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Theoretical perspectives on the infectiousness of Ebola virus disease
Theoretical Biology and Medical Modelling volume 12, Article number: 1 (2015)
Abstract
Background
Ebola virus disease (EVD) has generated a large epidemic in West Africa since December 2013. This minireview is aimed to clarify and illustrate different theoretical concepts of infectiousness in order to compare the infectiousness across different communicable diseases including EVD.
Methods
We employed a transmission model that rests on the renewal process in order to clarify theoretical concepts on infectiousness, namely the basic reproduction number, R_{0}, which measures the infectiousness per generation of cases, the force of infection (i.e. the hazard rate of infection), the intrinsic growth rate (i.e. infectiousness per unit time) and the percontact probability of infection (i.e. infectiousness per effective contact).
Results
Whereas R_{0} of EVD is similar to that of influenza, the growth rate (i.e. the measure of infectiousness per unit time) for EVD was shown to be comparatively lower than that for influenza. Moreover, EVD and influenza differ in mode of transmission whereby the probability of transmission per contact is lower for EVD compared to that of influenza.
Conclusions
The slow spread of EVD associated with the need for physical contact with body fluids supports social distancing measures including contact tracing and case isolation. Descriptions and interpretations of different variables quantifying infectiousness need to be used clearly and objectively in the scientific community and for risk communication.
Background
An epidemic of Ebola virus disease (EVD) centred in three West African countries has been ongoing since December 2013, with limited international spread to other countries in Africa, Europe and the USA [1]. It is likely that the duration of this EVD epidemic, associated with a high case fatality risk (CFR) estimated at ~70% [2, 3], will extend well into 2015. To investigate the ongoing EVD transmission dynamics and consider a range of possible countermeasures, it is vital to understand the natural history and epidemiological dynamics of this disease.
Owing to the rapid progression of the EVD epidemic in West Africa, attempts have been made to clarify the fundamental epidemiological characteristics of EVD [1, 2, 4]. For instance, several studies have reported statistical estimates of the reproduction number, i.e., the average number of secondary cases generated by a single primary case, as a measure of the transmission potential of EVD [2, 5–12]. Despite substantial progress, it remains unclear how measures of infectiousness (or the transmissibility) of EVD should be communicated to the public and interpreted in light of the set of control interventions that could be considered in practical settings. Hence, the purpose of this minireview is to comprehensively classify different theoretical aspects of infectiousness using a basic transmission model formulated in terms of a renewal process. This approach allows us to compare different measures of infectiousness across different communicable diseases and design possible countermeasures.
Discussion
Renewal process
Here we briefly review the definition of the basic reproduction number, R_{0} using the renewal process model [13]. Let i(t) represent the incidence (i.e. the transient number of new cases) at calendar time t. Assuming that the contribution of initial cases to the dynamics is negligible, the renewal process is written as
where A(s) is the rate of secondary transmission per single primary case at its infectionage (i.e., the time since infection) s. Using A(s), one can model the dependency of the transmission dynamics on infectionage [14]. By far the most commonly used measure of infectiousness is the basic reproduction number, R_{0}, which is computed as
and it can be interpreted as the number of secondary cases produced by a single primary case throughout its entire course of infection in a completely susceptible population. Although the concept of R_{0} is wellknown, it is important to note from (2) that R_{0} results from the integration over all infectionages. It is well known that the mathematical definition of R_{0} in a heterogeneously mixing population is described by using the multivariate version of (1) and the nextgeneration matrix that maps secondary transmissions between and within subpopulations. R_{0} is defined as the largest eigenvalue of this matrix [15, 16]. Similarly, the definition of R_{0} can be adapted to the situation of periodic infectious diseases by handling the seasonal dynamics using a vector and employing Floquet theory (see e.g., [17]).
