140 results on '"Hiptmair R"'
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102. A Coercive Combined Field Integral Equation for Electromagnetic Scattering
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Buffa, A., primary and Hiptmair, R., additional
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- 2004
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103. Current and voltage excitations for the eddy current model
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Hiptmair, R., primary and Sterz, O., additional
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- 2004
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104. Coupling of Finite Elements and Boundary Elements in Electromagnetic Scattering
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Hiptmair, R., primary
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- 2003
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105. Coercive combined field integral equations
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Hiptmair, R., primary
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- 2003
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106. Stabilized FEM-BEM Coupling for Maxwell Transmission Problems.
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Barth, Timothy J., Griebel, Michael, Keyes, David E., Nieminen, Risto M., Roose, Dirk, Schlick, Tamar, Ammari, Habib, Hiptmair, R., and Meury, P.
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- 2008
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107. Analysis of multilevel methods for eddy current problems
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Hiptmair, R., primary
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- 2002
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108. Multilevel Method for Mixed Eigenproblems
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Hiptmair, R., primary and Neymeyr, K., additional
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- 2002
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109. Natural Boundary Element Methods for the Electric Field Integral Equation on Polyhedra
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Hiptmair, R., primary and Schwab, C., additional
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- 2002
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110. Symmetric Coupling for Eddy Current Problems
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Hiptmair, R., primary
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- 2002
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111. Generators of $H_1(\Gamma_{h},\mathbbZ)$ for Triangulated Surfaces: Construction and Classification
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Hiptmair, R., primary and Ostrowski, J., additional
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- 2002
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112. HIGHER ORDER WHITNEY FORMS - Abstract
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Hiptmair, R., primary
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- 2001
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113. Discrete Hodge-Operators: an Algebraic Perspective - Abstract
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Hiptmair, R., primary
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- 2001
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114. Higher ORDER Whitney Forms
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Hiptmair, R., primary
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- 2001
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115. Discrete Hodge-Operators: An Algebraic Perspective
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Hiptmair, R., primary
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- 2001
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116. HIERARCHICAL ERROR ESTIMATOR FOR EDDY CURRENT COMPUTATION.
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BECK, R., HIPTMAIR, R., and WOHLMUTH, B.
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EDDY currents (Electric) ,MAGNETOSTATICS ,FINITE element method ,NUMERICAL analysis ,MATHEMATICAL models - Published
- 2000
117. Multigrid Method for Maxwell's Equations
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Hiptmair, R., primary
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- 1998
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118. Lösung gemischter Probleme zweiter Ordnung mit Multilevel-Vorkonditionierung und erweiteter Lagrange-Multiplikatoren-Technik
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Hiptmair, R., primary, Schiekofer, T., additional, and Wohlmuth, B., additional
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- 1996
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119. Current and voltage excitations for the eddy current model.
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Hiptmair, R. and Sterz, O.
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EDDY currents (Electric) , *ELECTRIC currents , *TOPOLOGY , *VOLTAGE regulators , *FINITE element method - Abstract
We present a systematic study of how to take into account external excitation in the eddy current model. Emphasis is put on mathematically sound variational formulations and on lumped parameter excitation through prescribed currents and voltages. We distinguish between local excitation at known contacts, known generator current distributions and non-local variants that rely on topological concepts. The latter case entails the violation of Faraday's law at so-called cuts and prevents us from reconstructing a meaningful electric field. Copyright © 2004 John Wiley & Sons, Ltd. [ABSTRACT FROM AUTHOR]
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- 2005
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120. GENERATORS OF H1(...h ,Z )FOR TRIANGULATED SURFACES: CONSTRUCTION AND CLASSIFICATION .
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Hiptmair, R. and Ostrowski, J.
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ALGORITHMS , *BOUNDARY element methods , *ELECTROMAGNETIC fields - Abstract
Describes an algorithm for constructing triangulated surfaces. Lipschitz-polyhedron in three-dimensional Euclidean space; Eddy currents; Association of edges of the surface mesh with their degrees of freedom; Discrete surface current; Boundary element methods of electromagnetic fields.
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- 2002
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121. GENERATORS OF H 1 (Γ[subh],Z )FOR TRIANGULATED SURFACES: CONSTRUCTION AND CLASSIFICATION.
