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  2. 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.
  3. 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.
  4. 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.
  5. 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.
  6. 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.
  7. 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
  8. 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
  9. 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.
  10. 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
  11. 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.

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