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Publications: Edited Volumes A. Iserles (ed.), Acta Numerica 27, ...
www.damtp.cam.ac.uk/user/na/people/Arieh/Arieh_Iserles/Edited.html23 May 2018: Iserles (ed.), Acta Numerica 24, Cambridge Univ. Press (2015). A. Iserles (ed.), Acta Numerica 23, Cambridge Univ. -
Our local environment and theeconomy Why nature needs to ...
www.damtp.cam.ac.uk/user/pvl/nature/workshop.pdf25 Oct 2018: Our local environment and theeconomy. Why nature needs to be taken into account in planning andeconomic decisions. Friday 28 September 2018, 12:45 – 17:30at Centre for Mathematical Sciences, Cambridge CB3 0WA. 12:45 Lunch13:30 Introductory talks -
On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...
www.damtp.cam.ac.uk/research/afha/anders/Asymptotic_10a.pdf24 Jul 2018: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... This can be coupled with hidden Markov treesto model the wavelet structure, such as in the Bayesian CS (22, 23)and TurboAMP (24) algorithms. -
Compact schemes for laser-matter interaction in Schrödinger equation …
www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_03.pdf21 Apr 2018: 1Ṽ , (3.4). where V̂ is an O(h3). perturbation of Ṽ ,. V̂ = Ṽ h2. 24 (Ṽ )>(Ṽ ). (3.5). The overall order-four scheme is obtained by substituting the central ... 2. 24 (Ṽ )>(Ṽ )). Thus, a fourth-order compact splitting,. e16 ihε. -
Preprint typeset in JHEP style - PAPER VERSION Easter ...
www.damtp.cam.ac.uk/user/examples/B6La.pdf19 Sep 2018: 6. First integrals and Fermat’s principle 24. 7. Constrained variation of functionals 27. ... 24 –. c1 BAn(z)dl, where the integral is along the path. -
On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...
www.damtp.cam.ac.uk/research/afha/people/anders/Asymptotic_10a.pdf24 Jul 2018: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... This can be coupled with hidden Markov treesto model the wavelet structure, such as in the Bayesian CS (22, 23)and TurboAMP (24) algorithms. -
Magnus–Lanczos methods with simplified commutators for the…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_01.pdf3 Apr 2018: h7), (2.23). Magnus–Lanczos methods with simplified commutators 15. where. ϕ1(h,ζ,ξ) = h2 4hξ 2ζξ, (2.24). -
Spectral computation of highly oscillatory integral equations in…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_04.pdf2 Nov 2018: operator (the case γ = 1) represents a challenge for spectral theory (Böttcher, Grudsky &. Iserles 2012). 24. Figure 4.3: The eigenvalues of the integral operator with ω = 100 for γ = -
Orthogonal systems with a skew-symmetric differentiation matrix Arieh …
www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_02.pdf17 Apr 2018: 24. (Levin & Lubinsky 2001, Van Assche 2018). Hermite polynomials form the simplestexample, other familiar cases are Q(x) = x4 tx2 for some t R and Q(x) = |x|(whereby smoothness fails -
Advanced Quantum Field Theory Lent Term 2013 Hugh Osborn ...
www.damtp.cam.ac.uk/user/examples/3P5a.pdf23 Jan 2018: qq′). (1.24). Upon the substitution p′ = p m(qq′). t this becomes. ... Z0[J] =. d[ϕ] e. i2. ddx (µϕ(x)µϕ(x)m. 2ϕ2(x))iddx J(x)ϕ(x). (2.24). This is an integral with a highly oscillating integrand; if
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