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Hiptmair, R. and Ostrowski, J.
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TOPOLOGY , *TRIANGULATION , *ALGORITHMS , *HOMOLOGY theory , *RESEARCH - Abstract
We consider a bounded Lipschitz-polyhedron &om; ⊂R[SUP3] of general topology equipped with a tetrahedral triangulation that induces a mesh Λ[SUBh] of the surface δ&om;. We seek a maximal set of surface edge cycles that are independent in H[SUB1](Λ[SUBh],Z) and bounding with respect to the exterior of &om;. We present an algorithm for constructing suitable 1-cycles in Λ[SUBh] : First, representatives of a basis of the homology group H[SUB1](Λ[SUBh], Z) are constructed, merely using the combinatorial description of the surface mesh Λ[SUBh]. Then, a duality pairing based on linking numbers is used to determine those combinations that are bounding with respect to R[SUP3]\&om;. This is the key to circumventing a triangulation of the exterior region R[SUP3]\&om; in the computations. For shape-regular, quasi-uniform families of meshes, the asymptotic complexity of the algorithm is shown to be O(N[SUP2]), where N is the number of edges of Λ[SUBh]. The scheme provides an essential preprocessing step for all boundary element methods for eddy current simulation, which rely on discrete divergence-free vectorfields and their description through stream functions. [ABSTRACT FROM AUTHOR]
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- 2001
122. Optimal operator preconditioning for Galerkin boundary element methods on 3D screens
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Urzua-Torres, C, Hiptmair, R, and Jerez-Hanckes, C
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Mathematics::Numerical Analysis - Abstract
We consider first-kind weakly singular and hypersingular boundary integral operators for the Laplacian on screens in R3 and their Galerkin discretization by means of low-order piecewise polynomial boundary elements. For the resulting linear systems of equations we propose novel Calder´on-type preconditioners based on (i) new boundary integral operators, which provide the exact inverses of the weakly singular and hypersingular operators on flat disks, and (ii) stable duality pairings relying on dual meshes. On screens obtained as images of the unit disk under bi-Lipschitz transformations, this approach achieves condition numbers uniformly bounded in the meshwidth even on locally refined meshes. Comprehensive numerical tests also confirm its excellent pre-asymptotic performance.
123. Auxiliary space preconditioning in H 0(curl; Ω)
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Hiptmair, R., Widmer, G., Zou, J., Hiptmair, R., Widmer, G., and Zou, J.
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We adapt the principle of auxiliary space preconditioning as presented in [J. Xu, The auxiliary space method and optimal multigrid preconditioning techniques for unstructured grids, Computing, 56 (1996), pp. 215-235.] to H (curl; ω)-elliptic variational problems discretized by means of edge elements. The focus is on theoretical analysis within the abstract framework of subspace correction. Employing a Helmholtz-type splitting of edge element vector fields we can establish asymptotic h-uniform optimality of the preconditioner defined by our auxiliary space method
124. Plane wave approximation of homogeneous Helmholtz solutions
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Moiola, A., Hiptmair, R., Perugia, I., Moiola, A., Hiptmair, R., and Perugia, I.
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In this paper, we study the approximation of solutions of the homogeneous Helmholtz equation Δu+ω 2 u=0 by linear combinations of plane waves with different directions. We combine approximation estimates for homogeneous Helmholtz solutions by generalized harmonic polynomials, obtained from Vekua's theory, with estimates for the approximation of generalized harmonic polynomials by plane waves. The latter is the focus of this paper. We establish best approximation error estimates in Sobolev norms, which are explicit in terms of the degree of the generalized polynomial to be approximated, the domain size, and the number of plane waves used in the approximations
125. Convergence analysis of finite element methods for H(div;Ω)-elliptic interface problems
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Hiptmair, R., Li, J., Zou, J., Hiptmair, R., Li, J., and Zou, J.
