Corrigendum to "Stabilized finite element method for the radial Dirac equation" [J. Comput. Phys. 236(2013) 426-442]

The authors regret for an error that went unnoticed in the previously published paper. In Table 5, h j+1 should be replaced by h j everywhere in the columns indexed by j − 1 and j − 1 + n. Upon this correction, the shape of the stability parameter τ should have the form τ := τ j = 9 35 (h j+1 − h j). This correction has no effects on the computation, i.e., the computation is almost the same. The authors would like to apologize for any inconvenience caused.