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Workshop on<br />

<strong>Wave</strong> <strong>Propagation</strong> <strong>and</strong> <strong>Scattering</strong>,<br />

<strong>Inverse</strong> <strong>Problems</strong>, <strong>and</strong> Applications in<br />

Energy <strong>and</strong> the Environment<br />

November 21-25, 2011<br />

as part of the<br />

Radon Special Semester 2011 on<br />

Multiscale Simulation & Analysis in Energy <strong>and</strong> the Environment


The efficient computation of wave propagation <strong>and</strong> scattering is a core problem in numerical mathematics,<br />

which is currently of great research interest <strong>and</strong> is central to many applications in energy <strong>and</strong> the environment.<br />

Two generic applications which resonate strongly with the central aims of this special semester<br />

are forward wave propagation in heterogeneous media <strong>and</strong> seismic inversion for subsurface imaging. As<br />

an example of the first application, modelling of absorption <strong>and</strong> scattering of radiation by clouds, aerosol<br />

<strong>and</strong> precipitation is used as a tool for interpretation of (e.g.) solar, infrared <strong>and</strong> radar measurements,<br />

<strong>and</strong> as a component in larger weather/climate prediction models in numerical weather forecasting. One<br />

key numerical component in this modelling is the prediction of the total optical properties <strong>and</strong> the full<br />

scattering matrix from an ensemble of irregular particles. The underlying mathematical problem is that<br />

of accurately computing high frequency wave propagation in a highly heterogeneous medium. As an<br />

example of the second application, inverse problems in wave propagation in heterogeneous media arise<br />

in the problem of imaging the subsurface below l<strong>and</strong> or marine deposits. Solutions to this problem have<br />

a number of environmental uses, for example in the location of hydrocarbon-bearing rocks, in the monitoring<br />

of pollution in groundwater or in earthquake modelling. A seismic source is directed into the<br />

ground <strong>and</strong> the material properties of the subsurface are inferred by analysing the observed scattered<br />

field, recorded by sensors. The inversion process (a large scale optimisation problem) is complicated by<br />

the presence of multiple reflections <strong>and</strong> the fact that the scales involved in the exploration of sub-marine,<br />

sub-basalt or sub-salt oil reservoirs can be many kilometres in extent, leading to a challenging multi-scale<br />

problem. Current iterative methods for solving the inverse problem involve repeated solution of the forward<br />

problem (the computational kernel), which is typically a frequency-domain reduction of the elastic<br />

(or scalar) wave equation with high frequency <strong>and</strong> typically highly spatially varying wave speed. If the<br />

inversion is to be competitive, the key underlying problem to be overcome is the design of robust <strong>and</strong><br />

scalable solvers for the large highly indefinite linear systems arising from these problems.<br />

The workshop will bring together key numerical mathematicians whose interest is in the analysis <strong>and</strong><br />

computation of wave propagation <strong>and</strong> scattering problems, <strong>and</strong> in inverse problems, together with practitioners<br />

from engineering <strong>and</strong> industry whose interest is in the applications of these core problems.<br />

Particular problems to be considered will be (i) The design of accurate methods for solving frequency<br />

domain problems; (ii) The use of wave enriched <strong>and</strong> other hybrid approximation strategies in the solution<br />

of high-frequency problems; (iii) Fast linear algebra solvers for frequency domain problems in heterogeneous<br />

media; (iv) advanced inverse problem approaches for wave problems such as reverse time migration<br />

which move away from traditional ray-based approaches in the high frequency case.<br />

Workshop Organizers<br />

Ivan G. Graham, University of Bath, UK<br />

Ulrich Langer, Johann Radon Institute & University of Linz, Austria<br />

Jens Markus Melenk, Vienna University of Technology, Austria<br />

Mourad Sini, Johann Radon Institute, Austria<br />

cover picture of tsunami simulation in Indian Ocean:<br />

courtesy of Jörn Behrens (KlimaCampus, Universität Hamburg) <strong>and</strong> Widodo S. Pranovo (Indonesia).


Welcome<br />

to Linz <strong>and</strong> thank you very much for participating in the sixth RICAM Special Semester on Multiscale<br />

Simulation & Analysis in Energy <strong>and</strong> the Environment, hosted by the Johann Radon Insitute for<br />

Computational <strong>and</strong> Applied Mathematics (RICAM) from October 3 to December 16, 2011.<br />

Technological advances have greatly improved our quality of life. However, they bring with them a<br />

huge surge in energy requirements which in turn puts at risk our entire bio-sphere. It is of paramount<br />

importance to predict these risks <strong>and</strong> to develop better solutions for the future. One of the central tasks<br />

is the accurate simulation of multiphase flow above <strong>and</strong> under ground. The risk analysis <strong>and</strong> uncertainty<br />

quantification, as well as the assimilation of data require statistical tools <strong>and</strong> efficient solvers for stochastic<br />

<strong>and</strong> deterministic PDEs as well as for the associated inverse problems. The key features that make it<br />

extremely hard to predict these physical phenomena accurately are the multiple time <strong>and</strong> length scales<br />

that arise, as well as the lack of <strong>and</strong> uncertainty in data. Because of the highly varying scales involved, the<br />

resolution of all scales is currently impossible even on the largest supercomputers. While there is a fairly<br />

long history of empirically successful robust computational techniques for certain multiscale problems,<br />

the rigorous (numerical) analysis of such methods is of extremely high current interest.<br />

The goal of the special semester is to provide a stimulating environment for civil engineers, hydrologists,<br />

meteorologists <strong>and</strong> other environmental scientists to address together with mathematicians working at<br />

the cutting edge of rigorous numerical analysis for multiscale (direct <strong>and</strong> inverse) problems the emerging<br />

challenges in the quantitative assessment of the risks <strong>and</strong> uncertainties of atmospheric <strong>and</strong> subsurface<br />

flow, focusing in particular on<br />

• Simulation of Flow in Porous Media <strong>and</strong> Applications in Waste Management <strong>and</strong> CO2 Sequestration<br />

• Large-Scale <strong>Inverse</strong> <strong>Problems</strong> <strong>and</strong> Applications in the Earth Sciences<br />

• Data Assimilation <strong>and</strong> Multiscale Simulation in Atmospheric Flow<br />

• <strong>Wave</strong> <strong>Propagation</strong> <strong>and</strong> <strong>Scattering</strong>, Direct <strong>and</strong> <strong>Inverse</strong> <strong>Problems</strong> <strong>and</strong> Applications in Energy <strong>and</strong><br />

the Environment<br />

• Multiscale Numerical Methods <strong>and</strong> their Analysis <strong>and</strong> Applications in Energy <strong>and</strong> the Environment<br />

• Stochastic Modelling of Uncertainty <strong>and</strong> Numerical Methods for Stochastic PDEs<br />

Specific activities planned for the Special Semester are<br />

• 4 thematic workshops addressing some of the key topics of the Special Semester;<br />

• Special Lecture Series on ”Multilevel Methods for Multiscale <strong>Problems</strong>”;<br />

• Graduate Seminar on ”Multiscale Discretization Techniques”;<br />

• Wednesday Research Kitchen;<br />

• Public Lecture by Prof. Jörn Behrens (KlimaCampus, Universität Hamburg) on<br />

“Tsunami Früh-Warnung: Mathematik und Wissenschaftliches Rechnen im Dienste der Sicherheit”.<br />

We sincerely hope that you enjoy your stay in Linz!<br />

Local Organizing Committee Program Committee<br />

Robert Scheichl, Bath & RICAM (Chair) Peter Bastian, University of Heidelberg, Germany<br />

Jörg Willems, RICAM (Coordinator) Mike Cullen, Met Office, Exeter, UK<br />

Johannes Kraus, RICAM (Co-Coordinator) Heinz Engl, RICAM & University of Vienna, Austria<br />

Erwin Karer, RICAM (Co-Coordinator) Melina Freitag, University of Bath, UK<br />

Ivan G. Graham, University of Bath, UK<br />

Ulrich Langer, RICAM & University of Linz, Austria<br />

Markus Melenk, TU Vienna, Austria<br />

Robert Scheichl, University of Bath, UK (Chair)<br />

Mary F. Wheeler, University of Texas at Austin, USA


Contents<br />

Information 2<br />

Workshop Information . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2<br />

Social Events . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2<br />

Restaurants <strong>and</strong> Cafes . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2<br />

General Information . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2<br />

Program 5<br />

Posters 7<br />

Abstracts 8<br />

Abstracts for Posters 17<br />

List of Participants 20<br />

1


Information<br />

Workshop Information<br />

Registration. The workshop registration will be on November 21st, 2011 from 9:00 - 9:40 am next to the<br />

seminar room SP2 416 on the 4th floor of the Science Park Building 2 (see floor plan). Participants<br />

that arrive later in the week can register at the special semester office SP2 456.<br />

Registration Fee. Non-invited participants are kindly asked to pay the registration fee in cash upon<br />

registration.<br />

Campus plan <strong>and</strong> overview map as well as a floor plan of the 4th floor of the workshop venue (Science<br />

Park Building 2) are located on the next pages.<br />

Seminar room. The workshop will take place in seminar room SP2 416 on the 4th floor of the Science<br />

Park Building 2 (see floor plan).<br />

Program. A time schedule for the workshop is located on the backside of this booklet.<br />

Coffee breaks. The coffee breaks will be in the corridor of the 4th floor of the Science Park Building 2.<br />

Internet access. There will be an extra information sheet regarding internet access available at registration.<br />

Social Events<br />

Welcome Reception & Poster Session. Monday, November 21st, 2011, 5:15 pm, on the 4th floor of<br />

the Science Park Building 2.<br />

Conference Dinner. Thursday, November 24th, 2011, 7:00 pm, at the restaurant “Kepler’s”, situated<br />

in the Mensa building<br />

Restaurants <strong>and</strong> Cafes<br />

• Mensa Markt (lunch time only) - Main canteen of the University (see campus plan)<br />

• KHG Mensa (lunch time only) - Smaller canteen - good traditional food (see overview map: “KHG<br />

Linz”)<br />

• Pizzeria “Bella Casa” - Italian <strong>and</strong> Greek restaurant (located next to the tram stop)<br />

• Chinese restaurant “Jadegarten” - (located close by the tram stop, adjacent to “Bella Casa”)<br />

• Asia restaurant “A2” - (located behind the Science Park on Altenbergerstrasse)<br />

• “Chat” cafe - coffee, drinks <strong>and</strong> s<strong>and</strong>wiches (located in the “Hörsaaltrakt” - see overview map)<br />

• Cafe “Sassi” - coffee, drinks <strong>and</strong> small snacks (located in the building “Johannes Kepler Universität”<br />

- see overview map)<br />

• Bakery “K<strong>and</strong>ur” - bakery <strong>and</strong> small cafe (located opposite the tram stop)<br />

General Information<br />

Accommodation. The arranged accomodation for invited participants is the “Sommerhaus” hotel. You<br />

can find its location in the overview map on page 4.<br />

Special Semester Office: Room SP2 456. The special semester administrator is Susanne Dujardin.<br />

Audiovisual & Computer Support. Room SP2 458, Wolfgang Forsthuber or Florian Tischler.<br />

2


Orientation/ Local Transport. From the railway station you have to take tram number 1 or 2 in<br />

direction “Universität”. It takes about 25 minutes to reach the desired end stop “Universität”.<br />

In order to get to the city center of Linz (“Hauptplatz”) <strong>and</strong> back you have to take again tram<br />

number 1 or 2 (about 20 minutes). For more information see www.ricam.oeaw.ac.at/location/.<br />

Taxi Numbers.<br />

+43 732 6969 Oberösterreichische Taxigenossenschaft<br />

+43 732 2244 2244 Linzer Taxi<br />

+43 732 781463 Enzendorfer Taxi & Transport<br />

+43 732 2214 Linzer Taxi<br />

+43 732 660217 LINTAX TaxibetriebsgesmbH<br />

Further important phone numbers.<br />

+43 (0)732 2468 5222 RICAM & Special Semester Office (Susanne Dujardin)<br />

+43 (0)732 2468 5250/5255 RICAM IT Support (Florian Tischler/ Wolfgang Forsthuber)<br />

+43 (0)732 2457-0 Reception of Hotel Sommerhaus<br />

133 General emergency number for the police<br />

144 General emergency number for the ambulance<br />

More information about RICAM can be found at www.ricam.oeaw.ac.at. See also the Special<br />

Semester webpage www.ricam.oeaw.ac.at/specsem/specsem2011/ for additional information.<br />

Figure 1: 4th floor of Science Park Building 2.<br />

Figure 2: Campus plan<br />

3


Figure 3: Overview map<br />

4


Program<br />

Monday, November 21st<br />

00:00 - 09:40 Registration<br />

09:40 - 09:50 Opening<br />

09:50 - 10:40 Ralf Hiptmair (ETH Zürich)<br />

10:40 - 11:10 Coffee Break<br />

“Convergence of truncated T-matrix approximation”<br />

11:10 - 12:00 Timo Betcke (University College London)<br />

12:00 - 14:00 Lunch Break<br />

“Modulated plane wave methods for Helmholtz problems in heterogeneous media”<br />

14:00 - 14:50 Susan Minkoff (University of Maryl<strong>and</strong>, Baltimore County)<br />

14:50 - 15:20 Coffee Break<br />

“Two scale wave equation modeling”<br />

15:20 - 16:10 Paul Childs (Schlumberger Cambridge Research)<br />

“Numerics of waveform inversion for seismic data”<br />

16:10 - 17:00 Chris Stolk (University of Amsterdam)<br />

“Seismic inverse scattering by reverse time migration”<br />

17:15 Poster Session & Welcome Reception<br />

Tuesday, November 22nd<br />

09:00 - 09:50 Martin G<strong>and</strong>er (University of Geneva)<br />

“Are absorbing boundary conditions <strong>and</strong> perfectly matched layers really so different?”<br />

09:50 - 10:40 Lothar Nannen (Vienna University of Technology)<br />

10:40 - 11:10 Coffee Break<br />

“Hardy space infinite elements for exterior Maxwell problems”<br />

11:10 - 12:00 Habib Ammari ( École Normale Supérieure)<br />

11:30 - 14:00 Lunch Break<br />

“Electromagnetic invisibility <strong>and</strong> super-resolution”<br />

14:00 - 14:50 Marcus Grote (University of Basel)<br />

14:50 - 15:20 Coffee Break<br />

“Discontinuous Galerkin methods <strong>and</strong> local time stepping for transient wave propagation”<br />

15:20 - 16:10 Joachim Schöberl (Vienna University of Technology)<br />

16:10 - 17:00 Break<br />

“Hybrid discontinuous Galerkin finite element methods for the Helmholtz equation”<br />

17:15 - 18:00 Radon colloquium by Martin G<strong>and</strong>er (University of Geneva)<br />

“From Euler, Schwarz, Ritz <strong>and</strong> Galerkin to Modern Computing”<br />

5


Wednesday, November 23rd<br />

09:00 - 09:50 Ronny Ramlau (University of Linz)<br />

“<strong>Inverse</strong> problems in adaptive optics”<br />

09:50 - 10:40 Frédéric Nataf (Université Paris 6, Laboratoire J.L. Lions)<br />

10:40 - 11:10 Coffee Break<br />

“Time reversed absorbing condition in the partial aperture case”<br />

11:10 - 12:00 Olaf Steinbach (Graz University of Technology)<br />

“Boundary element methods for acoustic <strong>and</strong> electromagnetic scattering problems”<br />

free afternoon (please feel free to make use of the seminar room <strong>and</strong> the Special<br />

Semester offices)<br />

Thursday, November 24th<br />

09:00 - 09:50 Rol<strong>and</strong> Potthast (Deutscher Wetterdienst & University of Reading)<br />

“Approaches to dynamical inverse scattering problems”<br />

09:50 - 10:40 Thanh Nguyen (RICAM)<br />

10:40 - 11:10 Coffee Break<br />

“<strong>Inverse</strong> obstacle scattering problems using multifrequency measurements”<br />

11:10 - 12:00 Guanghui Hu (WIAS Berlin)<br />

12:00 - 14:00 Lunch Break<br />

“Direct <strong>and</strong> inverse scattering of elastic waves by diffraction gratings”<br />

14:00 - 14:50 Jari Toivanen (University of Jyväskylä)<br />

14:50 - 15:20 Coffee Break<br />

“Domain decomposition <strong>and</strong> multigrid preconditioners for the Helmholtz equation<br />

in layered <strong>and</strong> heterogeneous media”<br />

15:20 - 16:10 Radek Tezaur (Stanford University)<br />

“The discontinuous enrichment method <strong>and</strong> its domain decomposition solver for<br />

the Helmholtz equation”<br />

16:10 - 17:00 Ira Livshits (Ball State University)<br />

“Algebraic multigrid algorithm for solving Helmholtz equations with large wave<br />

numbers”<br />

19:00 Conference dinner<br />

6


Friday, November 25th<br />

09:00 - 09:50 Manfred Kaltenbacher (University of Klagenfurt)<br />

“Spectral finite elements for a mixed formulation in computational acoustics taking<br />

flow effects into acount”<br />

09:50 - 10:40 Euan Spence (University of Bath)<br />

10:40 - 11:10 Coffee Break<br />

“Stability <strong>and</strong> conditioning of boundary integral methods for high frequency scattering”<br />

11:10 - 12:00 Simon Ch<strong>and</strong>ler-Wilde (University of Reading)<br />

12:00 Closing<br />

Posters<br />

“Numerical-Asymptotic Integral Equation Methods for High Frequency <strong>Scattering</strong>”<br />

The poster session will take place on the 4th floor of the 2nd Science Park Building. It will start<br />

at 5:15 pm on Monday, November 21st.<br />

Carlos Borges (Worcester Polytechnic Institute)<br />

“Numerical solution of the high frequency 2D direct scattering problem for convex objects using nonuniform<br />

B-splines”<br />

Victor A. Kovtunenko (University of Graz)<br />

“Variational methods for the identification of objects”<br />

Marie Kray (Université Paris 6)<br />

“Time reversed absorbing conditions: discrimination between one single inclusion <strong>and</strong> two close inclusions<br />

in a non-homogeneous medium”<br />

Jens Markus Melenk (Vienna University of Technology)<br />

“<strong>Wave</strong>number-explicit convergence analysis for the Helmholtz equation: hp-FEM <strong>and</strong> hp-BEM”<br />

Andrea Moiola (ETH Zürich)<br />

“Trefftz-discontinuous Galerkin methods for time-harmonic Maxwell’s equations”<br />

