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4 Dec 2008: Hg ;? S. A> <<FHJ >? S C?D R C<=O; KA> <<FA= C>?

9 Jan 2008: as follows. h01 h1 (18)h02 h2 mh1 (19). where m kh1, h2l/kh1, h1l is the GS coefficient and ka, blaHb.

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 May 2008: Condensation of Classical Nonlinear Waves in a Two-Component System. Hayder Salman and Natalia G. BerloffDepartment of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, CB3 0WA, UK. Abstract. We study the formation of

25 Nov 2008: inal. wor. kA. nin. vest. igat. ion. into. the. Law. sof.

28 Nov 2008: Titration curves were fitted to the data using the ORIGIN program (MicroCal Inc.) which yielded the stoichiometry (1), the binary association constant Ka (=Kd -1) and the enthalpy of binding. ... The entropy of binding (S) was calculated from the

31 Jul 2008: On modified asymptotic series involving confluent. hypergeometric functions. Alfredo DeañoDAMTP, Centre for Mathematical Sciences,. University of Cambridge,Wilberforce Road, CB3 0WA, UK. Nico M. TemmeCWI, P.O. Box 94079, 1090 GB Amsterdam, The

26 Jun 2008: KA&&,#- 25,. @32 <-2<3-322<2 322. @3 2- 3<-332< -2< 32. FA661,6#$#.# ,, ,$1?

18 Oct 2008: # 2008 The Authors. Journal compilation # 2008 Blackwell Publishing Ltd. doi: 10.1111/j.1600-0854.2008.00761.xTraffic 2008; 9: 1327–1343Blackwell Munksgaard. Membrane Localization is Critical for Activationof the PICK1 BAR Domain. Kenneth L.

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.