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Program - Université de Pau et des Pays de l'Adour

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2007 y 01 ,<br />

Fourth<br />

http://www.univ-pau.fr/~cgout/mata2007<br />

Deadline for abstract submission : Jan. 31, 2007<br />

Inverse problems, Level s<strong>et</strong> m<strong>et</strong>hods...<br />

In Numerical Algorithms (Springer)<br />

Scientific Committee: G. Albrecht, D. Apprato,<br />

C. Brezinski, C. <strong>de</strong> Boor, C. Gout, A. Kunoth,<br />

T. Lyche, M.-L. Mazure, C. Rabut, R. Schaback.<br />

Mira Bozzini<br />

Christian Gout<br />

Christophe Rabut<br />

Leonardo Traversoni<br />

Lay out: Marjory Lemière (<strong>Pau</strong>, Honolulu)<br />

Instituto Politécnico Nacional (CIC)<br />

INSA <strong>de</strong> Toulouse<br />

Università di Milano<br />

PROGRAM


Fourth International Conference on<br />

Multivariate Approximation:<br />

Theory and Applications<br />

at Cancun (WESTIN Spa & Resort), Mexico April 26-May 01, 2007.<br />

In<strong>de</strong>x<br />

I. Introduction................................................................................................... page 5<br />

II. Proceedings............................................................................................. page 7<br />

III. <strong>Program</strong>me - Schedules<br />

Table .....................................................................................................page 11<br />

Talks..................................................................................................... page 13<br />

IV. Participants .................................................................................................. page 17<br />

IV. Abstracts ....................................................................................................page 23<br />

3


Introduction<br />

You will find in this program all the schedule of the conference, and some other<br />

informations (proceedings, abstracts…).<br />

Thank you for your participation in MATA 2007.<br />

MATA 2007 - Scientific Committee<br />

Gudrun Albrecht (France), Dominique Apprato (France), Clau<strong>de</strong> Brezinski (France),<br />

Carl <strong>de</strong> Boor (USA), Christian Gout (France), Angela Kunoth (Germany), Tom Lyche<br />

(Oslo), Marie-Laurence Mazure (France), Christophe Rabut (Toulouse), Robert<br />

Schaback (Germany).<br />

Organizing Committee:<br />

Mira Bozzini<br />

Christian Gout<br />

(SIAM representative)<br />

Christophe Rabut<br />

Università di Milano<br />

Dipartimento di Matematica e Applicazioni<br />

Via R. Cozzi n. 53, 20125 Milano, Italy<br />

Tel: italy+026448+<br />

<strong>Université</strong> <strong>de</strong> Valenciennes<br />

LAMAV-ISTV2<br />

Mont Houy<br />

59313 Valenciennes ce<strong>de</strong>x 9, France<br />

chris_gout@cal.berkeley.edu<br />

INSA Toulouse<br />

Dpt Génie Mathématique<br />

135 av. <strong>de</strong> Rangueil<br />

31077 Toulouse ce<strong>de</strong>x 4, France,<br />

Tel: (+33) 561 559 322 : Fax number: +33 561 559 320<br />

christophe.rabut@insa-toulouse.fr<br />

Leonardo Traversoni<br />

Univ. Autonoma M<strong>et</strong>. (Iztapalapa),<br />

Ciencias Basicas e Ingenieria,<br />

Ap Post 55-532, C.P. 09340 Mexico D.F., Mexico, Tel: (52)<br />

5 7244646<br />

ltd@xanum.uam.mx<br />

In cooperation with<br />

- Ministère <strong>de</strong> l'Education Nationale <strong>et</strong> <strong>de</strong> la Recherche, France<br />

- SMAI - AFA (Association Française d'Approximation)<br />

- SIAM<br />

- UAM (Iztapalapa)<br />

- INSA <strong>de</strong> Toulouse<br />

- <strong>Université</strong> <strong>de</strong> Valenciennes <strong>et</strong> du Hainaut Cambresis<br />

- Instituto Politecnico Nacional (CIC)<br />

- Università di Milano<br />

5


Previous Conference of the series:<br />

First International Conference on Scattered Data Fitting<br />

Cancun, Mexico, Thursday, March 2- Wednesday, March 8, 1995<br />

Org. : A. Le Méhauté, L. L. Schumaker, L. Traversoni<br />

Second International Conference on Multivariate Scattered Data Fitting<br />

Puerto Vallarta, Jalisco, Mexico, April 15--20, 1999<br />

Org. : P. Gonzalez-Casanova, A. Le Méhauté, L. L. Schumaker, L. Traversoni<br />

Third International Conference on Multivariate Scattered Data Fitting<br />

Puerto Vallarta, Jalisco, Mexico, April 23--29, 2003<br />

Org. : C. Gout, C. Rabut, L. Traversoni<br />

http://www.univ-pau.fr/~mata2003/<br />

6


The proceedings<br />

of the conference will be edited as a special issue of<br />

Numerical Algorithms (SPRINGER).<br />

Some remarks:<br />

1) No difference will be ma<strong>de</strong> in the proceedings b<strong>et</strong>ween an oral talk (invited or regular)<br />

and a poster talk.<br />

2) To appear in the proceedings, it will be necessary to have ma<strong>de</strong> the communication in<br />

Cancun.<br />

3) The paper submitted to the proceedings must correspond to the talk presented in<br />

Cancun (though possibly actualized). No page limitation is given… But of course, it's<br />

important to submit a concise paper!<br />

4) A peer review will be ma<strong>de</strong>. The process will be the same as a classical submission<br />

in the journal "Numerical Algorithms"... The authors will have to take into account the<br />

"instructions for authors" of this journal (http://www.springerlink.com/link.asp?id=101751).<br />

The editors will take their <strong>de</strong>cision following the reports ma<strong>de</strong> by the referees.<br />

5) Deadline to submit a paper : OCTOBER 2007.<br />

Manuscript Presentation<br />

1. Manuscripts must be written in English and typed on one si<strong>de</strong> of the page only, with wi<strong>de</strong><br />

margins. A font size of 11 point is preferred. Manuscripts must inclu<strong>de</strong>:<br />

• A short title which will be used tog<strong>et</strong>her with author‘s names in the running headline.<br />

• The authors‘ name and addresses<br />

• A self-contained abstract, preferably without formulae<br />

• A list of keywords<br />

• AMS (MOS) classification<br />

2. Tables and figures should be numbered, have a self-contained caption, and their positions in<br />

the text must be clearly indicated. In the case of paper-only submission, figures should be<br />

on separate she<strong>et</strong>s. In the case of electronic submission, please supply your figures in<br />

Encapsulated Postscript form.<br />

References must be numbered. In the text, they should be indicated by a brack<strong>et</strong>ed number : [1].<br />

Figures : All photographs, graphs and diagrams should be referred to as a 'Figure' and they should be numbered<br />

consecutively (1, 2, <strong>et</strong>c.). Multi-part figures ought to be labelled with lower case l<strong>et</strong>ters (a, b, <strong>et</strong>c.). Please insert keys<br />

and scale bars directly in the figures. Relatively small text and great variation in text sizes within figures should be<br />

avoi<strong>de</strong>d as figures are often reduced in size. Figures may be sized to fit approximately within the column(s) of the<br />

journal. Provi<strong>de</strong> a <strong>de</strong>tailed legend (without abbreviations) to each figure, refer to the figure in the text and note its<br />

approximate location in the margin. Please place the legends in the manuscript after the references.<br />

Tables : Each table should be numbered consecutively (1, 2, <strong>et</strong>c.). In tables, footnotes are preferable to long explanatory<br />

material in either the heading or body of the table. Such explanatory footnotes, i<strong>de</strong>ntified by superscript l<strong>et</strong>ters, should<br />

be placed immediately below the table. Please provi<strong>de</strong> a caption (without abbreviations) to each table, refer to the table<br />

in the text and note its approximate location in the margin. Finally, please place the tables after the figure legends in<br />

the manuscript.<br />

References<br />

1. Journal article<br />

Hamburger, C.: Quasimonotonicity, regularity and duality for nonlinear systems of partial differential equations. Ann.<br />

Mat. Pura. Appl. 169, 321–354 (1995)<br />

7


2. Inclusion of issue number (optional)<br />

Campbell, S.L., Gear, C.W.: The in<strong>de</strong>x of general nonlinear DAES. Numer. Math. 72(2), 173–196 (1995)<br />

3. Journal issue with issue editor<br />

Smith, J. (ed.): Ro<strong>de</strong>nt genes. Mod. Genomics J. 14(6), 126–233 (1998)<br />

4. Journal issue with no issue editor<br />

Ro<strong>de</strong>nt genes: Mod. Genomics J. 14(6):126–233 (1998)<br />

5. Book chapter<br />

Broy, M.: Software engineering – from auxiliary to key technologies. In: Broy, M., Denert, E. (eds.) Software Pioneers, pp.<br />

10–13. Springer, Berlin Hei<strong>de</strong>lberg New York (2002)<br />

6. Book, authored<br />

Ged<strong>de</strong>s, K.O., Czapor, S.R., Labahn, G.: Algorithms for Computer Algebra. Kluwer, Boston (1992)<br />

7. Book, edited<br />

Seymour, R.S. (ed.): Conductive Polymers. Plenum, New York (1981)<br />

8. Chapter in a book in a series without volume titles<br />

MacKay, D.M.: Visual stability and voluntary eye movements. In: Jung, R., MacKay, D.M. (eds.) Handbook of Sensory<br />

Physiology, vol. 3, pp. 307–331. Springer, Berlin Hei<strong>de</strong>lberg New York (1973)<br />

9. Chapter in a book in a series with volume titles<br />

Smith, S.E.: Neuromuscular blocking drugs in man. In: Zaimis, E. (ed.) Neuromuscular Junction. Handbook of Experimental<br />

Pharmacology, vol. 42, pp. 593–660. Springer, Berlin Hei<strong>de</strong>lberg New York (1976)<br />

10. Proceedings as a book (in a series and sub-series)<br />

Zowghi, D., <strong>et</strong> al.: A framework for reasoning about requirements in evolution. In: Foo N., Goebel R. (eds.) Topics in<br />

Artificial Intelligence, 4th Pacific Rim Conference on Artificial Intelligence, Cairns, August 1996. Lecture Notes in<br />

Computer Science. Lecture Notes in Artificial Intelligence, vol. 1114, pp. 157–168. Springer, Berlin Hei<strong>de</strong>lberg New York<br />

(1996)<br />

11. Proceedings with an editor (without a publisher)<br />

Aaron, M.: The future of genomics. In: Williams, H. (ed.) Proceedings of the Genomic Researchers, Boston, 1999<br />

12. Proceedings without an editor (without a publisher)<br />

Chung, S.-T., Morris, R.L.: Isolation and characterization of plasmid <strong>de</strong>oxyribonucleic acid from Streptomyces fradiae.<br />

In: Abstracts of the 3rd International Symposium on the Gen<strong>et</strong>ics of Industrial Microorganisms, University of<br />

Wisconsin, Madison, 4–9 June 1978<br />

13. Paper presented at a conference<br />

Chung, S.-T., Morris, R.L.: Isolation and characterization of plasmid <strong>de</strong>oxyribonucleic acid from Streptomyces fradiae.<br />

Paper presented at the 3rd international symposium on the gen<strong>et</strong>ics of industrial microorganisms, University of<br />

Wisconsin, Madison, 4–9 June 1978<br />

14. Patent.<br />

Name and date of patent are optional<br />

L.O. Norman: Lightning rods. US Patent 4,379,752, 9 Sept 1998<br />

15. Dissertation, Ph.D. thesis (either text is acceptable)<br />

J.W. Trent: Experimental acute renal failure. Dissertation, University of California (1975)<br />

16. Institutional author (book)<br />

International Anatomical Nomenclature Committee: Nomina anatomica. (Excerpta Medica, Amsterdam 1966)<br />

17. Non-English publication cited in an English publication<br />

Wolf, G.H., Lehman, P.-F.: Atlas <strong>de</strong>r Anatomie, vol. 4/3, 4th edn. Fischer, Berlin (1976) [NB: Use the language of the<br />

primary document, not that of the reference for "vol" <strong>et</strong>c.!]<br />

18. Non-Latin alphab<strong>et</strong> publication.<br />

The English translation is optional.<br />

Marikhin, V.Y., Myasnikova, L.P.: Nadmolekulyarnaya struktura polimerov<br />

(The supramolecular structure of polymers). Khimiya, Leningrad (1977)<br />

19. Published and In press articles with or without DOI:<br />

19.1 In press:<br />

Wilson, M. <strong>et</strong> al. In: Wilson M (ed.): Style manual. Springer, Berlin Hei<strong>de</strong>lberg New York (2006)<br />

19.2. Article by DOI (with page numbers)<br />

Slifka, M.K., Whitton, J.L.: J. Mol. Med. 78:74–80. DOI 10.1007/s001090000086 (2001)<br />

19.3. Article by DOI (before issue publication with page numbers)<br />

Slifka, M.K., Whitton, J.L.:J. Mol. Med. (in press). DOI 10.1007/s001090000086 (2006)<br />

19.4. Article in electronic journal by DOI (no paginated version)<br />

Slifka, M.K., Whitton, J.L.: Dig. J. Mol. Med. DOI 10.1007/s801090000086 (2000)<br />

20. Intern<strong>et</strong> publication/Online document<br />

Doe, J. In: The dictionary of substances and their effects. Royal Soci<strong>et</strong>y of Chemistry.Available via DIALOG.<br />

http://www.rsc.org/dose/title of subordinate document. Cited 15 Jan 1999 (1999)<br />

8


20.1. Online database<br />

Healthwise Knowledgebase. US Pharmacopeia, Rockville. Http://www.healthwise.org. Cited 21 Sept 1998 (1998)<br />

Supplementary material/private homepage<br />

Doe, J.: Http://www.privatehomepage.com. Cited 22 Feb 2000 (2000)<br />

University site<br />

Doe, J.: Http://www.uni-hei<strong>de</strong>lberg.<strong>de</strong>/mydata.html. Cited 25 Dec 1999 (1999)<br />

FTP site<br />

Doe, J.: ftp://ftp.isi.edu/in-notes/rfc2169.txt. Cited 12 Nov 1999 (1999)<br />

Organization site<br />

ISSN International Centre: Global ISSN database. http://www.issn.org. Cited 20 Feb 2000 (1999)<br />

Online Manuscript Submission,<br />

Review and Tracking System for the journal - Numerical Algorithms<br />

TO SUBMIT A PAPER, IT WILL BE NECESSARY TO SUBMIT DIRECTLY TO NUM. ALGO<br />

USING THE JOURNAL WEBSITE.<br />

C. GOUT will send you more <strong>de</strong>tails, in pecular the LOGIN and PASSWORD related TO<br />

MATA 2007.<br />

So, do not submit paper before you have these informations (around mid-september).<br />

Authors: wi<strong>de</strong> range of submission file formats is supported, including: Word, WordPerfect, RTF, TXT,<br />

TIFF, GIF, JPEG, EPS, LaTeX2E, TeX, Postscript, PICT, Excel, Tar, Zip and Powerpoint. PDF is not an<br />

acceptable file format.<br />

9


April 26, THURSDAY April 27, FRIDAY April 28, SATURDAY April 30, MONDAY May 01, TUESDAY<br />

8.00: Registration<br />

8.30: Welcome session<br />

8.40 Larry Schumaker<br />

A C 1 quadratic trivariate macroelement<br />

space <strong>de</strong>fined over<br />

arbitrary t<strong>et</strong>rahedral partitions<br />

9.20 Hrushikesh N Mhaskar,<br />

Diffusion polynomial frames on<br />

m<strong>et</strong>ric measure spaces<br />

9.50 Steven Damelin<br />

Numerical integration, Energy and<br />

Discrepancy on Compact<br />

Homogenous manifolds<br />

10.20 Shayne Waldron,<br />

Tight frames and their symm<strong>et</strong>ries<br />

11.00 Mexican Coffee Break<br />

& Registration<br />

11.40 Carole Le Guya<strong>de</strong>r<br />

Self-repelling snakes for topologypreserving<br />

segmentation mo<strong>de</strong>ls.<br />

12.10 Nicolas Forca<strong>de</strong>l<br />

Image segmentation using a<br />

Generalized Fast Marching<br />

M<strong>et</strong>hod<br />

12.40 Knut Mørken<br />

Mathematical and computational<br />

challenges in some applications of<br />

medical imaging<br />

13.20 END<br />

8.00 Maria Cruz Lopez <strong>de</strong> Silanes<br />

An extension of a bound for functions<br />

in Sobolev spaces and its application to<br />

(m,s)-spline interpolation and<br />

smoothing<br />

8.40 Alexan<strong>de</strong>r Grebennikov,<br />

Rotating projection of image<br />

reconstruction and application for<br />

computer tomography<br />

9.10 Juarez Valencia Lorenzo<br />

Hector<br />

Numerical Simulation of a Viscous<br />

Pump by a High Or<strong>de</strong>r Finite Element<br />

M<strong>et</strong>hod<br />

9.40 Milvia Rossini<br />

Polyharmonic splines<br />

10.20 Mike Neamtu<br />

Splines for Surfaces of Arbitrary<br />

Topology<br />

11.00 Mexican Coffee Break<br />

11.40 Frank Sommen<br />

The Dirac equation for bivector mass<br />

12.20 Bram <strong>de</strong> Knock<br />

A new Hilbert transform in a m<strong>et</strong>ric<br />

<strong>de</strong>pen<strong>de</strong>nt Clifford s<strong>et</strong>ting<br />

