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20 Nov 2023: Brown [27–29]) and Toeplitztheory (see A. Böttcher & B. Silberman [24–26]).

1 Dec 2023: Received 24 February 2017; revised 22 May 2017; accepted 10 July 2017;first published online 30 August 2017).

1 Dec 2023: u = 0. (2.1). In place of the Navier–Stokes equations for an unconfined fluid, in a porous medium the Darcyvelocity u is governed by Darcy’s Law [23,24], which

29 Dec 2023: Z(1.24). If we make a measurement described by an operator Ô, then the probability that wefind ourselves in the eigenstate |ϕ⟩ is given by.

11 Jun 2024: There has been a proliferation of architectures inspiredby spectral graph theory [11], convolutional (GCN) [24], message passing (MPNN) [15] and atten-tional (GAT) [40] approaches. ... 24] T. N. Kipf and M. Welling. Semi-Supervised Classification with

19 Nov 2023: Part IIC Michaelmas term 2021. QUANTUM INFORMATION. AND COMPUTATION. Lecture notes. Richard Jozsa, DAMTP Cambridgerj310@cam.ac.uk. “Joy in looking and comprehending is nature’s most beautiful gift.”A. Einstein, aphorism 1953. 1. CONTENTS. 1

1 Dec 2023: J. Fluid Mech. (2020), vol. 882, A11. c Cambridge University Press 2019doi:10.1017/jfm.2019.812. 882 A11-1. Translating and squirming cylinders in aviscoplastic fluid. R. Supekar1,†, D. R. Hewitt2 and N. J. Balmforth3. 1Department of Mechanical

5 Jan 2024: JHEP 0304 (2003) 031, hep-th/0303151. [24] Comments on Condensates in Non-Supersymmetric Orbifold Field Theories.

1 Dec 2023: J. Fluid Mech. (2013), vol. 719, pp. 551–586. c Cambridge University Press 2013 551doi:10.1017/jfm.2013.23. Convective shutdown in a porous medium athigh Rayleigh number. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1.

1 Dec 2023: J. Fluid Mech. (2022), vol. 941, A56, doi:10.1017/jfm.2022.335. Evolution of convection in a layered porousmedium. Duncan R. Hewitt†. Department of Mathematics, University College London, 25 Gordon Street, London WC1H 0AY, UK. (Received 30

18 Dec 2023: 1. INTRODUCTION. In the wake of the many AI-based algorithms throughout the society and the sciences, potentially yielding hal-lucinations and instabilities [4, 23, 23, 24, 31, 34, 38, 40,

30 Oct 2023: If. u(x,y) =k,lZ. ûk,leiπ(kxly). 24. is the Fourier expansion of u, the bivariate versions of the algebra of Fourier expansions gives(denoting ux = u/x and

26 Jul 2023: are associated with banded differentiation and multiplication matrices, and expansion coefficients can be computed from function samples in quasi-linear time with the FFT [24]. ... J. Integral Equ. Appl. 19, 163– 207 (2007). 24. Iserles, A., Webb, M.:

11 Mar 2024: The kinematics of hexagonal magnetoconvection. Geo.Astro. Fluid Dyn., 24:109–136, 1983. 24. ... Phys. Fluids, 24,107103, 2012. 1975-1980 1981-1990 1991-2000 2001-2010 2011-2020 2021-2030. 184.

6 Apr 2024: Slide 23: Convergence of measures. Slide 24: Further convergence. Slide 25: Lorenz system.

26 Jun 2024: 2.1.2 The Infinite Potential Well 24. 2.1.3 The Gaussian Wavepacket 27. ... 24 –. easy to deal with. The Schrödinger equation equation is.

1 Dec 2023: J. Fluid Mech. (2021), vol. 920, A35, doi:10.1017/jfm.2021.449. High-Rayleigh-number convection inporous–fluid layers. Thomas Le Reun1,† and Duncan R. Hewitt2. 1Department of Applied Mathematics and Theoretical Physics, Centre for Mathematical

18 Dec 2023: Condition in optimisation: The concept of condition numbers has proven a crucial to computational math-ematics and numerical analysis for securing trustworthy algorithms that are accurate and stable [24, 35].J.

1 May 2024: 18] and Huybrechs & Olteanu [24]). In the current manuscript,we aim to provide an introductory but rigorous analysis of the least-squares oversampled col-location method. ... uχ′N‖2α chl2α‖u‖l, (22)‖uχ′N‖r2α chl2αr‖u‖l, (23). and

3 Jul 2024: 2.3.1 The Gravitational Field 22. 2.3.2 Escape Velocity 24. 2.3.3 Inertial vs Gravitational Mass 25.