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Date: Tue, 06 Aug 2019 07:23:13 -0700
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Subject: intitle:"discontinuous galerkin" - new results
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<!doctype html><html xmlns=3D"http://www.w3.org/1999/xhtml" xmlns:o=3D"urn:=
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e_alrt_title{text-decoration:none}.gse_alrt_title:hover{text-decoration:und=
erline} @media screen and (max-width: 599px) {.gse_alrt_sni br{display:none=
;}}</style></head><body><!--[if gte mso 9]><table cellpadding=3D"0" cellspa=
cing=3D"0" border=3D"0"><tr><td style=3D"width:600px"><![endif]--><div styl=
e=3D"font-family:arial,sans-serif;font-size:13px;line-height:16px;color:#22=
2;width:100%;max-width:600px"><h3 style=3D"font-weight:normal;margin:0;font=
-size:17px;line-height:20px;"><a href=3D"http://scholar.google.com/scholar_=
url?url=3Dhttps://www.sciencedirect.com/science/article/pii/S03770427193034=
37&amp;hl=3Den&amp;sa=3DX&amp;d=3D9222642871868013544&amp;scisig=3DAAGBfm3I=
Hl7UyTjMHOY7Seac24wm8mu8pA&amp;nossl=3D1&amp;oi=3Dscholaralrt&amp;hist=3Dy9=
_vR9YAAAAJ:17743408003912531268:AAGBfm2ie58E1eRXxYl0R6E3nn-dlaashg" class=
=3D"gse_alrt_title" style=3D"font-size:17px;color:#1a0dab">Multiscale hybri=
dizable <b>discontinuous Galerkin </b>method for elliptic problems in perfo=
rated domains</a></h3><div style=3D"color:#006621">K Cho, M Moon=C2=A0- Jou=
rnal of Computational and Applied Mathematics, 2019</div><div class=3D"gse_=
alrt_sni">We propose a multiscale hybridizable <b>discontinuous Galerkin </=
b>method in perforated <br>domains. Perforations may have various shapes an=
d sizes. Following Generalized <br>Multiscale Finite Element method, local =
snapshot spaces are constructed by solving=C2=A0=E2=80=A6</div><div style=
=3D"width:auto"><table cellpadding=3D"0" cellspacing=3D"0" border=3D"0"><tb=
ody><tr><td style=3D"padding-right:4px;mso-padding-alt:4px 16px 0 0;"><a hr=
ef=3D"http://scholar.google.com/scholar_share?hl=3Den&amp;oi=3Dscholaralrt&=
amp;ss=3Dtw&amp;url=3Dhttps://www.sciencedirect.com/science/article/pii/S03=
77042719303437&amp;rt=3DMultiscale+hybridizable+discontinuous+Galerkin+meth=
od+for+elliptic+problems+in+perforated+domains&amp;scisig=3DAAGBfm1Yr4oAKEp=
lXHH2AY3o-pEGMsnV8g" style=3D"text-decoration:none;display:inline-block;pad=
ding:4px 8px 4px 0;mso-padding-alt:0;"><img alt=3D"Twitter" src=3D"http://s=
cholar.google.com/intl/en/scholar/images/1x/tw-32.png" border=3D"0" height=
=3D"16" width=3D"16" style=3D"vertical-align:top"></a></td><td style=3D"pad=
ding-right:4px;mso-padding-alt:4px 16px 0 0;"><a href=3D"http://scholar.goo=
gle.com/scholar_share?hl=3Den&amp;oi=3Dscholaralrt&amp;ss=3Dfb&amp;url=3Dht=
tps://www.sciencedirect.com/science/article/pii/S0377042719303437&amp;rt=3D=
Multiscale+hybridizable+discontinuous+Galerkin+method+for+elliptic+problems=
+in+perforated+domains&amp;scisig=3DAAGBfm1Yr4oAKEplXHH2AY3o-pEGMsnV8g" sty=
le=3D"text-decoration:none;display:inline-block;padding:4px 8px;mso-padding=
-alt:0"><img alt=3D"Facebook" src=3D"http://scholar.google.com/intl/en/scho=
lar/images/1x/fb-32.png" border=3D"0" height=3D"16" width=3D"16" style=3D"v=
ertical-align:top"></a></td></tr></tbody></table></div><br><h3 style=3D"fon=
t-weight:normal;margin:0;font-size:17px;line-height:20px;"><a href=3D"http:=
//scholar.google.com/scholar_url?url=3Dhttp://congress.cimne.com/iga2019/ad=
