[cig-commits] r22787 - in seismo/3D/SPECFEM3D_GLOBE: branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL trunk/doc/USER_MANUAL

dkomati1 at geodynamics.org dkomati1 at geodynamics.org
Fri Sep 13 13:07:54 PDT 2013


Author: dkomati1
Date: 2013-09-13 13:07:54 -0700 (Fri, 13 Sep 2013)
New Revision: 22787

Modified:
   seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/bibliography.bib
   seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.pdf
   seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex
   seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/bibliography.bib
   seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.pdf
   seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex
Log:
added Ainsworth


Modified: seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/bibliography.bib
===================================================================
--- seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/bibliography.bib	2013-09-13 20:00:19 UTC (rev 22786)
+++ seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/bibliography.bib	2013-09-13 20:07:54 UTC (rev 22787)
@@ -14327,3 +14327,25 @@
 	less than plus or minus one~second}
 }
 
+ at article{AiWa09,
+author = {Ainsworth, M. and Wajid, H.},
+title = {Dispersive and Dissipative Behavior of the Spectral Element Method},
+journal = {SIAM Journal on Numerical Analysis},
+volume = {47},
+number = {5},
+pages = {3910-3937},
+year = {2009},
+doi = {10.1137/080724976}
+}
+
+ at article{AiWa10,
+author = {Ainsworth, M. and Wajid, H.},
+title = {Optimally Blended Spectral-Finite Element Scheme for Wave Propagation and NonStandard Reduced Integration},
+journal = {SIAM Journal on Numerical Analysis},
+volume = {48},
+number = {1},
+pages = {346-371},
+year = {2010},
+doi = {10.1137/090754017}
+}
+

Modified: seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.pdf
===================================================================
(Binary files differ)

Modified: seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex
===================================================================
--- seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex	2013-09-13 20:00:19 UTC (rev 22786)
+++ seismo/3D/SPECFEM3D_GLOBE/branches/SPECFEM3D_GLOBE_SUNFLOWER/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex	2013-09-13 20:07:54 UTC (rev 22787)
@@ -190,7 +190,7 @@
 it is then close to a particular case of the discontinuous Galerkin technique \citep{ReHi73,LeRa74,Arn82,JoPi86,BoMaHe91,FaRi99,HuHuRa99,CoKaSh00,GiHeWa02,RiWh03,MoRi05,GrScSc06,AiMoMu06,BeLaPi06,DuKa06,DeSeWh08,PuAmKa09,WiStBuGh10,DeSe10,EtChViGl10}, with optimized efficiency because of its tensorized basis functions \citep{WiStBuGh10,AcKo11}.
 In particular, it can accurately handle very distorted mesh elements \citep{OlSe11}.\\
 
-It has very good accuracy and convergence properties \citep{MaPa89,SePr94,DeFiMu02,Coh02,DeSe07,SeOl08,MeStTh12}.
+It has very good accuracy and convergence properties \citep{MaPa89,SePr94,DeFiMu02,Coh02,DeSe07,SeOl08,AiWa09,AiWa10,MeStTh12}.
 The spectral element approach admits spectral rates of convergence and allows exploiting $hp$-convergence schemes.
 It is also very well suited to parallel implementation on very large supercomputers \citep{KoTsChTr03,TsKoChTr03,KoLaMi08a,CaKoLaTiMiLeSnTr08,KoViCh10} as well as on clusters of GPU accelerating graphics cards \citep{KoMiEr09,KoErGoMi10,Kom11}. Tensor products inside each element can be optimized to reach very high efficiency \citep{DeFiMu02}, and mesh point and element numbering can be optimized to reduce processor cache misses and improve cache reuse \citep{KoLaMi08a}. The SEM can also handle triangular (in 2D) or tetrahedral (in 3D) elements \citep{WinBoyd96,TaWi00,KoMaTrTaWi01,Coh02,MeViSa06} as well as mixed meshes, although with increased cost and reduced accuracy in these elements, as in the discontinuous Galerkin method.\\
 

Modified: seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/bibliography.bib
===================================================================
--- seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/bibliography.bib	2013-09-13 20:00:19 UTC (rev 22786)
+++ seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/bibliography.bib	2013-09-13 20:07:54 UTC (rev 22787)
@@ -14327,3 +14327,25 @@
 	less than plus or minus one~second}
 }
 
+ at article{AiWa09,
+author = {Ainsworth, M. and Wajid, H.},
+title = {Dispersive and Dissipative Behavior of the Spectral Element Method},
+journal = {SIAM Journal on Numerical Analysis},
+volume = {47},
+number = {5},
+pages = {3910-3937},
+year = {2009},
+doi = {10.1137/080724976}
+}
+
+ at article{AiWa10,
+author = {Ainsworth, M. and Wajid, H.},
+title = {Optimally Blended Spectral-Finite Element Scheme for Wave Propagation and NonStandard Reduced Integration},
+journal = {SIAM Journal on Numerical Analysis},
+volume = {48},
+number = {1},
+pages = {346-371},
+year = {2010},
+doi = {10.1137/090754017}
+}
+

Modified: seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.pdf
===================================================================
(Binary files differ)

Modified: seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex
===================================================================
--- seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex	2013-09-13 20:00:19 UTC (rev 22786)
+++ seismo/3D/SPECFEM3D_GLOBE/trunk/doc/USER_MANUAL/manual_SPECFEM3D_GLOBE.tex	2013-09-13 20:07:54 UTC (rev 22787)
@@ -190,7 +190,7 @@
 it is then close to a particular case of the discontinuous Galerkin technique \citep{ReHi73,LeRa74,Arn82,JoPi86,BoMaHe91,FaRi99,HuHuRa99,CoKaSh00,GiHeWa02,RiWh03,MoRi05,GrScSc06,AiMoMu06,BeLaPi06,DuKa06,DeSeWh08,PuAmKa09,WiStBuGh10,DeSe10,EtChViGl10}, with optimized efficiency because of its tensorized basis functions \citep{WiStBuGh10,AcKo11}.
 In particular, it can accurately handle very distorted mesh elements \citep{OlSe11}.\\
 
-It has very good accuracy and convergence properties \citep{MaPa89,SePr94,DeFiMu02,Coh02,DeSe07,SeOl08,MeStTh12}.
+It has very good accuracy and convergence properties \citep{MaPa89,SePr94,DeFiMu02,Coh02,DeSe07,SeOl08,AiWa09,AiWa10,MeStTh12}.
 The spectral element approach admits spectral rates of convergence and allows exploiting $hp$-convergence schemes.
 It is also very well suited to parallel implementation on very large supercomputers \citep{KoTsChTr03,TsKoChTr03,KoLaMi08a,CaKoLaTiMiLeSnTr08,KoViCh10} as well as on clusters of GPU accelerating graphics cards \citep{KoMiEr09,KoErGoMi10,Kom11}. Tensor products inside each element can be optimized to reach very high efficiency \citep{DeFiMu02}, and mesh point and element numbering can be optimized to reduce processor cache misses and improve cache reuse \citep{KoLaMi08a}. The SEM can also handle triangular (in 2D) or tetrahedral (in 3D) elements \citep{WinBoyd96,TaWi00,KoMaTrTaWi01,Coh02,MeViSa06} as well as mixed meshes, although with increased cost and reduced accuracy in these elements, as in the discontinuous Galerkin method.\\
 



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