Skip to main content
. Author manuscript; available in PMC: 2019 May 3.
Published in final edited form as: J Phys Chem B. 2018 Apr 23;122(17):4700–4707. doi: 10.1021/acs.jpcb.8b02666

Figure 2.

Figure 2

Probability density of Uvv¯ at the γ = 0 state and the γ = 1 state for the homogeneous liquid. The probability density of Uvv¯ at the γ = 0 state spreads over a much boarder region than at the γ = 1 state. Note that Uvv¯ at the γ = 0 state has a long decreasing tail. The last bin on the right side of the figure (b) includes all the observations whose Uvv¯ is larger than 3000 kcal/mol. The total probability in the last bin is 52.0%. The insert shows the overlap of the probability density of Uvv¯ at the γ = 0 and the γ = 1 states.