Imbo Sim (University of Klagenfurt)<br />

“Stable absorbing layer for convective wave propagation”<br />

7


Abstracts<br />

“Electromagnetic invisibility <strong>and</strong> super-resolution”<br />

Habib Ammari<br />

École Normale Supérieure<br />

Abstract<br />

The aim of this talk is threefold: - to give a mathematical justification of cloaking due to anomalous<br />

localized resonance; - to provide an original method for enhancing near cloaking; - to achieve resolved<br />

inclusion imaging.<br />

“Modulated plane wave methods for Helmholtz problems in heterogeneous media”<br />

Timo Betcke<br />

Department of Mathematics<br />

University College London<br />

Gower Street, London, WC1E 6BT, UK<br />

Abstract<br />

A major challenge in seismic imaging is full waveform inversion in the frequency domain. If an<br />

acoustic model is assumed the underlying problem formulation is a Helmholtz equation of the form<br />

� �2 ω<br />

−∆u − u = f,<br />

c(x)<br />

where c(x) is the varying speed of sound in the heterogeneous medium. Typically, in seismic applications<br />

the solution u has many wavelengths across the computational domain, leading to very<br />

large linear systems after discretisation with st<strong>and</strong>ard finite element methods. Much progress has<br />

been achieved in recent years by the development of better preconditioners for the iterative solution<br />

of these linear systems. But the fundamental problem of requiring many degrees of freedom per<br />

wavelength for the discretisation remains.<br />

For problems in homogeneous media, that is c is constant, plane wave finite element methods have<br />

gained significant attention. The idea is that instead of polynomials on each element we use a linear<br />

combination of plane waves of the form e i ω c d j ·x , where the dj are direction vectors of unit length.<br />

These basis functions already oscillate with the right wavelength, leading to a significant reduction in<br />

the required number of unknowns. However, higher-order convergence is only achieved for problems<br />

with constant or piecewise constant media.<br />

In this talk we discuss the use of modulated plane waves of the form p(x)e i ω ¯c d j ·x for problems in<br />

heterogeneous media, where p is a polynomial of low degree (typically 2 or 3) <strong>and</strong> ¯c is a constant<br />

approximation to the speed of sound in an element. The idea is that high-order convergence in a<br />

varying medium is recovered due to the polynomial modulation of the plane waves. <strong>Wave</strong> directions<br />

are chosen based on information from raytracing or other fast solvers for the eikonal equation. This<br />

approach is related to the Amplitude FEM originally proposed by Giladi <strong>and</strong> Keller in 2001. However,<br />

for the assembly of the systems we will use a discontinuous Galerkin method, which allows a simple<br />

way of incorporating multiple phase information in one element. We will discuss the dependence of<br />

the element sizes on the wavelenth <strong>and</strong> the accuracy of the phase information, <strong>and</strong> present several<br />

examples that demonstrate the properties of modulated plane wave methods for heterogeneous media<br />

problems.<br />

“Numerical-asymptotic integral equation methods for high frequency scattering”<br />

Simon Ch<strong>and</strong>ler-Wilde<br />

Department of Mathematics <strong>and</strong> Statistics<br />

University of Reading<br />

Reading RG6 6AX, UK<br />

Abstract<br />

Conventional discretisation methods for wave propagation <strong>and</strong> scattering (finite elements, finite<br />

difference, boundary element, ...) have costs which increase rapidly as the frequency increases because<br />

of the need for large numbers of degrees of freedom to resolve the oscillatory solution. In particular,<br />

this is an issue in boundary element calculations for time harmonic problems, where in 3D the degrees<br />

of freedom need to increase in proportion to k 2 , where k is the wave number, in order to maintain a<br />

fixed number of degrees of freedom per wavelength, required to maintain accuracy. High frequency<br />

asymptotic methods, in the other h<strong>and</strong>, based on ray tracing/solving eikonal/transport equations,<br />

8


have a cost which is fixed as k increases, but have unacceptably low accuracy for many problems,<br />

except at very high k.<br />

In this talk, we overview progress in developing numerical methods for high frequency problems<br />

which try to combine st<strong>and</strong>ard numerical <strong>and</strong> asymptotic approaches. In particular, we focus on<br />

boundary integral equation based methods, describing progress in generating numerical schemes which<br />

deliver an arbitrarily high requested accuracy with a number of degrees of freedom which provably<br />

(through numerical analysis theorems <strong>and</strong> numerical experiments) needs only grow logarithmically<br />

as k increases.<br />

The methodology is to obtain knowledge of the phase structure of the solution, by rather elementary<br />

high frequency ray analysis, <strong>and</strong> to build this phase structure into the basis functions used to<br />

approximate the solution. This idea, in a simple form, dates back at least to [1], but the methodology<br />

has seen a wealth of new ideas in the last 5-10 years, see [1–6] <strong>and</strong> the references therein, which we<br />

review.<br />

[1] T. Abboud, J.C. Nédélec, B. Zhou, Méthode des équations intégrales pour les hautes fréquencies,<br />

C.R. Acad. Sci. Paris., 318 Série I (1994), 165-170.<br />

[2] O.P. Bruno, F. Reitich, High Order Methods for High-Frequency <strong>Scattering</strong> Applications, In:<br />

Modeling <strong>and</strong> Computations in Electromagnetics, H. Ammari (Ed.), Springer, 2007, pp. 129–164.<br />

[3] S.N. Ch<strong>and</strong>ler-Wilde, I.G. Graham, Boundary Integral Methods in High Frequency <strong>Scattering</strong>, In:<br />

Highly Oscillatory <strong>Problems</strong>, B. Engquist, T. Fokas, E. Hairer, A. Iserles (Eds.), Cambridge University<br />

Press, 2009, pp. 154–193.<br />

[4] M. Ganesh, S.C. Hawkins, A Fully Discrete Galerkin Method for High Frequency Exterior Acoustic<br />

<strong>Scattering</strong> in Three Dimensions, J. Comp. Phys. 230, (2011), 104–125.<br />

[5] A. Spence, S.N. Ch<strong>and</strong>ler-Wilde, I.G. Graham, V.P. Smyshlyaev, A New Frequency-Uniform Coercive<br />

Boundary Integral Equation for Acoustic <strong>Scattering</strong>, Comm. Pure Appl. Math., 64, (2011),<br />

1384-1415.<br />

[6] S.N. Ch<strong>and</strong>ler-Wilde, I.G. Graham, S. Langdon, E. Spence, Numerical-asymptotic boundary integral<br />

methods in high frequency acoustic scattering, to appear in Acta Numerica.<br />

“Numerics of waveform inversion for seismic data”<br />

Paul Childs<br />

Schlumberger Cambridge Research<br />

Abstract<br />

Depth imaging <strong>and</strong> inversion of seismic data is becoming commonplace within the seismic exploration<br />

industry. However, the inversion procedures used today often fail to find the global minimum,<br />

<strong>and</strong> careful multiscale data processing must be included in the workflow. Although developed by<br />

Tarantola et al in the 1980s, there are still numerous mathematical challenges remaining relating to<br />

non-uniqueness, size of the null space of the inversion operator, <strong>and</strong> the sheer computational size<br />

of industrial datasets. In this talk, we will review some approaches to improving the robustness<br />

of the full waveform inversion method, which today is regarded as a highly interpretive procedure.<br />

Because the PDE-constrained inversion procedure used in industry can be very expensive due to the<br />

large number of PDE solves required, we will review <strong>and</strong> address some of the numerical challenges<br />

in this area. The talk will serve as an introduction to the subject <strong>and</strong> will concentrate mainly on<br />

computational developments. Illustrations will be given with industrial examples from full waveform<br />

inversion of seismic data.<br />

“Are absorbing boundary conditions <strong>and</strong><br />

perfectly matched layers really so different?”<br />

Martin J. G<strong>and</strong>er<br />

Section of Mathematics<br />

University of Geneva<br />

2-4 Rue du Lièvre, CH–1211 Genève 4<br />

Abstract<br />

In order to truncate infinite computational domains, there are two major competitors: absorbing<br />

boundary conditions <strong>and</strong> perfectly matched layers. The former use approximations of the Dirichlet<br />

to Neumann map, <strong>and</strong> the latter adds a layer outside the truncated domain, in which a modified<br />

equation is solved, which absorbs outgoing parts of the solution.<br />

Using the concept of the pole condition, we show for a model problem that these two seemingly<br />

very different techniques are in fact related. For the particular case of an absorbing boundary<br />

condition given by a Pade approximation of the Dirichlet to Neumann map, we show that a natural<br />

implementation leads to a layer structure corresponding to a perfectly matched layer with an<br />

exponentially scaled outer problem.<br />

9


“From Euler, Schwarz, Ritz, <strong>and</strong> Galerkin to modern computing”<br />

Martin J. G<strong>and</strong>er<br />

Section of Mathematics, University of Geneva, 2-4 Rue du Lièvre, CH–1211 Genève 4<br />

Abstract<br />

The origins of modern computing are dispersed over centuries, often in the work of pure mathematicians,<br />

who invented methods in order to underst<strong>and</strong> mathematical objects <strong>and</strong> prove theorems.<br />

A typical example is the famous Schwarz method for parallel computing, whose origins lie in a problem<br />

in Riemann’s audacious proof of the Riemann mapping theorem. Another example is the finite<br />

element method, which has its origins in the variational calculus of Euler-Lagrange <strong>and</strong> in the thesis<br />

of Walther Ritz, who died just over 100 years ago at the age of 31 from tuberculosis. We will see<br />

in this talk that the path leading to modern computational methods <strong>and</strong> theory was a long struggle<br />

over three centuries requiring the efforts of many great mathematicians.<br />

“Discontinuous Galerkin methods <strong>and</strong> local time stepping for transient wave propagation”<br />