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In this article we analyze a finite element method for solving H(div;Ω)-elliptic interface problems in general three-dimensional Lipschitz domains with smooth material interfaces. The continuous problems are discretized by means of lowest order H(div;Ω)-conforming finite elements of the first family (Raviart-Thomas or Nédélec face elements) on a family of unstructured oriented tetrahedral meshes. These resolve the smooth interface in the sense of sufficient approximation in terms of a parameter δ that quantifies the mismatch between the smooth interface and the finite element mesh. Optimal error estimates in the H(div;Ω)-norms are obtained for the first time. The analysis is based on a so-called δ-strip argument, a new extension theorem for H 1(div)-functions across smooth interfaces, a novel non-standard interfaceaware interpolation operator, and a perturbation argument for degrees of freedom in H(div;Ω)-conforming finite elements. Numerical tests are presented to verify the theoretical predictions and confirm the optimal order convergence of the numerical solution
126. Comparison of approximate shape gradients
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Hiptmair, R., Paganini, A., Sargheini, S., Hiptmair, R., Paganini, A., and Sargheini, S.
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Shape gradients of PDE constrained shape functionals can be stated in two equivalent ways. Both rely on the solutions of two boundary value problems (BVPs), but one involves integrating their traces on the boundary of the domain, while the other evaluates integrals in the volume. Usually, the two BVPs can only be solved approximately, for instance, by finite element methods. However, when used with finite element solutions, the equivalence of the two formulas breaks down. By means of a comprehensive convergence analysis, we establish that the volume based expression for the shape gradient generally offers better accuracy in a finite element setting. The results are confirmed by several numerical experiments.
127. Multiple point evaluation on combined tensor product supports
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Hiptmair, R., Phillips, G., Sinha, G., Hiptmair, R., Phillips, G., and Sinha, G.
- Abstract
We consider the multiple point evaluation problem for an n-dimensional space of functions [ − 1,1[ d ↦ℝ spanned by d-variate basis functions that are the restrictions of simple (say linear) functions to tensor product domains. For arbitrary evaluation points this task is faced in the context of (semi-)Lagrangian schemes using adaptive sparse tensor approximation spaces for boundary value problems in moderately high dimensions. We devise a fast algorithm for performing m ≥ n point evaluations of a function in this space with computational cost O(mlog d n). We resort to nested segment tree data structures built in a preprocessing stage with an asymptotic effort of O(nlog d − 1 n)
128. Direct boundary integral equation method for electromagnetic scattering by partly coated dielectric objects
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Cranganu-Cretu, B., Hiptmair, R., Cranganu-Cretu, B., and Hiptmair, R.
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We present a new variational direct boundary integral equation approach for solving the scattering and transmission problem for dielectric objects partially coated with a PEC layer. The main idea is to use the electromagnetic Calderón projector along with transmission conditions for the electromagnetic fields. This leads to a symmetric variational formulation which lends itself to Galerkin discretization by means of divergence-conforming discrete surface currents. A wide array of numerical experiments confirms the efficacy of the new method
129. Multiple traces boundary integral formulation for Helmholtz transmission problems
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Hiptmair, R., Jerez-Hanckes, C., Hiptmair, R., and Jerez-Hanckes, C.
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We present a novel boundary integral formulation of the Helmholtz transmission problem for bounded composite scatterers (that is, piecewise constant material parameters in "subdomains”) that directly lends itself to operator preconditioning via Calderón projectors. The method relies on local traces on subdomains and weak enforcement of transmission conditions. The variational formulation is set in Cartesian products of standard Dirichlet and special Neumann trace spaces for which restriction and extension by zero are well defined. In particular, the Neumann trace spaces over each subdomain boundary are built as piecewise $\widetilde{H}^{-1/2}$ -distributions over each associated interface. Through the use of interior Calderón projectors, the problem is cast in variational Galerkin form with an operator matrix whose diagonal is composed of block boundary integral operators associated with the subdomains. We show existence and uniqueness of solutions based on an extension of Lions' projection lemma for non-closed subspaces. We also investigate asymptotic quasi-optimality of conforming boundary element Galerkin discretization. Numerical experiments in 2-D confirm the efficacy of the method and a performance matching that of another widely used boundary element discretization. They also demonstrate its amenability to different types of preconditioning
130. Vekua theory for the Helmholtz operator
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Moiola, A., Hiptmair, R., Perugia, I., Moiola, A., Hiptmair, R., and Perugia, I.