Although R_{0} is clearly a dimensionless quantity, the conceptual interpretation from the renewal process (1) permits us to regard R_{0} as the average number of infected cases produced “per generation”. For this reason, R_{0} could also be referred to as the basic reproductive ratio, as it could be calculated as the ratio of secondary to primary cases.
Adopting the mass action principle of the socalled Kermack and McKendrick epidemic model, a nonlinear version of the renewal equation (1) follows [13]:
where s(t) is the fraction susceptible at time t, β(s) the rate of transmission per single infected individual at infectionage s, and Γ(s) the survivorship of infectiousness at infectionage s. Here we define the force of infection, λ(t) as
which yields a measure of the risk of infection in a susceptible population. The force of infection can be interpreted as the hazard of infection in statistical sense  the rate at which susceptible individuals are infected [18]. In the classical Kermack and McKendrick epidemic model, λ(t) is modelled as proportional to the disease prevalence [13]. The force of infection is useful for the analysis of incidence data.
Comparison of three communicable diseases
Table 1 shows empirical estimates of R_{0} and the mean generation time for three different infectious diseases that are characterized by significantly different transmissibility and natural history parameters, i.e., measles, influenza H1N12009 and EVD [1, 19, 20]. The mean generation time, T_{g} can be mathematically derived from the transmission kernel in the renewal process (1), i.e.,
The mode of transmission greatly differs for three diseases considered (Table 1). Measles is transmitted efficiently through the air while the transmission of influenza mostly occurs via droplet although airborne transmission is also possible in a confined setting [23]. In contrast, transmission of EVD is greatly constrained to physical contacts via body fluids [1]. Despite the differences in the mode of transmission for these diseases, it is important to note that the estimates of R_{0} for H1N12009 and EVD are not too different (Table 1). Does that indicate that influenza (H1N12009) and Ebola are similarly infectious?
While the average R_{0} for influenza and Ebola are similar, here we underscore that their underlying transmission dynamics show fundamental differences. This can be understood by analysing the intrinsic growth rate r for both diseases. Assuming that the early growth of each disease follows an exponential form, i.e., i(t) = i_{0}exp(rt) (where i_{0} is a constant), the renewal equation (1) is rewritten as the socalled EulerLotka equation. Replacing i(t) in both sides of (1) by i_{0}exp(rt) and cancelling exp(rt) from both sides, we obtain
yielding the relationship between R_{0} and the generation time,
where g(s) is the probability density function of the generation time. Equation (7) frequently appears in discussions of mathematical demography [24] and theoretical epidemiology [25], which is useful to describe how the relationship is determined between R_{0} and the intrinsic growth rate r as a function of the generation time distribution. For instance, if the generation time distribution follows the exponential distribution or Kronecker delta function, we obtain the wellknown estimators of R_{0}, i.e., R_{0} = 1 + rT_{g} and R_{0} = exp(rT_{g}), respectively [26]. Assuming that g(s) follows a gamma distribution with the coefficient of variation k, we have
It should be noted that it is possible that the righttail of g(s) for EVD might have been underestimated if there were substantial number of secondary transmissions from deceased persons during funerals. Adopting the values of R_{0} and T_{g} given in Table 1, and assuming that the coefficient of variation of the generation time at 50%, the intrinsic growth rate of influenza H1N12009 is calculated as 0.125 per day, while that of EVD is calculated as 0.038 per day. Figure 1A compares the growth rates (r) of three representative communicable diseases for different values of the coefficient of variation of the generation time. An epidemic of measles appears to grow the fastest followed by one of influenza while an outbreak of EVD is expected to grow the slowest. Whereas the R_{0} for EVD is similar to that of influenza, the growth rate of EVD is far smaller than that of influenza. This is because each disease generation in the context of EVD transmission takes approximately two weeks, while each generation of new influenza cases occurs on a much shorter time scale  every 3 days on average. Moreover, EVD spreads comparatively slowly mainly by physical contact. This feature indicates that social distancing measures including contact tracing and case isolation could be powerful options for controlling EVD assuming that public health infrastructure exists for these interventions to be feasible [27].