Marcus J. Grote<br />

Mathematisches Institut<br />

Rheinsprung 21, CH–4051 Basel<br />

Abstract<br />

The accurate <strong>and</strong> reliable simulation of transient wave phenomena is of fundamental importance<br />

in a wide range of engineering applications such as fiber optics, wireless communication, seismic<br />

imaging, <strong>and</strong> non-invasive testing. Finite element methods are probably the most flexible approach<br />

for computational wave propagation in heterogeneous media or complex geometry. When combined<br />

with explicit time integrators, st<strong>and</strong>ard conforming finite element methods lead to efficient <strong>and</strong> highly<br />

parallel methods, if mass-lumping techniques are used. Alternatively, discontinuous Galerkin methods<br />

easily accommodate irregular non-matching grids <strong>and</strong> hp-refinement, while they inherently lead to<br />

block-diagonal mass matrices. Hence, they also lead to efficient <strong>and</strong> highly parallel methods when<br />

combined with explicit time-stepping schemes. Nonetheless, both suffer from the severe stability<br />

(CFL) condition imposed on the time step by the smallest elements in the mesh. To circumvent that<br />

CFL condition, we propose high-order explicit local time-stepping schemes, which allow smaller time<br />

steps precisely where the smallest elements in the mesh are located.<br />

This is joint work with J. Diaz (INRIA), T. Mitkova (Basel) <strong>and</strong> D. Schoetzau (UBC).<br />

“Direct <strong>and</strong> inverse scattering of elastic waves by diffraction gratings”<br />

Guanghui Hu<br />

WIAS Berlin<br />

Mohrenstr. 39<br />

D–10117 Berlin<br />

Abstract<br />

This talk is concerned with the scattering of a time-harmonic plane elastic wave by an unbounded<br />

periodic structure. Such structures are also called diffraction gratings <strong>and</strong> have many important<br />

applications in diffractive optics, radar imaging, non-destructive testing, etc.<br />

The talk is arranged into three sections. (i) Variational approach to scattering of plane elastic<br />

waves by an impenetrable two-dimensional periodic structure. Using a variational formulation in a<br />

bounded periodic cell involving a non-local boundary operator, uniqueness <strong>and</strong> existence of quasiperiodic<br />

solutions are presented under the first (Dirichlet), second (Neumann), third <strong>and</strong> fourth kind<br />

boundary conditions. (ii) Uniqueness for the inverse problem in determining a polygonal diffraction<br />

grating from near-field measurements under the third or fourth kind boundary conditions. We determine<br />

<strong>and</strong> classify all the unidentifiable grating profiles corresponding to one given incident pressure or<br />

shear wave, relying on the reflection principle of the Navier equation. (iii) An optimization method for<br />

the inverse problem in recovering an unknown grating profile from scattered elastic waves measured<br />

above the structure. Based on the Kirsch-Kress optimization scheme, we apply a two-step algorithm<br />

to both smooth <strong>and</strong> piecewise linear gratings for the Dirichlet boundary value problem of the Navier<br />

equation. Numerical reconstructions from exact <strong>and</strong> noisy data will be shown.<br />

Some results for bi-periodic structures will also be mentioned. This is joint work with Dr. J.<br />

Elschner under the DFG Project: ”Direct <strong>and</strong> inverse scattering problems for elastic waves”<br />

10


“Convergence of truncated T-matrix approximation”<br />

Ralf Hiptmair<br />

Seminar for Applied Mathematics<br />

ETH Zürich<br />

Abstract<br />

The T-matrix encodes the scattering properties of an obstacle independently of the incident <strong>and</strong><br />

receiver directions. It boils down to a basis representation of the operator mapping incident fields<br />

to the far field pattern with respect to (spherical) harmonics. Discretization can be achieved by<br />

truncating the T-matrix, which amounts to using a finite number of basis functions. The truncated<br />

T-matrix can be computed by solving several large forward scattering problems during a preparatory<br />

offline stage. Then, the scattering response to an incident field of any direction or source position<br />

can be computed very fast (online stage).<br />

My presentation is concerned with the a priori analysis of the effect of truncating the T-matrix for<br />

acoustic scattering. Detailed error estimates <strong>and</strong> predictions of the rates of exponential convergence<br />

are derived for both point-source <strong>and</strong> plane-wave incident waves. Errors in solving the forward<br />

problem are also taken into account.<br />

This is joint work with M. Ganesh (Colorado School of Mines) <strong>and</strong> S.C. Hawkins (Macquarie<br />

University, Sydney).<br />

References.<br />

M. Ganesh, S. Hawkins, <strong>and</strong> R. Hiptmair, Convergence analysis with parameter estimates<br />

for a reduced basis acoustic scattering T-matrix method, Report 2011-04, SAM, ETH Zürich, Zürich,<br />

Switzerl<strong>and</strong>, 2011. To appear in IMA J. Numer. Anal.<br />

“Spectral finite elements for a mixed formulation in computational acoustics taking flow effects into account”<br />

Manfred Kaltenbacher<br />

Applied Mechatronics<br />

University of Klagenfurt<br />

Austria<br />

Abstract<br />

Formulations which include effects of a mean flow on the acoustic wave propagation are mostly<br />

based on a splitting of the unknowns velocity �u, pressure p <strong>and</strong> density ρ into mean (denoted by an<br />

overline) <strong>and</strong> fluctuating (denoted by the superscript a) parts. Such an ansatz results, e.g., in the<br />

acoustic perturbation equations as used in computational aeroacoustics [1]<br />

∂p a<br />

∂t + c2 ρ ∇ · �u a + �u · ∇p a = qc ; ρ ∂�ua<br />

∂t + ρ(�u · ∇)�u a + ∇p a = �qm<br />

with c the speed of sound <strong>and</strong> qc, �qm acoustic source terms. Its variational formulation is then given as<br />

follows (for simplification we use homogeneous Dirichlet boundary conditions): Find (�u , p ′ ) ∈ V × W<br />

such that<br />

�<br />

∂<br />

∂t<br />

p a ϕ, dx − c 2 �<br />

ρ �u<br />

Ω<br />

a �<br />

· ∇ϕ dx + �u · ∇p<br />

Ω<br />

a �<br />

dx = qcϕ dx (1)<br />

ρ<br />

Ω<br />

∂<br />

�<br />

∂t<br />

�v a · � �<br />

ψ dx + ∇p a · � �<br />

ψ dx + ρ (�u · ∇)�u a �<br />

dx = �qm · � ψ dx (2)<br />

Ω<br />

for all ( � ψ , ϕ) ∈ V × W .<br />

Following [2] we apply a mixed formulation <strong>and</strong> use spectral elements with the following discrete<br />

spaces<br />

Wh = � ϕh ∈ H 1 �<br />

�<br />

�<br />

0 ϕh|Kj ◦ Fj ∈ PN ,<br />

�<br />

Vh = �φh ∈ [L 2 ] d � � |Jj|J −1<br />

j<br />

� φ|Kj ◦ Fj ∈ [PN ] d�<br />

In order to stabilize our formulation, we use similar techniques as for DG-approaches <strong>and</strong> reformulate<br />

the third term in (2) as a special flux term (upwinding) <strong>and</strong> furthermore add a jump-term in the<br />

acoustic particle velocity �u a along common element interfaces.<br />

This topic is a joint work with A. Hüppe (University of Klagenfurt), G. Cohen <strong>and</strong> S. Imperial (IN-<br />

RIA, Paris) <strong>and</strong> B. Wohlmuth (TU Munich).<br />

[1] R. Ewert <strong>and</strong> W. Schröder. Acoustic perturbation equations based on flow decomposition via<br />

source filtering. Journal of Comp. Phys., 188:365398, 2003.<br />

[2] G. Cohen <strong>and</strong> S. Fauqueux. Mixed finite elements with mass-lumping for the transient wave<br />

equation. Journal of Comp. Acoustics, 8:171188, 2000.<br />

Ω<br />

11<br />

Ω<br />

.


“Algebraic multigrid algorithm for solving Helmholtz equations with large wave numbers”<br />

Ira Livshits<br />

Department of Mathematical Sciences<br />

Ball State University<br />

USA<br />

Abstract<br />

In this talk we introduce a new adaptive algebraic multigrid approach for solving indefinite<br />

Helmholtz equations. The proposed approach is an interplay between the idea of multiple smooth<br />

representations of oscillatory kernel components of the Helmholtz operator on coarse grids, as in the<br />

geometric multigrid wave-ray algorithm, <strong>and</strong> a flexibility of a more recent least-squares Bootstrap<br />

AMG approach, which has demonstrated its potential in different types of applications. We present<br />

preliminary results in two dimensions <strong>and</strong> discuss future directions.<br />