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Vekua operators map harmonic functions defined on domain in $${\mathbb R^{2}}$$ to solutions of elliptic partial differential equations on the same domain and vice versa. In this paper, following the original work of I. Vekua (Ilja Vekua (1907-1977), Soviet-Georgian mathematician), we define Vekua operators in the case of the Helmholtz equation in a completely explicit fashion, in any space dimension N≥2. We prove (i) that they actually transform harmonic functions and Helmholtz solutions into each other; (ii) that they are inverse to each other; and (iii) that they are continuous in any Sobolev norm in star-shaped Lipschitz domains. Finally, we define and compute the generalized harmonic polynomials as the Vekua transforms of harmonic polynomials. These results are instrumental in proving approximation estimates for solutions of the Helmholtz equation in spaces of circular, spherical, and plane waves
131. The finite mass mesh method
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Bubeck, T., Hiptmair, R., Yserentant, H., Bubeck, T., Hiptmair, R., and Yserentant, H.
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The finite mass method is a purely Lagrangian scheme for the spatial discretisation of the macroscopic phenomenological laws that govern the flow of compressible fluids. In this article we investigate how to take into account long range gravitational forces in the framework of the finite mass method. This is achieved by incorporating an extra discrete potential energy of the gravitational field into the Lagrangian that underlies the finite mass method. The discretisation of the potential is done in an Eulerian fashion and employs an adaptive tensor product mesh fixed in space, hence the name finite mass mesh method for the new scheme. The transfer of information between the mass packets of the finite mass method and the discrete potential equation relies on numerical quadrature, for which different strategies will be proposed. The performance of the extended finite mass method for the simulation of two-dimensional gas pillars under self-gravity will be reported
132. Coercive combined field integral equations
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Hiptmair, R. and Hiptmair, R.
- Abstract
Many boundary integral equations for exterior Dirichlet and Neumann boundary value problems for the Helmholtz equation suffer from a motorious instability for wave numbers related to interior resonances. The so-called combined field integral equations are not affected. This article presents combined field integral equations on two-dimensional closed surfaces that possess coercivity in canonical trace spaces. For the exterior Dirichlet problem the main idea is to use suitable regularizing operators in the framework of an indirect method. This permits us to apply the classical convergence theory of conforming Galerkin methods
133. Convergence analysis with parameter estimates for a reduced basis acoustic scattering T-matrix method
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Ganesh, M., Hawkins, S. C., Hiptmair, R., Ganesh, M., Hawkins, S. C., and Hiptmair, R.
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The celebrated truncated T-matrix method for wave propagation models belongs to a class of the reduced basis methods (RBMs), with the parameters being incident waves and incident directions. The T-matrix characterizes the scattering properties of the obstacles independent of the incident and receiver directions. In the T-matrix method the reduced set of basis functions for representation of the scattered field is constructed analytically and hence, unlike other classes of the RBM, the T-matrix RBM avoids computationally intensive empirical construction of a reduced set of parameters and the associated basis set. However, establishing a convergence analysis and providing practical a priori estimates for reducing the number of basis functions in the T-matrix method has remained an open problem for several decades. In this work we solve this open problem for time-harmonic acoustic scattering in two and three dimensions. We numerically demonstrate the convergence analysis and the a priori parameter estimates for both point-source and plane-wave incident waves. Our approach can be used in conjunction with any numerical method for solving the forward wave propagation problem
134. Non-Reflecting Boundary Conditions for Maxwell's Equations
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Hiptmair, R., Schädle, A., Hiptmair, R., and Schädle, A.
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A new discrete non-reflecting boundary condition for the time-dependent Maxwell equations describing the propagation of an electromagnetic wave in an infinite homogenous lossless rectangular waveguide with perfectly conducting walls is presented. It is derived from a virtual spatial finite difference discretization of the problem on the unbounded domain. Fourier transforms are used to decouple transversal modes. A judicious combination of edge based nodal values permits us to recover a simple structure in the Laplace domain. Using this, it is possible to approximate the convolution in time by a similar fast convolution algorithm as for the standard wave equation
135. Archives of Orthopaedis and Trauma Surgery
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HIPTMAIR R
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- Humans, Foot, Foot Injuries, Joint Dislocations
