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Carlota M. Cuesta

Publications and source records attributed to Carlota M. Cuesta.

14 recordsLinked to original sources

A matrix-based spectral method for the numerical approximation of the fractional Laplacian and the fractional $p$-Laplacian of functions defined on $\mathbb R^n$

Given a function $u$ defined on $\mathbb R^n$, its fractional $p$-Laplacian is given by $$(-Δ)_p^su(\vec x)=C_1(n,s,p)\int_{\mathbb R^n}\frac{|u(\vec x)-u(\vec y)|^{p-2}(u(\vec x)-u(\vec y))}{\|\vec x-\vec y\|_2^{n+sp}}d\vec y,\quad\vec x\in\mathbb R^n,$$where the integral is understood in the principal value sense, $p\in(1,\infty)$, $s\in(0,1)$, and $C_1(n,s,p)$ is a normalization constant. A formally equivalent nonlinear Balakrishnan formulation is given by $$(-Δ)_p^su(\vec x)=C_4(n,s,p)\int_0^\inftyΔ(t-Δ)^{-1}\left[Φ_p(u(\vec x)-u(\cdot))\right](\vec x)\frac{dt}{t^{1-sp/2}},$$ where $C_4(n,s,p)$ is another normalization constant, and $Φ_p(t)=|t|^{p-2}t$. In this paper, we present a matrix-based spectral method to approximate numerically the fractional Laplacian (i.e., the linear case, where $p = 2$) and the fractional $p$-Laplacian for functions defined on $\mathbb R^n$. Our approach builds on the Balakrishnan representation, where we discretize the 2nd-order derivatives in $Δ$ using spectrally accurate differentiation matrices. A key advantage is that these matrices can be diagonalized in a well-conditioned manner, enabling a stable and robust numerical scheme that naturally extends to arbitrary spatial dimensions $n$. In particular, this diagonalization allows the fractional operator to act directly on the eigenvalue spectrum, effectively reducing the Balakrishnan integral to an analytical evaluation at the spectral level and thereby avoiding costly multidimensional quadrature. The resulting method also avoids domain truncation and variational formulations, making it both computationally efficient and conceptually straightforward. As a practical application, we simulate the evolution of $$\frac{\partial u}{\partial t}+(-Δ)^s_pu=0,$$in one and two spatial dimensions, being able to capture the self-similar solutions that arise as $t\to\infty$.

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A Non-Recursive, Dimension-Independent Schur-Decomposition Algorithm for $N$-Dimensional Sylvester Tensor Equations

In this paper we present a non-recursive direct solver, based on the Bartels-Stewart algorithm, for $N$-dimensional Sylvester tensor equations. The method relies only on Schur decompositions of the coefficient matrices and reduces the computation to a single sequential sweep over tensor entries, making it entirely independent of the dimension $N$. Its main advantages are simplicity, a dimension-independent formulation, and the ability to solve very high-dimensional problems limited only by available memory, which is used efficiently. We successfully solve cases up to $N=29$ on a standard laptop with $32$ GB RAM. Compared with the recursive blocked method of Chen and Kressner (state of the art), both approaches achieve identical accuracy. The recursive method is faster for large coefficient matrices, whereas our solver is competitive or superior when matrices are small, especially for large $N$, where recursive methods cannot effectively exploit BLAS-3 kernels. It also uses memory more efficiently: for near-capacity problems (e.g., matrices of order $19$ with $N=7$, where solution and right-hand side occupy $\approx 28$ GB), the Chen-Kressner method exceeds available memory, while ours succeeds. The method is also significantly simpler to implement, fully independent of $N$, and correctly handles singleton dimensions. We detail the algorithm and derive accurate cost estimates. For reproducibility, we provide pseudocode and complete MATLAB implementations. As an application, we compute solutions of linear $N$-dimensional ODE systems with constant coefficients at arbitrary times, and thus of evolutionary PDEs after spatial discretization, including highly accurate solutions of an advection-diffusion equation on $\mathbb{R}^N$.

