Corrigendum: Gyrokinetic modelling of the quasilinear particle flux for plasmas with neutral-beam fuelling (2018 Plasma Phys. Control. Fusion 60 025027)

This corrigendum reports an incorrect normalisation contained in the original paper. In the bottom line of table 2, ${\nu }_{\mathrm{ee}}/({c}_{{\rm{s}}}/R)$ is used as the notation of the e–e collision frequency. However, ${\nu }_{\mathrm{ee}}$ is normalised by ${v}_{{T}_{{\rm{e}}}}/(R\sqrt{2{T}_{{\rm{i}}}/{T}_{{\rm{e}}}})$ instead of ${c}_{{\rm{s}}}/R$, where ${v}_{{T}_{{\rm{e}}}}=\sqrt{2{T}_{{\rm{e}}}/{m}_{{\rm{e}}}}$ and ${c}_{s}=\sqrt{{T}_{{\rm{e}}}/{m}_{{\rm{i}}}}$. The corrected version of table 2 is provided below. The correct value is given by multiplying $\sqrt{{m}_{{\rm{i}}}{T}_{{\rm{e}}}/({m}_{{\rm{e}}}{T}_{{\rm{i}}})}$ and the original one. This change does not affect the calculation results presented in the paper.

Table 2.  Plasma parameters used for the GKW calculations. Here, q, s, ${\beta }_{{\rm{e}}}$ and ${\nu }_{\mathrm{ee}}$ are the safety factor, the magnetic shear, the electron beta defined as ${\beta }_{{\rm{e}}}=2{\mu }_{0}{n}_{{\rm{e}}}{T}_{{\rm{e}}}/{B}^{2}$, and the e–e collision frequency, respectively. Here, the magnetic field B is the vacuum toroidal magnetic field at $R=3.32\,{\rm{m}}$. In the calculations, $R/{L}_{{n}_{{\rm{e}}}}=R/{L}_{{n}_{{\rm{i}},{\rm{C}}}}$ is assumed.

	$\rho =0.3$	$\rho =0.4$	$\rho =0.5$	$\rho =0.6$
$R/{L}_{{n}_{{\rm{e}}}}$	2.3–6.1	2.5–6.1	1.9–5.5	1.1–5.7
$R/{L}_{{T}_{{\rm{e}}}}$	5.0–11.5	6.2–12.7	4.8–11.3	2.3–9.1
$R/{L}_{{T}_{{\rm{i}},{\rm{C}}}}$	6.3–12.9	6.5–12.0	4.9–10.6	4.2–7.5
q	1.2–1.5	1.3–1.8	1.5–2.2	1.8–2.5
s	0.32–0.64	0.53–0.83	0.61–0.88	0.61–1.12
${T}_{{\rm{e}}}/{T}_{{\rm{i}}}$	0.60–1.00	0.64–1.04	0.64–1.04	0.66–1.04
${\beta }_{{\rm{e}}}\,[{10}^{-2}]$	0.53–1.00	0.38–0.83	0.27–0.61	0.21–0.46
${\nu }_{\mathrm{ee}}/({c}_{{\rm{s}}}/R)$	0.042–0.33	0.049–0.41	0.066–0.53	0.083–0.72