journal = {Journal of Scientific Computing}
}
+%-------------------------------------------------------------------------------
+% Step 10
+%-------------------------------------------------------------------------------
+
+@incollection{Cangiani2012,
+ doi = {10.1007/978-3-642-33134-3_34},
+ url = {https://doi.org/10.1007/978-3-642-33134-3_34},
+ year = {2012},
+ month = nov,
+ publisher = {Springer Berlin Heidelberg},
+ pages = {315--322},
+ author = {A. Cangiani and J. Chapman and E. H. Georgoulis and M. Jensen},
+ title = {Implementation of the Continuous-Discontinuous Galerkin Finite Element Method},
+ booktitle = {Numerical Mathematics and Advanced Applications 2011}
+}
+
%-------------------------------------------------------------------------------
% Step 14
%-------------------------------------------------------------------------------
* degrees of freedom to the FE_Nothing cells, and this subregion is therefore
* implicitly deleted from the computation. step-10 and step-46 show use cases
* for this element. An interesting application for this element is also
- * presented in the paper A. Cangiani, J. Chapman, E. Georgoulis, M. Jensen:
- * <b>Implementation of the Continuous-Discontinuous Galerkin Finite Element
- * Method</b>, arXiv:1201.2878v1 [math.NA], 2012 (see
- * http://arxiv.org/abs/1201.2878).
+ * presented in the paper @cite Cangiani2012.
*
* Note that some care must be taken that the resulting mesh topology
* continues to make sense when FE_Nothing elements are introduced. This is