12.50 Liesbel Van <strong>de</strong> Voor<strong>de</strong><br />

Some results in discr<strong>et</strong>e Clifford<br />

analysis<br />

13.20 Klaus Gürlebeck<br />

On monogenic approximations of<br />

solutions of the Lamé system<br />

14.00 END<br />

9.00 Rafal Ablamowicz<br />

Computational algebraic geom<strong>et</strong>ry m<strong>et</strong>hods for<br />

curves and surfaces<br />

9.40 Pedro Gonzalez-Casanova<br />

A Dynamical No<strong>de</strong> Adaptive RBF M<strong>et</strong>hod to Solve<br />

PDE Problems.<br />

10.10 Karina Toscano<br />

Hand-written character recognition using spline<br />

wavel<strong>et</strong>s.<br />

10.40 Gabriele Steidl ,<br />

Diffusion Filters and Wavel<strong>et</strong>s<br />

11h20 Mexican Coffee Break<br />

12h 15: END<br />

POSTER SESSION, Monday 10.40<br />

- Mira Bozzini, A local m<strong>et</strong>hod for large and<br />

unevenly distributed data.<br />

- Anne Gaëlle Saint-Guirons, Approximation of<br />

surfaces with fault(s) and/or rapidly varying data,<br />

using segmentation process, D m spines and finite<br />

element m<strong>et</strong>hod.<br />

- Hermenegildo Cisneros, Isolated character<br />

recognition by using vector machines with a kernel<br />

of radial base.<br />

- Benjamin Cruz, Some formal aspects and<br />

applications of Cartan - Dieudonné theorem.<br />

- Xiang Feng Bu, Variational calculus and multigrid<br />

dynamical programmingon expo-rational surfaces<br />

and volume <strong>de</strong>formations: theory and applications<br />

- Sonia Charleston Forward and Inverse Problems<br />

for D<strong>et</strong>ermining Computer Simulated Respiratory<br />

Sound Sources<br />

- Christian Gout , Geo<strong>de</strong>sic Active contour un<strong>de</strong>r<br />

geom<strong>et</strong>rical constraints: Theory and 3D applications<br />

- Christophe Rabut, How to reduce Runge<br />

phenomenon<br />

- Jernej Kozak, Lattices on simplices<br />

8.00 Olivier Gibaru<br />

Param<strong>et</strong>ric L 1 polynomial splines<br />

interpolation<br />

8.40 Lubomir Dechevsky<br />

Expo-rational B-splines of a complex<br />

variable and their applications<br />

9.10 Victoria Hernan<strong>de</strong>z<br />

Umbrella based triangulation of regular<br />

param<strong>et</strong>ric surfaces<br />

9.40 Karine Dadourian<br />

Analysis of some bivariate non-linear<br />

interpolatory subdivision schemes and<br />

associated multiresolution<br />

10.10 Hoffman Micklos<br />

General formulae of B-spline curves with<br />

shape param<strong>et</strong>ers<br />

10.40 Mexican Coffee Break<br />

and<br />

POSTER SESSION<br />

12.00 Yi Xu<br />

QWT: R<strong>et</strong>rospective and New Applications<br />

12.40 Arne Lakså<br />

Generalized Expo-Rational B-splines<br />

13.10 Heriberto Casarrubias<br />

Using cubic spline for the velocity planning<br />

in mobile robots.<br />

13.40 Francesca Pitolli<br />

Sparse Approximation for Source Separation<br />

in the Magn<strong>et</strong>o-encephalography Inverse<br />

Problem<br />

8.00 Jeremy Levesley<br />

The or<strong>de</strong>r of approximation of transport<br />

equations by the kin<strong>et</strong>ic equation<br />

8.40 Leonardo Traversoni<br />

Wavel<strong>et</strong>s and Movements, different<br />

approaches<br />

9.10 Luis Eduardo Falcon<br />

Radon transform and harmonical<br />

analysis for 3D motion estimation using<br />

robot omnidirectional vision<br />

9.40 Rafael Resendiz<br />

Building solids using quaternions<br />

10.10 Mexican Coffee Break<br />

10.40 Wolfgang Sprößig<br />

Quaternionic holomorphic functions in<br />

fluid dynamics and elasticity<br />

11.20 Angela Kunoth<br />

Fast Multiscale M<strong>et</strong>hods for PDE-<br />

Constrained Control Problems<br />

12h00 Organizing Committee<br />

12h10 END<br />

14.20 END<br />

MATA 2007 Cancun, Mexico… April 26-May 01, 2007. Org. : M. Bozzini, C. Gout-C. Rabut-L. Traversoni<br />

Registration required to appear in the program…


APRIL 26, THURSDAY<br />

8.00: Registration<br />

8.30: Welcome session<br />

8.40 Larry Schumaker<br />

A C 1 quadratic trivariate macro-element space <strong>de</strong>fined over arbitrary t<strong>et</strong>rahedral partitions<br />

9.20 Hrushikesh N Mhaskar,<br />

Diffusion polynomial frames on m<strong>et</strong>ric measure spaces<br />

9.50 Steven Damelin<br />

Numerical integration, Energy and Discrepancy on Compact Homogenous manifolds<br />

10.20 Shayne Waldron,<br />

Tight frames and their symm<strong>et</strong>ries<br />

11.00 Mexican Coffee Break<br />

& Registration<br />

11.40 Luminita Vese<br />

Variational image <strong>de</strong>composition mo<strong>de</strong>ls into cartoon and texture<br />

12.20 Carole Le Guya<strong>de</strong>r<br />

Self-repelling snakes for topology-preserving segmentation mo<strong>de</strong>ls.<br />

12.50 Nicolas Forca<strong>de</strong>l<br />

Image segmentation using a Generalized Fast Marching M<strong>et</strong>hod<br />

11.40 Knut Mørken<br />

Mathematical and computational challenges in some applications of medical imaging<br />

14.00 END<br />

APRIL 27, FRIDAY<br />

8.00 Maria Cruz Lopez <strong>de</strong> Silanes<br />

An extension of a bound for functions in Sobolev spaces and its application to (m,s)-spline<br />

interpolation and smoothing<br />

8.40 Alexan<strong>de</strong>r Grebennikov<br />

Rotating projection of image reconstruction and application for computer tomography<br />

13


9.10 Juarez Valencia Lorenzo Hector<br />

Numerical Simulation of a Viscous Pump by a High Or<strong>de</strong>r Finite Element M<strong>et</strong>hod<br />

9.40 Milvia Rossini<br />

Polyharmonic splines<br />

10.20 Mike Neamtu<br />

Splines for Surfaces of Arbitrary Topology<br />

11.00 Mexican Coffee Break<br />

11.40 Frank Sommen<br />

The Dirac equation for bivector mass<br />

12.20 Bram <strong>de</strong> Knock<br />

A new Hilbert transform in a m<strong>et</strong>ric <strong>de</strong>pen<strong>de</strong>nt Clifford s<strong>et</strong>ting<br />

12.50 Liesbel Van <strong>de</strong> Voor<strong>de</strong><br />

Some results in discr<strong>et</strong>e Clifford analysis<br />

13.20 Klaus Guerlebeck<br />

TBA<br />

14.00 END<br />

APRIL 28, SATURDAY<br />

9.00 Rafal Ablamowicz<br />

Computational algebraic geom<strong>et</strong>ry m<strong>et</strong>hods for curves and surfaces<br />

9.40 Pedro Gonzalez-Casanova<br />

A Dynamical No<strong>de</strong> Adaptive RBF M<strong>et</strong>hod to Solve PDE Problems.<br />

10.10 Karina Toscano<br />

Hand-written character recognition using spline wavel<strong>et</strong>s.<br />

10.10 Martin Buhmann<br />

Radial Basis Function Interpolation with Param<strong>et</strong>ers<br />

10.40 Gabriele Steidl<br />

Diffusion Filters and Wavel<strong>et</strong>s<br />

11h20 Mexican Coffee Break<br />

12h 15: END<br />

14


APRIL 29, SUNDAY<br />

Group excursion to Chitzen Itza (or Tulum),<br />

APRIL 30, MONDAY<br />

8.00 Olivier Gibaru<br />

Param<strong>et</strong>ric L 1 polynomial splines interpolation<br />

8.40 Lubomir Dechevsky<br />

Expo-rational B-splines of a complex variable and their applications<br />

9.10 Victoria Hernan<strong>de</strong>z<br />

Umbrella based triangulation of regular param<strong>et</strong>ric surfaces<br />

9.40 Karine Dadourian<br />

Analysis of some bivariate non linear interpolatory subdivision schemes and associated<br />

multiresolution<br />

10.10 Hoffman Micklos<br />

General formulae of B-spline curves with shape param<strong>et</strong>ers<br />

10.40 Mexican Coffee Break and<br />

POSTER SESSION<br />

- Mira Bozzini, A local m<strong>et</strong>hod for large and unevenly distributed data<br />

- Anne Gaëlle Saint-Guirons, Surface Approximation of surfaces with fault(s) and/or rapidly<br />

varying data, using segmentation process, D m spines and finite element m<strong>et</strong>hod<br />

- Hermenegildo Cisneros, Isolated character recognition by using vector machines with a kernel<br />

of radial base<br />

- Benjamin Cruz, Some formal aspects and applications of Cartan - Dieudonné theorem<br />

- Xiang Feng Bu, Variational calculus and multigrid dynamical programmingon expo-rational<br />

surfaces and volume <strong>de</strong>formations: theory and applications<br />

- Sonia Charleston Forward and Inverse Problems for D<strong>et</strong>ermining Computer Simulated<br />

Respiratory Sound Sources<br />

- Christian Gout & Dominique Apprato, Geo<strong>de</strong>sic Active contour un<strong>de</strong>r geom<strong>et</strong>rical constraints:<br />

Theory and 3D applications<br />

- Christophe Rabut, How to reduce Runge phenomenon<br />

- Jernej Kozak, Lattices on simplices<br />

15


12.00 Yi Xu<br />

QWT: R<strong>et</strong>rospective and New Applications<br />

12.40 Arne Lakså<br />

Generalized Expo-Rational B-splines<br />

13.10 Heriberto Casarrubias<br />

Using cubic spline for the velocity planning in mobile robots<br />

13.40 Francesca Pitolli<br />

Sparse Approximation for Source Separation in the Magn<strong>et</strong>o-encephalography Inverse Problem<br />

14.20 END<br />

May 01, TUESDAY<br />

8.00 Eduardo Bayro-Corrochano<br />

Applications of quaternion wavel<strong>et</strong> transform: for robotic vision<br />

8.40 Leonardo Traversoni<br />

Wavel<strong>et</strong>s and Movements, different approaches<br />

9.10 Luis Eduardo Falcon<br />

Radon transform and harmonical analysis for 3D motion estimation using robot omnidirectional<br />

vision<br />

9.40 Rafael Resendiz<br />

Building solids using quaternions<br />

10.10 Wolfgang Sprößig<br />

Quaternionic holomorphic functions in fluid dynamics and elasticity<br />

10.50 Mexican Coffee Break<br />

11.30 Angela Kunoth<br />

Fast Multiscale M<strong>et</strong>hods for PDE-Constrained Control Problems<br />

12.10 Jeremy Levesley<br />

The or<strong>de</strong>r of approximation of transport equations by the kin<strong>et</strong>ic equation<br />

12h50 Organizing Committee<br />

13.00 END<br />

16


LIST OF PARTICIPANTS<br />

The 65 registered participants come from 18 different countries.<br />

Belgium (3): De Knock, Sommen, Van <strong>de</strong> Voor<strong>de</strong> China (1) : Xu Cuba (1): Hernan<strong>de</strong>z<br />

Ethiopia (1) : Gu<strong>de</strong>tta France (8): Apprato, Dadourian, Forca<strong>de</strong>l, Gibaru, Gout, Le Guya<strong>de</strong>r,<br />

Rabut, Saint-Guirons Germany (5): Buhmann, Guerlebeck, Kunoth, Sprößig, Steidl Hungary (2):<br />

Hoffmann, Juhasz Israël (1) : Ziegler Italy (3): Bozzini, Pitolli, Rossini Lybia (3) :<br />

Mexico (21): Arredondo, BarrÓn, Bayro Corrochano, Casarubbias,<br />

Cervantes, Charleston, Cisneros, Cruz, FalcÓn, Gloria, Gonzalez-Casanova, Grebennikov, Hector,<br />

Leon, LÓpez, Martinez, Rabinovitch, Resendiz, Sossa Azuela, Toscano, Traversoni New Zealand<br />

(1) : Waldron Norway (4) : Bu, Dechevsky, Lakså, Mørken Slovenia (1) : Kozak Spain<br />

(1): Lopez <strong>de</strong> Silanes United Kingdom (1): Levesley USA (6): Ablamowicz, Damelin, Mhaskar,<br />

Neamtu, Schumaker, Vese Russia (1) : Berdyshev<br />

Ablamowicz Rafal (saturday, 8.30)<br />

Department of Mathematics, Box 5054, Tennessee Technological University , Cookeville, TN 38505 U.S.A.<br />

rablamowicz@tntech.edu<br />

Apprato Dominique (monday, 10.40)<br />

<strong>Université</strong> <strong>de</strong> <strong>Pau</strong> UFR Sciences <strong>et</strong> Techniques <strong>de</strong> la Côte Basque 64600 Angl<strong>et</strong>. France<br />

<strong>Université</strong> <strong>de</strong> <strong>Pau</strong>, FR 2952 CNRS - IPRA-Av. <strong>de</strong> l <strong>Université</strong> - BP 1155 , 64018 <strong>Pau</strong> ce<strong>de</strong>x, France<br />

apprato@univ-pau.fr<br />

Arredondo Brenda<br />

Univ. Autonoma M<strong>et</strong>., Iztapalapa Ciencias Basicas e Ingenieria,<br />

Ap Post 55-532, C.P. 09340 Mexico, 9340 Mexico D.F. Mexico<br />

BarrÓn Ricardo<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9,<br />

Mexico City, 07738. Mexico<br />

rbarron@cic.ipn.mx<br />

Bayro Corrochano Eduardo (tuesday, 8.00)<br />

CINVESTAV Unidad Guadalajara, Apartado Postal 31-438, Plaza la Luna , 44550 Guadalajara, Jalisco. Mexico<br />

edb@gdl.cinvestav.mx<br />

Berdyshev Vitalii<br />

URAL University, Ekaterinbourg, Russia<br />

bvi@imm.uran.ru<br />

17


Bozzini Mira (monday, 10.40)<br />

Università di Milano, Dipartimento di Matematica e Applicazioni ,Via R. Cozzi n. 53, 20125 Milano, Italy<br />

mira.bozini@unimib.it<br />

Bu Xiang Feng (monday, 10.40)<br />

Narvik University College, P.O. Box 385, 2 Lodve Langes St., 8505 Narvik, Norway<br />

430492@stu<strong>de</strong>nt.hin.no<br />

Buhmann Martin (saturday, 10.10)<br />

Justus-Liebig-Universität Giessen, Arbeitsgruppe Numerische Mathematik, Mathematisches Institut, Heinrich-<br />

Buff-Ring 44, 35392 Giessen , Germany<br />

buhmann@uni-giessen.<strong>de</strong><br />

Casarubbias Heriberto (monday, 13.10)<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9,<br />

Mexico City, 07738. Mexico<br />

heribertocv@gmail.com<br />

Cervantes-Cabrera Daniel<br />

Unidad <strong>de</strong> Coputo Cientifico DGSCA<br />

UNAM Ciudad Universitaria, Circuto Exterior, Zona Cultural 44510 Mexico D.F.<br />

danielcc@rv.unam.mx<br />

Charleston Sonia (monday, 10.40)<br />

Electrical Engineering Department, 2 Health Science Department, Universidad Autónoma M<strong>et</strong>ropolitana-<br />

Iztapalapa, 09340 Mexico City, México<br />

schv@xanum.uam.mx<br />

Cisneros Hermenegildo (monday, 10.40)<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9,<br />

Mexico City, 07738. Mexico<br />

hcisneros@sagitario.cic.ipn.mx<br />

Cruz Benjamín (monday, 10.40)<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9,<br />

Mexico City, 07738. Mexico<br />

benjamincruz@sagitario.cic.ipn.mx<br />

Cruz Lopez <strong>de</strong> Silanes Maria (friday, 8.00)<br />

Departamento <strong>de</strong> Matemática Aplicada C.P.S., Univ. <strong>de</strong> Zaragoza, María <strong>de</strong> Luna, 3 - 50018 Zaragoza, Spain.<br />

mcruz@posta.unizar.es<br />

Dadourian Karine (monday, 9.40)<br />

<strong>Université</strong> <strong>de</strong> Provence <strong>et</strong> Monitrice à l'<strong>Université</strong> <strong>Pau</strong>l Cézanne. CMI, LATP - IMT/LATP,<br />

39 rue Frédéric Joliot-Curie, 13453 Marseille ce<strong>de</strong>x 13<br />

dadouria@cmi.univ-mrs.fr<br />

Damelin Steven (thursday, 9.50)<br />

Department of Mathematical Sciences, , Georgia Southern University, Postoffice Box 8093, Statesboro, GA<br />

30460-8093, U.S.A.<br />

damelin@georgiasouthern.edu<br />

Dechevsky Lubomir (monday, 8.40)<br />

Narvik University College, P.O. Box 385, 2 Lodve Langes St., 8505 Narvik, Norway<br />

18


Lubomir.T.Dechevsky@hin.no<br />

FalcÓn Luis Eduardo (tuesday, 9.10)<br />

CINVESTAV Av. CientifIca 1145, Colonia el Bajio, 45010 Zapopan, Mexico<br />

lfalcon@gdl.cinvestav.mx<br />

Forca<strong>de</strong>l Nicolas (thursday, 12.50)<br />

Ecole Nationale <strong>de</strong>s Ponts <strong>et</strong> Chaussées, CERMICS, 6 <strong>et</strong> 8 avenue Blaise Pascal, Cité Descartes - Champs sur<br />

