From 2cb5e4e94d1532790245c4b08462debbe1283785 Mon Sep 17 00:00:00 2001 From: Martin Kronbichler Date: Fri, 24 Apr 2020 16:22:49 +0200 Subject: [PATCH] Make myself co-author --- 9.2/paper.tex | 95 +++++++++++++++++++-------------------------------- 1 file changed, 35 insertions(+), 60 deletions(-) diff --git a/9.2/paper.tex b/9.2/paper.tex index 419b751..e67ab2a 100644 --- a/9.2/paper.tex +++ b/9.2/paper.tex @@ -44,7 +44,7 @@ % Graham Harper, Timo Heister, % Luca Heltai, -% Martin Kronbichler, + Martin Kronbichler, % Ross Maguire Kynch, % Matthias Maier, % Jean-Paul Pelteret, @@ -62,39 +62,39 @@ % Oak Ridge National Laboratory, 1 Bethel Valley Rd., % TN 37831, USA. % {\texttt{\{arndtd,turcksinbr\}@ornl.gov}}} -% +% % \author[2]{Wolfgang~Bangerth} % \affil[2]{Department of Mathematics, Colorado State University, Fort % Collins, CO 80523-1874, USA. % {\texttt{bangerth@colostate.edu}, % \texttt{harper@math.colostate.edu}}} -% +% % \author[3]{Thomas~C.~Clevenger} % \affil[3]{School of Mathematical and Statistical Sciences, % Clemson University, % Clemson, SC, 29634, USA % {\texttt{\{tcleven, heister\}@clemson.edu}}} -% +% % \author[4]{Denis~Davydov} % \affil[4]{Chair of Applied Mechanics, % Friedrich-Alexander-Universit\"{a}t Erlangen-N\"{u}rnberg, % Egerlandstr.\ 5, % 91058 Erlangen, Germany. % {\texttt{\{denis.davydov,jean-paul.pelteret\}@fau.de}}} -% +% % \author[5]{Marc~Fehling} % \affil[5]{Institute for Advanced Simulation, % Forschungszentrum J\"{u}lich GmbH, % 52425 J\"{u}lich, Germany. % {\texttt{m.fehling@fz-juelich.de}}} -% +% % \author[6]{Daniel Garcia-Sanchez} % \affil[6]{Sorbonne Universit\'es, UPMC Univ.\ Paris 06, CNRS-UMR 7588, % Institut des NanoSciences de Paris, F-75005, Paris, France % {\texttt{daniel.garcia-sanchez@insp.upmc.fr}}} -% +% % \author[2]{Graham Harper} -% +% \author[3]{Timo~Heister} \affil[3]{School of Mathematical and Statistical Sciences, Clemson University, @@ -108,30 +108,30 @@ % Via Bonomea 265, % 34136, Trieste, Italy. % {\texttt{luca.heltai@sissa.it}}} -% -% \author[9]{Martin~Kronbichler} -% \affil[9]{Institute for Computational Mechanics, -% Technical University of Munich, -% Boltzmannstr.~15, 85748 Garching, Germany. -% {\texttt{kronbichler@lnm.mw.tum.de}}} -% +% + \author[9]{Martin~Kronbichler} + \affil[9]{Institute for Computational Mechanics, + Technical University of Munich, + Boltzmannstr.~15, 85748 Garching, Germany. + {\texttt{kronbichler@lnm.mw.tum.de}}} +% % \author[10]{Ross~Maguire~Kynch} % \affil[10]{Zienkiewicz Centre for Computational Engineering, % College of Engineering, Swansea University, % Bay Campus, Fabian Way, Swansea SA1 8EN, Wales, UK. % {\texttt{rkynch@gmail.com}}} -% +% % \author[11]{Matthias~Maier} % \affil[11]{Department of Mathematics, % Texas A\&M University, % 3368 TAMU, % College Station, TX 77845, USA. % {\texttt{maier@math.tamu.edu}}} -% +% % \author[4]{Jean-Paul~Pelteret} -% +% % \author[*1]{Bruno~Turcksin} -% +% % \author[12]{David Wells} % \affil[12]{Department of Mathematics, University of North Carolina, % Chapel Hill, NC 27516, USA. @@ -213,14 +213,14 @@ that we briefly outline in the remainder of this section: % tensor product evaluators according to the performance analysis of % \cite{KronbichlerKormann2019} in the context of more quadrature points than % shape functions has been revised for better performance. -% +% % \item A new class \texttt{ParsedConvergenceTable} has been introduced % that greatly simplifies the construction of convergence tables, % reading the options for the generation of the table from a parameter % file, and providing methods that, combined with a parameter file, % allow one to generate convergence tables using one-liners in user % codes. -% +% % \item % The \texttt{FE\_BernardiRaugel} class implements the non-standard % Bernardi-Raugel (BR) element that can be used to construct a stable @@ -232,7 +232,7 @@ that we briefly outline in the remainder of this section: % stable but converges with only first-order at the cost of the large % number of velocity unknowns. The BR space is thus intermediate between the % $Q_1^d$ and $Q_2^d$ spaces. -% +% % The element is currently