- Published
- 1955
136. Dispersion analysis of plane wave discontinuous Galerkin methods.
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Gittelson, Claude J. and Hiptmair, Ralf
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HELMHOLTZ equation ,PLANE wavefronts ,GALERKIN methods ,DISPERSION (Chemistry) ,AMPLITUDE modulation - Abstract
SUMMARY The plane wave DG (PWDG) method for the Helmholtz equation was introduced and analyzed in [ GITTELSON, C., HIPTMAIR, R., AND PERUGIA, I. Plane wave discontinuous Galerkin methods: analysis of the h-version. Math. Model. Numer. Anal. 43 (2009), 297-331] as a generalization of the so-called ultra-weak variational formulation, see [ O. CESSENAT AND B. DESPRéS, Application of an ultra weak variational formulation of elliptic PDEs to the two-dimensional Helmholtz equation, SIAM J. Numer. Anal., 35 (1998), pp. 255-299]. The method relies on Trefftz-type local trial spaces spanned by plane waves of different directions, and links cells of the mesh through numerical fluxes in the spirit of DG methods. We conduct a partly empirical dispersion analysis of the method in a discrete translation-invariant setting by studying the mismatch of wave numbers of discrete and continuous plane waves traveling in the same direction. We find agreement of the wave numbers for directions represented in the local trial spaces. For other directions, the PWDG methods turn out to incur both phase and amplitude errors. This manifests itself as a pollution effect haunting the h-version of the method. Our dispersion analysis allows a quantitative prediction of the strength of this effect and its dependence on the wave number and number of plane waves. Copyright © 2014 John Wiley & Sons, Ltd. [ABSTRACT FROM AUTHOR]
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- 2014
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- View/download PDF
137. D5.1: Review of state-of-the-art for Pricing and Computation of VaR
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Nogueiras, Maria, Ordóñez Sanz, Gustavo, Vázquez Cendón, Carlos, Leitao Rodríguez, Álvaro, Manzano Herrero, Alberto, Musso, Daniele, Gómez, Andrés, Dunjko, Vedran, and Villalpando, Antonio
- Subjects
Derivatives Pricing ,Quantum Finance ,Quantum Amplitude Estimation ,QCoin ,VaR ,Risk Measures ,CVaR ,Finance - Abstract
Quantum Computing commenced in 1980’s with the pioneering work of Paul Benioff (Benioff, 1980) who proposed a quantum mechanical Turing machine. These ideas were also explored by the likes of Richard Feynman (Feynman, 1982) and Yuri Manin (Manin, 1980) who suggested that quantum computers could provide advantage over classical computers in certain tasks, such as the simulation of physical systems. In 1994, Peter Shor (Shor, 1994) published a groundbreaking paper demonstrating that a quantum algorithm could be used to for large integer factorisation in polynomial time, that is, exponentially faster than the best known classical algorithms. This was followed by Lov K. Grover who proposed a quantum computing algorithm that promised a quadratic speed up over database searches (L. K. Grover, 1996). Advances in Quantum Computing hardware technology in recent years have been accompanied by the acceleration on the development of quantum computing algorithms with applications across many different use cases in different industry sectors: Automotive, Energy, Logistics, Pharma, Chemical/Manufacturing and the Financial Services Industry. One of the use cases in Finance comes from the application of Quantum Computing for Derivative Pricing and Derivative Risk Management. The purpose of this document is toprovide a summary of the “state of the art” for these applications. However, it is important to note that the currently available quantum computers have limited number of qubits and these suffer from high levels of “noise” which limits the depth and length of the quantum circuits that can be implemented in real hardware. Therefore, near-term applications focus on implementations of quantum algorithms in Noisy Intermediate-Scale Quantum (NISQ) computers (Preskill, 2018). Derivatives contract form one of the fundamental pillars of modern financial markets and are routinely traded by both financial institutions and traders with a variety of objectives, such as financial risk hedging. A simple example of financial derivative is a European stock option. This contract provides the derivative holder with the right to purchase or sell the stock at some time in the future for a fixed price agreed today. Hence, providing with potential upside (should the stock increase in price at maturity) while limiting the investor’s downside. Derivatives pricing theory is the branch of financial mathematics that covers the fair valuation of financial derivatives such as options. This framework assumes that the underlying security (e.g. a single stock) follows some random (stochastic) process. The