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Graphene speeds pair to Sto...
www-g.eng.cam.ac.uk/nms/highlights-press/Nature_Nobel.pdf6 Oct 2010: radii, which show that in graphene, 24 carbon atoms are arranged in 7 hexagons in as small asquare as 0.9nm x 0.9nm (= 0.81 nm2). -
The Stiffness of Tensegrity Structures S.D. GuestDepartment of…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2011b.pdf22 Jun 2010: It consists of j = 12nodes, and b = 30 members, made up of 24 cables and 6 struts. ... The effect of this is to leave an 24 24 symmetric matrix,for which the eigenvalues are then found. -
Russians Win Physics Nobel ...
www-g.eng.cam.ac.uk/nms/highlights-press/Bloomberg_Nobel.pdf6 Oct 2010: NASDAQ 2394.09 -5.74 (-0.24%). Stocks on the Move. By Naomi Kresge - Oct 5, 2010 4:42 PM GMT. -
IASS2009_Final
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/golabchi2009.pdf22 Jun 2010: shifted along the direction. 0. 4. 8. 12. 16. 20. 24. -
graphane-suppFFMF.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/graphane-suppFFMF.pdf20 Jul 2010: 6% -0.55 220 80 80 1 0.24 60 1.422 639 90.2. ... 24] X. Blase, C. Adessi, D. Connétable, Phys. Rev. Lett. 93, 237004 (2004). -
Making Graphene Luminescent by Oxygen Plasma Treatment
www-g.eng.cam.ac.uk/nms/publications/pdf/Gokus_ACSNANO2009.pdf14 Jan 2010: D) decreaseswith decreasing La.24 In this case, I(D)/I(G) C=()La2,with C=(514.5 nm) 0.55 nm2.24 Combining the. ... 24. Ferrari, A. C.; Robertson, J. Interpretation of Raman Spectraof Disordered and Amorphous Carbon. -
Morphing of curved corrugated shells A.D. Norman, K.A. Seffen∗ ...
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/norman2009.pdf21 Jun 2010: s =. Y0. 1. (dZ. dY. )2dY (24). =. Y0. 1. -
arX iv:1 003. 4714 v1 [ cond -mat .oth ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_Arxiv2010_graphene.pdf25 Mar 2010: arX. iv:1. 003. 4714. v1 [. cond. -mat. oth. er]. 24. ... Express 16, 20943 (2008). [24] A. Schmidt, S. Rivier, W. B. -
320 fs pulse generation from an ultrafast laser inscribed ...
www-g.eng.cam.ac.uk/nms/publications/pdf/beecher_apl2010.pdf20 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 -
First-Principles Prediction of Doped Graphaneas a High-Temperature…
www-g.eng.cam.ac.uk/nms/publications/pdf/Savini_PRL2010.pdf15 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]. -
Scanning gate microscopy of current-annealed single layer grapheneM.…
www-g.eng.cam.ac.uk/nms/publications/pdf/Connolly_APL_2010.pdf16 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 -
Phonon-Assisted Electroluminescence fromMetallic Carbon Nanotubes and …
www-g.eng.cam.ac.uk/nms/publications/pdf/Essig_nanolett_2010.pdf21 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 -
Viscous State Effect on the Activity of FeNanocatalystsFelipe…
www-g.eng.cam.ac.uk/nms/publications/pdf/nn101883s.pdf3 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. -
Graphene Mode-Locked Ultrafast LaserZhipei Sun,† Tawfique Hasan,†…
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_ACSNANO_2010.pdf23 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. -
Nano Res (2010) 3: 404–411 404 Ultrafast Stretched-Pulse Fiber ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010.pdf21 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. -
Surface-Enhanced Raman Spectroscopyof GrapheneFred Schedin,†…
www-g.eng.cam.ac.uk/nms/publications/pdf/nn1010842.pdf28 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-. -
Nano Res. 2010, 3(9): 653–660 653 A Stable, Wideband ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010b.pdf10 Sep 2010: Appl. Phys. Lett. 2009, 95, 253102. [24] Kurashima, Y.; Yokota, Y.; Miyamoto, I.; Kataura, H.; Sakakibara, Y. -
Density Gradient Ultracentrifugation of Nanotubes: Interplay of…
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_JPCh_2010.pdf15 Oct 2010: crystals21. may form well-aligned systems leading to large nonlinear opticaleffects22,23 with enhanced electro-optical properties.24,25 Bundlescould be engineered to exploit exciton energy transfer (EET)26,27. -
Graphene photonics and optoelectronics
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_naturephoto_2010.pdf31 Aug 2010: In FLG, other absorption features can be seen at lower energies, associated with interband transitions23,24.
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