Marne, 77455 Marne la Vallée Ce<strong>de</strong>x 2, France<br />

forca<strong>de</strong>l@cermics.enpc.fr<br />

Gibaru Olivier (monday, 8.00)<br />

ENSAM Lille 8 Bd. Louis XIV, 59046 Lille France<br />

Olivier.Gibaru@lille.ensam.fr<br />

Gloria Rafael<br />

Univ. Autonoma M<strong>et</strong>., Iztapalapa Ciencias Basicas e Ingenieria<br />

Ap Post 55-532, C.P. 09340 Mexico, 9340 Mexico D.F. Mexico<br />

Gonzalez-Casanova Pedro (saturday, 10.10)<br />

Unidad <strong>de</strong> Coputo Cientifico DGSCA<br />

UNAM Ciudad Universitaria, Circuto Exterior, Zona Cultural 44510 Mexico D.F.<br />

pedrogc@plecticsdgsca2.unam.mx<br />

Gout Christian (monday 10.40)<br />

<strong>Université</strong> <strong>de</strong> Valenciernnes, LAMAV-ISTV2, Mont Houy, 59313 Valenciennes ce<strong>de</strong>x 9, France<br />

chris_gout@cal.berkeley.edu<br />

Grebennikov Alexan<strong>de</strong>r<br />

Autonomous University of Puebla , Puebla, MÉXICO<br />

agrebe@fcfm.buap.mx<br />

Guerlebeck Klaus (friday, 13.20)<br />

University of Weimar Math. Dpt, Coudraystr.13 99423 Weimar. Germany<br />

klaus.guerlebeck@bauing.uni-weimar.<strong>de</strong><br />

Le Guya<strong>de</strong>r Carole (thursday, 12.20)<br />

INSA <strong>de</strong> Rennes,20 Avenue <strong>de</strong>s Buttes <strong>de</strong> Coësmes, CS 14315, 35043 Rennes Ce<strong>de</strong>x , France<br />

carole.le-guya<strong>de</strong>r@insa-rennes.fr<br />

Hector Juarez Lorenzo Valencia (friday, 9.10)<br />

Departamento <strong>de</strong> Matematicas, Universidad Autonoma M<strong>et</strong>ropolitana-AV. San Rafael 186 Col. Vicentina, 9340<br />

Mexico city, Mexico<br />

hect@xanum.uam.mx<br />

Hernan<strong>de</strong>z Victoria (monday, 9.10)<br />

Instituto <strong>de</strong> Cibern<strong>et</strong>ica, Matematica y Fisica Calle E Nº 309, esquina a 15 - 10400 Vedado 10400 Vedado-La<br />

Habana. Cuba<br />

vicky@ci<strong>de</strong>t.icmf.inf.cu<br />

19


Hoffmann Micklos (monday, 10.10)<br />

Institute of Mathematics and Informatics University of Eger H-3300 Eger Hungary<br />

hofi@gemini.ektf.hu<br />

Juhasz Imre (monday, 10.10)<br />

Institute of Mathematics and Informatics University of Eger H-3300 Eger Hungary<br />

agtji@uni-miskolc.hu<br />

<strong>de</strong> Knock Bram (friday, 12.50)<br />

Department of Mathematical Analysis, Faculty of Engineering, Ghent University, Galglaan 2, 9000 Gent, Belgium<br />

Bram.DeKnock@UGent.be<br />

Kozac Jernej (monday, 10.40)<br />

FMF and IMFM, University of Ljubljana, Jadranska 19, 1000 Ljubljana, Slovenija<br />

Jernej.Kozak@fmf.uni-lj.si<br />

Kunoth Angela (tuesday, 11.30)<br />

Universität Bonn Institut für Angewandte Mathematik , Wegelerstr.6 53115 Bonn. Germany<br />

kunoth@iam.uni-bonn.<strong>de</strong><br />

Lakså Arne (monday, 12.40)<br />

Narvik University College, P.O. Box 385, 2 Lodve Langes St., 8505 Narvik, Norway<br />

Arne.Laksa@hin.no<br />

Leon Diana<br />

Univ. Autonoma M<strong>et</strong>., Iztapalapa Ciencias Basicas e Ingenieria<br />

Ap Post 55-532, C.P. 09340 Mexico, 9340 Mexico D.F. Mexico<br />

Levesley Jeremy (tuesday, 12.10)<br />

Leicester University Department of Mathematics and Computer Science LE1 7RH Leicester. UK<br />

jl1@mcs.le.ac.uk<br />

LÓpez Jesús<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Unidad Profesional Adolfo Lopez Mateos - Col. Nueva Industrial<br />

Vallejo - Delegacion Gustavo A. Ma<strong>de</strong>ro, Mexico City, 07738. Mexico<br />

jesuslrb06@sagitario.cic.ipn.mx<br />

Martinez Ileana<br />

Univ. Autonoma M<strong>et</strong>., Iztapalapa Ciencias Basicas e Ingenieria<br />

Ap Post 55-532, C.P. 09340 Mexico, 9340 Mexico D.F. Mexico<br />

Mhaskar Hrushikesh N. (thursday, 9.20)<br />

Department of Mathematics, California State University, Los Angeles, CA 90032, U. S. A.<br />

hmhaska@calstatela.edu<br />

Mørken Knut (thursday, 13.20)<br />

University of Oslo, Department of Informatics and Center of Mathematics of Applications, PO Box 1053,<br />

Blin<strong>de</strong>rn, Norway.<br />

knutm@ifi.uio.no<br />

Neamtu Mike (friday, 10.20)<br />

Van<strong>de</strong>rbilt University, Dpt of Mathematics, 1326 Stevenson Center, Nashville, TN 37240 USA<br />

neamtu@math.Van<strong>de</strong>rbilt.Edu<br />

20


Pitolli Francesca (monday 13.40)<br />

Univ. "la Sapienza" Roma Via Antonio Scarpa 16, 161 Roma. Italy<br />

pitolli@dmmm.uniroma1.it<br />

Rabinovitch Vladimir<br />

Instituto Politecnico Nacional, Mexico, ESIME Zacatenco, Edif.1, av. IPN, 07738, Mexico<br />

vladimir.rabinovich@gmail.com<br />

Rabut Christophe (monday 10.40)<br />

INSA Toulouse 135 av. <strong>de</strong> Rangueil, 31077 Toulouse ce<strong>de</strong>x4. France<br />

rabut@insa-toulouse.fr<br />

Resendiz Rafael (tuesday, 9.40)<br />

Universidad Autonoma M<strong>et</strong>ropolitana<br />

Ahuizotl 23 Col. Ancon Los Reyes la Paz 56410 Edomex, Mexico<br />

rafael.resendiz@gmail.com<br />

Rossini Milvia (friday, 9.40)<br />

Università di Milano, Dipartimento di Matematica e Applicazioni ,Via R. Cozzi n. 53, 20125 Milano, Italy<br />

rossini@matapp.unimib.it<br />

Saint-Guirons Anne-Gaëlle (monday 10.40)<br />

<strong>Université</strong> <strong>de</strong> <strong>Pau</strong>, Lab. Math. UMR 5142 CNRS - IPRA-Av. <strong>de</strong> l <strong>Université</strong> - BP 1155 , 64018 <strong>Pau</strong> ce<strong>de</strong>x, France<br />

Anne-gaelle.saint-guirons@univ-pau.fr<br />

Schumaker Larry L. (thursday, 8.00)<br />

Van<strong>de</strong>rbilt University, Dpt of Mathematics, 1326 Stevenson Center, Nashville, TN 37240 USA<br />

larry.schumaker@gmail.com<br />

Sommen Frank (friday, 11.40)<br />

Department of Mathematical Analysis, Faculty of Engineering, Ghent University, Galglaan 2, 9000 Gent, Belgium<br />

fs@cage.rug.ac.be<br />

Sossa Azuela Juan Humberto<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Av. Juan <strong>de</strong> Dios Bátiz, S/N Col. Nueva Industrial Vallejo, Mexico<br />

City, 07738. Mexico<br />

hsossa@cic.ipn.mx<br />

Sprößig Wolfgang (tuesday, 10.10)<br />

TU Bergaka<strong>de</strong>mie Freiberg, Fakultät für Mathematik und Informatik, Institut für Angewandte Analysis, 09596<br />

Freiberg, Germany<br />

sproessig@math.tu-freiberg.<strong>de</strong><br />

Steidl Gabriele (saturday, 10.50)<br />

Univ. of Mannheim, Dpt of Mathematics and Computer Science, A5-Room B107, 68131 Mannheim, Germany<br />

steidl@kiwi.math.uni-mannheim.<strong>de</strong><br />

Toscano Karina (saturday 9.40)<br />

Centro <strong>de</strong> Investigación en Computación – IPN, Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9,<br />

Mexico City, 07738. Mexico<br />

likatome@hotmail.com<br />

Traversoni Leonardo (tuesday, 8.40)<br />

21


Univ. Autonoma M<strong>et</strong>. (Iztapalapa Ciencias Basicas e Ingenieria, Ap Post 55-532, C.P. 09340 Mexico, 9340 Mexico<br />

D.F. Mexico<br />

ltd@xanum.uam.mx<br />

Van <strong>de</strong> Voor<strong>de</strong> Liesb<strong>et</strong> (friday, 12.50)<br />

Department of Mathematical Analysis, Faculty of Engineering, Ghent University, Galglaan 2, 9000 Gent, Belgium<br />

Liesb<strong>et</strong>.Van<strong>de</strong>Voor<strong>de</strong>@UGent.be<br />

Vese Luminita (thursday, 11.40)<br />

UC Los Angeles, 405, Hilgard Avenue, Los Angeles, CA 90095-1555, U.S.A.<br />

lvese@ucla.edu<br />

Waldron Shayne (thursday, 10.20)<br />

Department of Mathematics (Rm 410), University of Auckland, 28 Invermay Ave, Private Bag 92019, Auckland,<br />

Sandringham, New Zealand<br />

waldron@math.auckland.ac.nz<br />

Xu Yi (monday, 12.00)<br />

Shanghai Jiaotong University, School of electronic, information and electrical engineering, Institute of Image<br />

communication and information processing, Room 321-323,No. 5 Buliding, school of electronic, information and<br />

electrical engineering,Shanghai Jiaotong Univ, Dongchuan Rd. 800, 200240 Shanghai, China<br />

xuyi@sjtu.edu.cn<br />

22


Computational algebraic geom<strong>et</strong>ry m<strong>et</strong>hods<br />

for curves and surfaces<br />

Rafal Ablamowicz<br />

rablamowicz@tntech.edu<br />

ABSTRACT :<br />

Finding analytic (exact) formulas for parallel lines (envelopes) to<br />

parabolas, ellipses, hyperbolas, and other curves such as, for example, the Bézier<br />

cubic, is of importance in structure engineering and theory of mechanisms.<br />

Likewise, computation of parallel surfaces to the given surface, such, for<br />

example, a non <strong>de</strong>generate quadric, is also of great importance. Polynomials that<br />

implicitly <strong>de</strong>fine parallel lines or surfaces for the given offs<strong>et</strong> to a curve or a<br />

surface can be computed by finding Gröbner bases for suitable elimination<br />

i<strong>de</strong>als of a suitably <strong>de</strong>fined affine vari<strong>et</strong>y. Singularity of the lines parallel to the<br />

conics is discussed and their singular points are explicitly found as functions of<br />

the offs<strong>et</strong> and the param<strong>et</strong>ers of the conic. Critical values of the offs<strong>et</strong> are linked<br />

to the maximum curvature of each conic. This approach can be exten<strong>de</strong>d to<br />

parallel surfaces.<br />

Keywords: Affine vari<strong>et</strong>y, elimination i<strong>de</strong>al, Gröbner basis, homogeneous<br />

polynomial, singularity, family of curves, envelope, pitch curve, un<strong>de</strong>rcutting,<br />

cam surface.


Applications of quaternion wavel<strong>et</strong> transform:<br />

for robotic vision<br />

Eduardo Bayro Corrochano<br />

Eduardo Bayro <br />

Abstract: The QWT using visual cues is applied for 3D reconstruction and<br />

space-time motion coding. This coding can be used by humanoids as a<br />

compresed language for un<strong>de</strong>rstand and mimic human like behaviours.


A local m<strong>et</strong>hod for large<br />

and unevenly distributed data.<br />

MIRA BOZZINI<br />

Università di Milano<br />

Dipartimento di Matematica e Applicazioni<br />

Via R. Cozzi n. 53, 20125 Milano, Italy<br />

In this poster we present a technique based on a local thin plate spline to<br />

recover functions, when the <strong>de</strong>nsity of the data locations presents<br />

discontinuoties or steep gradients.


Some formal aspects and applications<br />

of Cartan – Dieudonné theorem<br />

Benjamín Cruz, Ricardo Barrón, Jesús López & Humberto Sossa<br />

Centro <strong>de</strong> Investigación en Computación – IPN<br />

Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9<br />

Mexico City, 07738. MEXICO<br />

E-mails: benjamincruz@sagitario.cic.ipn.mx, rbarron@cic.ipn.mx,<br />

jesuslrb06@sagitario.cic.ipn.mx ,hsossa@cic.ipn.mx<br />

Abstract<br />

One of the most important results in the area of Eucli<strong>de</strong>an geom<strong>et</strong>ry, about Eucli<strong>de</strong>an<br />

movements, is Cartan – Dieudonné theorem, Eucli<strong>de</strong>an movements in n -dimensional<br />

Eucli<strong>de</strong>an space are split in a certain number of reflections from hyperplanes of Eucli<strong>de</strong>an<br />

space itself.<br />

This theorem is as follows: Any orthogonal transformation in a lineal space of n -<br />

dimension can be performed at most by n single reflections.<br />

There are several proofs of this theorem, however only in some of them we find elements<br />

that allow us to achieve a practical calculus algorithm. In this work one of these proofs is<br />

studied and some formal steps that are important to base the proof are ad<strong>de</strong>d, these steps<br />

show us the power of Geom<strong>et</strong>ric Algebra as for simplicity and range.<br />

It is important to point out the role this theorem plays in practical applications like<br />

factorization of operators of movements and interpolation in virtual spaces generation,<br />

computer vision and graphics.<br />

In this paper besi<strong>de</strong>s formal aspects of the theorem, we show an algorithm and practical<br />

applications itself.


Variational calculus and multigrid dynamical programming<br />

on expo-rational surfaces and volume <strong>de</strong>formations:<br />

theory and applications<br />

Lubomir T. Dechevsky, Børre Bang, Xian Feng Bu, Arne Lakså<br />

Narvik University College, NORWAY<br />

In [1] and [2] we consi<strong>de</strong>red a vari<strong>et</strong>y of problems of variational calculus and optimal<br />

control theory with applications to geom<strong>et</strong>ric mo<strong>de</strong>lling with param<strong>et</strong>ric curves,<br />

surfaces, volume <strong>de</strong>formations and higher dimensional manifolds. As a numerical<br />

m<strong>et</strong>hod for approximate computation of the extremals, we proposed a fast multigrid<br />

dynamical programming algorithm. In [1] we used this m<strong>et</strong>hod for the fast<br />

computation of geo<strong>de</strong>sics on param<strong>et</strong>ric surfaces, and Section 7 of [1] contains a<br />

<strong>de</strong>tailed comparison of this algorithm with current state-of-the-art m<strong>et</strong>hods for exact<br />

and approximate computation of geo<strong>de</strong>sics on triangulated surfaces, as <strong>de</strong>scribed in<br />

[4] and the references therein. We pointed out that the algorithm from [1] has<br />

numerous significant advantages compared to the m<strong>et</strong>hods discussed in [4]. In the<br />

present communication we continue this analysis in the case when the original surface<br />

is approximated (by interpolation or by fitting) with an expo-rational surface (see [3]).<br />

We show that when the expo-rational interpolation is of Lagrange type, the algorithm<br />

from [1] emulates an enhanced version of the m<strong>et</strong>hods on triangulated surfaces. In the<br />

expo-rational s<strong>et</strong>ting it is very easy to upgra<strong>de</strong> the Lagrange interpolation to Hermite<br />

interpolation, whereby the extremal for the smooth Hermite expo-rational surface can<br />

be obtained as a small perturbation of the extremal for triangulated surfaces<br />

corresponding to Lagrange expo-rational approximation. In this presentation we shall<br />

<strong>de</strong>monstrate also several other ‘superproperties’ of the expo-rational B-splines in<br />

relevance to multidimensional variational and optimal-control problems with<br />

application to CAGD. One of the most important of these ‘superproperties’ is the ease<br />

of upgrading of the algorithm of [1] to higher dimensional manifolds (e.g., from<br />

geo<strong>de</strong>sics on surfaces to geo<strong>de</strong>sics in volume <strong>de</strong>formations and higher-dimensional<br />

vector-fields), while an analogous upgra<strong>de</strong> of the m<strong>et</strong>hods consi<strong>de</strong>red in [4] would be<br />

very cumbersome and labour-consuming, to the point of being beyond feasibility.<br />

References:<br />

[1] L. T. Dechevsky, L. M. Gulliksen. A multigrid dynamical programming algorithm<br />

for discr<strong>et</strong>e dynamical systems and its applications to numerical computation of<br />

global geo<strong>de</strong>sics. Int. J. Pure Appl. Math. (ISSN 1311-8080) 33(2) (2006) 257-285.<br />

[2] L. T. Dechevsky, L. M. Gulliksen. Application of a multigrid dynamical<br />

programming algorithm to optimal param<strong>et</strong>rization, and a mo<strong>de</strong>l solution of an<br />

industrial problem. Int. J. Pure Appl. Math. (ISSN 1311-8080) 33(3) (2006) 381-406.<br />

[3] L. T. Dechevsky, A. Lakså, B. Bang. Expo-rational B-splines. Int. J. Pure Appl.<br />

Math. (ISSN 1311-8080) 27(3) (2006) 319-367.<br />

[4] V. Surazhsky, T. Surazhsky, D. Kirsanov, S. J. Gortler, H. Hoppe. Fast exact and<br />

approximate geo<strong>de</strong>sics on meshes. ACM Transactions on Graphics (ISSN 0730-0301)<br />

4(3) (2005) 553-560.


