Non incremental strategies based on separated representations: applications in computational rheology
By Amine Ammar, M. Normandin, F. Daim, David González, Elías Cueto, Francisco Chinesta. 2010
76 citations recorded by the source corpus.
Subfields: Computational Mathematics, Molecular Biology, Statistical and Nonlinear Physics
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In Computational Mathematics
In Statistical and Nonlinear Physics
- Amine Ammar
- Elías Cueto
- Francisco Chinesta
- Antonio Huerta
- Adrien Leygue
- Felipe Bordeu
- Icíar Alfaro
- David González
Citations in the corpus
- A literature survey of low‐rank tensor approximation techniques (2013, neutral): “…of high-dimensional PDEs [30,113]; • the solution of the Boltzmann equation [129, 149], and the chemical master / Fokker-Planck equations [4,6,61,64,86,122,133,135,196] • the solution of high-dimensional Schr¨odinger equations [46,160,172,184,192,193]; • computational tasks in…”
- PGD-Based Computational Vademecum for Efficient Design, Optimization and Control (2013, methodology): “The treatment of non-linear models, compulsory for obtaining the handbook related to parametric non-linear models usually encountered in industrial applications, was addressed in some of our former works [6, 70] where standard linearization procedures where extended to the PGD framework.”
- Greedy Approximation of High-Dimensional Ornstein–Uhlenbeck Operators (2011, unknown): “…proposed in the engineering literature in a succession of papers by Ammar, Mokdad, Chinesta, Keunings and collaborators [AMCK06, AMCK07, AND + 10, GACC10, CALK11], for the numerical solution of high-dimensional Fokker–Planck equations in kinetic models of polymeric fluids under the names…”
- Recent Advances and New Challenges in the Use of the Proper Generalized Decomposition for Solving Multidimensional Models (2010, methodology): “For illustrating the treatment of non linear models we are treating the following simple nonlinear parabolic problem, that we considered in [6] ⎧ ⎪⎨ ⎪⎩ ∂u ∂t − aΔu = u2 + f (x, t) in Ω × (0, Tmax] u(x, t) = 0 on ∂Ω × (0, Tmax] u(x,0) = 0 in Ω (29)”