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Consider a space XX, such as a compact space of JJ-holomorphic stable maps with closed domain, that is the zero set of a Fredholm operator.

I will survey various results on applications and extensions of Hofer-Wysocki-Zehnder's polyfold theory: - fiber products of polyfold Fredholm sections - equivariant transversality - existence and obstructions - equivariant fundamental class -

23 Aug 2023: This. isa. spec. ific. indiv. idual’s. copy. of. the. note. s.P. lease. do. not. copy. and/or. redis. trib. ute. Mathematical Tripos: Part III PM. Contents. 0 Perturbation Methods (16 Lectures) i. 0.1 Introduction. i. 1 Algebraic Equations 1. 1.1

16 Oct 2007: 250 D. Vella and H. E. Huppert. C. Upon discretizing the contour C, (3.3) gives rise to a series of Fredholm integralequations of the second kind for the unknown parts

27 Apr 2019: Choosing the Green’s function that satisfies ahomogeneous Dirichlet boundary condition on the x-axis, the boundary integral equations giverise to the following Fredholm integral equation of the first kind.

26 Jul 2013: The slenderbody theory generates a system of Fredholm integral equa-tions of the first kind which are in general susceptible tooscillatory behavior or slow convergence in their numericalsolution, particularly when the

26 Mar 2011: However, in the case at hand wecan say more. There are explicit formulae for the Fredholm determinants ofWiener–Hopf operators with rational symbols. ... Iserles, and S. P. Nørsett, The spectral problem for a class ofhighly oscillatory Fredholm

We develop a continuous version of Kasteleyn theory to show that partition functions for bead configurations on T_n may be expressed in terms of Fredholm determinants of certain operators on

21 Apr 2006: We may therefore express the imaging process by the Fredholm integral,. ... x, y, z) = δ (xp) δ (z z0).Expressing the Fredholm integral of Equation 1 in terms of xp and yp, we obtaing (x, y, t) =. h (x′ cos θ y′

2 Jun 2015: O.F. BANDTLOW, I. ANTONIOU and Z. SUCHANECKI "Resonances of Dynamical Systems and Fredholm-Riesz Operators on Rigged Hilbert Spaces" Computers & Mathematics with Applications 34, 95-102 (1997).

26 Jul 2023: Sp 𝑇 = 𝜆 Ω: 𝑇 𝜆 is not invertible. Spd 𝑇 = 𝜆 Sp 𝑇 : 𝜆 isolated, 𝑇 𝜆 Fredholm.

12 Nov 2010: Spectral theory of large Wiener–Hopf operators with. complex-symmetric kernels and rational symbols. Albrecht Böttcher Sergei Grudsky Arieh Iserles. November 12, 2010. AbstractThis paper is devoted to the asymptotic behaviour of individual

2 Nov 2018: 2011), ‘The computation of the spectra of highly. oscillatory Fredholm integral operators’, J.

5 Feb 2008: SOIL DYNAMICS. Arnold Verruijt. Delft University of Technology. 1994, 2008. PREFACE. This book gives the material for a course on Soil Dynamics, as given for about 10 years at the Delft University of Technology for students ofcivil engineering, and

15 Jul 2023: Sp 𝑇 = 𝜆 Ω: 𝑇 𝜆 is not invertible. Spd 𝑇 = 𝜆 Sp 𝑇 : 𝜆 isolated, 𝑇 𝜆 Fredholm.

23 Sep 2020: royalsocietypublishing.org/journal/rspa. ResearchCite this article: Colbrook MJ, Kisil AV. 2020 AMathieu function boundary spectral methodfor scattering by multiple variable poro-elasticplates, with applications to metamaterials andacoustics.

19 Dec 2022: With respect to the standard complex structure, there are N families of smooth holomorphicdiscs of index 2, and they are all Fredholm regular.

22 Feb 2024: H. Brunner, A. Iserles & S. Nørsett, "The computation of the spectra of highly oscillatory Fredholm integral operators", J. ... Nørsett, "The spectral problem for a class of highly oscillatory Fredholm differential equations" IMA J.

30 May 2024: 2883. (doi: 10.1214/11-aos924). The computation of the spectra of highly oscillatory Fredholm integral operators.

30 May 2024: The Astrophysical Journal. (2008). 689,. 377. (doi: 10.1086/592374). The spectral problem for a class of highly oscillatory Fredholm integral operators.