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Molecular Physics
An International Journal at the Interface Between Chemistry and Physics
Volume 119, 2021 - Issue 19-20: Special Issue in honour of Michael L. Klein FRS
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Klein Special Issue

Effect of social distancing on super-spreading diseases: why pandemics modelling is more challenging than molecular simulation

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Article: e1936247 | Received 25 Feb 2021, Accepted 21 May 2021, Published online: 04 Jun 2021

Figures & data

Figure 1. Comparison of the probability distribution p(n,1) for a value of R = 5, which is in the range of the COVID19 variants that appeared in late 2020 [Citation8]. The grey bars correspond to a Poisson distribution; the chequered bars correspond to a negative binomial with k = 0.1. To improve the readability of the figure, the data points for n = 0 have not been included. For the Poisson case, p(0)0.0067, whereas for the case with k = 0.1, p(0,1)0.67, which means that 67% of all infectious persons infect nobody else.

Figure 1. Comparison of the probability distribution p(n,1) for a value of R = 5, which is in the range of the COVID19 variants that appeared in late 2020 [Citation8]. The grey bars correspond to a Poisson distribution; the chequered bars correspond to a negative binomial with k = 0.1. To improve the readability of the figure, the data points for n = 0 have not been included. For the Poisson case, p(0)≈0.0067, whereas for the case with k = 0.1, p(0,1)≈0.67, which means that 67% of all infectious persons infect nobody else.

Figure 2. Extinction probability P of an infection chain started by one infected individual, as a function of R and k. The negative binomial distribution (Equation (Equation1)) is not truncated.

Figure 2. Extinction probability P of an infection chain started by one infected individual, as a function of R and k. The negative binomial distribution (Equation (Equation1(1) p(n,1)=Γ(n+k)n!Γ(k)(kk+R)k(Rk+R)n,(1) )) is not truncated.

Figure 3. As an illustration of the effect of limiting the number of contacts of an individual to nt, the curves in this figure show how the threshold for an outbreak (Reff=1) depends on the bare reproduction number R and the dispersion factor k. For a given value of k, the area to the left of the curve corresponds to the parameter range where no outbreaks occur. In reality, this boundary will not be sharp. Clearly, the effect of limiting the number of contacts is largest for highly over-dispersed distributions (small k). We do not show the result for the Poisson distribution, because in that case truncating nt has no effect in the range of nt shown, unless R is very close to one.

Figure 3. As an illustration of the effect of limiting the number of contacts of an individual to nt, the curves in this figure show how the threshold for an outbreak (Reff=1) depends on the bare reproduction number R and the dispersion factor k. For a given value of k, the area to the left of the curve corresponds to the parameter range where no outbreaks occur. In reality, this boundary will not be sharp. Clearly, the effect of limiting the number of contacts is largest for highly over-dispersed distributions (small k). We do not show the result for the Poisson distribution, because in that case truncating nt has no effect in the range of nt shown, unless R is very close to one.

Figure 4. (A) Extinction probability P versus nt (see text) for R0=2, and k=0.1, 0.2, 0.4. (B) Extinction probability P versus nt for R0=5, and k=0.1, 0.2, 0.4. (C) Average number infected versus nt in a transient outbreak, for R0=2, and k = 0.1, 0.2, 0.4. (D) Average number infected versus nt in a transient outbreak, for R0=5, and k = 0.1, 0.2, 0.4.

Figure 4. (A) Extinction probability P versus nt (see text) for R0=2, and k=0.1, 0.2, 0.4. (B) Extinction probability P versus nt for R0=5, and k=0.1, 0.2, 0.4. (C) Average number infected versus nt in a transient outbreak, for R0=2, and k = 0.1, 0.2, 0.4. (D) Average number infected versus nt in a transient outbreak, for R0=5, and k = 0.1, 0.2, 0.4.