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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

13 Dec 2018: The new inversion technique has been applied to an area covering the offshore sandbanks at Gt Yarmouth on the East Coast of the UK.

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.

31 Dec 2018: positions, this doesn’t give us a new state of the system – it is the same state that we. ... But Maxwell was able to take. things further. He used kinetic theory to derive the first genuinely new prediction of.

18 Nov 2018: and a New Classification TheoryNovel Algorithms, Impossibility Results and Computer Assisted Proofs.

13 Dec 2018: vh. vy. þS0ðx;y; tÞ ð4Þ. where S0(x,y,t) is a new source function. ... An assessment of a new settling velocity pa-. rameterisation for cohesive sediment transport modelling.

24 Jul 2018: An example is shown later in 9. Effects and benefits of the new principles. ... The subsampling pattern forthe new CS approach is the the one used in Fig.

27 Nov 2018: s ξ. s(ξs)† = 12. This is obviously true if we choose the basis ξ1 = (1, 0) and ξ2 = (0, 1).A new basis that remains orthonormal can then be constructed

2 Nov 2018: observed to be smaller and exhibit fractal behaviour (Karman, McDonald, New & Wo-. ... present in this paper a new expression involving the error function for each entry of the.

17 Apr 2018: Orthogonal systems with a skew-symmetric. differentiation matrix. Arieh IserlesDepartment of Applied Mathematics and Theoretical Physics. Centre for Mathematical SciencesUniversity of Cambridge. Wilberforce Rd, Cambridge CB4 1LEUnited Kingdom.

14 May 2018: Taking our lead from Fourier analysis, we introduce a new bosonic scalar field h (sometimes. ... will be a symmetry of the quantum theory, and all new terms that are generated by RG.

3 Apr 2018: 2. 〈f〉0 = f; and. 3. 〈1〉2 = 2x. With this new notation in place and using (2.6), we can now simplify commutatorsto anti-commutators,. ... Singh. 2.6 Fourth order Magnus expansions. With this new notation in place, the Magnus expansions Θ2(h) and

28 Dec 2018: The code then calculates a new mesh by propagating the deformation throughout the.

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.

18 Apr 2018: PHYSICAL REVIEW FLUIDS 3, 043601 (2018). Collective dissolution of microbubbles. Sébastien Michelin,1,2, Etienne Guérin,3 and Eric Lauga2,†1LadHyX, Département de Mécanique, Ecole Polytechnique, CNRS, 91128 Palaiseau, France. 2Department of

13 Apr 2018: Crew and A. de Salvio, Dialogues Con-cerning Two New Sciences (Macmillan, New York, 1914). ... 20] M. Abramowitz and I. A. Stegun, Handbook of MathematicalFunctions (Dover, New York, 1965).

19 Jan 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: so nonlinear terms can produce new 23 M < n <43 M.

11 Oct 2018: We will seehowever that by adequately introducing new variables we can express it as a linear program.

13 Dec 2018: BAE Research Report, August 1995. 3 Kapp, D.A., and Brown, G.S.: ‘A new numerical method for roughsurface scattering calculations’, IEEE Trans.

13 Dec 2018: Mathematical modelling of shoreline evolu-tion, Proc. 16th Coast. Engrg. Conf., ASCE, New York, N.Y., p1163-1179. ... Coast. Struct. ’79,ASCE, New York, N.Y., p809-837. Wind, H.G., 1990. Influence functions, Proc.

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

13 Dec 2018: 3] Hsu, T-W., Ou, S-H & Wang, S-K., 1994. On the prediction of beach changes by a new 2-D empirical eigenfunction model, Coastal Engineering, 23, p255-270.

13 Dec 2018: lo] Mone P M and Feshbach H 1953 Methods of Zheoretical Physics I (New York: McGraw-Hill) [ll] Spivack M 1990 1 Acowf.

13 Dec 2018: Using the new Green’s function we can then derive extended forms of Eqs.4! ... 16Academic, New York, 1980! 2T. W. Dawson and J. A. Fawcett, ‘‘A boundary integral equation methfor acoustic scattering in a waveguide with nonplanar surfaces,’Acoust.

13 Dec 2018: 15A. Papoulis, Probability, Random Variables, and Stochastic Processes (McGraw-Hill, New York, 1981). ... 16A. Erd61yi, Tables oflntegral Transforms, I (McGraw-Hill, New York, 1954). 700 J.

13 Dec 2018: a new insight into the long-term spatial and temporal variations in coastline alignment. ... simplified solutions Proc. Comral Structue.es pp 809-36 (New York American Society of Civil Engineen).

10 Mar 2018: The remaining sixtypes define new transcendental functions and are given by the Painlevé equations. ... III. REDUCIBILITY AND FIRST INTEGRALS. The metrisable cases of PIII and PV do not define new transcendental functions but admit aquadrature and are

3 Aug 2018: shed new light on the physiology of gait control in flagellates,revealing its strongly nonequilibrium character.

13 Dec 2018: E. Wolf (Elsevier, New York, 1986). 5. A.G. Voronovitch, Wave Scattering from Rough Surfaces (Springer, Berlin, 1994). ... Nghiem-Phu, A new split-step Fourier algorithm, J. Acoust. Soc. Am. Suppl.

16 Jul 2018: At the end of a tum-ble, the motors return to their normal CCW state, the bundle reforms and the bacterium swims in a new direc-tion. ... E. coli in Motion. Biological and Medical Physics, Biomedical Engineering. Springer-Verlag New York (2004).

13 Dec 2018: implemented by a bounded operator. The proof constructs this operator. explicitly and hence yields a new and slightly more informative proof for nest.