Erratum to: Domain Size Distribution in Segregating Binary Superfluids

1 Erratum to: J Low Temp Phys (2016) 183:169–174 DOI 10.1007/s10909-016-1543-7

In the original article, there was an error in Eq. 5. Following is the corrected equation:

$$\begin{aligned} \rho (S,l) l(t)^{4} = c_{S} \tilde{S}^{-\tau }\equiv \tilde{\rho }(\tilde{S}) \end{aligned}$$

(5)

In addition, there were errors in the vertical axes of Figs. 1 and 2. Following are the corrected figures.

Fig. 1

Domain size distribution $\rho _0(S)$ in the initial pattern with $l=l_{0}$. A broken line represents the power law with the approximate value $\tau =2$ of the Fisher exponent. The distribution $\rho _0(S)$ obeys the power law in the scaling regime $l_0^2 \ll S \ll L^{D_S}$ with the fractal dimension $D_S=2-\beta /\nu$ with the critical exponents $\beta =5/36$ and $\nu =4/3$ of two-dimensional percolation theory

Fig. 2

Dynamic scaling plot of the domain size distribution $\rho (S,l)$ for $l(t)/l_{0}= 0.8, 1.0, 1.4, 2.0 ,2.8, 3.9$, and 5.6 with the effective system sizes $\tilde{L}=L/l(t)=81.5, 65.2, 46.6, 32.6, 23.3, 16.7$, and 11.6, respectively. The broken line represents the universal function $\tilde{\rho }(\tilde{S})$ with $c_S=0.1$ and $\tau =2$. The positions of $\tilde{S}=\tilde{L}^{D_S}$ for different values from $l(t)/l_0=0.8$ to $l(t)/l_0=5.6$ are represented by thick arrows from right to left (Color figure online)