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UID:news1840@dmi.unibas.ch
DTSTAMP;TZID=Europe/Zurich:20250313T150350
DTSTART;TZID=Europe/Zurich:20250320T121500
SUMMARY:Bernoullis Tafelrunde: Remo Von Rickenbach (Universität Basel)
DESCRIPTION:Many problems from physics or engineering  result in partial d
 ifferential equations.   In both cases\, the unknown function \\(u\\) can
 \,  in most practically relevant applications\, only be approximated nume
 rically. Therefore\, it is essential to use efficient algorithms to approx
 imate \\(u\\) at as low costs as possible.\\r\\nTo build efficient algorit
 hms\, one first needs to understand how well a function of a given regular
 ity can be approximated. For example\, by using finite elements of grid si
 ze \\(h\\)  on the unit interval \\(I\\)\,  it is well established that 
 the approximation error decays as \\begin{align*}     \\inf_{v_h \\in V
 _h} \\|u - v_h\\|_{L^2(I)}     \\leq C h^s \\|u\\|_{H^{s}(I)}\,     
 \\quad 0 \\leq s \\leq d\, \\end{align*} where \\(d \\in \\mathbb{N}\\) is
  the polynomial order  of the trial functions involved.\\r\\nHowever\, wh
 at can we say about the approximation order if  \\(u\\) is only piecewise
  regular\,  but admits a singularity and is therefore not in \\(H^{s}(I)\
 \)? For this\,  adaptive schemes\, which rely on the concept of \\emph{no
 nlinear approximation}\, need to be studied.\\r\\nIn this talk\, some basi
 c concepts and examples of approximation theory will be introduced and we 
 will characterise the approximation spaces with respect to some common bas
 is systems. In particular\, we will see that the approximation spaces with
  respect to nonlinear approximation by wavelet bases contain Besov spaces 
 which are strictly larger than the corresponding\, classical finite elemen
 t approximation spaces\,  showing that adaptive schemes strictly outperfo
 rm classical schemes in the case of limited regularity.\\r\\nabstract [t3:
 //file?uid=3857]
X-ALT-DESC:<p>Many problems from physics or engineering&nbsp\;<br /> result
  in partial differential equations. &nbsp\;<br /> In both cases\, the unkn
 own function \\(u\\) can\,&nbsp\;<br /> in most practically relevant appli
 cations\,<br /> only be approximated numerically.<br /> Therefore\, it is 
 essential to use efficient algorithms to approximate<br /> \\(u\\) at as l
 ow costs as possible.</p>\n<p>To build efficient algorithms\, one first ne
 eds to understand how well a function<br /> of a given regularity can be a
 pproximated.<br /> For example\, by using finite elements of grid size \\(
 h\\)&nbsp\;<br /> on the unit interval \\(I\\)\,&nbsp\;<br /> it is well e
 stablished that the approximation error decays as<br /> \\begin{align*}<br
  /> &nbsp\;&nbsp\; &nbsp\;\\inf_{v_h \\in V_h} \\|u - v_h\\|_{L^2(I)}<br /
 > &nbsp\;&nbsp\; &nbsp\;\\leq C h^s \\|u\\|_{H^{s}(I)}\,<br /> &nbsp\;&nbs
 p\; &nbsp\;\\quad 0 \\leq s \\leq d\,<br /> \\end{align*}<br /> where \\(d
  \\in \\mathbb{N}\\) is the polynomial order&nbsp\;<br /> of the trial fun
 ctions involved.</p>\n<p>However\, what can we say about the approximation
  order if&nbsp\;<br /> \\(u\\) is only piecewise regular\,&nbsp\;<br /> bu
 t admits a singularity and is therefore not in \\(H^{s}(I)\\)?<br /> For t
 his\,&nbsp\;<br /> adaptive schemes\, which rely on the concept of \\emph{
 nonlinear approximation}\,<br /> need to be studied.</p>\n<p>In this talk\
 , some basic concepts and examples of approximation theory will be<br /> i
 ntroduced and we will characterise the approximation spaces with respect t
 o<br /> some common basis systems.<br /> In particular\, we will see that 
 the approximation spaces with respect to<br /> nonlinear approximation by 
 wavelet bases contain Besov spaces which are strictly<br /> larger than th
 e corresponding\, classical finite element approximation spaces\,&nbsp\;<b
 r /> showing that adaptive schemes strictly outperform classical schemes i
 n the case<br /> of limited regularity.</p>\n<p><a href="t3://file?uid=385
 7">abstract</a></p>
DTEND;TZID=Europe/Zurich:20250320T130000
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