Thus, based on the infectiousness as measured by the growth rate of cases per unit time, it is very encouraging that EVD is far less dispersible than influenza. Although static countermeasures (e.g. mass vaccination at a certain age) can be planned using R_{0}, the feasibility to deploy dynamic countermeasures, such as contact tracing and case isolation rests on the competition between the growth of cases and public health control, and in this context, the key parameter of infectiousness to assess the feasibility of control interventions is the intrinsic growth rate of cases.
Per contact risk of infection
We further decompose the rate of secondary transmission per single primary case in the renewal equation (3) into the product of the contact rate c(s) and the percontact probability of infection p(s), i.e.,
Assuming that the per contact probability of infection, p is independent of infectionage, we have
The interpretation of p is straightforward, i.e., it can be regarded as the risk of successful secondary transmission given an infectious contact to a susceptible individual. Assuming that everyone is susceptible at time zero, R_{0} in (2) is rewritten as
As mentioned above, R_{0} for EVD is similar to that of influenza. Nevertheless, the infectious period, modelled by Γ(s) for EVD is longer than that of influenza. Assuming an identical contact rate, c, between EVD and influenza, equation (11) indicates that the percontact probability of infection for EVD is smaller than that for influenza.
The mode of transmission differs across communicable diseases. Figure 2 illustrates the physical range of “contact” that can potentially lead to infection for three representative infectious diseases. Measles causes airborne transmission, and thus, it can lead to secondary infections across different rooms (or sometimes even across buildings). The extent of contact for EVD is very limited as it is highly constrained to physical contacts with body fluids. Hence, effective contact for EVD is limited to close contacts that might be unavoidable among healthcare workers and household members of cases.
Conclusion
We have comparatively discussed concepts of infectiousness for EVD in relation to other communicable diseases from a mathematical modelling point of view. The measure of infectiousness per generation of cases is R_{0}. R_{0} offers a threshold principle and we have discussed that this measure is important for planning some static countermeasures such as mass vaccination. Based on R_{0}, the overall infectiousness of EVD may be perceived to be similar to that of influenza. Nevertheless, the infectiousness per unit time for EVD was shown to be comparatively lower than influenza. The slow spread of EVD supports social distancing measures including contact tracing and case isolation. Moreover, the percontact probability of infection for EVD is lower than that for influenza, and the mode of transmission also differs. These findings should also be regarded as encouraging news for healthcare workers who would have to have unavoidable and protected contact with EVD cases. In summary, there is a need for the use of clear and objective descriptions and interpretations of different variables quantifying infectiousness among the scientific community and for risk communication.
Abbreviations
 R _{0} :

The basic reproduction number
 EVD:

Ebola virus disease
 CFR:

Case fatality risk.
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Acknowledgements
HN received funding support from the Japan Science and Technology Agency (JST) CREST program, RISTEX program for Science of Science, Technology and Innovation Policy, and St Luke’s Life Science Institute Research Grant for Clinical Epidemiology Research 2014. GC acknowledges financial support from the NSF grant 1414374 as part of the joint NSFNIHUSDA Ecology and Evolution of Infectious Diseases program, UK Biotechnology and Biological Sciences Research Council grant BB/M008894/1, and the Division of International Epidemiology and Population Studies, The Fogarty International Center, US National Institutes of Health.
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Authors’ contributions
HN conceived of the study. HN conducted mathematical analyses and drafted the manuscript. HN and GC drafted figures and table together and revised the manuscript. All authors read and approved the final manuscript.
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Nishiura, H., Chowell, G. Theoretical perspectives on the infectiousness of Ebola virus disease. Theor Biol Med Model 12, 1 (2015). https://doi.org/10.1186/17424682121
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Keywords
 Influenza
 Measle
 Renewal Process
 Communicable Disease
 Basic Reproduction Number