min/files/fileabstract/a214.pdf&amp;hl=3Den&amp;sa=3DX&amp;d=3D153370534435=
86414985&amp;scisig=3DAAGBfm3D_15tBDGWfEKhIFgTbHikCr1JBw&amp;nossl=3D1&amp;=
oi=3Dscholaralrt&amp;hist=3Dy9_vR9YAAAAJ:17743408003912531268:AAGBfm2ie58E1=
eRXxYl0R6E3nn-dlaashg" class=3D"gse_alrt_title" style=3D"font-size:17px;col=
or:#1a0dab">An Arbitrary Lagrangian Eulerian Formulation for Isogeometric <=
b>Discontinuous Galerkin </b>Schemes</a></h3><div style=3D"color:#006621">S=
 Pezzano, R Duvigneau</div><div class=3D"gse_alrt_sni">In this work the Iso=
geometric <b>Discontinuous Galerkin </b>[1] method for solving <br>hyperbol=
ic conservation laws is extended to time dependent geometries using an <br>=
Arbitrary Lagrangian Eulerian (ALE) approach. Among the various ALE formula=
tions=C2=A0=E2=80=A6</div><div style=3D"width:auto"><table cellpadding=3D"0=
" cellspacing=3D"0" border=3D"0"><tbody><tr><td style=3D"padding-right:4px;=
mso-padding-alt:4px 16px 0 0;"><a href=3D"http://scholar.google.com/scholar=
_share?hl=3Den&amp;oi=3Dscholaralrt&amp;ss=3Dtw&amp;url=3Dhttp://congress.c=
imne.com/iga2019/admin/files/fileabstract/a214.pdf&amp;rt=3DAn+Arbitrary+La=
grangian+Eulerian+Formulation+for+Isogeometric+Discontinuous+Galerkin+Schem=
es&amp;scisig=3DAAGBfm23nT1WVM4DidjuNf53fW60y00lmw" style=3D"text-decoratio=
n:none;display:inline-block;padding:4px 8px 4px 0;mso-padding-alt:0;"><img =
alt=3D"Twitter" src=3D"http://scholar.google.com/intl/en/scholar/images/1x/=
tw-32.png" border=3D"0" height=3D"16" width=3D"16" style=3D"vertical-align:=
top"></a></td><td style=3D"padding-right:4px;mso-padding-alt:4px 16px 0 0;"=
><a href=3D"http://scholar.google.com/scholar_share?hl=3Den&amp;oi=3Dschola=
ralrt&amp;ss=3Dfb&amp;url=3Dhttp://congress.cimne.com/iga2019/admin/files/f=
ileabstract/a214.pdf&amp;rt=3DAn+Arbitrary+Lagrangian+Eulerian+Formulation+=
for+Isogeometric+Discontinuous+Galerkin+Schemes&amp;scisig=3DAAGBfm23nT1WVM=
4DidjuNf53fW60y00lmw" style=3D"text-decoration:none;display:inline-block;pa=
dding:4px 8px;mso-padding-alt:0"><img alt=3D"Facebook" src=3D"http://schola=
r.google.com/intl/en/scholar/images/1x/fb-32.png" border=3D"0" height=3D"16=
" width=3D"16" style=3D"vertical-align:top"></a></td></tr></tbody></table><=
/div><br><h3 style=3D"font-weight:normal;margin:0;font-size:17px;line-heigh=
t:20px;"><a href=3D"http://scholar.google.com/scholar_url?url=3Dhttp://cong=
ress.cimne.com/iga2019/admin/files/fileabstract/a197.pdf&amp;hl=3Den&amp;sa=
=3DX&amp;d=3D11420218679413567025&amp;scisig=3DAAGBfm3q_EhUxa2JRDFl6YPXctUs=
05VWqg&amp;nossl=3D1&amp;oi=3Dscholaralrt&amp;hist=3Dy9_vR9YAAAAJ:177434080=
03912531268:AAGBfm2ie58E1eRXxYl0R6E3nn-dlaashg" class=3D"gse_alrt_title" st=
yle=3D"font-size:17px;color:#1a0dab">Shape Sensitivity Analysis for Hyperbo=
lic Systems using an Isogeometric <b>Discontinuous Galerkin </b>Method</a><=
/h3><div style=3D"color:#006621">M Stauffert, R Duvigneau</div><div class=
=3D"gse_alrt_sni">The framework of this work is the Isogeometric <b>Discont=
inuous Galerkin </b>(IDG) method, <br>presented in [1], which relies on the=
 coupling of a <b>Discontinuous Galerkin </b>formulation <br>and NURBS repr=
esentations. This methodology allows to solve partial differential=C2=A0=E2=
=80=A6</div><div style=3D"width:auto"><table cellpadding=3D"0" cellspacing=
=3D"0" border=3D"0"><tbody><tr><td style=3D"padding-right:4px;mso-padding-a=
lt:4px 16px 0 0;"><a href=3D"http://scholar.google.com/scholar_share?hl=3De=
