Figures
Figs 1, 2, 3, 4, 5 and 6 are incorrect. The figures should be formatted as EPS files. The publisher apologizes for the error. The authors have provided a corrected version here.
The functions of the CC model are set to be N(t) = 5, ∣Di∣ = 0.2β(θi)ti for the case in Panel(a), and N(t) = [e0.1t], ∣Di∣ = 0.15β(θi)[e0.1ti] for the case in Panel(b). β(⋅) is given by Equation (2) for both cases.
The influence region of the CC model is the counterpart of the future light cone.
The functions of the CC model are set as follows: N(t) = [e0.1t], ∣Di∣ = 0.15β(θi)[e0.1ti], and β(⋅) is given by Equation (2). The fitting functions in Panel (a) are the Poisson distribution f(k) = ake−ak! and the mixture Poisson distribution given byEquation (13). The fitting functions in Panel (b) are the power-law functions f(k) = ak−2 and f(k) = k−γ∑n = 0∞(n+xmin)−γ.
The fitting curves for the data between 1946–2012 in Panels(a, b) are f(t) = 5.397 × 10−34e4.23 × 10−2 t (R2: 0.974, RMSE: 224.2) and f(t) = 0.5085t − 982.6 (R2: 0.958, RMSE: 2.112) respectively. The fitting curve in Panel(c) is f(t) = 6.038 × 10−88e0.106t(R2: 0.9828, RMSE: 7249).
Panels(b, c, e, f) show the fitting effects of the in-degree distributions of the nodes with in-degree larger than 9 by the power-law functions f(k) = ak−2 and f(k) = k−γ∑n = 0∞(n+xmin)−γ.
The fitting model is the mixture generalized Poisson distribution (Equation (14).
Reference
Citation: The PLOS ONE Staff (2015) Correction: Modeling the Citation Network by Network Cosmology. PLoS ONE 10(10): e0140413. https://doi.org/10.1371/journal.pone.0140413
Published: October 30, 2015
Copyright: © 2015 The PLOS ONE Staff. This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited