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pages = {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.

15 Oct 2010: Herman Oestrich considering turbojet designs at Siemens (date unconfirmed). Russia. Lyul’ka’s proposal for a turbojet (date unconfirmed).

10 Dec 2007: However, we have shownthat the BOA breaks down in the description of KA indoped graphene [28, 29]. ... to the Fermi-Dirac distribution and determines the shape of the KA.At thermal equilibrium Ti = Te = T.

6 Jul 2011: structure (Ka denotes the "Penalty"-value of the stiffness). Ka should be chosen at. ... grid points. A much larger Ka value may slow down convergence or cause.

12 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.

3 Feb 2014: 3. Norman AD, Seffen KA, Guest SD. Multistable corrugated shells. Proc R Soc A 2008;464:1653–1672. ... 4. Seffen KA, Pellegrino S. Deployment dynamics of tape-springs. Proc. R.

24 Jan 2012: 41, No. 7-8, 2004, pp. 2801-2820. [5] Seffen KA, and Guest S, “Prestressed Morphing Bistable and Neutrally Stable Shells”, Journal of Applied Mechanics, ASME, Vol. ... 464, No. 2099, 2008, p. 2949. [9] Seffen KA, “Morphing bistable orthotropic

28 May 2008: B.R. Bu"ka, I.V. Dinu and M. T- olea 2614. Ion irradiation of carbon nanotubes encapsulating cobalt crystals. ... 2294Bournel, A. 2294Buc, D. 2247Bu"ka, B.R. 2614Bullough, T.J. 2457. C. Calogero, G.

6 Jul 2011: PROO. F COPY [ST/2003/023989] 009708Q. ST Predicting Failure in Glass—A General Crack Growth Model. M. Overend1; G. A. R. Parke2; and D. Buhagiar3. Abstract: The successful design of glass as a structural element depends mainly on the ability to

4 Apr 2013: 1(a)of the main text). Thus, KA can occur for q = Γ orq = K22. ... The presence of KA explainsthe difference in the Raman spectra of semiconductingand metallic tubes25,56.

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.

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).

6 Feb 2014: 16. Seffen KA (2012) Compliant shell mechanisms. Philos Trans R Soc Lond A 370(1965):2010–2026.

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,

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

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

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

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

8 Jan 2008: Keywords: bistable; orthotropic; elliptical; morphing structures; Gaussian curvature. ka. RecAcc. 1.

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

7 Apr 2008: at 514 nm, the influence ofdynamic effects is expected to be negligible, because the phononsgiving rise to the 2D peak are far away from the KA at K.

23 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

27 Feb 2016: edge K,5,12,13 is activeby double resonance (DR),14,15 and is strongly dispersive withexcitation energy due to a Kohn Anomaly (KA) at K.16 DR canalso happen as

6 Dec 2006: The p band energies alongGK M innearest-neighbor tight-binding approximation are. E5 6 gu11 2 cos ka!u, 1! ... 11 2 cos ka!5 2a. L a3! or sin(Dka)'a/()La) for small Dk, whereDk is the k dis-.

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 Anomaly (KA) at

11 Apr 2016: 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 Ni-filtrated Cu-Ka

13 Aug 2011: Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and Optoelectronics. T. Hasan, V. Scardaci, P.H. Tan, F. Bonaccorso, A.G. Rozhin, Z. Sun,and A.C. Ferrari. Abstract Polymer composites are an attractive near-term means to exploit