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  2. 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.pdf
    26 Jul 2010: SE14 paper Dev of design methods of glass structures:Layout 3 15/7/10 10:24 Page 18. ... Further specific advice on the use of FEA in glassstructures is also available2, 24.
  3. 320 fs pulse generation from an ultrafast laser inscribed ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/beecher_apl2010.pdf
    20 Sep 2010: Single wall carbon nanotubes SWNTs12–22 andgraphene12,13 are promising saturable absorbers SAs formode-locking fiber,12–17 waveguide,6 solid-state,23 and semi-conductor lasers.24 They have several ... complex processes, such as molecular beam epitaxy
  4. First-Principles Prediction of Doped Graphaneas a High-Temperature…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Savini_PRL2010.pdf
    15 Jul 2010: In particular, it was proposed thatfully hydrogenated graphene (graphane) would be stable[24]. ... The main difference between graphene and graphaneis that, while the former is fully sp2 bonded, the latter issp3, as diamond [24].
  5. Innoglast report_090710mo

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/Innoglast%20report_090710mo_%28low%20res%29.pdf
    12 Jul 2010: Handling Time 24 hrs 24hrs 1 hr 2-3 mins 8-12 hrs 40s Curing Time 7 days 7 days 2-3 hrs 5 mins 7 days 40s. ... Innoglast report_090710mo.doc Page 24. 5 Conclusions and Recommendations The principal aim of this study was to provide initial data on the
  6. Scanning gate microscopy of current-annealed single layer grapheneM.…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Connolly_APL_2010.pdf
    16 Mar 2010: in situ the improvement is limited due to there-adsorption of atmospheric gases and water vapor.22 Cur-rent annealing has been used for in situ removal ofadsorbates,23,24 in
  7. Phonon-Assisted Electroluminescence fromMetallic Carbon Nanotubes and …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Essig_nanolett_2010.pdf
    21 May 2010: The spectra can be deconvo-luted in two Gaussians centered at 1.35 and 1.76 eV, witha full width at half-maximum (FWHM) of 0.28 and 0.24 ... In addi-tion, we observed that controlled oxidation with meta-chloroperbenzoic acid (MCPBA)24 does not increase
  8. Viscous State Effect on the Activity of FeNanocatalystsFelipe…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn101883s.pdf
    3 Dec 2010: Lindemann index,. 24. Here, we analyze the nanoparticles near. the melting point by investigating, as func-. ... SolidLiquidPhase Behavior in Microclusters. Adv. Chem. Phys. 1988, 70,75–138. 24. Lindemann, F.
  9. Graphene Mode-Locked Ultrafast LaserZhipei Sun,† Tawfique Hasan,†…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_ACSNANO_2010.pdf
    23 Feb 2010: passively mode-lock an erbium-doped fiber laser working at 1559 nm, with a 5.24 nm spectral bandwidth and. ... arXiv:0908.0154, 2009. 24. Eberlein, T.; Bangert, U.; Nair, R. R.; Jones, R.; Gass, M.;Bleloch, A.
  10. Nano Res (2010) 3: 404–411 404 Ultrafast Stretched-Pulse Fiber ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010.pdf
    21 Jun 2010: These have been used to mode-lock fiber [8–23], waveguide [24], solid-state [25–27], and semiconductor lasers [28]. ... Langmuir 2008, 24, 5070–5078. [37] Hasan, T; Tan, P. H.; Bonaccorso, F; Rozhin, A.
  11. Surface-Enhanced Raman Spectroscopyof GrapheneFred Schedin,†…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn1010842.pdf
    28 Oct 2010: diative and nonradiative dipole fields. Since eq 24 does not consider multiple reflections. ... tions of eq 6 (near-field) and eq 24 (full-field). As ex-.

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