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Simulations of H–He mixtures using the van der Waals density functional – CORRIGENDUM

Published online by Cambridge University Press:  13 March 2019

Manuel Schöttler  and
Ronald Redmer
Manuel Schöttler*
Affiliation:
University of Rostock, D-18059 Rostock, Germany
Ronald Redmer
Affiliation:
University of Rostock, D-18059 Rostock, Germany
*
†Email address for correspondence: manuel.schoettler@uni-rostock.de
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Abstract

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Information

Type
Corrigendum
Information
Journal of Plasma Physics , Volume 85 , Issue 2 , April 2019 , 945850201
Copyright
© Cambridge University Press 2019 

We hereby correct an error in figure 4(b) of Schöttler & Redmer (Reference Schöttler and Redmer2018). The shown data corresponds to a temperature of 1000 K and not 10 000 K as indicated in the caption. The correct data for 10 000 K is given in figure 1. Note that the ratio of partial volumes is not changed significantly. This error only affects the displayed data. All conclusions of Schöttler & Redmer (Reference Schöttler and Redmer2018) remain unchanged.

Figure 1.

(a) Volume versus He fraction for three pressures at 10 000 K. The determination of partial volumes for H and He is demonstrated for three He fractions. Partial volumes are indicated by the crosses. (b) Partial volumes and their ratio at $T=10\,000$  K and $r_{\text{s}}=1.4~a_{0}$ for all considered He fractions.

Acknowledgement

We thank M. Desjarlais for bringing the hereby corrected error to our attention.

References

Schöttler, M. & Redmer, R. 2018 Simulations of H–He mixtures using the van der Waals density functional. J. Plasma Phys. 84, 755840401.Google Scholar
Figure 0

Figure 1. (a) Volume versus He fraction for three pressures at 10 000 K. The determination of partial volumes for H and He is demonstrated for three He fractions. Partial volumes are indicated by the crosses. (b) Partial volumes and their ratio at $T=10\,000$ K and $r_{\text{s}}=1.4~a_{0}$ for all considered He fractions.