n&amp;oi=3Dscholaralrt&amp;ss=3Dtw&amp;url=3Dhttp://congress.cimne.com/iga2=
019/admin/files/fileabstract/a197.pdf&amp;rt=3DShape+Sensitivity+Analysis+f=
or+Hyperbolic+Systems+using+an+Isogeometric+Discontinuous+Galerkin+Method&a=
mp;scisig=3DAAGBfm33SjYlPgIWozgZnPQywZnZJO3lxA" style=3D"text-decoration:no=
ne;display:inline-block;padding:4px 8px 4px 0;mso-padding-alt:0;"><img alt=
=3D"Twitter" src=3D"http://scholar.google.com/intl/en/scholar/images/1x/tw-=
32.png" border=3D"0" height=3D"16" width=3D"16" style=3D"vertical-align:top=
"></a></td><td style=3D"padding-right:4px;mso-padding-alt:4px 16px 0 0;"><a=
 href=3D"http://scholar.google.com/scholar_share?hl=3Den&amp;oi=3Dscholaral=
rt&amp;ss=3Dfb&amp;url=3Dhttp://congress.cimne.com/iga2019/admin/files/file=
abstract/a197.pdf&amp;rt=3DShape+Sensitivity+Analysis+for+Hyperbolic+System=
s+using+an+Isogeometric+Discontinuous+Galerkin+Method&amp;scisig=3DAAGBfm33=
SjYlPgIWozgZnPQywZnZJO3lxA" style=3D"text-decoration:none;display:inline-bl=
ock;padding:4px 8px;mso-padding-alt:0"><img alt=3D"Facebook" src=3D"http://=
scholar.google.com/intl/en/scholar/images/1x/fb-32.png" border=3D"0" height=
=3D"16" width=3D"16" style=3D"vertical-align:top"></a></td></tr></tbody></t=
able></div><br><h3 style=3D"font-weight:normal;margin:0;font-size:17px;line=
-height:20px;"><a href=3D"http://scholar.google.com/scholar_url?url=3Dhttp:=
//congress.cimne.com/iga2019/admin/files/fileabstract/a206.pdf&amp;hl=3Den&=
amp;sa=3DX&amp;d=3D11456305957596265494&amp;scisig=3DAAGBfm0utF7FCmBU1PKa_4=
g8_-gbMI1rWg&amp;nossl=3D1&amp;oi=3Dscholaralrt&amp;hist=3Dy9_vR9YAAAAJ:177=
43408003912531268:AAGBfm2ie58E1eRXxYl0R6E3nn-dlaashg" class=3D"gse_alrt_tit=
le" style=3D"font-size:17px;color:#1a0dab">Adaptive Refinement for Compress=
ible Flow Analysis using an Isogeometric <b>Discontinuous Galerkin </b>Meth=
od</a></h3><div style=3D"color:#006621">R Duvigneau, A Jaeschke, M M=C3=B6l=
ler, M M=C3=B6ller=E2=80=A6</div><div class=3D"gse_alrt_sni">This work aims=
 at developping an efficient isogeometric approach to simulate <br>compress=
ible flows including shocks. The use of the classical isogeometric analysis=
 <br>method based on a finite-element formulation [1] is tedious in this co=
ntext, due to the=C2=A0=E2=80=A6</div><div style=3D"width:auto"><table cell=
padding=3D"0" cellspacing=3D"0" border=3D"0"><tbody><tr><td style=3D"paddin=
g-right:4px;mso-padding-alt:4px 16px 0 0;"><a href=3D"http://scholar.google=
.com/scholar_share?hl=3Den&amp;oi=3Dscholaralrt&amp;ss=3Dtw&amp;url=3Dhttp:=
//congress.cimne.com/iga2019/admin/files/fileabstract/a206.pdf&amp;rt=3DAda=
ptive+Refinement+for+Compressible+Flow+Analysis+using+an+Isogeometric+Disco=
ntinuous+Galerkin+Method&amp;scisig=3DAAGBfm3WaZFnuqnrYAqUzFxqL_X5dp5pRw" s=
tyle=3D"text-decoration:none;display:inline-block;padding:4px 8px 4px 0;mso=
-padding-alt:0;"><img alt=3D"Twitter" src=3D"http://scholar.google.com/intl=
/en/scholar/images/1x/tw-32.png" border=3D"0" height=3D"16" width=3D"16" st=
yle=3D"vertical-align:top"></a></td><td style=3D"padding-right:4px;mso-padd=
ing-alt:4px 16px 0 0;"><a href=3D"http://scholar.google.com/scholar_share?h=
l=3Den&amp;oi=3Dscholaralrt&amp;ss=3Dfb&amp;url=3Dhttp://congress.cimne.com=
/iga2019/admin/files/fileabstract/a206.pdf&amp;rt=3DAdaptive+Refinement+for=
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thod&amp;scisig=3DAAGBfm3WaZFnuqnrYAqUzFxqL_X5dp5pRw" style=3D"text-decorat=
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