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1 - 10 of 20 search results for KaKaoTalk:vb20 200 |u:www-g.eng.cam.ac.uk where 0 match all words and 20 match some words.

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  2. Symmetric prismatic tensegrity structures: Part I. Configuration and…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestD.pdf
    6 Feb 2014: Higher-Order Rigidity – What Is the Proper Definition. Discrete & Computational Geometry 11, 193–200.Connelly, R., Terrell, M., 1995.

  3. Graphene saturable absorbers for VECSELs V. J. Wittwer*a, C. ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/89660X.pdf
    14 Mar 2014: W- 3XU). -0C. a)> 2ÚNU). cebs 1.3 1. 400 0 -400 -200 0 200 400z(nm). ... 400 -200 0 200z(nm). DBR. 2.0. C0 1.5E4)UCÇ 1.0a). 0.5ü=. I I ' I.

  4. STh3N.8.pdf CLEO:2014 © 2014 OSA Nanotube mode-locked, low repetition …

    www-g.eng.cam.ac.uk/nms/publications/pdf/STh3N.8.pdf
    10 Jun 2014: Express21, 23261 (2013).10. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.

  5. Luminsescence: The Instrumental Key to the Future of Nanotechnology

    www-g.eng.cam.ac.uk/nms/publications/pdf/Acf_Ch06_2014.pdf
    5 Mar 2014: In the 1,200–1,350 nm emission range, exciton-exciton resonances of SWNTs such as (13,2), (12,4), (10,5), (9,7), (10,6), (8,7), (11,4), ... 6.4a) with respect to other tubes. The strong PL emission in the 1,080–1,200 nm range.

  6. 1077-260X (c) 2013 IEEE. Translations and content mining are ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf
    22 Aug 2014: Hasan, F. Wang, and A. C. Ferrari, "Sub 200 fs pulse generation from a graphene mode-locked fiber.

  7. High performance bilayer-graphene terahertz detectors Davide…

    www-g.eng.cam.ac.uk/nms/publications/pdf/spirito_APL_2014.pdf
    14 Feb 2014: High performance bilayer-graphene terahertz detectors. Davide Spirito,1 Dominique Coquillat,2 Sergio L. De Bonis,1 Antonio Lombardo,3. Matteo Bruna,3 Andrea C. Ferrari,3 Vittorio Pellegrini,1,4 Alessandro Tredicucci,1. Wojciech Knap,2 and Miriam S.

  8. doi:10.1098/rspa.2008.0164

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2008GuestA.pdf
    6 Feb 2014: P. W. Fowler et al.3242. on February 6, 2014rspa.royalsocietypublishing.orgDownloaded from. (Tarnai & Gáspár 1983a) is 5185025.200. ... The edge length is 49833021.200, intermediate between the Kólya–Goldbergand Tarnai–Gáspár arrangements.

  9. Photodetectors based on graphene, other two-dimensional materials and …

    www-g.eng.cam.ac.uk/nms/publications/pdf/nnano.2014.215.pdf
    6 Oct 2014: Because the optical phonon energy in graphene is large45,46 (200  meV), hot carriers created by the radiation field can remain at a tempera-ture Te (and thus energy kBTe, with ... 100. –200. –300. –400. –500. Phot. ocur. rent. (nA. ). Gate

  10. STu1I.2.pdf CLEO:2014 © 2014 OSA Synchronously coupled fiber lasers…

    www-g.eng.cam.ac.uk/nms/publications/pdf/STu1I.2.pdf
    10 Jun 2014: Express 20, 25077 (2012).8. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.

  11. RAPID COMMUNICATIONS PHYSICAL REVIEW B 89, 121402(R) (2014) Effects…

    www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB.89.121402.pdf
    6 Mar 2014: 200 K. 230 K260 K. 1300120011001000. Raman Shift (cm-1. ). 30 T(b) (1,1). ... Vunit. l3B. 2B. γ 21. 2v. V1B 4.1 106 cm1. This value leads to W (kz) 104 cm1 at 30 T and 200 K,too small to explain the observed

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