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11 - 20 of 27 search results for KA :ZA31 |u:www-g.eng.cam.ac.uk where 0 match all words and 27 match some words.

  1. Results that match 1 of 2 words

  2. Original Article On zero stiffness Mark Schenk and Simon ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestF.pdf
    23 Apr 2015: Int J Solids Struct 2004; 41:2801–2820. 27. Seffen KA and Guest SD. ... 78: 011002–011008.28. Seffen KA and McMahon RA. Heating of a uniform.

  3. Surface-Enhanced Raman Spectroscopyof GrapheneFred Schedin,†…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn1010842.pdf
    28 Oct 2010: p ) ε0Rnp(ω)E ε0Rnp(ω)E0x̂ (7). Rnp(ω) )6πik3. ñψ1(ñka)ψ1′ (ka) - ψ1(ka)ψ1′ (ñka)ñψ1(ñka)1′ (ka) - 1(ka)ψ1′ (ñka).

  4. pnas201217998 3276..3281

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestD.pdf
    6 Feb 2014: 16. Seffen KA (2012) Compliant shell mechanisms. Philos Trans R Soc Lond A 370(1965):2010–2026.

  5. A stable, power scaling, graphene-mode-locked all-fiber oscillator D. …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Popa21.pdf
    7 Aug 2017: A stable, power scaling, graphene-mode-locked all-fiber oscillator. D. Popa,1,a) Z. Jiang,1 G. E. Bonacchini,1 Z. Zhao,1 L. Lombardi,1 F. Torrisi,1 A. K. Ott,1. E. Lidorikis,2 and A. C. Ferrari11Cambridge Graphene Centre, University of Cambridge,

  6. 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.pdf
    26 Jul 2010: In such cases dynamic crack branching mechanics. expP kA f1f f rkmv= - - - h h.

  7. Nano Res (2010) 3: 404–411 404 Ultrafast Stretched-Pulse Fiber ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010.pdf
    21 Jun 2010: In metallic tubes, the LO mode is affected by a Kohn anomaly (KA) [43, 44], which causes the softening of this phonon [43, 44]. ... Since KA are not present in semiconducting SWNTs, the G+, G– assignment in metallic SWNTs is the opposite of

  8. pone.0095695 1..12

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestG.pdf
    23 Apr 2015: Contractile and Mechanical Properties of Epithelia withPerturbed Actomyosin DynamicsSabine C. Fischer1, Guy B. Blanchard2, Julia Duque4, Richard J. Adams2, Alfonso Martinez Arias1,. Simon D. Guest3, Nicole Gorfinkiel4. 1 Buchmann Institute for

  9. Conversionless efficient and broadband laser light diffusers for high …

    www-g.eng.cam.ac.uk/nms/publications/pdf/396.pdf
    7 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

  10. doi:10.1098/rspa.2006.1750

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/seffen2007b.pdf
    8 Jan 2008: Keywords: bistable; orthotropic; elliptical; morphing structures; Gaussian curvature. ka. RecAcc. 1.

  11. Characterization of carbon nanotube--thermotropic nematic liquid…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Trushkevych_JPD2008.pdf
    29 May 2008: Inmetallic tubes, the LO mode is affected by a Kohn anomaly(KA), which causes the softening of this phonon [43, 44].Since KA are not present in semiconducting SWNTs, theG+, G

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