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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