price of the derivative hence depends on the particular realisation of such process at a given point in time (e.g. the option maturity). The best known example of option pricing model is the Black-Scholes model (Black, 1976). This model proves that a fair value of an option can be derived under certain assumptions (e.g. absence of arbitrage, continuous and unlimited long and short trading). However, in general the Black-Sholes model is too simplistic to fit actual quoted prices in the market and other more complex models are used instead, at the cost of requiring numerical approximations to find the fair price of the derivative. Two main numerical approaches are currently used in the industry, Monte Carlo-based simulation techniques and partial differential equation (PDEs) approaches. The key advantage of the former is that it is easy to implement, very general and scales well with the dimension of the problem. On the other hand, Monte Carlo simulation tends to converge slowly to the required solution. It is also difficult to obtain risk sensitivities (i.e. how the derivative price depends on changes to the price underlying) using Monte Carlo. PDEs approaches are generally faster and permit the easy calculation of risk sensitives, however it is usually a difficult problem to solve PDEs for more complex derivatives, specially those that depend on several risk factors (curse of dimensionality). Monte Carlo simulation is therefore the tool of choice for financial risk management where risk metrics need to be estimated at the portfolio level where thousands of derivatives need to be covered. Quantum computing, and in particular the Quantum Amplitude Estimation (QAE) algorithm promises a potential quadratic speed up over classical Monte Carlo approaches but maintaining its main advantages: easy of implementation and linear scaling to higher dimensions. This document covers these topics in more detail and presents some new results, such as the application of the “Quantum Coin” algorithms as an alternative to QAE. Despite the highly promising advantages of quantum computing for derivative pricing and risk management, huge challenges remain open for real-world applications. Some of them are technological, such as the relative small number of qubits currently available and the fact that these are “noisy” (i.e. not always reliable). Others are more theoretical, such as the lack of understanding on how to load classical information (such as probability distributions) to quantum registers, or how to represent relatively complex pay-off functions with quantum circuits that are as small as possible., {"references":["Aaronson, S., & Rall, P. (2020). Quantum approximate counting, simplified. Symposium on simplicity in algorithms (pp. 24–32). 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A quantum algorithm for the sensitivity analysis of business risks [arXiv:2103.05475].","Carr, P., & Madan, D. B. (1999). Option valuation using the fast Fourier transform. Journal of Computational Finance, 2, 61–73.","Carrera Vazquez, A., Hiptmair, R., & Woerner, S. (2020). Enhancing the quantum linear systems algorithm using Richardson extrapolation [arXiv:2009.04484].","Carrera Vazquez, A., & Woerner, S. (2021). Efficient state preparation for quantum amplitude estimation. Physical Review Applied, 15, 034027.","Chakrabarti, S., Krishnakumar, R., Mazzola, G., Stamatopoulos, N., Woerner, S., & Zeng, W. J. (2020). A threshold for quantum advantage in derivative pricing [arXiv:2012.03819].","Childs, A. M., & Wiebe, N. (2012). Hamiltonian simulation using linear combinations of unitary operations. Quantum Information & Computation, 12(11–12), 901–924.","Clopper, C. J., & Pearson, E. S. (1934). The use of confidence or fiducial limits illustrated in the case of the binomial. 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- Published
- 2021
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138. Auxiliary Space Preconditioners for a DG Discretization of H(curl; Ω)-Elliptic Problem on Hexahedral Meshes
- Author
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Blanca Ayuso de Dios, Ralf Hiptmair, Cecilia Pagliantini, Ayuso de Dios, B, Hiptmair, R, and Pagliantini, C
- Subjects
Auxiliary Space, H(curl)-problems, Hexahedral Meshes ,Curl (mathematics) ,N/A ,Discretization ,Mathematical analysis ,Discontinuous galerkin discretization ,Polygon mesh ,Hexahedron ,Classification of discontinuities ,Computer Science::Numerical Analysis ,Mathematics::Numerical Analysis ,Mathematics - Abstract
We present a family of preconditioners based on the auxiliary space method for a discontinuous Galerkin discretization on cubical meshes of H(curl;Ω)-elliptic problems with possibly discontinuous coefficients. We address the influence of possible discontinuities in the coefficients on the asymptotic performance of the proposed solvers and present numerical results in two dimensions.