Radial Basis Function Interpolants with Param<strong>et</strong>ers<br />

Martin Buhmann, University of Giessen, Germany<br />

Abstract<br />

A major tool for multivariate approximations by interpolation and other means is the m<strong>et</strong>hod<br />

of radial basis functions. Using the well-known radial basis functions such as Gaussians or multiquadrics<br />

and its generalisations has many advantages such as well-posedness of the interpolation<br />

problem in high dimensions and fast convergence, with little or no conditions on the geom<strong>et</strong>ry of<br />

the data points. These radial basis functions are extremely popular with engineering and other<br />

applications.<br />

√<br />

However, many radial basis functions have param<strong>et</strong>ers, such as the param<strong>et</strong>er c ∈ Φ(r) =<br />

r 2 + c 2 or Φ(r) =exp−c 2r2 , and especially in the numerical solution of the interpolation problems,<br />

conditioning problems arise if the param<strong>et</strong>ers tend to zero or infinity. Changing these<br />

param<strong>et</strong>ers can be very important in practical applications, and although they will never tend to<br />

infinity in applications, large param<strong>et</strong>ers may be nee<strong>de</strong>d. As for example Fornberg and Larsson<br />

and collaborators noticed, sensible limits of the interpolating functions as a whole can som<strong>et</strong>imes<br />

be i<strong>de</strong>ntified and computed even in these difficult cases. This is the main theme we wish to discuss<br />

in this talk and present results with have been found in collaboration with Dinew.


Using cubic spline for the velocity<br />

planning in mobile robots<br />

Heriberto Casarrubias, Humberto Sossa, Ricardo Barrón<br />

Centro <strong>de</strong> Investigación en Computación – IPN<br />

Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9<br />

Mexico City, 07738. MEXICO<br />

E-mails: heribertocv@gmail.com, hsossa@cic.ipn.mx, rbarron@cic.ipn.mx,<br />

Abstract<br />

The velocity regulation for a mobile robot is a problem of visual control that allows it to<br />

travel complex trajectories and eva<strong>de</strong> obstacles and achieve objectives even if they are in<br />

movement. In this work shows how to use the cubic splines to control the position,<br />

orientation, and velocity of a differential mobile robot got no<strong>de</strong>s from an image, being careful<br />

of the kinematic constraints.<br />

Also practical applications and results are showed.


Forward and Inverse Problems for D<strong>et</strong>ermining Computer Simulated Respiratory<br />

Sound Sources<br />

S. Charleston-Villalobos 1 , J. Cruz-García 1 , R. González-Camarena 2 , T. Aljama-Corrales 1<br />

1<br />

Electrical Engineering Department, 2 Health Science Department,<br />

Universidad Autónoma M<strong>et</strong>ropolitana-Iztapalapa, 09340 Mexico City, México<br />

Pulmonary auscultation represents a common clinical procedure to discover and to track<br />

respiratory diseases by the analysis of breathing sounds (BS) through physician’s ear. Lung<br />

structural and functional changes due to pathologies lead up to changes in sounds<br />

production and transmission, acoustical information that could be useful for clinical<br />

diagnosis. Regarding these aspects, several efforts have been ma<strong>de</strong> to <strong>de</strong>termine the sites of<br />

production of inspiratory and expiratory BS as well as lung acoustic characteristics using<br />

mainly experimental protocols, sound speed measurements and acoustic mo<strong>de</strong>ls. The<br />

findings were compatible with the i<strong>de</strong>a of a central origin for expiratory BS while flow<br />

turbulence seems to be the mechanism of origin. Possibly both, the expiratory and<br />

inspiratory sounds, have a multi-centre origin. Concerning BS speed and transmission in<br />

lung, different works have established that possibly BS travels in part through airways and,<br />

in part through lung parenchyma. In fact, lung parenchyma constitutes 90% of the total<br />

volume of the lung and at frequencies below the audible range, the parenchyma could be<br />

consi<strong>de</strong>red as a medium composed of bubbles in a fluid, i.e., a homogeneous mixture<br />

capable of sound attenuation by thermal losses.<br />

All previous efforts attempt to solve in certain way the forward and inverse problems<br />

but just recently the localization of BS sources has been established through the solution of<br />

a formal inverse problem. However, several factors affect the estimated sources. Among<br />

them, the numerical algorithm to provi<strong>de</strong> the solution, the transfer function, the number of<br />

measurements taken into account (or microphones used), the sources <strong>de</strong>pth and, the<br />

measurement noise. In the present work, we present preliminary results to the solution of<br />

the BS inverse problem establishing firstly, the forward problem in terms of a priori<br />

information and secondly, evaluating the performance of three inverse linear solution<br />

algorithms consi<strong>de</strong>ring the effect of the some of the mentioned factors, by a systematic<br />

study in computer simulated scenarios.<br />

Three different algorithms were analyzed and compared: Over<strong>de</strong>termined Least-Square<br />

(LSIS), Un<strong>de</strong>r<strong>de</strong>termined Minimum Norm (MNIS) and Focal Un<strong>de</strong>r<strong>de</strong>termined System<br />

Solution (FOCUSS). Besi<strong>de</strong>s visual evaluation of estimated sources, the algorithms<br />

performance was numerically assessed by MSE. Computer simulations inclu<strong>de</strong>d the<br />

estimation of single and multiples sources as well as the study of the influence of source<br />

<strong>de</strong>pth, number of microphones, and thoracic volume discr<strong>et</strong>isation on the inverse solution.<br />

In particular, for multiple single and non-single point RS sources. Overall, our results<br />

suggest that the FOCCUS algorithm performed b<strong>et</strong>ter than the LSIS and the MNIS, as it<br />

provi<strong>de</strong>d more a<strong>de</strong>quate solutions for shape, number, amplitu<strong>de</strong> and position of sound<br />

sources, in 3D space. Furthermore, FOCCUS required less number of sensors and it was<br />

less affected by volume discr<strong>et</strong>isation.


Isolated character recognition by using Support<br />

Vector Machines with a kernel of Radial Base<br />

Hermenegildo Cisneros, Ricardo Barrón, Benjamín Cruz<br />

Centro <strong>de</strong> Investigación en Computación – IPN<br />

Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9<br />

Mexico City, 07738. MEXICO<br />

E-mails: hcisneros@sagitario.cic.ipn.mx, rbarron@cic.ipn.mx, benjamincruz@sagitario.cic.ipn.mx<br />

Abstract<br />

In this work, we present a combination of techniques for the recognition of isolated<br />

hand-written characters. We <strong>de</strong>scribe a way to obtain the feature vector that allow us to<br />

<strong>de</strong>scribe an isolated character. Flusser invariant moments and other geom<strong>et</strong>ric measures are<br />

combined as objects <strong>de</strong>scriptors. We implement an off-line system. We use the so-called<br />

Support Vector Machines Multi-class [SVM] with a kernel of radial base as the main<br />

classifiers. Its know that radial base functions can interpolate and smooth functions, they can<br />

outline in an efficient way the boundary b<strong>et</strong>ween the classes, and precisely by this reason we<br />

propose to use in this work. Some experiments and results are showed.


An extension of a bound for functions in Sobolev spaces<br />

and its application to (m, s)–spline interpolation and smoothing<br />

Arcangéli, Rémi 1 ; López <strong>de</strong> Silanes, María Cruz 2 ; Torrens, Juan José 3<br />

1 Route <strong>de</strong> Barat, 31160 Arbas, France<br />

2 Depto. <strong>de</strong> Matemática Aplicada, CPS, Universidad <strong>de</strong> Zaragoza, 50018 Zaragoza, Spain<br />

3 Depto. <strong>de</strong> Ingeniería Matemática e Informática, Universidad Pública <strong>de</strong> Navarra, 31006 Pamplona, Spain<br />

L<strong>et</strong> f be a function <strong>de</strong>fined over a boun<strong>de</strong>d open subs<strong>et</strong> Ω of R n with a Lipschitz–continuous boundary.<br />

In this talk, we present a Sobolev bound involving the values of f at finitely many points of Ω. This<br />

result extends those obtained by H. Wendland and co–workers (cf. [9, 11]).<br />

We then apply the Sobolev bound to <strong>de</strong>rive error estimates for interpolating and smoothing (m, s)–splines<br />

(cf. [3, 1]). For interpolating (m, s)–splines, these results generalize those given by various authors (cf.,<br />

for example, [4, 7, 12, 6, 5, 9]). For smoothing (m, s)–splines, we first consi<strong>de</strong>r the case of exact data.<br />

We pay special attention to the behaviour of these splines according to the smoothing param<strong>et</strong>er ε and<br />

the number N of data. These results generalize those given by various authors (cf. [7, 11, 10]).<br />

Finally, we consi<strong>de</strong>r the problem of noisy data. Then, in the stochastic case of data perturbed by a<br />

noise, un<strong>de</strong>r a classic random noise hypothesis, we give error estimates in the sense of mathematical<br />

expectation, for the smoothing D m –splines (the particular case s = 0), which improve previous results<br />

by various authors (cf. [10, 8, 2]).<br />

References<br />

[1] R. Arcangéli, M. C. López <strong>de</strong> Silanes, and J. J. Torrens. Multidimensional Minimizing Splines.<br />

Kluwer Aca<strong>de</strong>mic Publishers, Dordrecht, 2004.<br />

[2] R. Arcangéli and B. Ycart. Almost sure convergence of smoothing D m –splines for noisy data. Numer.<br />

Math., 66:281–294, 1993.<br />

[3] J. Duchon. Splines minimizing rotation–invariant semi–norms in Sobolev spaces. Lectures Notes<br />

Math., 571:85–100, 1977.<br />

[4] J. Duchon. Sur l’erreur d’interpolation <strong>de</strong>s fonctions <strong>de</strong> plusieurs variables par les D m –splines.<br />

RAIRO Anal. Numer., 12(4):325–334, 1978.<br />

[5] M. J. Johnson. An error analysis for radial basis function interpolation. Numer. Math., 98:675–694,<br />

2004.<br />

[6] W. Light and H. Wayne. On power functions and error estimates for radial basis function interpolation.<br />

J. Approx. Theory, 92:245–266, 1998.<br />

[7] M. C. López <strong>de</strong> Silanes and R. Arcangéli. Estimations <strong>de</strong> l’erreur d’approximation par splines<br />

d’interpolation <strong>et</strong> d’ajustement d’ordre (m, s). Numer. Math., 56:449–467, 1989.<br />

[8] M. C. López <strong>de</strong> Silanes and R. Arcangéli. Sur la convergence <strong>de</strong>s D m –splines d’ajustement pour <strong>de</strong>s<br />

données exactes ou bruitées. Rev. Mat. Univ. Complut. Madrid, 4(2–3):279–294, 1991.<br />

[9] F. J. Narcowich, J. D. Ward and H. Wendland. Sobolev bounds on functions with scattered zeros,<br />

with applications to radial basis fuction surface fitting. Math. Comp., 74:743–763, 2005.<br />

[10] F. Utreras. Convergence rates for multivariate smoothing spline functions. J. Approx. Theory, 52:1–<br />

27, 1988.<br />

[11] H. Wendland and C. Rieger. Approximate interpolation with applications to selecting smoothing<br />

param<strong>et</strong>ers. Numer. Math., 101:643–662, 2005.<br />

[12] Z. M Wu and R. Schaback. Local error estimates for radial basis function interpolation to sacattered<br />

data. IMA J. Numer. Anal., 13:13–27, 1993.


Analysis of some bivariate non-linear interpolatory subdivision<br />

schemes and associated multiresolution<br />

K. Dadourian ∗ , J. Liandrat<br />

February 20, 2007<br />

For linear subdivision schemes or multiresolution analyses, generalisation from univariate to<br />

multivariate framework can be performed easily by tensorial product. In<strong>de</strong>ed, tensorial product<br />

of univariate limit (or scaling) functions provi<strong>de</strong> the limit (or scaling) function in the multivariate<br />

framework.<br />

This work is <strong>de</strong>voted to non linear subdivision schemes and associated multiresolution transforms<br />

<strong>de</strong>rived by tensor product of some univariate non linear schemes. More precisely, we consi<strong>de</strong>r<br />

univariate subdivision schemes S NL that can be written as a perturbation of a linear convergent<br />

scheme S as:<br />

∀f ∈ l ∞ ,S NL (f) = S(f) + F(δ(f)),<br />

where the perturbation F is a non linear operator and δ is a linear continuous operator (for example<br />

δf = d k f where df = (f n+1 − f n )).<br />

In [1], it has been shown that un<strong>de</strong>r natural conditions on F, δ and S, the subdivision scheme<br />

S NL is convergent and stable as well as the associated multiresolution.<br />

Here we analyse the bivariate scheme obtained by iterating alternatively on lines and rows the<br />

non linear univariate scheme. Results on convergence and stability will be shown. Our results are in<br />

agreements with the performances of non linear schemes like WENO or PPH for image processing<br />

([3], [2]).<br />

References<br />

[1] Amat, S., K. Dadourian and J. Liandrat, Analysis of a class of subdivision schemes and<br />

associated non-linear multiresolution transforms, submitted.<br />

[2] Amat, S., R. Donat, J. Liandrat and J. C. Trillo, Analysis of a new non-linear subdivision<br />

scheme: applications in image processing, Foundations of Computational Mathematics 225<br />

(2005), 193–225.<br />

[3] Cohen, A., N. Dyn and B.Matei, Quasi linear subdivision schemes with applications to ENO<br />

interpolation, Applied and Computational Harmonic Analysis 15 (2003), 89–116.


Numerical integration, Energy and Discrepancy on Compact<br />

Homogenous manifolds.<br />

Abstract:<br />

Dr Steven Damelin<br />

In this talk, we will review a program of research of the author and his collaborators on<br />

numerical integration estimates on compact homogenous spaces in terms of energy criteria.<br />

Even for the sphere, our approach is compl<strong>et</strong>ely new. This is joint work with P<strong>et</strong>er Grabner<br />

(Graz), Levesley (Leicester), Sun (Missouri) and Hinkernell (IIT)<br />

Dr Steven Damelin<br />

Work Address:<br />

Department of Mathematical Sciences,<br />

Georgia Southern University, Postoffice Box 8093,<br />

Statesboro, GA 30460-8093, U.S.A.


Expo-rational B-splines of a complex variable and their<br />

applications<br />

Lubomir T. Dechevsky<br />

Narvik University College<br />

I begin by introducing the several possible <strong>de</strong>finitions of multivariate ERBS (exporational<br />

B-splines, as introduced in [1]) and then concentrate on the bivariate case and<br />

its translation into complex-variable language. I consi<strong>de</strong>r several applications of the<br />

ERBS of a complex variable. In particular, if the spectrum of a compact operator<br />

acting on a Banach space be triangulated (as scattered point s<strong>et</strong> in the plane), then a<br />

minimally supported infinitely smooth ERBS-based partition of unity can be<br />

constructed. This allows explicit computation of the Cauchy-Riesz-Dunford integral<br />

representation of analytic functions of this compact operator. One application of this<br />

is for <strong>de</strong>riving sharp estimates of the norms of operator resolvents. Another<br />

application is the possibility to param<strong>et</strong>rize the auto-diffeomorphisms on the unit ball<br />

in the N-dimensional Eucli<strong>de</strong>an space. When N is 2 or 3, this has important<br />

applications to registration problems in brain imaging and other applications relevant<br />

to computer tomography.<br />

Reference:<br />

[1] L. T. Dechevsky, A. Lakså, B. Bang. Expo-rational B-splines. Int. J. Pure Appl.<br />

Math. (ISSN 1311-8080) 27(3) (2006) 319-367.


Radon transform and harmonical analysis for 3D<br />

motion estimation using robot omnidirectional vision<br />

Luis Eduardo Falcon<br />

and<br />

Eduardo Bayro-Corrochano<br />

edb@gdl.cinvestav.mx<br />

Abstract:<br />

Since images taken by omnidirectional sensors can be mapped to the sphere, the<br />

problem to estimate the 3D rotation of a camera can be treated as a problem of<br />

estimating rotations b<strong>et</strong>ween spherical images. In recent years harmonic<br />

analysis has been used in computer vision to obtain 3D rotations with the Radon<br />

and Hough transform, evaluating the Fourier transform on the unit sphere S2<br />

and on the rotation group SO(3). In particular, we used the Radon transform on<br />

the space of lines of the omninidrectional images, to recover the relative<br />

position b<strong>et</strong>ween two cameras.


IMAGE SEGMENTATION USING A<br />

GENERALIZED FAST MARCHING METHOD<br />

Nicolas Forca<strong>de</strong>l 1 , Carole Le Guya<strong>de</strong>r 2 and Christian Gout 3,4<br />

1<br />

: Ecole Nationale <strong>de</strong>s Ponts <strong>et</strong> Chaussées<br />

CERMICS, 6 <strong>et</strong> 8 avenue Blaise Pascal<br />

Cité Descartes - Champs sur Marne<br />

77455 Marne la Vallée Ce<strong>de</strong>x 2, France<br />

2<br />

: INSA <strong>de</strong> Rennes<br />

20 Avenue <strong>de</strong>s Buttes <strong>de</strong> Coësmes, CS 14315<br />

35043 Rennes Ce<strong>de</strong>x , France<br />

3 : <strong>Université</strong> <strong>de</strong> Valenciennes<br />

LAMAV - ISTV2, Le Mont Houy<br />

59313 Valenciennes ce<strong>de</strong>x 9, France<br />

4 : INRIA Futurs MAGIQUE 3D<br />

<strong>Université</strong> <strong>de</strong> <strong>Pau</strong>, IPRA, UMR Math CNRS 5142<br />

Av. <strong>de</strong> l’<strong>Université</strong>s, BP 1155<br />

64013 <strong>Pau</strong> ce<strong>de</strong>x, France<br />

Abstract :<br />

In previous work, Carlini <strong>et</strong> al. (2005& 2006) have introduced a new Fast<br />

Marching algorithm for a non-convex eikonal equation mo<strong>de</strong>ling front evolutions in<br />

the normal direction. The algorithm corresponds to extension of the Fast Marching<br />

<strong>de</strong>veloped by S<strong>et</strong>hian (1996).<br />

After a presentation of this new m<strong>et</strong>hod, we propose to <strong>de</strong>velop & integrate it<br />

for some applications in image segmentation.<br />

We give the mo<strong>de</strong>lling and some theor<strong>et</strong>ical results of this approach, its<br />

discr<strong>et</strong>ization is given, and we present numerical examples to show the potentiality of<br />

this novel m<strong>et</strong>hod.<br />

References :<br />

E. Carlini, M. Falcone, N. Forca<strong>de</strong>l, R. Monneau, Convergence of a Generalized Fast<br />

Marching M<strong>et</strong>hod for a non-convex eikonal equation, 2006.<br />

E. Carlini, E. Cristiani, N. Forca<strong>de</strong>l, A non-monotone Fast Marching scheme for a Hamilton-<br />

Jacobi equation mo<strong>de</strong>ling dislocation dynamics, Numerical Mathematics and Advanced<br />

Applications Proceedings of ENUMATH 2005, Santiago <strong>de</strong> Compostela, Spain, July 2005<br />

Berm<strong>de</strong>z <strong>de</strong> Castro, A.; Gmez, D.; Quintela, P.; Salgado, P. (Eds.).<br />

J. A. S<strong>et</strong>hian, Level S<strong>et</strong> M<strong>et</strong>hods and Fast Marching M<strong>et</strong>hods: Evolving Interfaces in<br />

Computational Geom<strong>et</strong>ry, Fluid Mechanics, Computer Vision, Computer-Ai<strong>de</strong>d Design,<br />

Optimal Control and Material Sciences , Broché, 2 nd Edition, 1999.


C 1 and C 2 -continuous polynomial param<strong>et</strong>ric L p splines (p ≥ 1)<br />

P. Auquiert (1) ,O.Gibaru (2) ,E.Nyiri (2)<br />

(1) (LAMAV) <strong>Université</strong> <strong>de</strong> Valenciennes <strong>et</strong> du Hainaut-Cambrésis<br />

Le Mont Houy, F-59313 Valenciennes ce<strong>de</strong>x 9<br />

(2) (L2MA) C.E.R. Ecole Nationale Supérieure d’Arts <strong>et</strong> Métiers <strong>de</strong> Lille<br />

8 Bld Louis XIV, F-59046 Lille Ce<strong>de</strong>x<br />

We introduce L p (1 ≤ p ≤∞) piecewise polynomial param<strong>et</strong>ric splines of <strong>de</strong>gree 3 or 5 which<br />

smoothly interpolate data points. The coefficients of these polynomial splines are calculated by<br />

minimizing the L p norm of the second <strong>de</strong>rivative. We <strong>de</strong>monstrate that the C 1 -continuous cubic<br />

(resp. G 1 -continuous cubic and C 2 -continuous quintic) L p polynomial splines are unique for<br />

1


A Dynamical No<strong>de</strong> Adaptive RBF M<strong>et</strong>hod<br />

to Solve PDE Problems.<br />

Pedro González-Casanova 1 ; José Antonio Muñoz Gómez 2 and Gustavo Rodríguez<br />

Gómez 2 .<br />

The numerical approximation of PDE problems whose solution presents sharp<br />

gradients is a difficult task. This is particularly true when large real life problems are<br />

consi<strong>de</strong>red. Some algorithms have appeared in the radial basis functions literature<br />

to <strong>de</strong>al with this problem. In this work, we purpose a new RBF algorithm -based on<br />

Kansa’s radial basis functions unsymm<strong>et</strong>ric collocation m<strong>et</strong>hod-, which combines a<br />

local no<strong>de</strong> adaptive technique with a domain <strong>de</strong>composition m<strong>et</strong>hod. Specifically, a<br />

no<strong>de</strong> refinement technique based on local error interpolation estimates and a<br />

quad-tree type algorithm is formulated. This m<strong>et</strong>hod is then further combined with a<br />

multiplicative Schwarz domain <strong>de</strong>composition technique with overlapping regions.<br />

The refinement strategy is <strong>de</strong>signed to keep the load balance in each subdomain.<br />

This objective is achieved by dynamically adapting the number of subdomains in<br />

accordance with the knot insertion-remotion technique. Numerical results applied<br />

to stationary partial differential equations in two dimensions, shows that the<br />

dynamic partition of data, combined with the domain <strong>de</strong>composition m<strong>et</strong>hod,<br />

reduce the computational cost and can be used to solve problems with a large<br />

number of no<strong>de</strong>s.<br />

1 Unidad <strong>de</strong> Investigación En Computo Aplicado, DGSCA, Universidad Nacional<br />

Autónoma <strong>de</strong> México, D. F, México.<br />

2 Ciencias Computacionales, Instituto Nacional <strong>de</strong> Óptica y Electrónica (INAOE), Puebla<br />

Tonanzintla, México.


Geo<strong>de</strong>sic active contour un<strong>de</strong>r geom<strong>et</strong>rical conditions:<br />

Theory and 3D Applications<br />

Christian Gout §,$ and Carole Le Guya<strong>de</strong>r ♥ .<br />

§ :INSA<strong>de</strong>Rouen<br />

Laboratoire <strong>de</strong> Mathématiques <strong>de</strong> l’INSA<br />

Place Emile Blon<strong>de</strong>l, BP 08<br />

76 131 Mont-Saint-Aignan ce<strong>de</strong>x, France.<br />

chris gout@cal.berkeley.edu.<br />

$ :<strong>Université</strong> <strong>de</strong> Valenciennes - LAMAV-ISTV2<br />

Mont Houy, 59313 Valenciennes ce<strong>de</strong>x 9, France<br />

♥ : INSA <strong>de</strong> Rennes<br />

Centre <strong>de</strong> Mathématiques <strong>de</strong> l’INSA<br />

20, Avenue <strong>de</strong>s Buttes <strong>de</strong> Coësmes, CS 14315<br />

35043 Rennes ce<strong>de</strong>x, France<br />

carole.le-guya<strong>de</strong>r@insa-rennes.fr<br />

Abstract:<br />

We will first give a survey of some m<strong>et</strong>hods we have <strong>de</strong>veloped for image segmentation<br />

un<strong>de</strong>r geom<strong>et</strong>rical constraints.<br />

We then propose a new scheme for both <strong>de</strong>tection of boundaries and fitting of geom<strong>et</strong>rical<br />

data based on a geom<strong>et</strong>ric partial differential equation, which allows for a rigorous<br />

mathematical analysis. The mo<strong>de</strong>l is a geo<strong>de</strong>sic-active-contour-based mo<strong>de</strong>l, in which we<br />

are trying to <strong>de</strong>termine a curve that best approaches the given geom<strong>et</strong>rical conditions (for<br />

instance a s<strong>et</strong> of points or curves to approach) while <strong>de</strong>tecting the object un<strong>de</strong>r consi<strong>de</strong>ration.<br />

Formal results concerning existence, uniqueness (viscosity solution) and stability are<br />

presented as well. We give the discr<strong>et</strong>ization of the m<strong>et</strong>hod using an Additive Operator<br />

Splitting scheme which is very efficient for this kind of problem. We also give numerical<br />

examples on 3D real data s<strong>et</strong>s.<br />

Key words: Geo<strong>de</strong>sic active contours, Level s<strong>et</strong> m<strong>et</strong>hod, viscosity solution, approximation<br />

of points.<br />

AMS classification: 35XX, 49L25, 74G65, 65D18, 53A10, 68U10.


ROTATING PROJECTION ALGORITHM OF IMAGE RECONSTRUCTION<br />

AND APPLICATION FOR COMPUTER TOMOGRAPHY<br />

Alexan<strong>de</strong>r Grebennikov , J. G. Vázquez Luna, T. Valencia Perez, M. Najera Enriquez<br />

Autonomous University of Puebla , Puebla, MÉXICO<br />

agrebe@fcfm.buap.mx<br />

ABSTRACT<br />

We consi<strong>de</strong>r the problem of the image reconstruction of the structure, consisting of the component<br />

with different characteristics, un<strong>de</strong>r the influence of the known external physical field. The image of the<br />

distribution of these characteristics is <strong>de</strong>scribed insi<strong>de</strong> the space domain Ω with by some<br />

function g( x, y, z ) that must be reconstructed based on indirect boundary observations. This problem can<br />

be resolved by tomography that corresponds to the used external field. There are some tomographies such<br />

as electrical, infrared, acoustic, Roentgen (radiography), <strong>et</strong>c. [1], [2]. The traditional approach requires<br />

scanning the object and calculating the inversion of the Radon transform. It seems necessary for difficult<br />

structures and can be realized in sufficiently fast manner. But som<strong>et</strong>imes the investigating object has the<br />

simple structure, so its reconstruction consists only in localization of some elements with different<br />

characteristic insi<strong>de</strong> of the homogeneous (or quasi homogeneous) region. In [3] it was proposed the<br />

simplified variant of scanning algorithm without application of the inverse Radon transform. We call it as<br />

“Rotating Projection” algorithm. In [3] this algorithm was applied for electric tomography. Here we use<br />

this i<strong>de</strong>a and <strong>de</strong>velop the approach for abstract computer tomography.<br />

We explain the i<strong>de</strong>a of this algorithm in the simplest plane case for one element to be localized.<br />

Suppose that we know values of function ν ( p, ϕ ) (projections) which characterizes the intensiveness of<br />

passed through the object rays for some fixed angles ϕ and all linear coordinates p of scanning. By<br />

another words, we know for some fixed angles ϕ i , i = 1,..., n corresponding number of one dimensional<br />

images (projections) as functions of one variable p.<br />

We need the next steps.<br />

1. Prolongation on a plane of calculated projections ν ( p, ϕ i ) for every p along the direction,<br />

corresponding to angleϕ i , to obtain the exten<strong>de</strong>d two dimensional image.<br />

2. Rotation, i.e., changing number i (scanning for different ϕ ) of prolonged projections and localization<br />

of the areas of intersection of projections with the same values.<br />

If we do not interesting in the exact geom<strong>et</strong>rical form of the element and want to localize it as a<br />

rectangle, it is sufficient [4] to use n=2.<br />

We <strong>de</strong>veloped the explained scheme for the space (three dimensional) case to localize some point<br />

wise elements and continuous objects, constructed corresponding algorithm and computer programs in<br />

MATLAB system and justified these programs by a lot of numerical mo<strong>de</strong>l experiments.<br />

One of the important applications of constructed algorithm and programs was realized by authors for<br />

the medicine diagnostics of cancer of the female bosom. In this case it is important to reduce the time of<br />

the radiation treatment in the tomography process, by other words – to reduce the number of angles of<br />

scanning. The special algorithms of data pre-processing were <strong>de</strong>veloped also for reducing real data for<br />

the simplified form consi<strong>de</strong>red above. This part of investigations was realized in the frame of the Project<br />

No SALUD 2004-01-021, supported by SSA/IMSS/ISSSTE-CONACYT of Mexico.<br />

REFERENCES<br />

1. R.A. Williams and M.S. Beck, Process Tomography: Principles, Techniques and Applications.<br />

Butterworth-Heinemann, Oxford, 1995.<br />

2. M.S. Beck and B.H. Brown, Process tomography: a European innovation and its application.<br />

Measurement Science and Technology, 7, 215–224 (1996).<br />

3. A. Grebennikov, J. G. Vázquez Luna, M. A. Cruz Gama, Fast Linear Algorithms for Image<br />

Processing in Electric Tomography. III Taller Internacional sobre Física Aplicada. La Habana,<br />

Noviembre 30 – Diciembre 3, 2004.<br />

4. G. Germen, Reconstruction of images using projections. Moscow, Mir, 1983.


On monogenic approximations of solutions of the Lamé system<br />

K.Gürlebeck<br />

Abstract: The talk begins with a short introduction to the function theory of quaternion-valued<br />

monogenic functions. Basic i<strong>de</strong>as of the construction of polynomial basis systems will be<br />

briefly explained. We will then focus to the <strong>de</strong>rivatives and primitives of such basis functions.<br />

To approximate also solutions with singularities like cracks we will <strong>de</strong>fine systems of rational<br />

monogenic functions. All this will then be applied to construct spatial generalizations of the<br />

well-known Kolossov-Muschelishvili formulas from the plane case of linear elasticity.


Self-repelling snakes for topology-preserving<br />

segmentation mo<strong>de</strong>ls.<br />

by<br />

Carole Le Guya<strong>de</strong>r (INSA <strong>de</strong> Rennes, France)<br />

and<br />

Luminita Vese. (UC Los Angeles, USA)<br />

The implicit framework of the level s<strong>et</strong> m<strong>et</strong>hod has proved to be very powerful in<br />

tracking propagating fronts. In<strong>de</strong>ed, the evolving contour is embed<strong>de</strong>d in a higherdimensional<br />

level s<strong>et</strong> function and its evolution can be phrased in terms of an Eulerian<br />

formulation.<br />

The ability of this mo<strong>de</strong>lling to handle topological changes, its being param<strong>et</strong>er-free<br />

and intrinsic make it useful in a wi<strong>de</strong> range of fields and particularly in image segmentation.<br />

Nevertheless, in some applications, this topological flexibility turns out to be un<strong>de</strong>sirable, for<br />

instance when the shape to be <strong>de</strong>tected has a known topology, when the resulting shape must<br />

be homeomorphic to the initial one.<br />

Thus we propose in this talk a segmentation mo<strong>de</strong>l which preserves topology and<br />

which is based on an implicit formulation and on the geo<strong>de</strong>sic active contours. Experimental<br />

results on various synth<strong>et</strong>ic and real images in 2 or 3 dimensions will be given.


Numerical Simulation of a Viscous Pump by a High Or<strong>de</strong>r Finite<br />

Element M<strong>et</strong>hod<br />

L. Héctor Juárez V.<br />

e-mail: hect@xanum.uam.mx<br />

Departamento <strong>de</strong> Matemáticas<br />

Universidad Autónoma M<strong>et</strong>ropolitana-I<br />

México<br />

Flow generated by a circular rotating cylin<strong>de</strong>r eccentrically placed b<strong>et</strong>ween parallel plates in a two<br />

dimensional channel is studied numerically. This simulation <strong>de</strong>scribe a pumping <strong>de</strong>vice appropriate<br />

form microelectromechanical systems (MEMS). The <strong>de</strong>vice is shown to be capable of generating a n<strong>et</strong><br />

flow due to the differential viscous resistance b<strong>et</strong>ween small and large gaps. The numerical simulation<br />

is carried out by a high–or<strong>de</strong>r Lagrange Finite Element M<strong>et</strong>hod in combination with a second or<strong>de</strong>r<br />

time–integration scheme.