only implemented for parallelogram meshes due to % difficulties associated with the mapping of shape functions: The shape % functions of the $Q_1^d$ part of the element need to be mapped as @@ -242,7 +242,7 @@ that we briefly outline in the remainder of this section: % element. \dealii{} does not currently have the ability to use different % mappings for individual shape functions, though this functionality is % planned for the next release. -% +% % \item % The \texttt{FE\_NedelecSZ} class is a new implementation of the % N{\'e}d{\'e}lec element on quadrilaterals and hexahedra. It is based on @@ -256,7 +256,7 @@ that we briefly outline in the remainder of this section: % assigning a globally defined orientation to local edges and faces. A % detailed overview of the implementation of the \texttt{FE\_NedelecSZ} % element in \dealii{} can be found in \cite{Kynch2017}. -% +% % \item All of the elementary geometrical objects of the library (namely % \texttt{Point}, \texttt{Segment}, and % \texttt{BoundingBox}) have been augmented with the traits @@ -302,40 +302,15 @@ part of this release. In particular, we have converted many places that now allow for simpler code through the use of C++11 features such as range-based for loops and lambda functions. -In addition, there are four new tutorial programs and one new code -gallery program: +In addition, there are seven new tutorial programs: \begin{itemize} -\item -% \texttt{step-61} is a program that implements the ``weak -% Galerkin'' method to solve the Laplace equation. Weak Galerkin -% methods are related to the Hybridized Discontinuous Galerkin method -% in that they introduce degrees of freedom on the interfaces between -% cells, but they do not require the reformulation of the problem as a -% first-order system and instead re-define what the gradient of a -% discontinuous function is. -% -% \item \texttt{step-62} demonstrates the solution of problems related -% to phononic or photonic crystals. Among the techniques shown in this -% program is the solution of complex-valued linear systems, and the -% use of absorbing boundary conditions through the Perfectly Matched -% Layer technique. -% -% \item \texttt{step-63} implements a geometric multigrid preconditioner -% and solver for the advection-diffusion equation, yielding optimal -% complexity. The tutorial compares -% point-based smoothers to cell-based smoothers and -% demonstrates the effect of downstream ordering on smoother performance. -% -% \item \texttt{step-64} demonstrates the usage of matrix-free methods on Nvidia GPUs. -% GPUs are shown to be advantageous for these kind of operations because of their superior -% hardware characteristics, in particular a higher memory bandwidth than server -% CPUs within a given power envelope. -% -% \item The \texttt{MCMC-Laplace} code gallery program is a code useful -% for the forward solution used as a building block in -% Bayesian inverse problems, and for sampling the parameter space -% through a Metropolis--Hastings sampler (a kind of Monte Carlo -% Markov Chain method). +\item \texttt{step-47} +\item \texttt{step-50} +\item \texttt{step-58} +\item \texttt{step-65} +\item \texttt{step-67} +\item \texttt{step-69} +\item \texttt{step-70} \end{itemize} @@ -343,8 +318,8 @@ gallery program: \subsection{Incompatible changes} The 9.2 release includes -\href{https://dealii.org/developer/doxygen/deal.II/changes_between_9_0_1_and_9_1_0.html} - {around 15 incompatible changes}; see \cite{changes91}. The majority of these changes +\href{https://dealii.org/developer/doxygen/deal.II/changes_between_9_1_1_and_9_2_0.html} + {around 15 incompatible changes}; see \cite{changes92}. The majority of these changes should not be visible to typical user codes; some remove previously deprecated classes and functions; and the majority change internal interfaces that are not usually used in external @@ -450,7 +425,7 @@ Please consider citing the appropriate references if you use interfaces to these libraries. The two previous releases of \dealii can be cited as -\cite{dealII85,dealII90}. +\cite{dealII90,dealII91}. \section{Acknowledgments} -- 2.39.5