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Doubly nonlinear parabolic equation involving a mixed local-nonlocal operator and a convection term

In this paper we study a doubly degenerate parabolic equation involving a convection term and the operator $\mathcal{A}_μu:=-Δ_p u +μ(-Δ)^s_q u$ which is a linear combination of the $p$-Laplacian and the fractional $q$-Laplacian, and results in a mixed local-nonlocal nonlinear operator. The problem we study is the following, \begin{equation*} \begin{cases} \partial_t β(u)+ \mathcal{A}_μu= div (\overset{\to}{f}(u))+g(t,x,u) \quad \text{in} \;Q_T:=(0,T)\times Ω, u=0 \quad \text{in} \; (0,T)\times (\mathbb{R}^d \backslash Ω), u(0)=u_0 \text{ in } Ω. \end{cases}\ \end{equation*} We discuss existence, uniqueness and qualitative behavior of, what we call {\it weak-mild} solutions, that is weak solutions of this problem that when interpreted as $v=β(u)$ they are a mild solutions. In particular, we investigate stabilization to steady state, extinction and blow up in finite time and show how the occurrence of such behaviors depend on specific conditions on the nonlinearities $β$ (typically of porous media type), $\overset{\to}{f}$ and the source term $g$, and on their relation, in terms of certain regularity and growth conditions.

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Numerical Approximation of Riesz-Feller Operators on $\mathbb R$

In this paper, we develop an accurate pseudospectral method to approximate numerically the Riesz-Feller operator $D_γ^α$ on $\mathbb R$, where $α\in(0,2)$, and $|γ|\le\min\{α, 2 - α\}$. This operator can be written as a linear combination of the Weyl-Marchaud derivatives $\mathcal{D}^α$ and $\overline{\mathcal{D}^α}$, when $α\in(0,1)$, and of $\partial_x\mathcal{D}^{α-1}$ and $\partial_x\overline{\mathcal{D}^{α-1}}$, when $α\in(1,2)$. Given the so-called Higgins functions $λ_k(x) = ((ix-1)/(ix+1))^k$, where $k\in\mathbb Z$, we compute explicitly, using complex variable techniques, $\mathcal{D}^α[λ_k](x)$, $\overline{\mathcal{D}^α}[λ_k](x)$, $\partial_x\mathcal{D}^{α-1}[λ_k](x)$, $\partial_x\overline{\mathcal{D}^{α-1}}[λ_k](x)$ and $D_γ^α[λ_k](x)$, in terms of the Gaussian hypergeometric function ${}_2F_1$, and relate these results to previous ones for the fractional Laplacian. This enables us to approximate $\mathcal{D}^α[u](x)$, $\overline{\mathcal{D}^α}[u](x)$, $\partial_x\mathcal{D}^{α-1}[u](x)$, $\partial_x\overline{\mathcal{D}^{α-1}}[u](x)$ and $D_γ^α[u](x)$, for bounded continuous functions $u(x)$. Finally, we simulate a nonlinear Riesz-Feller fractional diffusion equation, characterized by having front propagating solutions whose speed grows exponentially in time.

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Numerical computation of the half Laplacian by means of a fast convolution algorithm

In this paper, we develop a fast and accurate pseudospectral method to approximate numerically the half Laplacian $(-Δ)^{1/2}$ of a function on $\mathbb{R}$, which is equivalent to the Hilbert transform of the derivative of the function. The main ideas are as follows. Given a twice continuously differentiable bounded function $u\in\mathcal C_b^2(\mathbb{R})$, we apply the change of variable $x=L\cot(s)$, with $L>0$ and $s\in[0,π]$, which maps $\mathbb{R}$ into $[0,π]$, and denote $(-Δ)_s^{1/2}u(x(s)) \equiv (-Δ)^{1/2}u(x)$. Therefore, by performing a Fourier series expansion of $u(x(s))$, the problem is reduced to computing $(-Δ)_s^{1/2}e^{iks} \equiv (-Δ)^{1/2}[(x + i)^k/(1+x^2)^{k/2}]$. On a previous work, we considered the case with $k$ even for the more general power $α/2$, with $α\in(0,2)$, so here we focus on the case with $k$ odd. More precisely, we express $(-Δ)_s^{1/2}e^{iks}$ for $k$ odd in terms of the Gaussian hypergeometric function ${}_2F_1$, and also as a well-conditioned finite sum. Then, we use a fast convolution result, that enable us to compute very efficiently $\sum_{l = 0}^Ma_l(-Δ)_s^{1/2}e^{i(2l+1)s}$, for extremely large values of $M$. This enables us to approximate $(-Δ)_s^{1/2}u(x(s))$ in a fast and accurate way, especially when $u(x(s))$ is not periodic of period $π$. As an application, we simulate a fractional Fisher's equation having front solutions whose speed grows exponentially.

