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

    www-g.eng.cam.ac.uk/nms/publications/pdf/89660X.pdf
    14 Mar 2014: 24 by controlling the electric field intensity in SLG on a high-reflection mirror. ... 24. ai 3Ea). À/4 Si02. À/8 Si 02. À/12 Si02. no Si02.
  3. VOL. 53 (2012) No. 3 contents n. 173 September ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012GuestA.pdf
    6 Feb 2014: 4.1 Switch-Pitch Structure with Point Group Symmetry dT. As shown in Figure 3, this switch-pitch structure consists of 16 nodes and 24 members. ... Γ||(e) 24 0 0 0 2. Γf 48 0 0 0 4.
  4. 5_WG3

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20pubblication/5_WG3%20%281%29.pdf
    27 Feb 2014: Voss E, Overend M, Stevens W. 'A building information modelling-based tool for heuristically assessing facade manufacturability', Proceedings of the IASS Annyal Symposium, Seoul, South Korea, May 21-24, 2012.
  5. nl400516a 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nl400516a.pdf
    4 Sep 2014: 24,12 While bulkMoS2 is a semiconductor with an indirect band gap of 1.3 eV,. ... E.; Heinz, T. F.; Hone, J.; Ryu, S. ACSNano 2010, 4 (5), 26952700.(24) Zhang, X.; Han, W.
  6. This content has been downloaded from IOPscience. Please scroll ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestA.pdf
    6 Feb 2014: received 24 May 2013; accepted in final form 17 June 2013published online 2 July 2013. ... Γ(Tx,Ty) 2 1 1 2 0 0= 24 0 0 0 0 0.
  7. 1 INTRODUCTION Contemporary architecture often encourages transparent …

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Shelton%27s%20publication/NHAMOINESU_SILVESTRU_24_10_2013%20%281%29.pdf
    27 Feb 2014: 15,0 15,3 13,7 19,7. 31,0 33,4 31,7 8,8. 19,5 24,0 23,2 11,7. ... 36,6 30,3 37,4. 18,3 24,6 21,7. 17,6 19,0 17,3. C1 C2 C3 C4.
  8. 1672 IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 26, NO. 16, ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/06832525.pdf
    21 Aug 2014: 24, pp. 3025–3027,2008. [3] S. Kobtsev, S. Kukarin, and Y. Fedotov, “Ultra-low repetition ratemode-locked fiber laser with high-energy pulses,” Opt. ... Mater., vol. 20, no. 21, pp. 4040–4043, 2008. [24] T. Hasan et al., “Nanotube–polymer
  9. doi:10.1016/j.sna.2006.04.016

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2007SensAct.pdf
    3 Feb 2014: CB. [C2. B2 C. A. ]0.5(24). nserting the smallest root back into Eq. ... The corresponding F/V ratios are giveny Eq. (24) and, after some manipulation, it can be shown that:.
  10. Graphene modelocked VECSELs C.A. Zaugg1*, V.J. Wittwer2, Z. Sun2, ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/896607.pdf
    14 Mar 2014: due to various processes [27, 28], including carrier-carrier and carrier-phonon scattering, as well as radiative electron-hole recombination (non-linear photoluminescence [24, 43, 44]). ... 24] F. Bonaccorso, Z. Sun, T. Hasan, and A. C. Ferrari,
  11. Symmetric prismatic tensegrity structures. Part II: Symmetry-adapted…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestC.pdf
    6 Feb 2014: 24 351 0 00 1 00 0 1. 35 Nnþv Cv Sv 0Sv Cv 00 0 1. ... k1 Ek. 24 J.Y. Zhang et al. / International Journal of Solids and Structures 46 (2009) 15–30.
  12. acs_nn_nn-2014-02676g 1..10

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf
    15 Jul 2014: Ref 9measured I(D)/I(G) for irradiated single layer. Address correspondence toacf26@eng.cam.ac.uk. Received for review May 16, 2014and accepted June 24, 2014. ... Lett. 2010, 104, 227401. 24. Kalbac, M.; Reina-Cecco, A.; Farhat, H.; Kong, J.; Kavan,
  13. , 20120029, published 30 December 2013372 2014 Phil. Trans. ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestA.pdf
    6 Feb 2014: The unit cell contains 24 joints and 72 bars, andscalar counting using (2.1) gives m s = 3. ... 2006 The flexibility window in zeolites. Nat. Mater. 5, 962–965. (doi:10.1038/nmat1784)24.
  14. 1077-260X (c) 2013 IEEE. Translations and content mining are ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf
    22 Aug 2014: locked pulses has potential applications in nonlinear frequency. conversion [23] and surgery [24]. ... 24 cm-1. larger than in individual flakes [2]. Thus, even if the.
  15. Symmetry Perspectives on Some Auxetic Body-Bar Frameworks

