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26 May 2010: A.1 Ultrasound image formation. The A-lines of an ultrasound imaging system can be mathematically modelled as a Fredholm in-.

26 Jul 2013: J. Fluid Mech. (2012), vol. 700, pp. 105–147. c Cambridge University Press 2012 105doi:10.1017/jfm.2012.101. Hydrodynamics of self-propulsion near aboundary: predictions and accuracy of. far-field approximationsSaverio E. Spagnolie1,2† and Eric

15 Jun 2020: COMPUTING SPECTRA - ON THE SOLVABILITY COMPLEXITY INDEX HIERARCHYAND TOWERS OF ALGORITHMS. J. BEN-ARTZI, M. J. COLBROOK, A. C. HANSEN, O. NEVANLINNA, AND M. SEIDEL. 1. INTRODUCTION. This paper resolves the long-standing computational spectral problem

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.

29 Jan 2019: σess(T) = {z C : T zI is not Fredholm}, ress(T) = sup{|z| : z σess(T)}.

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

17 Jun 2019: Part II 2003. 24. A2/17 Mathematical Methods. (i) Explain how to solve the Fredholm integral equation of the second kind,.

17 Feb 2017: CRITICAL SURFACE OF THE 1-2 MODEL. GEOFFREY R. GRIMMETT AND ZHONGYANG LI. Abstract. The 1-2 model on the hexagonal lattice is a model of statistical me-chanics in which each vertex is constrained to have degree either 1 or 2. Thereare three

22 Oct 2016: Complexity Issues in Computing Spectra, Pseudospectra. and Resolvents. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, Cambridge CB3 0WA. United Kingdom. Olavi NevanlinnaDepartment of Mathematics and

15 Jul 2023: Spd 𝑇 = 𝜆 Sp 𝑇 : 𝜆 isolated, 𝑇 𝜆 Fredholm.