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Large time behaviour of a conservation law regularised by a Riesz-Feller operator: the sub-critical case

We study the large time behaviour of the solutions of a non-local regularisation of a scalar conservation law. This regularisation is given by a fractional derivative of order $1+α$, with $α\in(0,1)$, which is a Riesz-Feller operator. The non-linear flux is given by the locally Lipschitz function $|u|^{q-1}u/q$ for $q>1$. We show that in the sub-critical case, $1<q < 1 +α$, the large time behaviour is governed by the unique entropy solution of the scalar conservation law. Our proof adapts the proofs of the analogous results for the local case (where the regularisation is the Laplacian) and, more closely, the ones for the regularisation given by the fractional Laplacian with order larger than one, see Ignat and Stan (2018). The main difference is that our operator is not symmetric and its Fourier symbol is not real. We can also adapt the proof and obtain similar results for general Riesz-Feller operators.

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A fast convolution method for the fractional Laplacian in $\mathbb{R}$

In this article, we develop a new method to approximate numerically the fractional Laplacian of functions defined on $\mathbb R$, as well as some more general singular integrals. After mapping $\mathbb R$ into a finite interval, we discretize the integral operator using a modified midpoint rule. The result of this procedure can be cast as a discrete convolution, which can be evaluated efficiently using the Fast-Fourier Transform (FFT). The method provides an efficient, second order accurate, approximation to the fractional Laplacian, without the need to truncate the domain. We first prove that the method gives a second-order approximation for the fractional Laplacian and other related singular integrals; then, we detail the implementation of the method using the fast convolution, and give numerical examples that support its efficacy and efficiency; finally, as an example of its applicability to an evolution problem, we employ the method for the discretization of the nonlocal part of the one-dimensional cubic fractional Schrödinger equation in the focusing case.

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Numerical Approximation of the Fractional Laplacian on $\mathbb R$ Using Orthogonal Families

In this paper, using well-known complex variable techniques, we compute explicitly, in terms of the ${}_2F_1$ Gaussian hypergeometric function, the one-dimensional fractional Laplacian of the Higgins functions, the Christov functions, and their sine-like and cosine-like versions. After discussing the numerical difficulties in the implementation of the proposed formulas, we develop a method using variable precision arithmetic that gives accurate results.

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Vanishing viscosity limit of a conservation law regularised by a Riesz-Feller operator

We study a nonlocal regularisation of a scalar conservation law given by a fractional derivative of order between one and two. The nonlocal operator is of Riesz-Feller type with skewness two minus its order. This equation describes the internal structure of hydraulic jumps in a shallow water model. The main purpose of the paper is the study of the vanishing viscosity limit of the Cauchy problem for this equation. First, we study the properties of the solution of the regularised problem and then we show that solutions converge to the entropy solution of the scalar conservation law in this limit in $C([0,T];L^1_{loc}(\mathbb{R}))$ for initial data in $L^\infty(\mathbb{R})$, and in $C([0,T];L^1(\mathbb{R}))$ for initial data in $ L^\infty(\mathbb{R})\cap BV(\mathbb{R})$. In order to prove these results we use weak entropy inequalities and the double scale technique of Kruzhkov. Such techniques also allow to show the $L^1(\mathbb{R})$ contraction of the regularised problem. For completeness, we study the behaviour in the tail of travelling wave solutions for genuinely nonlinear fluxes. These waves converge to shock waves in the vanishing viscosity limit, but decay algebraically as $x-ct \to \infty$, rather than exponentially, the latter being a behaviour that they exhibit as $x-ct \to- \infty$, however. Finally, we generalise the results concerning the vanishing viscosity limit to Riesz-Feller operators.