“Two Scale <strong>Wave</strong> Equation Modeling”<br />

Susan E. Minkoff<br />

Department of Mathematics <strong>and</strong> Statistics<br />

University of Maryl<strong>and</strong>, Baltimore County<br />

1000 Hilltop Circle<br />

Baltimore, MD 21250, USA<br />

Email: sminkoff@umbc.edu<br />

Abstract<br />

Imaging the Earth’s subsurface requires determination of the “important information” inherent in<br />

data that ranges over multiple scales. While numerical upscaling is a common approach for speeding<br />

up solution of the fluid flow equations, simulation of waves through the same Earth is generally<br />

accomplished using single scale finite differences. We describe a two-scale finite-element based wave<br />

simulator <strong>and</strong> the associated adjoint problem. Operator-based upscaling decomposes the solution<br />

into coarse <strong>and</strong> subgrid components. The subgrid solution lives at the fine nodes inside each coarse<br />

cell. Fine-scale solution information is incorporated in the coarse solution. After adapting operatorbased<br />

upscaling to the acoustic <strong>and</strong> elastic wave equations in 2 <strong>and</strong> 3D, we give a matrix analysis of<br />

this two-stage process that produces the first explanation of the underlying physical equations being<br />

solved by this technique. We see that the coarse grid solution involves solving a matrix problem<br />

with entries that are averages of the original parameter field on coarse grid boundaries. Calculation<br />

of the adjoint for the upscaled wave equation simulator is straight-forward if differentiation of the<br />

continuous pde model is accomplished before discretization. The result is that the adjoint problem<br />

can be solved by the same upscaling method as the st<strong>and</strong>ard acoustic wave equation.<br />

“Hardy space infinite elements for exterior Maxwell problems”<br />

Lothar Nannen<br />

Institute for Analysis <strong>and</strong> Scientific Computing<br />

Vienna University of Technology<br />

Austria<br />

Abstract<br />

In this talk we present an infinite element method for solving electromagnetic scattering <strong>and</strong><br />

resonance problems posed on unbounded domains. As our motivation is to solve Maxwell’s equations<br />

we take care that these infinite elements fit into the discrete de Rham diagram, i.e. they span discrete<br />

spaces, which together with the exterior derivative form an exact sequence.<br />

The theoretical framework of the method is the so called pole condition, which characterizes<br />

radiating solutions via the poles or singularities of the Laplace transformed solutions: The Laplace<br />

transform in radial direction of an outgoing wave belongs to a certain Hardy space of holomorphic<br />

functions, while the Laplace transform of an incoming wave does not. Hence, the Hardy space infinite<br />

elements are constructed using tensor products of Hardy space basis functions with st<strong>and</strong>ard finite<br />

element surface basis functions.<br />

Numerical tests indicate super-algebraic convergence in the number of additional unknowns per<br />

degree of freedom on the coupling boundary.<br />

12


“Time reversed absorbing condition in the partial aperture case”<br />

Frédéric Nataf<br />

Laboratoire J.L. Lions <strong>and</strong> CNRS UMR7598<br />

University Pierre & Marie Curie<br />

Paris, France<br />

Abstract<br />

The time-reversed absorbing conditions (TRAC) method introduced in Time Reversed Absorbing<br />

Condition: Application to <strong>Inverse</strong> <strong>Problems</strong>, Assous, Kray <strong>and</strong> Nataf (<strong>Inverse</strong> <strong>Problems</strong>, 2011) enables<br />

one to “recreate the past” without knowing the source which has emitted the signals that are backpropagated.<br />

It has been applied to inverse problems for the reduction of the computational domain<br />

size <strong>and</strong> for the determination, from boundary measurements, of the location <strong>and</strong> volume of an<br />

unknown inclusion. The method does not rely on any a priori knowledge of the physical properties<br />

of the inclusion. We present the extension of the TRAC method to the partial aperture configuration<br />

<strong>and</strong> to discrete receivers with various spacing. In particular the TRAC method is applied to the<br />

differentiation between a single inclusion <strong>and</strong> a two close inclusion case. Subwavelength resolution<br />

can be achieved even with more than 20% noise in the data.<br />

“<strong>Inverse</strong> obstacle scattering problems using multifrequency measurements”<br />

Trung Thành Nguyen<br />

RICAM<br />

Altenbergerstrasse 69, A-4040 Linz<br />

Abstract<br />

In this talk, we consider the problem of reconstructing the shapes of sound-soft acoustic obstacles<br />

using far field measurements associated with only one or a few incident directions but at multiple<br />

frequencies. The motivation for using multifrequency data is explained as follows. On the one h<strong>and</strong>,<br />

we know that the reconstruction problem is uniquely solvable at low frequencies, but its stability is<br />

poor (only of log-type). That means, at low frequencies, it is difficult to reconstruct small details<br />

of the obstacle. On the other h<strong>and</strong>, at high frequencies, this inverse problem may not be uniquely<br />

solvable but it is more stable. To take the advantages of both low <strong>and</strong> high frequencies, we use the following<br />

approach. We first reconstruct a rough approximation of the obstacles at the lowest frequency<br />

using the least-squares approach. This reconstruction is then refined by using recursive optimization<br />

methods at higher frequencies. This approach enables us to obtain an accurate reconstruction of the<br />

parts of the obstacles’ boundary illuminated by the incident waves without requiring a good initial<br />

guess. The analysis of this approach is divided into three steps.<br />

In the first step, we derive a quantitative estimate of the set of local convexity of the objective<br />

functional at a fixed frequency. Our analysis shows that, the size of this set is inversely proportional<br />

to the used frequency. As a consequence, if the obstacles are expected to be contained in a known<br />

domain, the lowest frequency should be chosen small enough so that the set of convexity of the<br />

objective functional contains this domain <strong>and</strong> any shape in this domain can be used as an initial<br />

guess.<br />

The appropriate choice of the lowest frequency avoids the need of a good initial guess to obtain<br />

an approximation of the true shapes. However, due to the lack of good stability at low frequencies,<br />

we can only expect a rough approximation. To enhance the accuracy, our idea is then to use this<br />

rough approximation as an initial guess for minimizing the objective functional at higher frequencies.<br />

For this purpose, we make use of recursive optimization methods. The second step is devoted to the<br />

convergence of the recursive optimization algorithms.<br />

To analyze the reconstruction accuracy, in the third step, we discuss the stability at high frequencies.<br />

We justify a conditional asymptotic Lipschitz stability estimate of the so-called support function<br />

on the parts of the obstacles’ boundary illuminated by the incident wave. This result explains why<br />

we can reconstruct small details of the illuminated parts at high frequencies.<br />

The results presented are joint work with Mourad Sini (RICAM).<br />

“Approaches to dynamical inverse scattering problems”<br />

Rol<strong>and</strong> Potthast<br />

Deutscher Wetterdienst, University of Reading, University of Göttingen<br />

Abstract<br />

We discuss several different approaches to dynamics inverse scattering problems. Dynamical<br />

problems are widely spread in nature. Dynamics can refer to the dynamics to the scattered field,<br />

i.e. when we have time-dependent fields. In this case several new methods have been developed<br />

13


over the past years <strong>and</strong> we will describe dynamical approaches like the time-domain probe method<br />

<strong>and</strong> orthogonality sampling. When the scatterers under consideration are time-dependent, we need<br />

additional techniques from the area of data assimilation. We will provide a survey for the case where<br />

scale separation can be employed for the time-scales of the scatterer <strong>and</strong> the waves.<br />

“<strong>Inverse</strong> problems in adaptive optics”<br />

Ronny Ramlau<br />

Institute for Industrial Mathematics<br />

Johannes Kepler University Linz<br />

Austria<br />

Abstract<br />

Most of the large earthbound astronomical telescopes use Adaptive Optics technology (AO) in order<br />

to enhance the image quality. The degradation of the measured images is caused by atmospheric<br />

turbulences. The correction is achieved by the use of deformable mirrors, where the deformation is<br />

obtained from the measurements of the light of a bright natural star or artificial stars (laser guide<br />

stars). We consider <strong>Inverse</strong> <strong>Problems</strong> that arise form Single Conjugate Adaptive Optics (SCAO) <strong>and</strong><br />

Multi Conjugate Adaptive Optics (MCAO). In order to measure the incoming wavefront, different<br />

types of sensors are used. We consider the so called Shack - Hartmann sensor which measures an<br />

average of the gradient of the wavefront. For SCAO, the <strong>Inverse</strong> Problem is now the reconstruction<br />

of the wavefront from the (noisy) sensor measurements. Besides the reconstruction quality the<br />

reconstruction time is most important, as the reconstructions have to be carried out in real time.<br />

The presented reconstruction algorithms for SCAO are also an ingredient for the computation of the<br />

mirror deformation for MCAO, which is based on a tomography of the atmosphere. The analytical<br />

results are illustrated by numerical experiments.<br />

“Hybrid discontinuous Galerkin finite element methods for the Helmholtz equation”<br />

Joachim Schöberl<br />

Institute for Analysis <strong>and</strong> Scientific Computing<br />

Vienna University of Technology<br />

Abstract<br />

In this paper we present Hybrid Discontinuous Galerkin (HDG) Methods to discretize the Helmholtz<br />

equation. In constrast to elliptic equations, we introduce two hybrid variables, one for the Dirichlet<br />

<strong>and</strong> one for Neumann data. Thanks to this choice, the element equations can be formulated using<br />

impedance traces.<br />

We present computational results for iterative solvers with BDDC–type domain decomposition<br />

preconditioners.<br />

This talk contains joint work with A. Pechstein, P. Monk, M. Huber, A. Hannukainen, <strong>and</strong> G.<br />

Kitzler.<br />

“Stability <strong>and</strong> conditioning of boundary integral methods for high frequency scattering”<br />

Euan A. Spence<br />

Department of Mathematical Sciences<br />

University of Bath<br />

Bath, BA2 7AY, UK<br />

Abstract<br />

Boundary integral equations are a classical tool for solving acoustic scattering problems modelled<br />

by the Helmholtz equation.<br />

This talk will discuss the following two questions:<br />

1. How do the condition numbers of the integral operators depend on the wavenumber k (in<br />

particular for k large)?<br />

2. Can one give a k-explicit error analysis, (a) for methods using conventional piecewise polynomial<br />

basis functions (which require the number of degrees of freedom to grow as k increases to<br />

preserve accuracy), <strong>and</strong> (b) for methods using novel k-dependent basis functions (which have<br />

the potential to give almost uniform accuracy independent of k – see the next talk by Simon<br />