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestD.pdf
    7 Aug 2014: The new symmetry theorem for equiauxetics gives an opportunity to look back at some frameworksthat were first discussed [20–23] before the term “auxetic” came into use [24] and to see ... 23. Tarnai, T. Folded Structures. Symmetry Art Sci. 2002, 2,
  16. High performance bilayer-graphene terahertz detectors Davide…

    www-g.eng.cam.ac.uk/nms/publications/pdf/spirito_APL_2014.pdf
    14 Feb 2014: reports.10,20,24 This is interpreted as due to the larger gate. length, as predicted by the photo-induced voltage equation:15. ... Teppe, A. Tredicucci, and T. Nagatsuma,. Nanotechnology 24, 214002 (2013).11A. Lisauskas, S.
  17. 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: B dependence can beexplained through the Slonczewski-Weiss-McClure (SWM)model [22–24]. ... q̃ = 2mlB V1. kzmV1. cos θ. sin2 θ V 24/V 21 cos.
  18. 18 April 2012 first published online, doi: 10.1098/rspa.2012.0116468…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012GuestB.pdf
    6 Feb 2014: Figure 8 shows cubewrappings with (b, c) = (1, 0), (1, 1), (2, 0), (2, 1), which are derived from 6-, 12-,24- and 30-vertex octahedrites, respectively. ... Figure 8. Wrappings of the cube. The tiling T in each case is the dual of an octahedrite
  19. doi:

    www-g.eng.cam.ac.uk/nms/publications/pdf/c4nr00256c.pdf
    5 Jun 2014: 3HT and (b) 24% GNR with P3HT. The insets show the scan at a larger. ... 23 V, for 0%, 11%, and 24% blends. However, itwas slightly higher, ca.
  20. 26 August 2009 first published online, doi: 10.1098/rspa.2009.0307465 …

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestA.pdf
    6 Feb 2014: The network contains 33.5per cent pentagons, 24 per cent heptagons and 4.5 per cent octagons and appearsdisordered.
  21. Designing Folding Rings using PolynomialContinuation Andrew D.…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestE.pdf
    7 Aug 2014: 24].The polyhedral homotopy algorithm is based largely on workpublished by Li [19], while the path following algorithm waswritten specifically for this application. ... 
  22. Resonant Raman spectroscopy of twisted multilayer graphene

    www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6309.pdf
    10 Nov 2014: ARTICLE. Received 24 Jan 2014 | Accepted 19 Sep 2014 | Published 10 Nov 2014. ... The G peakcorresponds to the high-frequency E2g phonon at G. The Dpeak is due to the breathing modes of six-atom rings and requiresa defect for its activation16,22–24.
  23. doi:10.1016/j.ijmecsci.2006.08.003

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2007IJMS.pdf
    3 Feb 2014: kst 6f. h3s M s(24). ARTICLE IN PRESSK.A. Seffen, R.A. McMahon / International Journal of Mechanical Sciences 49 (2007) 230–238238.
  24. 1.1 Gigahertz Multi-Transistor Graphene Integrated Circuits

    www-g.eng.cam.ac.uk/nms/publications/pdf/06724538.pdf
    4 Feb 2014: Bandgap engineering is usually attempted by patterning into graphene nanoribbons (GNRs) (24,11), but GNRs tend to have low mobilities (<200 cm2V1s1) (27) as a consequence of carrier scattering on disordered ... 6, no. 24, pp. 2822-2825, 2010. (26) X. Yang
  25. acs_nn_nn-2014-00767b 1..12

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn500767b.pdf
    5 Jun 2014: These results arecomparable to those obtained with SWNTs at 1 μm.23,24. ... Opt. Lett. 2009, 34, 3526–3528. 24. Kelleher, E. J. R.; Travers, J.
  26. When is a symmetric pin-jointed framework isostatic?

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestB.pdf
    6 Feb 2014: Frameworks of higher symmetry, such as the icosahedral ðjGj 120 or 60Þ or cubic groups ðjGj 48; 24 or 12Þ cannotsatisfy even the isostatic scalar Maxwell count without having structural components
  27. Anomalous low-temperature Coulomb drag in graphene-GaAs…

    www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6824.pdf
    23 Dec 2014: Science 335, 947–950 (2012). 24. Rojo, A. G. Electron-drag effects in coupled electron systems.
  28. When is a symmetric body-hinge structure isostatic? Bernd Schulze∗ ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestC.pdf
    7 Aug 2014: 24. (a) (b). Figure 8: (a) A body-hinge structure with C3 symmetry, where each body is a flat panel.The hinge lines between panels are marked with a dashed line, ... SIAM. Journal on Discrete Mathematics, 24(4):1291–1312. Schulze, B., Sljoka, A., and
  29. 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: 6.6a,b. 0.00.20.40.60.81.01.21.41.61.82.02.22.42.62.83.03.23.43.63.84.04.24.44.64.85.0. 600. ... 24. Y. Sakakibara, A. G. Rozhin, H. Kataura, Y. Achiba, M.
  30. doi:10.1098/rspa.2008.0164

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2008GuestA.pdf
    6 Feb 2014: J. Solids Struct. 22, 409–428. (doi:10.1016/0020-. 7683(86)90014-4). Robinson, R. M. 1961 Arrangement of 24 points on a sphere.
  31. 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: Graphene is just one of a large number of possible two-dimen-ional (2D) crystals that are only now beginning to be investi-gated23,24.

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