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A Pseudospectral Method for the One-Dimensional Fractional Laplacian on $\mathbb R$

In this paper, we propose a novel pseudospectral method to approximate accurately and efficiently the fractional Laplacian without using truncation. More precisely, given a bounded regular function defined over $\mathbb R$, we map the unbounded domain into a finite one, then we represent the function as a trigonometrical series. Therefore, the central point of this paper is the computation of the fractional Laplacian of an elementary trigonometric function. As an application of the method, we also do the simulation of Fisher's equation with fractional Laplacian in the monostable case.

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Self-similar lifting and persistent touch-down points in the thin-film equation

We study self-similar solutions of the thin-film equation, with mobility exponent m in (0,4], that describe the lifting of an isolated touch-down point given by an initial profile of the form |x|. This provides a mechanism for non-uniqueness of the thin-film equation with m in (2,4), since solutions with a persistent touch-down point also exist in this case. In order to prove existence of the self-similar solutions, we need to study a four-dimensional continuous dynamical system. The proof consists of a shooting argument based on the identification of invariant regions and on suitable energy formulas.

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Addendum to "Travelling waves for a non-local Korteweg-de Vries-Burgers equation" [J. Differential Equations 257 (2014), no. 3, 720--758]

We add a theorem to [J. Differential Equations 257 (2014), no. 3, 720--758] by F. Achleitner, C.M. Cuesta and S. Hittmeir. In that paper we studied travelling wave solutions of a Korteweg-de Vries-Burgers type equation with a non-local diffusion term. In particular, the proof of existence and uniqueness of these waves relies on the assumption that the exponentially decaying functions are the only bounded solutions of the linearised equation. In this addendum we prove this assumption and thus close the existence and uniqueness proof of travelling wave solutions.

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Interfaces determined by capillarity and gravity in a two-dimensional porous medium

We consider a two-dimensional model of a porous medium where circular grains are uniformly distributed in a squared container. We assume that such medium is partially filled with water and that the stationary interface separating the water phase from the air phase is described by the balance of capillarity and gravity. Taking the unity as the average distance between grains, we identify four asymptotic regimes that depend on the Bond number and the size of the container. We analyse, in probabilistic terms, the possible global interfaces that can form in each of these regimes. In summary, we show that in the regimes where gravity dominates the probability of configurations of grains allowing solutions close to the horizontal solution is close to one. Moreover, in such regimes where the size of the container is sufficiently large we can describe deviations from the horizontal in probabilistic terms. On the other hand, when capillarity dominates while the size of the container is sufficiently large, we find that the probability of finding interfaces close to the graph of a given smooth curve without self-intersections is close to one.

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Existence of solutions describing accumulation in a thin-film flow

We consider a third order non-autonomous ODE that arises as a model of fluid accumulation in a two dimensional thin-film flow driven by surface tension and gravity. With the appropriate matching conditions, the equation describes the inner structure of solutions around a stagnation point. In this paper we prove the existence of solutions that satisfy this problem. In order to prove the result we first transform the equation into a four dimensional dynamical system. In this setting the problem consists of finding heteroclinic connections that are the intersection of a two dimensional centre-stable manifold and a three-dimensional centre-unstable one. We then use a shooting argument that takes advantage of the information of the flow in the far-field, part of the analysis also requires the understanding of oscillatory solutions with large amplitude. The far-field is represented by invariant three-dimensional subspaces and the flow on them needs to be understood, most of the necessary results in this regard are obtained in \cite{CV}. This analysis focuses on the understanding of oscillatory solutions and some results are used in the current proof, although the structure of oscillations is somewhat more complicated.

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