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Graphene saturable absorbers for VECSELs V. J. Wittwer*a, C. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/89660X.pdf14 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. -
VOL. 53 (2012) No. 3 contents n. 173 September ...
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012GuestA.pdf6 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. -
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.pdf27 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. -
nl400516a 1..6
www-g.eng.cam.ac.uk/nms/publications/pdf/nl400516a.pdf4 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. -
This content has been downloaded from IOPscience. Please scroll ...
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestA.pdf6 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. -
5_WG3
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20pubblication/5_WG3%20%281%29.pdf27 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. -
1672 IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 26, NO. 16, ...
www-g.eng.cam.ac.uk/nms/publications/pdf/06832525.pdf21 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 -
Symmetric prismatic tensegrity structures. Part II: Symmetry-adapted…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestC.pdf6 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. -
Graphene modelocked VECSELs C.A. Zaugg1*, V.J. Wittwer2, Z. Sun2, ...
www-g.eng.cam.ac.uk/nms/publications/pdf/896607.pdf14 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, -
, 20120029, published 30 December 2013372 2014 Phil. Trans. ...
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestA.pdf6 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. -
acs_nn_nn-2014-02676g 1..10
www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf15 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, -
doi:
www-g.eng.cam.ac.uk/nms/publications/pdf/c4nr00256c.pdf5 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. -
doi:10.1016/j.sna.2006.04.016
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2007SensAct.pdf3 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:. -
1077-260X (c) 2013 IEEE. Translations and content mining are ...
www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf22 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. -
Symmetry Perspectives on Some Auxetic Body-Bar Frameworks
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestD.pdf7 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, -
RAPID COMMUNICATIONS PHYSICAL REVIEW B 89, 121402(R) (2014) Effects…
www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB.89.121402.pdf6 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. -
Designing Folding Rings using PolynomialContinuation Andrew D.…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestE.pdf7 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. ... -
High performance bilayer-graphene terahertz detectors Davide…
www-g.eng.cam.ac.uk/nms/publications/pdf/spirito_APL_2014.pdf14 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. -
18 April 2012 first published online, doi: 10.1098/rspa.2012.0116468…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012GuestB.pdf6 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 -
Resonant Raman spectroscopy of twisted multilayer graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6309.pdf10 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.
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