From 69cc6035bc26ed603ba6b07e1009a30f83d53925 Mon Sep 17 00:00:00 2001 From: Jiuhua Hu Date: Wed, 7 Aug 2019 16:07:14 -0600 Subject: [PATCH] replace the paper by index --- examples/step-51/doc/intro.dox | 7 +------ 1 file changed, 1 insertion(+), 6 deletions(-) diff --git a/examples/step-51/doc/intro.dox b/examples/step-51/doc/intro.dox index fb63724b66..68e71d234e 100644 --- a/examples/step-51/doc/intro.dox +++ b/examples/step-51/doc/intro.dox @@ -30,12 +30,7 @@ for systems of equations in 2 or 3 dimensions. To alleviate the computational cost of solving such large linear systems, the hybridizable discontinuous Galerkin (HDG) methodology was introduced by Cockburn and co-workers -(see the references in the recent HDG overview article by - N.C. Nguyen and J. Peraire: - Hybridizable discontinuous Galerkin methods for partial differential - equations in continuum mechanics, Journal of Computational Physics, - 2012, 231:18, 5955-5988. - [DOI]). +(see the references in the recent HDG overview article by N.C. Nguyen and J. Peraire @cite{Ngu2012}). The HDG method achieves this goal by formulating the mathematical problem using Dirichlet-to-Neumann mappings. The partial differential equations are first written as a first -- 2.39.5