Ch<strong>and</strong>ler-Wilde)?<br />

14


Both these questions are interesting because the st<strong>and</strong>ard analysis of boundary integral equations<br />

for the Helmholtz equation does not yield k-explicit results.<br />

This talk will give an overview of some recent developments in answering these questions <strong>and</strong> will<br />

discuss joint work with Timo Betcke (University College London), Simon Ch<strong>and</strong>ler-Wilde (Reading),<br />

Ivan Graham (Bath), <strong>and</strong> Valery Smyshlyaev (University College London), as well as independent<br />

work by Markus Melenk (Vienna).<br />

“Boundary element methods for acoustic <strong>and</strong> electromagnetic scattering problems”<br />

Olaf Steinbach<br />

Institut für Numerische Mathematik<br />

TU Graz<br />

Steyrergasse 30<br />

8010 Graz<br />

Austria<br />

Abstract<br />

For the numerical solution of acoustic <strong>and</strong> electromagnetic scattering problems we discuss stabilized<br />

boundary integral formulations <strong>and</strong> related boundary element methods. For problems with<br />

piecewise local wave numbers we apply a tearing <strong>and</strong> interconnecting domain decomposition approach<br />

which is based on modified Robin interface conditions to ensure unique solvability.<br />

The talk is based on joint work with Sarah Engleder <strong>and</strong> Markus Windisch.<br />

“Seismic inverse scattering by reverse time migration”<br />

Chris Stolk<br />

University of Amsterdam<br />

Korteweg-de Vries Institute for Mathematics<br />

Science Park 904<br />

1098 XH, Amsterdam<br />

The Netherl<strong>and</strong>s<br />

Abstract<br />

We will consider the linearized inverse scattering problem from seismic imaging. While the first<br />

reverse time migration algorithms were developed some thirty years ago, they have only recently become<br />

popular for practical applications. We will analyze a modification of the reverse time migration<br />

algorithm that turns it into a method for linearized inversion, in the sense of a parametrix. This is<br />

proven using tools from microlocal analysis. We will also discuss the limitations of the method <strong>and</strong><br />

show some numerical results.<br />

“The discontinuous enrichment method <strong>and</strong> its domain decomposition solver for the Helmholtz equation”<br />

Radek Tezaur<br />

Stanford University<br />

Aeronautics <strong>and</strong> Astronautics<br />

496 Lomita Mall<br />

Stanford, CA 94305-4035, USA<br />

Abstract<br />

The Discontinuous Enrichment Method (DEM) is a discretization method designed for an efficient<br />

solution of multi-scale problems. It is based on a hybrid variational formulation with Lagrange<br />

multipliers. In addition to an optional polynomial field, it employs free-space solutions of the governing<br />

differential equation for approximating large gradients or highly oscillatory components of the<br />

solution. It relies on Lagrange multipliers to enforce a weak form of the inter-element continuity<br />

of the solution. Recent developments <strong>and</strong> applications of DEM are discussed. These include the<br />

solution of acoustic scattering <strong>and</strong> structural dynamics problems in the medium frequency regime,<br />

<strong>and</strong> advection-diffusion problems with high Peclet numbers. Comparisons to other method are shown<br />

<strong>and</strong> variable coefficient ideas are discussed.<br />

Then, a nonoverlapping domain decomposition method is presented for the solution of Helmholtz/structural<br />

dynamics problems discretized by DEM with <strong>and</strong> without the optional polynomial field. In this domain<br />

decomposition method, the primal subdomain degrees of freedom are eliminated by local static<br />

condensations to obtain an algebraic system of equations formulated in terms of the interface Lagrange<br />

multipliers only. As in the FETI-H <strong>and</strong> FETI-DPH domain decomposition methods for continuous<br />

15


Galerkin discretizations, this system of Lagrange multipliers is iteratively solved by a Krylov method<br />

equipped with both a local preconditioner based on subdomain data, <strong>and</strong> a global one using a coarse<br />

space. Numerical experiments performed for two- <strong>and</strong> three-dimensional acoustic problems demonstrate<br />

the scalability of the method with respect to the size of the global problem <strong>and</strong> the number of<br />

subdomains.<br />

The principal co-authors of this talk are Charbel Farhat <strong>and</strong> Jari Toivanen. Other co-authors will<br />

be acknowledged during the talk.<br />

“Domain decomposition <strong>and</strong> multigrid preconditioners for the Helmholtz equation in layered <strong>and</strong> heterogeneous<br />

media”<br />

Jari Toivanen<br />

Department of Mathematical Information Technology, University of Jyväskylä<br />

FI-40100 Jyväskylä<br />

Finl<strong>and</strong><br />

Abstract<br />

We consider the efficient numerical solution of time-harmonic acoustic scattering problems.<br />

For layered media, we propose a domain decomposition preconditioner which is based on domain<br />

embedding subdomain preconditioners <strong>and</strong> a fast direct solver. The iterations can be carried out on<br />

small subspaces associated to the interfaces between layers/subdomains. The numerical experiments<br />

demonstrate the capability to solve very large scale two-dimensional <strong>and</strong> three-dimensional problems<br />

with up to billions of unknowns. The number of iterations seems to behave roughly logarithmically<br />

with respect to the frequency.<br />

For heterogeneous media, we consider a multigrid preconditioner which is based on an algebraic<br />

multigrid method <strong>and</strong> a physically damped operator. Numerical experiments show this approach to<br />

lead to efficient solution procedure for low <strong>and</strong> medium frequency problems. The number of iterations<br />

grows roughly linearly with respect to the frequency.<br />

This is joint work with Tuomas Airaksinen (University of Jyväskylä) <strong>and</strong> Kazufumi Ito (North<br />

Carolina State University, Raleigh, NC).<br />

16


Abstracts for Posters<br />

“Numerical solution of the high frequency 2D direct scattering problem for convex objects using nonuniform<br />

B-splines”<br />

Carlos Borges<br />

Worcester Polytechnic Institute<br />

100 Institute Rd<br />

Worcester, MA<br />

USA<br />

Abstract<br />

We present a method for the numerical solution of the acoustic two dimensional direct scattering<br />

problem for non penetrable convex scatterers for high frequencies. The method takes advantage of the<br />

fact that, for the integral formulation considered for the problem, the solution to the integral equation<br />

is a physical quantity <strong>and</strong> thereby can be written as the product of a known highly oscillatory function<br />

<strong>and</strong> a unknown slow oscillatory function. We solve the problem for the slow oscillatory function using<br />

a collocation method <strong>and</strong> we approximate the solution by a linear combination of non-uniform Bsplines,<br />

where the density of control points corresponding will be higher where more resolution is<br />

needed. To perform the integrations, we use ideas of the method of stationary phase, techniques<br />

of integration of high oscillatory functions <strong>and</strong> singular kernels. Numerical results of the proposed<br />

method are presented.<br />

“Variational methods for the identification of objects”<br />

Victor A. Kovtunenko<br />

Institute for Mathematics <strong>and</strong> Scientific Computing<br />

KF-University of Graz<br />

Heinrichstr.36, A-8010 Graz<br />

Lavrent’ev Institute of Hydrodynamics<br />

630090 Novosibirsk, Russia,<br />

e-mail: victor.kovtunenko@uni-graz.at<br />

Abstract<br />

Topology optimization problems for identification <strong>and</strong> reconstruction of small geometric objects of<br />

arbitrary shapes <strong>and</strong> unknown boundary conditions are addressed. By arbitrary shapes we mean the<br />

most general, i.e., the least restrictive, geometric assumptions which are commonly used in variational<br />

formulations. We refer to singular geometric objects such as thin obstacles, cracks, multi-dimensional<br />

junks, <strong>and</strong> alike. For unknown boundary conditions we consider Robin type boundary conditions<br />

described by unknown parameters, which are discrete or distributed. Thus, the boundary conditions<br />

are determined a-posteriori, i.e., after solving the optimization problem.<br />

From a mathematical point of view, identification of unknown objects is an inverse problem, which<br />

belongs to the field of shape <strong>and</strong> topology optimization <strong>and</strong> parameter estimation. Our approach<br />

to the identification problems is based on variational methods supported with generalized methods<br />

of singular perturbations. The key ingredients of the optimization approach are as follows. Firstly,<br />

we consider the identification problem as a state-constrained optimization problem <strong>and</strong> apply proper<br />

duality principles providing us with optimality conditions in the weak setting, thus accounting for<br />

the features above. Second, we employ asymptotic methods of singular perturbation theory to obtain<br />

approximate, geometry-dependent models. While the the first-order terms are somewhat known in<br />

the literature as the topological derivative, we get the second-order terms to determine the boundary<br />

conditions. Third, from multi-parametric optimization we get semi-analytical solution strategies.<br />

We consider an example of inverse scattering problem. Some numerical aspects of the topology<br />

optimization will be discussed.<br />

17


“Time reversed absorbing conditions:<br />

discrimination between one single inclusion <strong>and</strong> two close inclusions in a non-homogeneous medium”<br />

