Nature 438, 197–200 (2005). 28. Zhang, Y. B., Tan, Y. W., Stormer, H.
  13. 1 The Glass & Façade Technology (gFT) Research Group ...

    www-g.eng.cam.ac.uk/gft/media/News%20letter/Glass%20and%20Facade%20Research%20Technology%20Group%20Newsletter%20-%20Autumn%20Winter%202011.pdf
    23 Dec 2011: This is a deviation from standard wind tunnel practice, where buildings are modelled at scales in the region of 1:200 to 1:400.
  14. Ultrafast Raman laser mode-locked by nanotubesC. E. S. Castellani,1,* …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Raman_CNT_OL2011.pdf
    5 Oct 2011: Rev. A 77,0238 (2008). 20 10 0 10 200. 0.25. 0.5.
  15. ZAMMIT

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Kenneth%20Publications/080130%20KZ%20MO%20DH%20Paper%20-%20Challenging%20Glass.pdf
    10 Jul 2011: 200. 0. 200. 400. 600. 800. 1000. 0 10 20 30 40 50 60. ... 0.6. 0.65. 0.7. 0.75. 0.8. 0.85. 0.9. 0.95. 1. 0 100 200 300 400 500.
  16. Dynamic Catalyst Restructuring during Carbon Nanotube Growth

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn102118y.pdf
    6 Jan 2011: At alater time (Figure 4b, t 200 ns), a substantial numberof outer layer atoms have moved outside the CNT, cov-ering the head surface. ... METHODSETEM Measurements. We use a modified Tecnai F20 ETEM, oper-. ated at 200 kV, equipped with a differential
  17. PROO F COPY [ST/2003/023989] 009708Q ST Predicting Failure in ...

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/Overend%20ASCE%20paper_draft.pdf
    6 Jul 2011: usable stress of 1,200 MPa Sedlacek et al. ... of a 51-mm-diameter steel loading ring and one of threedifferent steel reaction rings with 65, 127, and 200 mm diametersFig.
  18. Nano Res. 2011, 4(4): 343–359 343 Photoluminescence of CdSe ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_NanoRes_2011.pdf
    3 May 2011: Here, we have thicker nanostructures (20–200 nm), and the power density is always kept lower than 104 W/cm2. ... to the smaller diameter of Au-NWs (30 nm) compared to SG-NWs (200 nm).
  19. THE PERFORMANCE AND OPTIMISATION OF A NOVEL FAÇADE PANEL FOR…

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Qian%27s%20publication/THE%20PERFORMANCE%20AND%20OPTIMISATION%20OF%20A%20NOVEL%20FA%C3%87ADE%20PANEL%20FOR%20ENERGY-EFFICIENT%20BUILDINGS.pdf
    6 Jul 2011: 200). Finite element analysis and optimisation are performed by ANSYS v11.0. Firstly, an initial model is built.
  20. High pressure Raman scattering of silicon nanowires

    www-g.eng.cam.ac.uk/nms/publications/pdf/0957-4484_22_19_195707.pdf
    30 Mar 2011: The initial characterization of the sample is performedwith a 200 kV transmission electron microscope (TEM)(Tecnai G220 from FEI).
  21. Cover

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Qian%27s%20publication/Report%20TR.235.pdf
    5 May 2011: 4 44. 11 ; (200 1600)1 exp( 1.017 0.00558 ). φ = ζ ζ. ... Clear with high performance solar control Low E coating 175-200 187.5.
  22. Development of a universal stress sensor for graphene and carbon…

    www-g.eng.cam.ac.uk/nms/publications/pdf/NatComm_2011.pdf
    29 Mar 2011: Graphene. Graphene monolayers were prepared by mechanical cleavage from natural graphite (Nacional de Grafite) and transferred onto the poly methyl meth-acrylate acetate (PMMA) CB covered by a 200-nm-thick
  23. Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and…

    www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_bookchapter.pdf
    13 Aug 2011: This can, in principle, be fine-tuned by modifying the growth parameters [191, 200, 249].
  24. Structural Engineering International 2/2007 Science and Technology…

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/Diagnostic_Interpretation_of_Glass_Failure_DRAFT.pdf
    6 Jul 2011: str. ess. (MP. a). 250. 200. 150. 0,00. 16,00 4,00 1,78 1,00 0,64 0,44 0,33 0,25 0,20 0,16.

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