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16 Nov 2007: ". #$! % &! '$#%. ( )& #-,.-. /1032546087:9<;>=@?AB08CEDGF@HJIK2>4. LNMPORQTSVUWXSLNY[ZTZT][. _PUabcdOfehgig[j. kmlonpnKqsrptpuvtplowyxznp{-|}ltKtKqwVrtp-q. kdqsVrpqsq@wVikdwtKwVrwV[_lowynKwVa. "!#$% '&)( ,-. /.

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.

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.

20 Nov 2007: Conway, KA, Lee, SJ, Rochet, JC, Ding, TT, Williamson, RE, andLansbury, PT (2000).

24 Apr 2007: 56. Smith LJ, Bolin KA, Schwalbe H, MacArthur MW, Thornton JM,Dobson CM: Analysis of main chain torsion angles in proteins:prediction of NMR coupling constants for native and randomcoil conformations.

25 Jan 2007: N M Mt 2ik2[σ3, M ] kA(x, t)M B(x, t)M. (4.3.13).

27 Nov 2007: 0 ikeika ikeika k̃ek̃a.  = 0which yields. tan ka =2kk̃.

17 Apr 2007: It therefore followsfrom (22) that Xa, Xa, Ya Y a are gradients and that Ka = Ya Y a is a Killing vector.

27 Jul 2007: K bb Ka = 12ηKa. Thus K is automatically geodesic, and if it is pure then its trajectories are parameterizedby an affine parameter.

29 Jul 2007: Ka = αAβ̂A′ α̂AβA′ is a Killing vector, and deduce the form of themetric.