Marie Kray<br />

Jacques-Louis Lions Laboratory, Pierre et Marie Curie University<br />

Paris, France<br />

kray@ann.jussieu.fr<br />

Abstract<br />

We introduce the time-reversed absorbing conditions (TRAC) in time-reversal methods. They<br />

enable one to “recreate the past” without knowing the source which has emitted the signals that<br />

are back-propagated. We present two applications in inverse problems: the reduction of the size of<br />

the computational domain <strong>and</strong> the determination, from boundary measurements, of the location <strong>and</strong><br />

volume of an unknown inclusion. The method does not rely on any a priori knowledge of the physical<br />

properties of the inclusion. Numerical tests with the wave equation illustrate the efficiency of the<br />

method. Moreover the TRAC method is fairly insensitive with respect to the magnitude of noise on<br />

the recorded data.<br />

In order to be closer to realistic cases as in geophysics, mine detection, medical imaging, ..., we<br />

consider non homogeneous media (r<strong>and</strong>om or layered media). The application we propose is to investigate<br />

the ability of the TRAC method to discriminate a unique inclusion from two distinct close<br />

inclusions in a non-homogeneous medium. This test is inspired by a more realistic setting. Our intent<br />

is to detect one or two iron or plastic mines in a background medium that can be r<strong>and</strong>om or layered.<br />

The physical equation we use is a scalar wave equation derived from the Maxwell equations.<br />

Joint work with Franck Assous (Bar-Ilan University & Ariel University Center, Israel,<br />

franckassous@netscape.et) <strong>and</strong> Frédéric Nataf (Université Paris 6, nataf@ann.jussieu.fr)<br />

Publications:<br />

• F. Assous, M. Kray, F. Nataf, Time Reversed Absorbing Condition in the Partial Aperture Case,<br />

http://hal.archives-ouvertes.fr/hal-00581291/fr/<br />

• F. Assous, M. Kray, F. Nataf, E. Turkel, Time Reversed Absorbing Condition: Application to<br />

inverse problem, <strong>Inverse</strong> <strong>Problems</strong> (2011), Vol. 27, no 6, pp 065003.<br />

• F. Assous, M. Kray, F. Nataf, E. Turkel, Time Reversed Absorbing Conditions, Comptes Rendus<br />

Mathmatiques, Serie I (2010), Vol. 348, no 19-20, pp 1063-1067, doi:10.1016/j.crma.2010.09.014<br />

.<br />

“<strong>Wave</strong>number-explicit convergence analysis for the Helmholtz equation: hp-FEM <strong>and</strong> hp-BEM”<br />

J.M. Melenk<br />

Vienna University of Technology<br />

Abstract<br />

We consider boundary value problems for the Helmholtz equation at large wave numbers k. In<br />

order to underst<strong>and</strong> how the wave number k affects the convergence properties of discretizations of<br />

such problems, we develop a regularity theory for the Helmholtz equation that is explicit in k. At<br />

the heart of our analysis is the decomposition of solutions into two components: the first component<br />

is an analytic, but highly oscillatory function <strong>and</strong> the second one has finite regularity but features<br />

wavenumber-independent bounds.<br />

This underst<strong>and</strong>ing of the solution structure opens the door to the analysis of discretizations of the<br />

Helmholtz equation that are explicit in their dependence on the wavenumber k. As a first example,<br />

we show for a conforming high order finite element method that quasi-optimality is guaranteed if<br />

(a) the approximation order p is selected as p = O(logk) <strong>and</strong> (b) the mesh size h is such that kh/p<br />

is small. As a second example, we consider combined field boundary integral equation arising in<br />

acoustic scattering. Also for this example, the same scale resolution conditions as in the high order<br />

finite element case suffice to ensure quasi-optimality of the Galekrin discretization.<br />

This work presented is joint work with Stefan Sauter (Zürich) <strong>and</strong> Maike Löhndorf (Vienna).<br />

18


“Trefftz-discontinuous Galerkin methods for time-harmonic Maxwell’s equations”<br />

Andrea Moiola<br />

Seminar for Applied Mathematics<br />

ETH Zürich<br />

Rämistrasse 101, CH–8092 Zürich<br />

moiola@sam.math.ethz.ch<br />

Abstract<br />

The propagation <strong>and</strong> the interaction of time-harmonic electric waves are described by the Maxwell<br />

equations ∇ × (∇ × E) − ω 2 E = 0. The need of resolving oscillating solutions <strong>and</strong> the so-called<br />

pollution effect make their numerical discretization through st<strong>and</strong>ard finite element schemes extremely<br />

expensive for high frequencies. The Trefftz methods offer a way to tackle this problem: the trial <strong>and</strong><br />

the test functions are solution of the PDE inside each element, thus they are oscillating functions<br />

<strong>and</strong> we can expect to be able to approximate the solution with smaller discrete spaces. The basis<br />

functions are often chosen as vector plane waves.<br />

We formulate a class of Trefftz-discontinuous Galerkin (TDG) methods that includes the wellknown<br />

ultra weak variational formulation (UWVF) of Cessenat <strong>and</strong> Després, <strong>and</strong> we study the<br />

convergence of their p-version (spectral version) for an impedance boundary value problem. Wellposedness<br />

<strong>and</strong> quasi-optimality in a mesh skeleton norm follow from the coercivity of the bilinear<br />

form defining the method on the Trefftz function space. A novel vector Rellich-type identity allows to<br />

prove new (wavenumber-independent) stability <strong>and</strong> regularity estimates for the considered boundary<br />

value problem in star-shaped polyhedral domains; these estimates, in turn, are used in a duality<br />

argument to prove error bounds in a mesh-independent norm.<br />

The abstract convergence analysis is carried out for any Trefftz trial space. In the case of vector<br />

plane or spherical waves, concrete error bounds are obtained by using best approximation estimates<br />

for general Maxwell solutions that are proved from the analogous scalar (Helmholtz) results. The<br />

convergence is algebraic both in the dimension of the local trial space <strong>and</strong> in the meshwidth <strong>and</strong> all<br />

the bounds are explicit in the wavenumber.<br />

This work is part of my PhD thesis, carried out under the supervision of Ralf Hiptmair (ETH<br />

Zürich) <strong>and</strong> Ilaria Perugia (Università di Pavia).<br />

“Stable absorbing layer for convective wave propagation”<br />

Imbo Sim<br />

University of Klagenfurt<br />

Abstract<br />

In a multi-model approachfor computational aeroacoustics (CAA) one often uses within the acoustic<br />

source region some kind of acoustic perturbation equations <strong>and</strong> then in the ambient region the<br />

convective wave equation. Thereby, an efficient approach to model free field radiation conditions are<br />

required for the convective wave equation. The perfectly matched layer (PML) approach has proved<br />

a flexible <strong>and</strong> accurate method, which consists in surrounding the computational domain by an absorbing<br />

layer. However, most PML formulations require wave equations stated in their st<strong>and</strong>ard<br />

second-order form to be reformulated as first-order hyperbolic systems, thereby introducing many<br />

additional unknowns. Here, we propose instead a simple stable PML formulation directly for the<br />

second-order convective wave equation both in two <strong>and</strong> in three space dimensions.<br />

The work presented is joint work with Manfred Kaltenbacher (Klagenfurt).<br />

19


List of Participants<br />

Akindeinde Saheed Ojo RICAM saheed.akindeinde@oeaw.ac.at<br />

Alyaev Sergey University of Bergen cobxo3bot@gmail.com<br />

Ammari Habib École Normale Supérieure habib.ammari@ens.fr<br />

Arnold Thomas WIAS Berlin Thomas.Arnold@wias-berlin.de<br />

Betcke Timo University College London t.betcke@reading.ac.uk<br />

Borges Carlos Worcester Polytechnic Institute ceduardo@wpi.edu<br />

Buck Marco Fraunhofer Institute for<br />

Industrial Mathematics<br />

marco.buck@itwm.fraunhofer.de<br />

Buckwar Evelyn Johannes Kepler Universität<br />

Linz<br />

Evelyn.Buckwar@jku.at<br />

Challa Durga Prasad RICAM durga.challa@oeaw.ac.at<br />

Ch<strong>and</strong>ler-Wilde Simon University of Reading s.n.ch<strong>and</strong>ler-wilde@reading.ac.uk<br />

Childs Paul Schlumberger Cambridge<br />

Research<br />

CHILDS4@slb.com<br />

Engl Heinz RICAM & University of Vienna heinz.engl@oeaw.ac.at<br />

Ernst Oliver TU Bergakademie Freiberg ernst@math.tu-freiberg.de<br />

Freitag Melina University of Bath m.freitag@maths.bath.ac.uk<br />

G<strong>and</strong>er Martin University of Geneva Martin.G<strong>and</strong>er@unige.ch<br />

Georgiev Ivan RICAM ivan.georgiev@oeaw.ac.at<br />

Gessese Alelign University of Canterbury alelign.gessese@pg.canterbury.ac.nz.<br />

Graham Ivan University of Bath i.g.graham@bath.ac.uk<br />

Grote Marcus University of Basel Marcus.Grote@unibas.ch<br />

Hegedüs Gabor RICAM gabor.hegedues@oeaw.ac.at<br />

Helin Tapio RICAM tapio.helin@oeaw.ac.at<br />

Hiptmair Ralf ETH Zürich hiptmair@sam.math.ethz.ch<br />

Hoang Viet Ha NTU, Singapore vhhoang@ntu.edu.sg<br />

Hrtus Rostislav Institute of Geonics of the AS<br />

CR, v.v.i., Ostrava, CZ<br />

hrtus@ugn.cas.cz<br />

Hu Guanghui WIAS Berlin Guanghui.Hu@wias-berlin.de<br />

Kaltenbacher Barbara University of Klagenfurt barbara.kaltenbacher@uni-graz.at<br />

