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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.

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

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

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

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

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.

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.

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

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.

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).