Correction to: Scientific Reportshttps://doi.org/10.1038/s41598-019-46125-8, published online 10 July 2019


This Article contains errors.


Firstly, there is an error in Equation 1.

$${x}_{0}=\frac{1}{3} \alpha$$

should read:

$${x}_{0}=K \alpha$$

As a result of the error in Equation 1, the following accompanying definition is also incorrect:


“with r2 = 0.9996”


should read:


\(K\) equals 1.4 with r2 = 0.99 when calculated based on selected TGSDs of Table 1 (i.e. TGSDs which could be fitted by a Rosin-Rammler distribution with a fitting correlation coefficient ≥ 0.99).”


In the Results section:


“In literature, the length scale parameter \({x}_{0}\) (Eq. 8) has been empirically linked with various percentiles of the original distribution22.”


should read:


“In literature, the length scale parameter \({x}_{0}\) (Eq. 8) has been linked with various percentiles of the original distribution22, however, here we estimate it based on the best fit of empirical data.”


“For the reasons above, the fitting improves when considering only particles coarser than fine ash (≤ 5 φ; Fig. 4b) or particles with size comprised from lapilli (< − 6 φ) to coarse ash (< − 1 φ) (Fig. 4c).”


should read:


“For the reasons above, the fitting improves when considering only particles coarser than fine ash (≤ 4 φ; Fig. 4b) or particles with size comprised from lapilli (> − 6 φ) to coarse ash (≤ 4 φ) (Fig. 4c).”


The following sentence in the Results should also be omitted:


“TGSDs can thus be satisfactorily reconstructed only based on the median grain-size of the studied deposit within a given range of the shape parameter l provided by literature data.”


In the Discussion section:


“This implies that even if l is not known, the tails of the distribution can be satisfactorily described by modeling the TGSD by a Rosin-Rammler distribution after empirical estimation of the deposit median grain-size (or \({x}_{0}\)) assuming that l lies in the range of most of published TGSDs (0.5–1; Fig. 3).”


should read:


“In case the TGSD is not well fitted by a Rosin-Rammler distribution (r2 < 0.99), the tails of the distribution can be satisfactorily described after estimation of \({x}_{0}\) based on the deposit median grain-size (Eq. 1) assuming that l lies in the range of most of published TGSDs (0.5–1; Fig. 3).”


In the Conclusive Remarks:


“Amongst all tested strategies used to fit particle distributions, the Rosin-Rammler shows the best compromise between fitting capacity (e.g., highest Pearson correlation coefficient) and stability with respect to sampling bias.”


should read:


“Amongst all tested strategies used to fit particle distributions, the Rosin-Rammler shows the best compromise between fitting capacity (e.g., highest correlation coefficient) and stability with respect to sampling bias.”


In the Methods section:


“Similar analyses were also carried out for the Schumann and Mott distributions which are commonly used to model rock fragmentation31, but did not provide acceptable fits (Pearson correlation coefficient r2 are always lower than the models proposed in this paper) and, therefore, are only presented as Supplementary Material.”


should read:


“Similar analyses were also carried out for the Schumann and Mott distributions which are commonly used to model rock fragmentation31, but did not provide acceptable fits (correlation coefficient r2 are always lower than the models proposed in this paper) and, therefore, are only presented as Supplementary Material.”


In Figure Legends 4 and 6:


“Pearson correlation coefficient”


should read:


“correlation coefficient”


In the Figure 5 Legend:


“Variability of D versus Pearson correlation coefficient r2 obtained from the power-law fitting of cumulative number of particles all the TGSDs considered (Eq. 5, Table 1); (a) entire distribution; (b) particles coarser than fine ash (< 0.64 mm); (c) lapilli (64–2 mm) to coarse ash (2–0.063 mm) particles.”


should read:


“Variability of D versus correlation coefficient r2 obtained from the power-law fitting of cumulative number of particles all the TGSDs considered (Eq. 5, Table 1); a) entire distribution; b) particles coarser than fine ash (> 0.063 mm); c) lapilli (64–2 mm) to coarse ash (2–0.063 mm) particles.”


In Supplementary Information Table S1, the value under column “\({x}_{0}\) (m)” for row “Hekla 1991” should read 0.00515.


Furthermore, the axes in Figure 3 were incorrectly switched, and the data point mentioned above in Supplementary Table S1 is incorrect in Figure 3. The correct Figure 3 is reproduced below as Fig. 1.

Figure 1
figure 1

(a) Pearson correlation coefficient r2 of the Rosin-Rammler distribution fitting vs. l of the studied distributions. (b) Variability of the parameter x0 of the Rosin-Rammler distribution fitting vs. the empirical median diameter (α) of the studied distributions. The dashed line indicates the best-fit linear correlation between the two parameters. (c) Variability of the parameter l vs. column height of the associated eruptions. Symbols as in Fig. 2.


Lastly, Figure 7 is incorrect as a result of the error in Equation 1. The correct Figure 7 is reproduced below as Fig. 2.

Figure 2
figure 2

Results of variation of l parameter in the Rosin-Rammler distribution fitting of the 1996 Ruapehu TGSD. (a) Real distribution (black dots) and distribution fitted after fixing the l parameter to 0.5, 0.6, 0.7, 0.8, 0.9, and 1 (colored curves); (b) weight-fraction based (χ) distributions for the same fittings as in (a); (c) residuals (difference of calculated weight fraction χcalc and the empirical weight fraction (χreal) of the distribution fitting, according to the same distribution as in (a). l values are indicated by different colors according to legend of (a). Wd is the weight fraction of particles of diameter smaller or equal to d.