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Advanced Structures Group
www-g.eng.cam.ac.uk/advancedstructures/publications.htmlpages = {3276--3281}, doi = {10.1073/pnas.1217998110} }. 2012. Loukaides EG, Maurini C and Seffen KA (2012), "Elementary Morphing Shells: Their Complete Behaviour", In Proceedings of IASS Symposium. ... Seoul, South Korea, 21-24 May, 2012. [Abstract: In -
arX iv:0 711. 4533 v1 [ cond -mat .mtr ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_CM2007.pdf10 Dec 2007: In general, lat-tice dynamics is calculated within the Born-Oppenheimeradiabatic framework [24, 25]. ... However, we have shownthat the BOA breaks down in the description of KA indoped graphene [28, 29]. -
PROO F COPY [ST/2003/023989] 009708Q ST Predicting Failure in ...
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/Overend%20ASCE%20paper_draft.pdf6 Jul 2011: Brown 1974 15.50 11.85. Beason 1980 10.19 7.20. Beason and Morgan 1984 26.24 20.89. -
Optical phonons in carbon nanotubes: Kohn anomalies, Peierls…
www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_PRB2007.pdf12 Feb 2007: Finally, we prove that dynamic effects inducesignificant changes in KA occurrence and shape. ... Most importantly, we observethat at only the LO mode is affected by KA. -
Original Article On zero stiffness Mark Schenk and Simon ...
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestF.pdf23 Apr 2015: stress. The specific self-stress t thus becomes. t l1k1l2k2. rðk1 þk2Þ. 24. ... 78: 011002–011008.28. Seffen KA and McMahon RA. Heating of a uniform. -
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-. -
pone.0095695 1..12
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestG.pdf23 Apr 2015: Drosophila strains and microscopyThe following stocks were used: ubiECad-GFP –hereinafter. ECadGFP [24], sGMCA [12,25]; zipperCPTI002907 (available. ... MbsN300 (24 embryos/115 vertices) (B), ASGal4/UAS-ctMLCK (17 embryos/101 vertices) (C), and -
A stable, power scaling, graphene-mode-locked all-fiber oscillator D. …
www-g.eng.cam.ac.uk/nms/publications/pdf/Popa21.pdf7 Aug 2017: Received 24 February 2017; accepted 28 May 2017; published online 12 June 2017). ... Express 24, 14152 (2016).46J. Park, K. Park, D. Spoor, B. Hall, and Y.-W. -
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.pdf26 Jul 2010: In such cases dynamic crack branching mechanics. expP kA f1f f rkmv= - - - h h. ... Further specific advice on the use of FEA in glassstructures is also available2, 24. -
SUPPLEMENTARY INFORMATIONDOI: 10.1038/NNANO.2013.46 NATURE…
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano201346si.pdf4 Apr 2013: 1(a)of the main text). Thus, KA can occur for q = Γ orq = K22. ... 56,59, once an-harmonic ef-fects are taken into account21,24,59. -
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. -
Conversionless efficient and broadband laser light diffusers for high …
www-g.eng.cam.ac.uk/nms/publications/pdf/396.pdf7 Apr 2020: However, the so-called “efficiency droop”still limits the operation of LEDs to very low input power den-sities, with current densities 0.01 kA cm2 2,9. ... In contrast to LEDs, laser diodes (LDs) can be operatedat much higher current densities (>10 -
Characterization of carbon nanotube--thermotropic nematic liquid…
www-g.eng.cam.ac.uk/nms/publications/pdf/Trushkevych_JPD2008.pdf29 May 2008: are the catalyst metals(metal impurities in the studied CNT material are estimatedto be 4%wt by the manufacturer [24]). ... 23] www.merck.de[24] http://www.sigma-aldrich.com[25] Rugar D and Hansma P 1990 Atomic force microscopy. -
nn5b06631 1..8
www-g.eng.cam.ac.uk/nms/publications/pdf/acsnano.5b06631.pdf27 Feb 2016: light detected in an experiment, γ (see Figure 5). This dependson the collection angle:24. ... Phys. Rev. Lett. 2001, 87, 023901.(24) Böhmler, M.; Hartmann, N.; Georgi, C.; Hennrich, F.; Green,A.; Hersam, M.; Hartschuh, A. -
nnano.2008.67 210..215
www-g.eng.cam.ac.uk/nms/publications/pdf/Das_NN2008.pdf7 Apr 2008: A similar behaviour isobserved for the longitudinal optic (LO) G2 peak of dopedmetallic nanotubes8,9,24, for exactly the same reasons. ... Phys. Rev. B 73, 155426 (2006). 24. Tsang, J. C., Freitag, M., Perebeinos, V., Liu, J. & -
USING STANDARD SYSTE
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PRB2000b.pdf6 Dec 2006: Received 24 November 1999! The model and theoretical understanding of the Raman spectra in disordered and amorphous carbon aregiven. ... become localized.24 Olefinic CvCbonds are shorter than aromatic bonds, so they have hi. -
Exp Astron (2009) 23:809–847DOI 10.1007/s10686-008-9115-8 O R I G ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Kuppers_EA2008.pdf23 Feb 2009: An additional Ka-band link for Doppler measurementsis proposed in order to allow a precise determination of the comet’s gravityfield even at low angles between the Earth and the Sun -
Light-enhanced liquid-phase exfoliation and current photoswitching in …
www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms11090.pdf11 Apr 2016: kcis-trans. = –0.03 h–1. ktrans-cis. = –0.79 h–1. kcis-trans. = –0.24 h–1. ... The collected precipitate is dried undervacuum for 24 h. The powder X-ray diffraction patterns are obtained using a BrukerAXS D2 Phaser (LYNXEYE detector) with -
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. ... It comes from TO phononsaround the Brillouin Zone (BZ) edge K16,22, is active by doubleresonance (DR)24, and is strongly dispersive with excitationenergy due to a Kohn -
Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and…
www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_bookchapter.pdf13 Aug 2011: Covalent functionalization of SWNTs disrupts the extended π -network,hence changes their optoelectronic properties [20, 23, 24, 57, 254].
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