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Corrigendum: Understanding charged vesicle suspensions as Wigner glasses: dynamical aspects (2021 J. Phys.: Condens. Matter33 104001)

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Published 15 December 2023 © 2023 IOP Publishing Ltd
, , Citation G Porpora et al 2024 J. Phys.: Condens. Matter 36 129501 DOI 10.1088/1361-648X/ad1300

This is a correction for 2021 J. Phys.: Condens. Matter 33 104001

0953-8984/36/12/129501

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We recently realized that there was an error in a line of the simulation code used for our article [1]. The error concerned the strength of the electric double layer (EDL) potential ${W_{ij}^{\mathrm{EDL}}}$ (only between particles of different species), resulting in smaller values as compared to the nominal ones. After having corrected the code, we have performed new simulations to quantify the impact of the error on the results presented in our article [1].

We have verified that there is no qualitative difference between the new simulations and the original ones, but only quantitative changes. Going into details, the error does not have any significant effect on the simulations at the two highest salt concentrations, $[NaI] = 10$ and $1\,\textrm{mM}$, corresponding to the smallest Debye lengths. For the two lowest salt concentrations, $[NaI] = 0.1$ and $0.01\,\textrm{mM}$ (largest Debye lengths), instead, the new simulations show an enhanced slowing down of the dynamics on increasing the vesicle volume fractions φ, eventually leading to an (estimated) glass transition at smallest φ values as compared to the original simulations.

To concretely illustrate this change, we first focus on the structural relaxation time τα . Figure 1 shows τα as a function of φ, for the two lowest salt concentrations, comparing results from the new simulations and the original data (see figure 5(b) of our article [1]). It is apparent that the growth of τα on increasing φ is much steeper for the new datasets, especially at the lowest salt concentration. Data for the two highest values of $[NaI]$ are not included in figure 1, as there are no detectable differences among the new simulations and the original ones.

Figure 1.

Figure 1. Structural relaxation times τα as a function of the vesicle volume fraction φ, for the two lowest values of salt concentration, as indicated. Data from the new simulations are plotted as large points. Data from the original simulations (as in figure 5(b) of our article [1]) are plotted as line-points.

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In figure 2, for the case of φ = 0.25, $[NaI] = 0.1\,\textrm{mM}$, we report the mean square displacement (MSD) (panel (a)) and the intermediate self scattering function (ISSF) (panel (b)), as defined in [1], comparing once again the new simulations with the original ones (see figures 1 and 2 of our article [1]). As it is apparent also here, glassy aspects of the system dynamics are more marked within the new corrected simulations.

Figure 2.

Figure 2. MSD (a) and ISSF (b) as a function of time, for the new corrected simulations (blue line) and the original ones [1] (orange line), at vesicle volume fraction φ = 0.25 and salt concentration $[NaI] = 0.1\,\textrm{mM}$. The dashed line in panel (a) is indicative of a standard Brownian behavior.

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Overall, we can state that the key conclusion of our article [1] is not only confirmed but even strengthened by the new simulations: at low salt concentration, the investigated vesicles suspensions form Wigner glasses even at very low volume fractions.

Conflict of interest

There are no conflicts of interest to declare.

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10.1088/1361-648X/ad1300