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5 Oct 2013: exponential convergence whenevern = O (. m). We note that the use of polynomial least squares for overcoming the Gibbs phenomenon, as op-posed to the Runge phenomenon, is far less well known.

13 Jan 2013: AAA. Part IB of the Mathematical Triposof the University of Cambridge. Michaelmas 2012. Linear Algebra. Lectured by:Prof. I. Grojnowski. Notes by:Alex Chan. Comments and corrections should be sent to awlc2@cam.ac.uk. This work is licensed under a

24 Sep 2013: documenten te maken die zijn geoptimaliseerd voor weergave op een beeldscherm, e-mail en internet.

2 Apr 2013: with distinct electrical, vibrational, and op-tical properties, not necessarily given bysimple superpositions of those of the innerand outer layers.11.

14 Jan 2013: Current insights in the analytic theory of fractional Cherninsulators rely on the analysis of the projected density op-erator algebra [18,19] or of emergent symmetries in the exactmany-body spectrum

18 Mar 2013: Theorem 6.1. P is a smooth point of V iff mP OP is a principal ideal. ... So in OP we have. xj = hj(x1,. ,xn) (x21,x1x2,. ,x2n) = m2P , (2 j n).

18 Mar 2013: It is not hard to show that P is just the module of differentials OP /k.). ... Proof. Obviously OP dπP P. Let f = f(P) πP g OP = k mP.

13 Jun 2013: c)n are needed,. which can be estimated from adaptation data. This factorisedadaptation is possible due to the independence between twofactor transforms, as explained in the magnifier: when the op-erating ... The constraint inEq. (4) implies that for any

19 Oct 2013: PLUMB (op. cit.) refers to this transition between the profiles o f Figs. ... waves (ANDREWS and MCINTYRE, op.

19 Oct 2013: 23 Nov 2004 1:27 AR AR235-FL37-11.tex AR235-FL37-11.sgm LaTeX2e(2002/01/18) P1: IBD10.1146/annurev.fluid.37.061903.175710. Annu. Rev. Fluid Mech. 2005. 37:263–93doi: 10.1146/annurev.fluid.37.061903.175710. Copyright c 2005 by Annual Reviews. All