Umbrella based triangulation<br />

of regular param<strong>et</strong>ric surfaces<br />

Victoria Hernán<strong>de</strong>z, Instituto <strong>de</strong> Cibernética, Matemática y Física, ICIMAF,<br />

La Habana, Cuba, e-mail: vicky@icmf.inf.cu<br />

Pedro L. <strong>de</strong>l Angel, Centro <strong>de</strong> Investigaciones Matemáticas, CIMAT,<br />

Guanajuato, México, e-mail: luis@cimat.mx<br />

Jorge Estrada, Instituto <strong>de</strong> Cibernética, Matemática y Física, ICIMAF,<br />

La Habana, Cuba, e-mail: jestrada@icmf.inf.cu<br />

Abstract<br />

Param<strong>et</strong>ric surfaces are the standard in Computer Ai<strong>de</strong>d Design and Manufacturing<br />

(CAD/CAM) systems. Therefore, a lot of work has been done to obtain good discr<strong>et</strong>izations<br />

of param<strong>et</strong>ric surfaces, suitable for visualization as well as for numerical solution of partial<br />

differential equations using finite elements m<strong>et</strong>hod (FEM) or boundary elements m<strong>et</strong>hod<br />

(BEM). Triangulation of param<strong>et</strong>ric surfaces is also an essential problem in computer<br />

graphics and computational geom<strong>et</strong>ry. The most common discr<strong>et</strong>ization of a surface is a<br />

triangular mesh, due to its flexibility for representing complex geom<strong>et</strong>ries and also because<br />

current graphics hardware and software are tuned to handle triangular meshes. The simplest<br />

way of constructing a triangular mesh on a param<strong>et</strong>ric surface consists in generating a (nice)<br />

triangulation in param<strong>et</strong>er space and lifting it to the surface by means of the param<strong>et</strong>rization.<br />

Unfortunately, this triangular mesh could be very distorted.<br />

In this talk we propose an advancing front m<strong>et</strong>hod for generating an isotropic triangular mesh<br />

on a regular param<strong>et</strong>ric surface. Starting from a point on the surface, the m<strong>et</strong>hod computes a<br />

s<strong>et</strong> of points in the intersection curve b<strong>et</strong>ween the surface and the sphere centered at that point<br />

with a prescribed radius. These points are the vertices of a cell composed by triangles<br />

approximately equilateral. The mesh grows repeating the <strong>de</strong>scribed computation with<br />

boundary vertices of the cell as starting points. The resulting isotropic mesh can be refined in<br />

or<strong>de</strong>r to g<strong>et</strong> a b<strong>et</strong>ter approximation of the surface, making the m<strong>et</strong>hod also useful for<br />

visualization of the surface. Finally, we obtain a sufficient condition ensuring that a surface<br />

triangulation is of Delaunay type. As a particular case, we prove that any isotropic<br />

triangulation (with vertices on a surface) which provi<strong>de</strong>s a good approximation of a surface<br />

is a Delaunay triangulation.<br />

Keywords: Param<strong>et</strong>ric surfaces, triangular meshes


GENERAL FORMULAE OF B-SPLINE CURVES WITH SHAPE PARAMETERS<br />

MIKL OS HOFFMANN AND IMRE JUH ASZ<br />

In spite of the recently <strong>de</strong>veloped curve <strong>de</strong>sign m<strong>et</strong>hods, B-spline curve still plays essential role in<br />

computer ai<strong>de</strong>d geom<strong>et</strong>ric <strong>de</strong>sign. The generalization of this curve, however, is also in the forefront of<br />

research due to its importance in applications. Several authors attempted to extend the approximation<br />

abilities of the B-spline curve by some shape param<strong>et</strong>er which allows the user to improve the shape<br />

of the approximating curve. Obviously, the most known result of this attempt is the NURBS curve<br />

(c.f. [3]), but this curve has rational coecient functions, thus alternative m<strong>et</strong>hods tried to incorporate<br />

shape param<strong>et</strong>ers into the original, polynomial basis functions. One of the earliest m<strong>et</strong>hods in this way<br />

is -spline curve with two global param<strong>et</strong>ers ([6], [7]). Further m<strong>et</strong>hods have been provi<strong>de</strong>d by direct<br />

generalization of B-spline curves as B-splines in [2], [4] and recently as GB-splines in [1] or as SPB-splines<br />

in [5]. Some alternative spline curves with shape param<strong>et</strong>ers can be found in [8] and [9].<br />

The various generalizations of the B-spline curve dier from each other in the modied basis functions<br />

of the curve. Unfortunately, most of the papers provi<strong>de</strong> the <strong>de</strong>nition of the modied basis functions with<br />

no further explanations. The aim of this paper is to give a general approach and formulae of B-spline<br />

curves with shape param<strong>et</strong>ers, including all the previously mentioned m<strong>et</strong>hods and give a chance for a<br />

comparative study.<br />

It will be shown, that all the curves provi<strong>de</strong>d by these m<strong>et</strong>hods can be consi<strong>de</strong>red as a linear blending<br />

3X<br />

3X<br />

of the classical B-spline curve b (t) = B i (t) p i and another curve g (t) = G i (t) g i . Thus, the<br />

i=0<br />

modied curve with shape param<strong>et</strong>er is of the form<br />

c (; t) = q () b (t) + (1 q ()) g (t) ; q () 2 [0; 1] :<br />

In most of the cases g (t) turns to be the param<strong>et</strong>erized line segment p 1 p 2 , in other cases g (t) is a<br />

4 th or<strong>de</strong>r curve. In this content we give a general framework of spline curves with shape param<strong>et</strong>ers,<br />

provi<strong>de</strong> a comparative study of the previous m<strong>et</strong>hods and <strong>de</strong>ne a curve which, in some sense, the best<br />

approximation m<strong>et</strong>hod by generalizing the classical B-spline curve. Using this framework multivariate<br />

shape control with several shape param<strong>et</strong>ers as well as non-uniform param<strong>et</strong>erization and continuity of<br />

the subsequent arcs are also discussed in the paper.<br />

i=0<br />

References<br />

[1] Guo, Q., 2005. Cubic GB-spline curves. Journal of Information and Computational Science 3, 465{471.<br />

[2] Loe, K.F., 1996. B-spline: a linear singular blending B-spline. The Visual Computer 12, 18{25.<br />

[3] Piegl, L., Tiller, W., 1995. The NURBS book. Springer Verlag.<br />

[4] Tai, C.L., Wang, G.J., 2004. Interpolation with slackness and continuity control and convexity-prservation using singular<br />

blending. Journal of Computational and Applied Mathematics 172, 337{361.<br />

[5] Yin, M., Wang, Q., 2005. B-spline curve of or<strong>de</strong>r 4 with two shape param<strong>et</strong>ers. Journal of Computational Information<br />

Systems 1, 609{614.<br />

[6] Barsky, B.A., Beatty, J.C., 1983. Local control of bias and tension in splines. ACM Transactions on Graphics, 2,<br />

109-134.<br />

[7] Barsky, B.A.,1988. Computer graphics and geom<strong>et</strong>ric mo<strong>de</strong>ling using splines. Springer-Verlag, Berlin.<br />

[8] Habib Z., Sakai M. and Sarfraz M. 2004. Interactive Shape Control with Rational Cubic Splines, International Journal<br />

of Computer-Ai<strong>de</strong>d Design & Applications, 1, 709-718.<br />

[9] Habib Z., Sarfraz M. and Sakai M., 2005. Rational cubic spline interpolation with shape control, Computers & Graphics<br />

29, 594-605.<br />

E-mail address: hofi@ektf.hu<br />

E-mail address: JuhaszI@abrg.uni-miskolc.hu<br />

Institute of Mathematics and Computer Science, Karoly Eszterhazy University, Eger, Hungary<br />

Department of Descriptive Geom<strong>et</strong>ry, University of Miskolc, Miskolc, Hungary


A new Hilbert transform in a m<strong>et</strong>ric <strong>de</strong>pen<strong>de</strong>nt Clifford s<strong>et</strong>ting<br />

F. Brackx, B. De Knock, H.DeSchepper<br />

Department of Mathematical Analysis, Faculty of Engineering, Ghent University<br />

Galglaan 2, 9000 Gent, Belgium<br />

e-mail: Bram.DeKnock@UGent.be<br />

In one—dimensional signal processing, the Hilbert transform has become an indispensable tool in signal<br />

analysis: it un<strong>de</strong>rlies the concept of analytic signal (see e.g. [1]), which is crucial in the construction of so—<br />

called quadrature filters, used for obtaining selective spectral information. Mathematically, if f ∈ L 2 (R)<br />

is a real valued signal of finite energy, and H[f] <strong>de</strong>notes its Hilbert transform, i.e. the convolution with<br />

1<br />

the principal value kernel<br />

π<br />

Pv 1 x , then the corresponding analytic signal is the function 1 2 f + i 2 H[f],<br />

which belongs to the Hardy space H 2 (R),andarisesastheL 2 non-tangential boundary value for y → 0+<br />

of the holomorphic Cauchy transform of f in the upper half of the complex plane.<br />

The Hilbert transform has been generalized to higher dimension (see e.g. [2]) and higher dimensional<br />

applications have already been addressed as well, for instance in [3], where the concept of analytic signal<br />

was generalized to two dimensions in or<strong>de</strong>r to <strong>de</strong>sign appropriate quadrature filters for pattern recognition,<br />

using a two—dimensional Hilbert transform, also referred to as Riesz transform. Several of the<br />

higher dimensional generalizations were established in Clifford analysis, a comprehensive theory offering<br />

an elegant and powerful generalization to higher dimension of the theory of holomorphic functions in<br />

the complex plane. In its most simple y<strong>et</strong> still useful s<strong>et</strong>ting, flat (m + 1)—dimensional Eucli<strong>de</strong>an space,<br />

Clifford analysis focusses on monogenic functions, i.e. null solutions of the Clifford-vector valued Dirac<br />

operator ∂ = P m<br />

j=0 e j∂ xj where (e 0 ,... ,e m ) forms an orthogonal basis for the quadratic space R m+1<br />

un<strong>de</strong>rlying the construction of the Clifford algebra R 0,m+1 (see e.g. [4],[5]).<br />

The above <strong>de</strong>scribed form of Clifford analysis may be referred to as isotropic, since the m<strong>et</strong>ric in the<br />

un<strong>de</strong>rlying space is the standard Eucli<strong>de</strong>an one. In our talk however, we will adopt the i<strong>de</strong>a of a m<strong>et</strong>ric<br />

<strong>de</strong>pen<strong>de</strong>nt, also called anisotropic or m<strong>et</strong>rodynamical, Clifford s<strong>et</strong>ting (see e.g. [6]), which offers the<br />

possibility of adjusting the co-ordinate system to preferential, and not necessarily mutually orthogonal,<br />

directions in the m—dimensional signal to be analyzed. This leads to the introduction of a m<strong>et</strong>ric <strong>de</strong>pen<strong>de</strong>nt<br />

generalized Hilbert transform in R m ⊂ R m+1 , a special case of which was already introduced and<br />

used for two—dimensional image processing in [3].<br />

References<br />

[1] A.D. Poularikas (ed.), The transforms and applications handbook, CRC Press, Boca Raton, 1996.<br />

[2] J. Gilbert and M. Murray, Clifford Algebras and Dirac Operators in Harmonic Analysis, Cambridge<br />

University Press, Cambridge, 1991.<br />

[3] M. Felsberg, Low-Level Image Processing with the Structure Multivector, PhD-thesis, Christian-<br />

Albrechts-Universität, Kiel, 2002.<br />

[4] F. Brackx, R. Delanghe and F. Sommen, Clifford Analysis, Pitman Publishers, Boston-London-<br />

Melbourne, 1982.<br />

[5] R. Delanghe, F. Sommen and V. Souček, Clifford Algebra and Spinor-Valued Functions, Kluwer<br />

Aca<strong>de</strong>mic Publishers, Dordrecht, 1992.<br />

[6] F. Brackx, N. De Schepper and F. Sommen, M<strong>et</strong>ric Depen<strong>de</strong>nt Clifford Analysis with Applications to<br />

Wavel<strong>et</strong> Analysis. D. Alpay (ed.), Wavel<strong>et</strong>s, Multiscale Systems and Hypercomplex Analysis, Series<br />

”Operator Theory: Advances and Applications”, 167, Birkhäuser Verlag, Basel, 2006, 17-67.


Lattices on simplices<br />

Gašper Jaklič*,JernejKozak,Marj<strong>et</strong>aKrajnc,<br />

Vito Vitrih, Emil Žagar<br />

FMF and IMFM, University of Ljubljana, Slovenia<br />

In contrast to the univariate case, uniqueness of the solution of a multivariate<br />

Lagrange polynomial interpolation problem <strong>de</strong>pends not only on the fact that<br />

interpolation points should be distinct but also on their geom<strong>et</strong>ry. Lattices are<br />

perhaps the most often used configurations of prescribed interpolation points.<br />

In this talk, three-pencil lattices on triangulations will be consi<strong>de</strong>red. The<br />

explicit representation of a lattice, based upon barycentric coordinates, will be<br />

presented. This enables us to construct lattice points in a simple and numerically<br />

stable way and carries over to triangulations in a natural way.<br />

A generalization to 3D simplex partitions will be presented.


Fast Multiscale M<strong>et</strong>hods for PDE-Constrained Control Problems<br />

Angela Kunoth<br />

Institut für Angewandte Mathematik, Universität Bonn, Wegelerstr. 6, 53115 Bonn, Germany,<br />

kunoth@iam.uni-bonn.<strong>de</strong> www.iam.uni-bonn.<strong>de</strong>/∼kunoth<br />

The fast numerical solution of PDE-constrained control problems provi<strong>de</strong>s a formidable<br />

challenge, in particular, for problems constrained by time-<strong>de</strong>pen<strong>de</strong>nt PDEs. For a single<br />

elliptic PDE which may be consi<strong>de</strong>red as the core system to be solved in any case, there<br />

exist by now three classes of preconditioners, all of which are of multiscale structure<br />

(multigrid, BPX and wavel<strong>et</strong> preconditioners), which assure uniformly boun<strong>de</strong>d spectral<br />

condition numbers of the system matrix in<strong>de</strong>pen<strong>de</strong>nt of the discr<strong>et</strong>ization.<br />

In my talk I wish to address fast multiscale solvers for control problems constrained<br />

by elliptic PDEs with distributed as well as Dirichl<strong>et</strong> boundary control. I will present<br />

the main ingredients for obtaining theor<strong>et</strong>ical estimates which guarantee optimality of<br />

the multilevel preconditioners. Tog<strong>et</strong>her with employing iterative solvers and a nested<br />

iteration scheme, I will show that they therefore provi<strong>de</strong> the solution ingredients of the<br />

control problem (state, costate and control) up to discr<strong>et</strong>ization error accuracy in optimal<br />

linear complexity. Corresponding numerical results confirming these estimates will be<br />

shown.<br />

Finally, I would like to address PDE-constrained control problems with additional<br />

inequality constraints on the control which pose substantial difficulties for fast numerical<br />

solution schemes.


Generalized Expo-Rational B-splines<br />

Lubomir T. Dechevsky, Arne Lakså, Børre Bang<br />

Narvik University College, NORWAY<br />

We formalize the fundamental structure and properties of expo-rational B-splines, as<br />

<strong>de</strong>fined and <strong>de</strong>rived in [1], and i<strong>de</strong>ntify the maximal class of possible generalized B-<br />

splines which share the same fundamental structure and properties. We consi<strong>de</strong>r this<br />

maximal class for param<strong>et</strong>ric curves, tensor-product surfaces, triangulated surfaces<br />

and simplectified multivariate manifolds. We show that besi<strong>de</strong>s the true expo-rational<br />

B-splines, there are also some classical piecewise-polynomial B-splines which satisfy<br />

the above formal constraints and form closed subspaces in usual classical piecewisepolynomial<br />

B-spline spaces of higher <strong>de</strong>gree and/or dimension of the knot-vector. We<br />

consi<strong>de</strong>r in <strong>de</strong>tail the simplest case of piecewise-polynomial generalized expo-rational<br />

B-spline which can be computed explicitly (including in the case of triangulated<br />

surfaces and simplectified multi-dimensional manifolds). Visualization and a<br />

discussion on applications are also inclu<strong>de</strong>d in the talk.<br />

Reference:<br />

[1] L. T. Dechevsky, A. Lakså, B. Bang. Expo-rational B-splines. Int. J. Pure Appl.<br />

Math. (ISSN 1311-8080) 27(3) (2006) 319-367.


The or<strong>de</strong>r of approximation of tranport<br />

equations by the kin<strong>et</strong>ic equation<br />

Jeremy Levesley<br />

Leicester University<br />

Department of Mathematics and Computer Science<br />

LE1 7RH Leicester. UK<br />

jl1@mcs.le.ac.uk<br />

The Lattice Boltzmann m<strong>et</strong>hod is a technique for simulating material transport<br />

via a dynamical system generated by a kin<strong>et</strong>ic equation in phase space. The<br />

macroscopic quantities of interest (e.g. <strong>de</strong>nsity or momentum) are moments of<br />

the phase space distribution. We will outline how Navier-Stokes' equation can be<br />

viewed as free flight in phase space, followed by an equilibration process. We<br />

will <strong>de</strong>scribe a novel numerical m<strong>et</strong>hod for simulating fluid flow which<br />

implements the above free flight and equilibration at high Reynolds' number and<br />

discuss how well this m<strong>et</strong>hod approximates the Navier-Stokes' equations. We<br />

will also look at m<strong>et</strong>hods of stabilisation of this process based around various<br />

sorts of filter.


Diffusion polynomial frames on m<strong>et</strong>ric measure spaces<br />

We construct a multiscale tight frame based on an arbitrary orthonormal<br />

basis for the L 2 space of an arbitrary sigma finite measure space. The approximation<br />

properties of the resulting multiscale are studied in the context of<br />

Besov approximation spaces, which are characterized both in terms of suitable<br />

K—functionals and the frame transforms. The only major condition required is<br />

the uniform boun<strong>de</strong>dness of a summabilility operator. We give sufficient conditions<br />

for this to hold in the context of a very general class of m<strong>et</strong>ric measure<br />

spaces, where the assumption of finite speed of wave propagation might not<br />

hold. The theory is illustrated using the approximation of characteristic functions<br />

of caps on a dumbell manifold, and applied to the problem of recognition of<br />

hand—written digits. Our m<strong>et</strong>hods outperforms comparable m<strong>et</strong>hods for semi—<br />

supervised learning. This is joint work with Professor Mauro Maggioni, Duke<br />

University.<br />

H. N. Mhaskar<br />

Department of Mathematics<br />

California State University<br />

Los Angeles, CA 90032<br />

U. S. A.


Mathematical and computational challenges in some<br />

applications of medical imaging<br />

Knut Mørken<br />

knutm@ifi.uio.no<br />

University of Oslo<br />

CMA, P.O. Box 1053, Blin<strong>de</strong>rn, 0316 Oslo, Norway<br />

The ability to capture images of the interior of the human body has revolutionized<br />

both medical diagnosis and therapy. Today, a number of different imaging<br />

technologies are available, such as CT (Computed Tomography), MRI (Magn<strong>et</strong>ic<br />

Resonance Imaging), PET (Positron Emission Tomography), ultrasound, X-ray, photo<br />

and vi<strong>de</strong>o. The first three techniques provi<strong>de</strong> 3D samples in uniform grids; ultrasound<br />

can give both 2D and 3D images, while X-ray gives 2D images, but is also the basis<br />

for CT imaging. Although these technologies have already radically changed many<br />

aspects of medicine, with for instance the emergence of minimally invasive surgery,<br />

new surgery techniques based on imaging are likely to further transform both<br />

diagnosis and therapy in even more profound ways.<br />

A fundamental challenge in medical imaging is to combine data from different<br />

imaging techniques to produce a synth<strong>et</strong>ic image that provi<strong>de</strong>s more information than<br />

any of the individual images. This is the image fusion problem, which in turn is<br />

<strong>de</strong>pen<strong>de</strong>nt on the image registration problem, i.e., the problem of aligning two images<br />

(2D or 3D) in a common coordinate system. In general, these are extremely<br />

challenging problems, both mathematically and computationally.<br />

This talk will give a brief introduction to medical imaging and the image registration<br />

and image fusion problems on a fairly nontechnical level. In addition, we will<br />

consi<strong>de</strong>r some specific applications of medical imaging such as temperature<br />

monitoring via MRI during heating of tissue, and monitoring of the frozen area during<br />

freezing of tissue.


