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Statistical moments for rough surface scatter from two-way parabolic…
www.damtp.cam.ac.uk/user/ms100/PAPERS/pebacksc-JModOpt.pdf13 Dec 2018: As an illustration of the method, Figure 1 shows comparisons between the firstand second iterations of the operator series with ’exact’ computations from (24 ),restricted to the rough portion of the ... αr r′. = f(r,r′) (24). the expression (23) -
Coherent Field and Specular Reflection At Grazing Incidence on a…
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA94spec.pdf13 Dec 2018: 0 Zl ( (•(x,zi))=--• Do(X)-- likzi cos 0 --• COS 2 0 eikXx+ h(x)• ,. (24). where • is the variance of the surface height. Here we have neglected an O(a ... 29) Collecting terms, and using (25), (26), and (29), Eq. (24) can now be written. ( {• -
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). -
The Computational Spectral Problem and a New Classification Theory…
www.damtp.cam.ac.uk/user/mjc249/talks/SCI_colbrook_berkeleytalk.pdf16 Nov 2018: Doyle and C. McMullen [24]: “But can be solved in the case ofthe quartic and the quintic using several limits (towers of generallyconvergent iterative maps linked serially).”. ... P. Doyle and C. McMullen [24]: “But can be solved in the case ofthe -
Recovery of rough surface in ducting medium from grazing ...
www.damtp.cam.ac.uk/user/ms100/PAPERS/main-JAP.pdf13 Dec 2018: h(Xn) = z |Sn(xn Xn)3/2. αφ(Xn)δ|. (24). 2. Medium with Linear Profile. ... Reconstruct the surface h(Xn) by eq. (24) for uniformmedium or (26) for linear profile using Φ obtained aboveend for. -
Metrisability of Painlevé equations
www.damtp.cam.ac.uk/user/md327/cd18.pdf10 Mar 2018: A different approach was developed by Painlevé, Kowalevskaya, and Gambier who studied 2ndorder ODEs in the complex domain.16,24. ... Proc. Cambridge Philos. Soc. 156, 99–113. (2014).24 Painlevé, P., “Sur les équations différentielles du -
Efficient boundary integral solution for acousticwave scattering by…
www.damtp.cam.ac.uk/user/ms100/PAPERS/acoust3d_eabe_b.pdf13 Dec 2018: 2.1. Formal solution and splitting series. The method of solution is analogous to that applied to the electromagneticproblem in 2-d or 3-d [23, 24]. ... 24] M. Spivack, J. Ogilvy, C. Sillence, Electromagnetic scattering by large com-plex scatterers in 3d, -
Jumps, folds and singularities of Kodaira moduli spaces
www.damtp.cam.ac.uk/user/md327/DGT18.pdf19 Jul 2018: Thus the space oforbits of K2 in MC admits a Toda Einstein–Weyl structure [3, 24].• There exists a combination of self-dual two-forms which is degenerate when the harmonic. ... Roy. Soc. A363 (1978) 289–295.24. R. S. Ward, ‘Einstein-Weyl spaces -
The Computational Spectral Problem and a New Classification Theory…
www.damtp.cam.ac.uk/user/mjc249/talks/SCI_colbrook_irvinetalk.pdf18 Nov 2018: Doyle and C. McMullen [24]: “But can be solved in the case ofthe quartic and the quintic using several limits (towers of generallyconvergent iterative maps linked serially).”. ... P. Doyle and C. McMullen [24]: “But can be solved in the case ofthe -
Research Article Journal of the Optical Society of America ...
www.damtp.cam.ac.uk/user/ms100/PAPERS/rough-surface-reconstruction.pdf13 Dec 2018: For scalar wave fields witharbitrary incident angles the scattered field obeys the Helmholtzboundary integral equation [1, 24]. ... Sel. Top. Appl. Earth Obs. Remote. Sens. 7,1573–1583 (2014). 24. J.
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