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19 Jan 2018: Start from one solution u0 for α0. Make a small increment to α0 δαFind first estimate of new solution u0 δu from. ... new soltions. -. 6. rα. u. Jump over with big δα steps.

13 Dec 2018: Theory, Ed. A. Talbot, (Academic Press, New York, 1970). [3] K.R.

6 Nov 2018: Start from one solution u0 for α0. Make a small increment to α0 δαFind first estimate of new solution u0 δu from. ... Possible bifurcation.Two eigenvalues Re(λ) = 0. Eigenvectors give directions of. new soltions.

6 Nov 2018: Start from one solution u0 for α0. Make a small increment to α0 δαFind first estimate of new solution u0 δu from. ... Possible bifurcation.Two eigenvalues Re(λ) = 0. Eigenvectors give directions of. new soltions.

19 Jan 2018: No oscillations but lots of damping. Need new idea. 3. Total Variation Diminishing. ... No spurious oscillations with new minima and maxima. Preserves the monotonicity of a section of the solution.

4 Feb 2018: No oscillations but lots of damping. Need new idea. 3. Total Variation Diminishing. ... No spurious oscillations with new minima and maxima. Preserves the monotonicity of a section of the solution.

5 Feb 2018: x1. Finding LU is O(n3)but solving LUx = b for a new b is only O(n2). ... Need new direction v which does not reset u minimisation. f (xn αu βv) = f (xn) αu fn 12α2uT Au.

19 Oct 2018: andBijuj = 0,. with mass M and stiffness K as before, and two new couplingmatrices.

13 Dec 2018: to constant impedance; once this has been obtained the second term is evaluated by applyingC1 and solving again forC10 , with the term in square brackets acting as a new driving ... D A Kapp & G S Brown, A new numerical method for rough surface

13 Dec 2018: doesnot work well with existing Web services tooling” and is“too ‘object oriented’ ”. The new WS-Resource Frame-work (WS-RF) [1] proposed by the Globus Alliance, IBM,HP and others

1 Feb 2018: ρ (Miju̇j Qijkujuk ) = Bjipj µKijuj,. andBijuj = 0,. with mass M and stiffness K as before, and two new couplingmatrices.

29 Jan 2018: 3.6 Staggered grid – algorithm 4. New idea – a staggered grid with different variables at differentlocations.

6 Dec 2018: Wright (Columbia). Breaking the coherence barrier - A new theory for compressed sensing The Bath/RAL Numerical Analysis Day, Bath, UK, Jan. ... Laine (Columbia), Y. Lu (Harvard). Compressed Sensing in the Real World - The Need for a New Theory Compressed

11 Oct 2018: 3.6 Staggered grid – algorithm 4. New idea – a staggered grid with different variables at differentlocations.

4 Feb 2018: so nonlinear terms can produce new 23 M < n <43 M.

19 Oct 2018: andBijuj = 0,. with mass M and stiffness K as before, and two new couplingmatrices.

13 Dec 2018: We. would expect the matrix σ to change too: let its new components be σ′ij. ... Its components should then be unaltered by a rota-. tion of 90 about the 3-axis, i.e., with respect to new axes.

30 May 2018: 3 We can converge to dominant invariant subspaces. 4 These results allow new classification results in SCI hierarchy (notshown).

13 Dec 2018: Nghiem-Phu, A new split-step Fourier algorithm, J. Acoust. Soc. Am.Suppl. 1 77 (1987) S101. ... 22) D.A. Kapp & G.S. Brown, A new numerical method for rough surface scattering calcu-lations, IEEE Trans.

1 Feb 2018: ρ (Miju̇j Qijkujuk ) = Bjipj µKijuj,. andBijuj = 0,. with mass M and stiffness K as before, and two new couplingmatrices.