Splines for Surfaces of Arbitrary Topology<br />

Mike Neamtu, Van<strong>de</strong>rbilt University<br />

Abstract:<br />

There is a well-<strong>de</strong>veloped theory of bivariate splines on planar triangulations,<br />

which allows one to construct splines of arbitrary smoothness. However, such<br />

splines can only be used to obtain param<strong>et</strong>ric surfaces that are topologically<br />

equivalent to a planar region. This theory of bivariate splines fails compl<strong>et</strong>ely<br />

when one wants to <strong>de</strong>fine smooth surfaces of arbitrary topological genus. In this<br />

talk we shall address the causes of this serious gap in the spline theory and<br />

discuss a possible remedy.


Sparse Approximation for Source Separation<br />

in the Magn<strong>et</strong>oencephalography Inverse Problem<br />

Francesca Pitolli<br />

Dip. MeMoMat, Università diRoma”La Sapienza”, Italy.<br />

The aim of magn<strong>et</strong>oencephalography (MEG) is the analysis of brain functionality through the<br />

measurements of the tiny magn<strong>et</strong>ic field generated by neuronal currents (see, for instance, [2] and<br />

references therein). As a matter of fact, since neuron cells functioning is mediated by electric<br />

currents, to un<strong>de</strong>rstand brain functionality it is important to gain knowledge about the current<br />

distribution within the head. Therefore, looking from the physics si<strong>de</strong>, the final goal of MEG is<br />

to accurately <strong>de</strong>termine the current <strong>de</strong>nsity flowing within the volume of the head in the working<br />

human brain.<br />

The neuromagn<strong>et</strong>ic field is only in the or<strong>de</strong>r of 10 −13 Tesla in magnitu<strong>de</strong>, that is much smaller<br />

than the environmental noise. To successfully resolve the current <strong>de</strong>nsity flowing within the brain it<br />

is mandatory to use low noise superconducting magn<strong>et</strong>om<strong>et</strong>ers as well as sophisticated signal processing.<br />

In addition, the magn<strong>et</strong>ic field measured externally the head has a poor spatial resolution<br />

- at present MEG <strong>de</strong>vices have at most a few hundred sensors - and can be generated by several<br />

possible current <strong>de</strong>nsity configurations. Hence, the i<strong>de</strong>ntification of a specific current source configuration<br />

from the measured magn<strong>et</strong>ic fields is an ill-conditioned inverse problem, and is one of the<br />

challenging aspects of this technology. The main goal of this paper is to give an efficient and stable<br />

numerical scheme to compute the solution of the MEG inverse problem assuming that the currents<br />

flowing in the brain satisfy a sparsity constraint [1,3,4].<br />

This is a joint work with M. Fornasier and V. Pizzella.<br />

[1] I. Daubechies, M. Defrise, and C. De Mol, An iterative thresholding algorithm for linear inverse<br />

problems with a sparsity constraint, Commun. Pure Appl. Math., 57 (2004) 1413–1457.<br />

[2] C. Del Gratta, V. Pizzella, F. Tecchio, and G. L. Romani, Magn<strong>et</strong>oencephalography - a noninvasive<br />

brain imaging m<strong>et</strong>hod with 1ms time resolution, Rep. Prog. Phys., 64 (2001) 1759–1814.<br />

[3] M. Fornasier, and H. Rauhut, Recovery algorithms for vector valued data with joint sparsity<br />

constraints, Report 2006-27, Johann Radon Institute for Computational and Applied Mathematics<br />

(RICAM),<br />

http://www.ricam.oeaw.ac.at/publications/reports/06/rep06-27.pdf.<br />

[4] M. Fornasier, F. Pitolli and V. Pizzella, Blind Source Separation with Sparsity Constraints for<br />

Magn<strong>et</strong>oencephalography, Proc. of SIMAI 2006...<br />

Francesca Pitolli<br />

Dipartimento di M<strong>et</strong>odi e Mo<strong>de</strong>lli Matematici per le Scienze Applicate<br />

Università diRoma“LaSapienza”<br />

ViaA.Scarpa16<br />

I-00161 Roma, Italy<br />

email: pitolli@dmmm.uniroma1.it<br />

WWW: http://www.dmmm.uniroma1.it/∼pitolli


How to reduce Runge Phenomenon<br />

Christophe Rabut,Toulouse University, (INSA), France<br />

Two ways are presented to reduce Runge phenomenon (strong oscillations<br />

for polynomial interpolation). The first one is done for equidistant interpolation<br />

points and gives some kind of flexibility to the interpolation values. The<br />

second one is for any point repartition and consists in giving some more freedom<br />

by a <strong>de</strong>gree elevation and using the so-obtained freedom for minimizing<br />

a norm significative of the oscillation of the polynomial.<br />

First m<strong>et</strong>hod: The points to be interpolated being ( i , y n i) i=0:n , we first<br />

use the fact that the Bezier polynomial p 0 (x) = ∑ n<br />

( ) i=0 y i B i (x) (where B i (x) =<br />

n<br />

i x i (1 − x) n−i is the i th <strong>de</strong>gree n Bernstein polynomial) oscilates no more<br />

than the data points (variation diminishing prop<strong>et</strong>y), and so we start from<br />

this polynomial. However we would like a polynomial closer the data. To<br />

g<strong>et</strong> it, we construct, for any k in IN by induction the family (Bi k ) i=0:n<br />

by the following : Bi<br />

k = Bi<br />

k−1 + ∑ n<br />

j=0 (δ ij − Bi<br />

k−1 (x j )) , Bj<br />

k−1 = 2 Bi<br />

k−1 −<br />

∑ nj=0<br />

Bi<br />

k−1 (x j )) , Bj<br />

k−1 . Then the polynomial p k (x) = ∑ n<br />

i=0 y i Bi k (x) is proved<br />

to converge to the interpolating polynomial of the points ( i , y n i) i=0:n and<br />

presents far less oscillations of the interpolation polynomial, even when values<br />

at x = i are very close to y n i.<br />

Second m<strong>et</strong>hod: For any k ≥ n,we <strong>de</strong>fine the polynomial p k as being<br />

the <strong>de</strong>gree k polynomial interpolating the data points (x i , y i ) i=0:n and minimizing,<br />

over all polynomials p interpolating the data points, the quantity<br />

∫ xn<br />

x 0<br />

(p ′′ (x)) 2 dx. We so use the <strong>de</strong>gree of freedom given by the <strong>de</strong>gree of the<br />

polynomial to cut down the oscillations. Numerical experiments give the<br />

evi<strong>de</strong>nce that p k converges (over [x 0 ..x n ]) to the interpolating natural cubic<br />

spline of the data points, which shows that the oscillations are effectively cut<br />

down.<br />

Graphs of both the m<strong>et</strong>hods will be presented.


BUILDING SOLIDS USING QUATERNIONS<br />

Universidad Autónoma M<strong>et</strong>ropolitana<br />

Rafael Reséndiz<br />

rafael.resendiz@gmail.com<br />

We show a way to make solid mo<strong>de</strong>lling taking the solid surface like a<br />

trajectory of a particle; it is well known that a trajectory is seen as a<br />

rational Bézier curve, so we make a dual quaternionic param<strong>et</strong>rization<br />

of mentioned trajectory. Then the main i<strong>de</strong>a is to pick a surface given<br />

by either scattered data or regularly distributed and be able to<br />

reproduce it carving it in some material.


Polyharmonic B-Splines<br />

Milvia Rossini<br />

Dipartimento di Matematica e Applicazioni, Università di Milano Bicocca<br />

Polyharmonic splines are consi<strong>de</strong>red very often in the literature, because of<br />

their good properties.<br />

The aim of this talk is to present the recent results obtained jointly by the<br />

Milano-Bicocca group and Christophe Rabut on some classes of polyharmonic<br />

B-spline having attractive properties for the applications.<br />

In particular after giving their construction and presenting their properties,<br />

we discuss the results related to the construction of a multiresolution analysis<br />

of L 2 (R 2 ). Examples of applications to different problems will be also shown.<br />

Milvia Rossini<br />

Dipartimento di Matematica e Applicazioni<br />

Università di Milano-Bicocca<br />

Via Cozzi 53<br />

I-20125 Milano, Italy<br />

email: milvia.rossini@unimib.it


Surface Approximation of surfaces with fault(s) and/or rapidly varying<br />

data, using segmentation process, D m spines and finite element m<strong>et</strong>hod.<br />

C. Gout 1,2 , C. Le Guya<strong>de</strong>r 3 , H. Huru 4 , L. Romani 5 , *A.G. Saint-Guirons 6<br />

1 <strong>Université</strong> <strong>de</strong> Valenciennes<br />

LAMAV - ISTV2, Le Mont Houy<br />

59313 Valenciennes ce<strong>de</strong>x 9, France<br />

2 INSA <strong>de</strong> Rouen - LMI<br />

Place Emile Blon<strong>de</strong>l, BP 08<br />

76 131 Mont-Saint-Aignan ce<strong>de</strong>x, France<br />

3 INSA <strong>de</strong> Rennes<br />

20 Avenue <strong>de</strong>s Buttes <strong>de</strong> Coësmes, CS 14315<br />

35043 Rennes Ce<strong>de</strong>x , France<br />

4 University of Tromsoe<br />

Department of Mathematics and Statistics,<br />

University of Tromsoe, N-9037 Tromsoe, Norway,.<br />

5 Università di Milano,<br />

Dipartimento di Matematica e Applicazioni ,Via R.<br />

Cozzi n. 53, 20125 Milano, Italy.<br />

6 <strong>Université</strong> <strong>de</strong> <strong>Pau</strong><br />

LMA UMR 5142, Avenue <strong>de</strong> l’<strong>Université</strong>,<br />

64018 <strong>Pau</strong> ce<strong>de</strong>x, France<br />

In many problems of geophysical interest, one has to <strong>de</strong>al with data that exhibit complex fault structures or at<br />

least large variations (rapidly varying data). This occurs for instance when <strong>de</strong>scribing the topography of<br />

seafloor surfaces, mountain ranges, volcanoes, islands, or the shape of geological entities, that can present<br />

large and rapid variations due for instance to the presence of faults in the structure.<br />

The usual approximation m<strong>et</strong>hods use to lead to instability phenomena or un<strong>de</strong>sirable oscillations. The key<br />

point to g<strong>et</strong> a good approximant consists in precisely <strong>de</strong>fine the locations of the large variations and the<br />

faults. To do that, we propose a m<strong>et</strong>hod <strong>de</strong>veloped by Le Guya<strong>de</strong>r and Gout (2005) to "segment" the data.<br />

Then, having the knowledge about the location of the discontinuities of the surface, we can generate a mesh<br />

using triangles (which takes into account the s<strong>et</strong> of discontinuities) and a specific spline approximant is then<br />

computed. We discuss the convergence of the m<strong>et</strong>hod when the number of data tends to infinity. We show<br />

the efficiency of this technique applying it to real datas<strong>et</strong>s in Oceanography and in the Geosciences. This last<br />

part is crucial because our propose m<strong>et</strong>hod is generated<br />

Key words: Level s<strong>et</strong> m<strong>et</strong>hods, finite element m<strong>et</strong>hods, spline, surfaces having faults, spline functions...<br />

Meshing constraints<br />

Without information about the location of the large variations, the usual approximation m<strong>et</strong>hods lead to<br />

instability phenomenae or un<strong>de</strong>sirable oscillations that can locally and even globally hin<strong>de</strong>r the<br />

approximation. Here is the Tonga trench after the segmentation process on the datas<strong>et</strong> (we g<strong>et</strong> 3 patches).<br />

We then apply a spline approximant in or<strong>de</strong>r to<br />

g<strong>et</strong> a surface whithout oscillations, and where the<br />

large gradients are correctly given. This spline is<br />

discr<strong>et</strong>ized on a finite element space , the<br />

meshing taking into account the patches obtained<br />

after the segmentation process.


A C 1 quadratic trivariate macro-element space<br />

<strong>de</strong>fined over arbitrary t<strong>et</strong>rahedral partitions<br />

Larry Schumaker<br />

larry.schumaker@gmail.com<br />

Abstract:<br />

In 1988 Worsey and Piper constructed a trivariate macro-element based on C 1<br />

quadratic splines <strong>de</strong>fined over the Powell-Sabin splitof a t<strong>et</strong>rahedron.<br />

Unfortunately, their element can only be used with t<strong>et</strong>rahedral partitions that<br />

satisfy some very restrictive geom<strong>et</strong>ric constraints. We show that by further<br />

refining their split, it is possible to construct a macro-element (based on the<br />

same spline space) that can be used with arbitrary t<strong>et</strong>rahedral partitions. The<br />

resulting macro-element space is stable and provi<strong>de</strong>s full approximation power.<br />

It is of dimension 4V + 2E + 4F, where V,E,F are the numbers of vertices, edges,<br />

and faces in the partition.


The Dirac equation for bivector mass<br />

by Frank Sommen<br />

The classical Klein Gordon equation may be factorized by means of the Dirac operator<br />

using the Clifford algebra R 3,2 with generators e 1 , e 2 , e 3 , w = -i e 4 and v = -i e 5 whereby<br />

the elements e j satisfy the standard <strong>de</strong>fining relations e j e k + e k e j = -2 δ jk . The Dirac<br />

operator that factorizes the Klein-Gordon operator is then given by ∂ x = ∂ x1 e 1 + ∂ x2 e 2<br />

+ ∂ x3 e 3 + w ∂ t + v m , whereby m is the scalar mass. Within the same algebra one may<br />

also consi<strong>de</strong>r the bivectorial operator v( ∂ x1 e 1 + ∂ x2 e 2 + ∂ x3 e 3 + w ∂ t ) + M whereby M<br />

is a bivector in the space-time Clifford basis e 1 , e 2 , e 3 , w. There is no reason why the<br />

vectorial Dirac operator has physical relevance while this bivectorial operator wouldn't; it<br />

is also Lorentz invariant and the first part corresponds to the usual space-time Dirac<br />

operator for massless particals. It is in other words an alternative extension of this<br />

operator leading to an alternative notion of mass. In our presentation we study this<br />

operator from the function theor<strong>et</strong>ic point of view as well as the corresponding Klein-<br />

Gordon operator which has the form ∆+ m 0 + e 123 w M 0 + S whereby ∆ is the Laplacian,<br />

m 0 the standard mass, M 0 the "Klein mass" and S the mass-momentum interaction<br />

operator.


Hyperholomorphic functions in elasticity and fluid dynamics<br />

Wolfgang Sproessig<br />

Institute of Applied Analysis<br />

Freiberg University of Mining and Technology<br />

09596 Freiberg, Germany/Saxony<br />

Abstract: During the last twenty years Clifford analysis has become increasingly important<br />

tool also for the analysis of (initial) boundary value problems of partial differential<br />

equations and their applications to problems of mathematical physics and engineering. In<br />

particular we will apply real and complex quaternions. The Clifford calculus covers a<br />

branch of mathematics which uses computational techniques for solving problems from a<br />

wi<strong>de</strong> vari<strong>et</strong>y of physical systems which mathematically mo<strong>de</strong>led in 3,4 and more dimensions.<br />

In my talk I will try to reflect some main i<strong>de</strong>as in the field of applications. Above<br />

all I intent to discuss a quaternion operator calculus and its application to boundary and<br />

initial value problems including lines of a suitable numerical analysis. Examples in the<br />

applications area will be chosen from problems in elasticity theory and hydrodynamics .<br />

We start with an algebraic introduction. Then a brief discourse in function theory in R n<br />

will follow. We <strong>de</strong>fine versions of the generalized Cauchy-Riemann operator, the Teodorescu<br />

transform and the so-called Cauchy-Fu<strong>et</strong>er operator. Formulas of Borel-Pompeiu<br />

type compl<strong>et</strong>e the function theor<strong>et</strong>ic part. Moreover, we introduce a singular integral<br />

operator (Bitzadse operator) over the boundary of a sufficient smooth boun<strong>de</strong>d domain in<br />

R n , corresponding Plemelj projections will be <strong>de</strong>scribed. A Hodge <strong>de</strong>composition of the<br />

quaternionic Hilbert space follows. One of the associated orthoprojections is a generalized<br />

version of the well-known Bergman projection. Now we enter in the part with applications<br />

and start with problems in linear elasticity. Neuber-Papkovic statements are inclu<strong>de</strong>d. We<br />

present in this case a quaternionic multipole m<strong>et</strong>hod. Furthermore, we consi<strong>de</strong>r m<strong>et</strong>hods<br />

for the solution of initial-boundary problems in fluid dynamics and forecasting equations<br />

on the sphere. The we will explain a corresponding associated discr<strong>et</strong>ization concept and<br />

show the interplay b<strong>et</strong>ween the discr<strong>et</strong>e and continuous mo<strong>de</strong>l. We finish our lecture with<br />

a brief sk<strong>et</strong>ch of further interesting fields. Basic results are inclu<strong>de</strong>d in [1], [2],[3],[4], [5],[6]<br />

and [7].<br />

References<br />

[1] Brackx F., Delanghe R. and Sommen F.(1982) Clifford analysis. Pitman Research Notes in<br />

Math., Boston, London, Melbourne.<br />

[2] K. Gürlebeck and Sprössig W.(1990) Quaternionic Analysis and Boundary Value Problems,<br />

Birkhäuser Verlag, Basel.<br />

[3] K. Gürlebeck and Sprössig W.(1997) Quaternionic and Clifford calculus for physicists and<br />

engineers, John Wiley, Chichester.<br />

[4] K. Gürlebeck and Sprössig W.(2002) Representation theory for classes of initial value problems<br />

with quaternionic analysis, Mathematical M<strong>et</strong>hods in the Applied Sciences; 25; 1371 — 1382.<br />

[5] K. Gürlebeck, K. Hab<strong>et</strong>ha and Sprössig, W.(2006) Function theory in the plane and in the<br />

space, (German), Birkhäuser, Basel. (English version in preparation, August 2007)<br />

[6] Kravchenko, V.V. and Shapiro,M.V.(1996) Integral representations for spatial mo<strong>de</strong>ls of mathematical<br />

physics, Pitman research notes Mathematics Series 351.<br />

[7] Mitrea, M.(1994) Clifford wavel<strong>et</strong>s, singular integrals and Hardy Spaces, Lecture Notes in<br />

Mathematics 1575, Springer, New York.