- Published
- 2018
139. Auxiliary space preconditioners for SIP-DG discretizations of H(curl)-elliptic problems with discontinuous coefficients
- Author
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Cecilia Pagliantini, Blanca Ayuso de Dios, Ralf Hiptmair, Ayuso De Dios, B, Hiptmair, R, Pagliantini, C, Ayuso de Dios, Blanca, Hiptmair, Ralf, and Pagliantini, Cecilia
- Subjects
Discretization ,H(curl ,General Mathematics ,Discontinuous Galerkin methods ,discontinuous Galerkin method ,010103 numerical & computational mathematics ,01 natural sciences ,discontinuous coefficients ,Mathematics::Numerical Analysis ,auxiliary space preconditioning ,H(curl,Ω)-elliptic problems ,Discontinuous Galerkin method ,Auxiliary space preconditioning ,Discontinuous coefficients ,Boundary value problem ,discontinuous Galerkin methods, H(curl,Ω)-elliptic problems, auxiliary space preconditioning, discontinuous coefficients ,0101 mathematics ,Mathematics ,Curl (mathematics) ,Quadrilateral ,Ω)-elliptic problem ,Preconditioner ,H(curl?)-elliptic problems ,Applied Mathematics ,Mathematical analysis ,Computer Science::Numerical Analysis ,Finite element method ,010101 applied mathematics ,Computational Mathematics ,Piecewise - Abstract
We propose a family of preconditioners for linear systems of equations arising from a piecewise polynomial symmetric interior penalty discontinuous Galerkin discretization of H(curl,Ω)-elliptic boundary value problems on conforming meshes. The design and analysis of the proposed preconditioners rely on the auxiliary space method (ASM) employing an auxiliary space of H(curl,Ω)-conforming finite element functions together with a relaxation technique (local smoothing). On simplicial meshes, the proposed preconditioner enjoys asymptotic optimality with respect to mesh refinement. It is also robust with respect to jumps in the coefficients ν and β in the second- and zeroth-order parts of the operator, respectively, except when the problem changes from curl-dominated to reaction-dominated and vice versa. On quadrilateral/hexahedral meshes some of the proposed ASM solvers may fail, since the related H(curl,Ω)-conforming finite element space does not provide a spectrally accurate discretization. Extensive numerical experiments are included to verify the theory and assess the performance of the preconditioners., IMA Journal of Numerical Analysis, 37 (2), ISSN:0272-4979, ISSN:1464-3642
- Published
- 2017
140. Dispersion analysis of plane wave discontinuous Galerkin methods
- Author
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Ralf Hiptmair and Claude Jeffrey Gittelson
- Subjects
Numerical Analysis ,Amplitude ,Helmholtz equation ,Discontinuous Galerkin method ,Generalization ,Applied Mathematics ,Mathematical analysis ,General Engineering ,Plane wave ,Phase (waves) ,Wavenumber ,Dispersion (water waves) ,Mathematics - Abstract
SUMMARY The plane wave DG (PWDG) method for the Helmholtz equation was introduced and analyzed in [GITTELSON, C., HIPTMAIR, R., AND PERUGIA, I. Plane wave discontinuous Galerkin methods: analysis of the h-version. Math. Model. Numer. Anal. 43 (2009), 297–331] as a generalization of the so-called ultra-weak variational formulation, see [O. CESSENAT AND B. DESPReS, Application of an ultra weak variational formulation of elliptic PDEs to the two-dimensional Helmholtz equation, SIAM J. Numer. Anal., 35 (1998), pp. 255–299]. The method relies on Trefftz-type local trial spaces spanned by plane waves of different directions, and links cells of the mesh through numerical fluxes in the spirit of DG methods. We conduct a partly empirical dispersion analysis of the method in a discrete translation-invariant setting by studying the mismatch of wave numbers of discrete and continuous plane waves traveling in the same direction. We find agreement of the wave numbers for directions represented in the local trial spaces. For other directions, the PWDG methods turn out to incur both phase and amplitude errors. This manifests itself as a pollution effect haunting the h-version of the method. Our dispersion analysis allows a quantitative prediction of the strength of this effect and its dependence on the wave number and number of plane waves. Copyright © 2014 John Wiley & Sons, Ltd.
- Published
- 2014
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