Kaltenbacher Manfred University of Klagenfurt manfred.kaltenbacher@uni-graz.at<br />

Kar Manas RICAM manas.kar@oeaw.ac.at<br />

Karer Erwin RICAM erwin.karer@oeaw.ac.at<br />

Kollmann Markus Doctoral Program<br />

Computational Mathematics,<br />

Johannes Kepler University<br />

markus.kollmann@dk-compmath.jku.at<br />

Kolmbauer Michael Institute of Computational<br />

Mathematics<br />

kolmbauer@numa.uni-linz.ac.at<br />

Kovtunenko Victor KF-University Graz; Lavrent’ev<br />

Institute of Hydrodynamics<br />

victor.kovtunenko@uni-graz.at<br />

Kraus Johannes RICAM johannes.kraus@oeaw.ac.at<br />

Kray Marie Laboratoire J-L Lions, UPMC kray@ann.jussieu.fr<br />

Langer Ulrich University of Linz ulanger@numa.uni-linz.ac.at<br />

Leindl Mario Montanuniversität Leoben,<br />

Institut für Mechanik<br />

mario.leindl@unileoben.ac.at<br />

Livshits Irene Ball State University ilivshits@bsu.edu<br />

Melenk Jens Markus TU Wien melenk@tuwien.ac.at<br />

Migliorati Giovanni Department of Mathematics,<br />

Politecnico di Milano<br />

giovanni.migliorati@gmail.com<br />

Minkoff Susan Dept. of Mathematics <strong>and</strong><br />

Statistics, University of<br />

Maryl<strong>and</strong> Baltimore County<br />

sminkoff@umbc.edu<br />

20


Mitrovic Darko University of Bergen Darko.Mitrovic@math.uib.no<br />

Mohamed Menad University of Chlef<br />

Moiola Andrea SAM - ETH Zürich <strong>and</strong>rea.moiola@sam.math.ethz.ch<br />

Motamed Mohammad KAUST mohammad.motamed@nullkaust.edu.sa<br />

Nannen Lothar TU Vienna lothar.nannen@tuwien.ac.at<br />

Nataf Frédéric Laboratoire J.L Lions <strong>and</strong><br />

CNRS<br />

nataf@ann.jussieu.fr<br />

Naumova Valeriya RICAM valeriya.naumova@oeaw.ac.at<br />

Nayak Sridhara Indian Institute of Technology<br />

Kharagpur<br />

sridharanayakiitkgp@gmail.com<br />

Nguyen Trung Thanh RICAM trung-thanh.nguyen@oeaw.ac.at<br />

Nordbotten Jan Martin University of Bergen jan.nordbotten@math.uib.no<br />

Pechstein Clemens Institute of Computational<br />

Mathematics, Johannes Kepler<br />

University Linz<br />

clemens.pechstein@numa.uni-linz.ac.at<br />

Polydorides Nick Cyprus Institute nickpld@cyi.ac.cy<br />

Potthast Rol<strong>and</strong> Deutscher Wetterdienst, Univ.<br />

of Reading, Uni Göttingen<br />

r.w.e.potthast@reading.ac.uk<br />

Ramlau Ronny Industrial Mathematics<br />

Institute, Kepler University<br />

Linz, Austria<br />

ronny.ramlau@jku.at<br />

Rieder Andreas Department of Mathematics,<br />

Karlsruhe Institute of<br />

Technology<br />

<strong>and</strong>reas.rieder@kit.edu<br />

Sarkis Marcus Mathematical Sciences<br />

Dept./Worcester Polytechnic<br />

Institute<br />

msarkis@wpi.edu<br />

Scheichl Robert University of Bath r.scheichl@bath.ac.uk<br />

Schicho Josef RICAM josef.schicho@oeaw.ac.at<br />

Schöberl Joachim Vienna UT joachim.schoeberl@tuwien.ac.at<br />

Shanks Douglas University of Bath J.D.Shanks@bath.ac.uk<br />

Sim Imbo University of Klagenfurt imbo.sim@uni-klu.ac.at<br />

Sini Mourad RICAM mourad.sini@oeaw.ac.at<br />

Sokol Vojtěch Institute of Geonics of the AS<br />

CR, v.v.i., Ostrava, CZ<br />

sokol.vojtech@gmail.com<br />

Spence Euan University of Bath e.a.spence@bath.ac.uk<br />

Spillane Nicole Laboratoire Jacques Louis Lions<br />

(Paris) - Michelin<br />

spillane@ann.jussieu.fr<br />

Steinbach Olaf TU Graz o.steinbach@tugraz.at<br />

Stolk Chris University of Amsterdam C.C.Stolk@uva.nl<br />

Talagr<strong>and</strong> Olivier Laboratoire de Météorologie<br />

Dynamique, École Normale<br />

Supérieure, Paris, France<br />

talagr<strong>and</strong>@lmd.ens.fr<br />

Teckentrup Aretha University of Bath, Department<br />

of Mathematical Sciences<br />

A.L.Teckentrup@bath.ac.uk<br />

Tezaur Radek Stanford University rtezaur@stanford.edu<br />

Toivanen Jari Stanford University toivanen@stanford.edu<br />

Tomar Satyendra RICAM satyendra.tomar@ricam.oeaw.ac.at<br />

Wachsmuth Daniel RICAM daniel.wachsmuth@oeaw.ac.at<br />

Willems Jörg RICAM joerg.willems@ricam.oeaw.ac.at<br />

Wohlmuth Barbara Technische Universität<br />

München<br />

wohlmuth@ma.tum.de<br />

Wolfmayr Monika Institute of Computational<br />

Mathematics, University of Linz<br />

monika.kowalska@numa.uni-linz.ac.at<br />

Yang Huidong RICAM huidong.yang@oeaw.ac.at<br />

Zikatanov Ludmil The Pennsylvania State<br />

University<br />

ltz@math.psu.edu<br />

Zulehner Walter Johannes Kepler University<br />

Linz<br />

zulehner@numa.uni-linz.ac.at<br />

21


Monday Tuesday Wednesday Thursday Friday<br />

Registration (9:00-9:40) Martin G<strong>and</strong>er Ronny Ramlau Rol<strong>and</strong> Potthast Manfred Kaltenbacher<br />

9:00-9:50<br />

Spectral finite elements for a<br />

mixed formulation in<br />

Are absorbing boundary<br />

Approaches to dynamical inverse<br />

scattering problems<br />

<strong>Inverse</strong> problems in adaptive<br />

optics<br />

conditions <strong>and</strong> perfectly matched<br />

layers really so different?<br />

Opening (9:40-9:50)<br />

computational acoustics taking<br />

flow effects into acount<br />

Ralf Hiptmair Lothar Nannen Frédéric Nataf Thanh Nguyen Euan Spence<br />

9:50-10:40<br />

Stability <strong>and</strong> conditioning of<br />

boundary integral methods for<br />

<strong>Inverse</strong> obstacle scattering<br />

problems using multifrequency<br />

Time reversed absorbing<br />

condition in the partial aperture<br />

case<br />

Hardy space infinite elements for<br />

exterior Maxwell problems<br />

Convergence of truncated<br />

T-matrix approximation<br />

high frequency scattering<br />

measurements<br />

Coffee Coffee Coffee Coffee Coffee<br />

Timo Betcke Habib Ammari Olaf Steinbach Guanghui Hu Simon Ch<strong>and</strong>ler-Wilde<br />

11:10-12:00<br />

Modulated plane wave methods<br />

Boundary element methods for Direct <strong>and</strong> inverse scattering of Numerical-asymptotic integral<br />

Electromagnetic invisibility <strong>and</strong><br />

for Helmholtz problems in<br />

acoustic <strong>and</strong> electromagnetic elastic waves by diffraction<br />

equation methods for high<br />

super-resolution<br />

heterogeneous media<br />

scattering problems<br />

gratings<br />

frequency scattering<br />

Lunch Lunch Lunch Lunch Closing<br />

Susan Minkoff Marcus Grote free afternoon Jari Toivanen<br />

14:00-14:50<br />

Domain decomposition <strong>and</strong><br />

multigrid preconditioners for the<br />

Helmholtz equation in layered<br />

(please feel free to make use of<br />

the seminar room <strong>and</strong> the Special<br />

Discontinuous Galerkin methods<br />

<strong>and</strong> local time stepping for<br />

Two scale wave equation<br />

modeling<br />

Semester offices)<br />

transient wave propagation<br />

<strong>and</strong> heterogeneous media<br />

Coffee Coffee Coffee<br />

Paul Childs Joachim Schöberl Radek Tezaur<br />

15:20-16:10<br />

The discontinuous enrichment<br />

method <strong>and</strong> its domain<br />

Hybrid discontinuous Galerkin<br />

finite element methods for the<br />

decomposition solver for the<br />

Numerics of waveform inversion<br />

for seismic data<br />

Helmholtz equation<br />

Helmholtz equation<br />

Chris Stolk Ira Livshits<br />

16:10-17:00<br />

Algebraic multigrid algorithm for<br />

solving Helmholtz equations with<br />

Seismic inverse scattering by<br />

reverse time migration<br />

large wave numbers<br />

Radon Colloquium<br />

Martin G<strong>and</strong>er<br />

17:15<br />

Posters & Reception<br />

Conference Dinner<br />

(19:00)<br />

From Euler, Schwarz, Ritz <strong>and</strong><br />

Galerkin to modern computing<br />

Each talk is 40 minutes long. After the end of each talk, there are 10 minutes for discussion.

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