Diffusion Filters and Wavel<strong>et</strong>s<br />

Gabriele Steidl,<br />

University of Mannheim,<br />

Faculty of Mathematics and Computer Science<br />

Abstract<br />

Nonlinear diffusion filtering and wavel<strong>et</strong> shrinkage are two m<strong>et</strong>hods<br />

that can be applied for discontinuity-preserving <strong>de</strong>noising. In this talk we<br />

give a survey on relations b<strong>et</strong>ween both paradigms when space discr<strong>et</strong>e<br />

or fully discr<strong>et</strong>e versions of nonlinear diffusion filters are consi<strong>de</strong>red. We<br />

study a class of numerical schemes for nonlinear diffusion filtering that<br />

offers insights on the <strong>de</strong>sign of novel wavel<strong>et</strong> shrinkage rules for isotropic<br />

and anisotropic image enhancement. These schemes utilise analytical or<br />

semi-analytical solutions to dynamical systems that result from spacediscr<strong>et</strong>e<br />

nonlinear diffusion filtering on minimalistic images with 2 × 2<br />

pixels. They are applicable to singular nonlinear diffusion filters such as<br />

TV flow, to boun<strong>de</strong>d nonlinear diffusion filters of Perona—Malik type, and<br />

to tensor-driven anisotropic m<strong>et</strong>hods such as edge-enhancing or coherenceenhancing<br />

diffusion filtering. The fact that these schemes use processes<br />

within 2 × 2-pixel blocks allows to connect them to shift-invariant Haar<br />

wavel<strong>et</strong> shrinkage. This interpr<strong>et</strong>ation leads to novel shrinkage rules for<br />

two- and higher-dimensional images that are scalar- or vector-valued. Unlike<br />

classical shrinkage strategies they employ a diffusion-inspired coupling<br />

of the wavel<strong>et</strong> channels that guarantees an approximation with an excellent<br />

<strong>de</strong>gree of rotation invariance. Conversely, previousely used shrinkage<br />

functions can be i<strong>de</strong>ntified as corresponding to well—known diffusifities.<br />

Th<strong>et</strong>alkisbasedonjointworkwithJ.Weickert,M.Welk,P.Mrázek<br />

from the Saarland University.


Hand-written character recognition using spline wavel<strong>et</strong>s<br />

Karina Toscano, Ricardo Barrón, Humberto Sossa<br />

Centro <strong>de</strong> Investigación en Computación – IPN<br />

Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9<br />

Mexico City, 07738. MEXICO<br />

E-mails: likatome@hotmail.com, rbarron@cic.ipn.mx, hsossa@cic.ipn.mx<br />

Abstract<br />

Hand-written character recognition is important in multiple artificial intelligence<br />

applications. Many of the existent solutions use soft-computing mo<strong>de</strong>ls like neural n<strong>et</strong>works,<br />

support vector machines, and so on.<br />

Lately it has been propose to use mo<strong>de</strong>ls base on splines, to capture the trace essence to<br />

adjust no<strong>de</strong>s to the character an be able to make comparisons.<br />

In this work is generalized this i<strong>de</strong>a but using spline wavel<strong>et</strong>s to capture the characteristic<br />

of trace in different scales and be able to make discrimination more robust.<br />

Finally experiments are ma<strong>de</strong> to compare results and show advantages of the proposed<br />

m<strong>et</strong>hod.


Hand-written character recognition using spline wavel<strong>et</strong>s<br />

Karina Toscano, Ricardo Barrón, Humberto Sossa<br />

Centro <strong>de</strong> Investigación en Computación – IPN<br />

Av. Juan <strong>de</strong> Dios Bátiz, esq. Miguel Othon <strong>de</strong> Mendizábal 9<br />

Mexico City, 07738. MEXICO<br />

E-mails: likatome@hotmail.com, rbarron@cic.ipn.mx, hsossa@cic.ipn.mx<br />

Abstract<br />

Hand-written character recognition is important in multiple artificial intelligence<br />

applications. Many of the existent solutions use soft-computing mo<strong>de</strong>ls like neural n<strong>et</strong>works,<br />

support vector machines, and so on.<br />

Lately it has been propose to use mo<strong>de</strong>ls base on splines, to capture the trace essence to<br />

adjust no<strong>de</strong>s to the character an be able to make comparisons.<br />

In this work is generalized this i<strong>de</strong>a but using spline wavel<strong>et</strong>s to capture the characteristic<br />

of trace in different scales and be able to make discrimination more robust.<br />

Finally experiments are ma<strong>de</strong> to compare results and show advantages of the proposed<br />

m<strong>et</strong>hod.


WAVELETS AND MOVEMENTS<br />

DIFFERENT APPROACHES<br />

Leonardo Traversoni<br />

Univ. Autonoma M<strong>et</strong>. (Iztapalapa)<br />

Ciencias Basicas e Ingenieria,<br />

Ap Post 55-532, C.P. 09340 Mexico, 9340 Mexico D.F. Mexico<br />

ltd@xanum.uam.mx<br />

We present several approaches on movement <strong>de</strong>tection and recognition using<br />

wavel<strong>et</strong>s as well as the classical speed tuned wavel<strong>et</strong>s. As an alternative we propose<br />

to use a mother wavel<strong>et</strong> that actually <strong>de</strong>scribes a movement, a simple one, in or<strong>de</strong>r<br />

to build any other given by sparse data. We build such wavel<strong>et</strong> using stereoscopic<br />

vision and we show that in or<strong>de</strong>r to do that there are also several different<br />

approaches with advantages and disadvantages


Some results in discr<strong>et</strong>e Clifford analysis<br />

H. De Schepper, F. Sommen and L. Van <strong>de</strong> Voor<strong>de</strong><br />

Clifford Research Group, Department of Mathematical Analysis, Faculty of Engineering, Ghent University<br />

L<strong>et</strong> (e 1 ,... ,e m ) be the usual Eucli<strong>de</strong>an basis, taken as a s<strong>et</strong> of generators un<strong>de</strong>rlying the construction<br />

of the Clifford algebra R 0,m , where the geom<strong>et</strong>ric multiplication is governed through the <strong>de</strong>fining relations<br />

e 2 j = −1, j =1,... ,m and e je k + e k e j =0,j, k =1,... ,m. Standard (or orthogonal) Clifford analysis<br />

then usually focusses on the study of so—called monogenic functions, i.e. R 0,m valued null solutions of<br />

the Dirac operator ∂ = P m<br />

j=1 e j∂ xj . In this way, Clifford analysis is often seen as a direct and elegant<br />

generalization to higher dimensions of the theory of holomorphic functions in the complex plane, since the<br />

Dirac operator generalizes in a natural way the well—known Cauchy—Riemann operator. Crucial in the<br />

<strong>de</strong>velopment of the function theory is the factorization of the Laplacian by the Dirac operator: ∂ 2 = −∆,<br />

a basic feature un<strong>de</strong>rlying the proofs of the most important properties an d results. It is at the same<br />

time the reason why Cliffordanalysisisalsoconsi<strong>de</strong>redasarefinement of classical harmonic analysis,<br />

since monogenic functions refine the properties of harmonic functions.<br />

More recently, discr<strong>et</strong>ization has emerged as a new topic in Clifford analysis, focussing on discr<strong>et</strong>e<br />

counterparts of the concepts and results of the continuous function theory, in view of the eventual numerical<br />

treatment of boundary value problems and problems from potential theory. In this presentation,<br />

we aim at contributing to the further <strong>de</strong>velopment of a theor<strong>et</strong>ical framework for these discr<strong>et</strong>e versions<br />

of Clifford analysis. We use the factorization of the Laplacian, mentioned above for the continuous case,<br />

asastartingpointfor<strong>de</strong>fining, on specific geom<strong>et</strong>ric structures, discr<strong>et</strong>e Dirac operators which factorize<br />

a given discr<strong>et</strong>e Laplacian. A first example is the so—called “cross Laplacian” on Z m :<br />

Lf(x) =<br />

mX<br />

[f(x + e j ) − f(x − e j )] − 2mf(x)<br />

j=1<br />

In this case, factorizing Dirac operators has already been established by K. Guerlebeck and A. Hommel<br />

[1, 2], as well as by U. Kaehler and N. Faustino [3]. More generally, one may consi<strong>de</strong>r discr<strong>et</strong>e Laplacians<br />

with weight coefficients on a 3 m -cube centered around a point in Z m . However, in that case, no first<br />

or<strong>de</strong>r factorizations can be found within the usual context of the Clifford algebra R 0,m . A new axiomatic<br />

framework is nee<strong>de</strong>d, built on the notions of two new Clifford bases, e + j and e− j , j =1,... ,m, corresponding<br />

to the observation that also the partial <strong>de</strong>rivative ∂ xj shows two discr<strong>et</strong>ized versions: f(x + e j ) − f(x)<br />

and f(x) − f(x − e j ). Moreover, so—called curvature vectors have to be introduced. Based on these i<strong>de</strong>as,<br />

we <strong>de</strong>velop a theory of discr<strong>et</strong>e Dirac operators on rectangular and triangular grids in the two and three<br />

dimensional case, the techniques used leading to a factorization of any discr<strong>et</strong>e Laplacian in a cube or<br />

hexagon. Naturally, we also aim at discr<strong>et</strong>e versions of the function theor<strong>et</strong>ic properties of the Dirac<br />

operator, in particular a discr<strong>et</strong>e Borel-Pompeiu theorem as well as Cauchy’s integral forms, making use<br />

of a discr<strong>et</strong>e notion of boundary. In this presentation, we will present our first results.<br />

References<br />

[1]K.Guerlebeck,A.Hommel: Onfinite difference potentials and their applications in a discr<strong>et</strong>e<br />

function theory, Mathematical M<strong>et</strong>hods in the Applied Sciences 25 (2002), 1563—1576.<br />

[2] K. Guerlebeck, A. Hommel: On finite difference Dirac operators and their fundamental solutions,<br />

Advances in Applied Clifford Algebras 11 (2003), 89—106.<br />

[3] N. Faustino, U. Kaehler: Fischer <strong>de</strong>composition for difference Dirac operators, Advances in Applied<br />

Clifford Algebras 17 (2007), 37—58.


Variational image <strong>de</strong>composition mo<strong>de</strong>ls into cartoon and texture<br />

Luminita VESE<br />

Department of Mathematics, UCLA<br />

405, Hilgard Avenue<br />

Los Angeles, CA 90095-1555, U.S.A<br />

http://www.math.ucla.edu/~lvese<br />

In 2001, in an American Mathematical Soci<strong>et</strong>y lecture series entitled<br />

"Oscillating Patterns in Image Processing and Nonlinear Evolution Equations", Yves<br />

Meyer has analyzed and questioned the total variation minimization mo<strong>de</strong>l (Rudin,<br />

Osher, Fatemi) for separating cartoon from texture. He therefore proposed several<br />

refined variants of the TV mo<strong>de</strong>l, by substituting the L 2 norm to the square of the<br />

fi<strong>de</strong>lity term v=f-u by<br />

weaker norms of generalized functions. In particular, he proposed to mo<strong>de</strong>l the texture<br />

component v in a u+v mo<strong>de</strong>l by one of the spaces of generalized functions<br />

G=div(Linfinity), F=div(BMO) and E=Laplacian(B 1 _{infinity,infinity}).<br />

David Mumford and Basilis Gidas also show that images can be seen as samples<br />

from probability distributions of random variables supported on spaces of generalized<br />

functions, not on spaces of functions.<br />

However, it is not easy to solve such mo<strong>de</strong>ls in practice. In this talk, I will<br />

review Meyer's mo<strong>de</strong>ls and present some computational approaches for image<br />

restoration and image <strong>de</strong>composition into cartoon and texture.


Tight frames and their symm<strong>et</strong>ries<br />

Shayne Waldron<br />

Department of Mathematics (Rm 410)<br />

University of Auckland<br />

Private Bag 92019, Auckland<br />

New Zealand<br />

Frame <strong>de</strong>compositions are useful because they are technically similar to orthogonal expansions<br />

(they simply have more terms) and can be constructed to have <strong>de</strong>sirable properties that may be<br />

impossible for an orthogonal basis, e.g., in the case of wavel<strong>et</strong>s certain smoothness and small<br />

support properties.<br />

Here we show that frames are of interest for finite dimensional spaces where the <strong>de</strong>sirable<br />

properties are symm<strong>et</strong>ries of the un<strong>de</strong>rlying space (which an orthogonal basis cannot express).<br />

We present a number of (hopefully compelling) examples of tight frames. One of these is for the<br />

orthogonal polynomials of several variables for a weight which has some symm<strong>et</strong>ries. Another,<br />

which is important in quantum measurement theory, is the so called Heisenberg frames of d 2<br />

vectors in C d which have minimum cross correlation. We introduce the class of harmonic frames<br />

of n vectors in C d , which are generated by an abelian subgroup of symm<strong>et</strong>ries. For each n and d<br />

there are a finite number of harmonic frames, and we discuss how they can be obtained by using<br />

a symbolic algebra package such as MAGMA.


QWT: R<strong>et</strong>rospective and New Applications<br />

Author: Yi Xu<br />

Email: xuyi@sjtu.edu.cn<br />

Abstract: Quaternion wavel<strong>et</strong> transform (QWT) achieves much attention in recent years as a new<br />

multiscale analysis tool for geom<strong>et</strong>ric image structures. It is an extension of the real wavel<strong>et</strong><br />

transform and complex wavel<strong>et</strong> transform (CWT) by using the quaternion algebra and the 2-D<br />

Hilbert transform of filter theory. It brings exciting properties to many image applications as color<br />

image processing, object recognition, optical flow estimation and stereo matching. To give an<br />

overview of the <strong>de</strong>velopment of QWT and investigate its potential applications, this paper is<br />

organized as four parts.<br />

Section I provi<strong>de</strong>s a brief introduction of QWT. Section II presents a r<strong>et</strong>rospective of the<br />

evolution of QWT and its dominant applications. Compared with discr<strong>et</strong>e wavel<strong>et</strong> transform (DWT)<br />

and CWT, the <strong>de</strong>velopment of QWT is reviewed. The principles of quaternion wavel<strong>et</strong> construction<br />

are explored for achieving the important properties in multiscale analysis of geom<strong>et</strong>ric image<br />

structures, including the linear-phase property, shift-invariance property and compact support<br />

property with reduced computational complexity. Then the dominant applications of QWT in the<br />

existing research works are summarized. It indicates that the mechanism of adaptive scale<br />

representation of geom<strong>et</strong>ry features is important for such multiscale image analysis tasks. The<br />

improvement of the robustness and accuracy in two application instances of uncalibrated stereo<br />

matching and optical flow estimation stresses the importance of the mechanism.<br />

Section III switches its focus on the potential of QWT in new applications such as image fusion<br />

and registration. As for image fusion application, the reversibility of QWT is discussed. And then a<br />

new fusion scheme is advanced, incorporating Contourl<strong>et</strong> transform (CT) into the quaternion<br />

wavel<strong>et</strong> <strong>de</strong>composition scheme to enhance the direction selectivity of QWT. Because edges and<br />

textures are the intrinsic information in image representation, it is important to enhance them and<br />

thus improve the spatial resolution. CT involves the basis functions that are oriented at any<br />

power-of-two number of directions with flexible aspect ratios. Therefore the introduction of<br />

Contourl<strong>et</strong> into QWT scheme brings great probabilities to g<strong>et</strong> a b<strong>et</strong>ter representation of edges and<br />

textures than the original quaternion wavel<strong>et</strong> <strong>de</strong>composition scheme. The potential of modified<br />

QWT scheme in the new application of image fusion is then supported by the encouraging<br />

experimental results. As for image registration application, the 2-D phase concept of QWT is<br />

utilized to give an invariant feature <strong>de</strong>tector in scale space. 2-D phase congruency mo<strong>de</strong>l is<br />

discussed and then a dimensionless feature measure is proposed. The accordingly extracted features<br />

are important for the robust estimation of the image affine transform in registration task. We<br />

provi<strong>de</strong> several registration experiments with quantitative assessments to testify the proposed<br />

registration m<strong>et</strong>hod.<br />

Brief conclusion on the QWT <strong>de</strong>velopment experience is given in Section IV. In all, this paper<br />

aims to give a useful reference for the future use of QWT.<br />

KeyWords: Quaternion wavel<strong>et</strong> transform (QWT), multiscale image analysis

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