General Assumptions
Since dengue serotypes are reported to be pairwise similar in their transmission characteristics (Carrington and Simmons 2014), we considered only two serotypes, referred to as \(\mathcal {S}_1\) and \(\mathcal {S}_2\). Tertiary infections are reported very rarely (Halstead 2003), and therefore most studies assume that individuals are immune to all four serotypes of dengue after two heterologous infections. In line with previous work, we disregard heterologous superinfection. Serotypes \(\mathcal {S}_1\) and \(\mathcal {S}_2\) considered here do not necessarily correspond to the actual DENv1 and DENv2, but rather represent co-circulation of two serotypes that have different transmissibility. Our model incorporates \(\mathcal {S}_1\) and \(\mathcal {S}_2\) with different rates for human-to-mosquito and mosquito-to-human transmission (Carrington and Simmons 2014). While the incubation period and the infectious period of dengue in humans may vary for different serotypes (Carrington and Simmons 2014), we follow previous work and assume that these periods are the same for dengue caused by \(\mathcal {S}_1\) and \(\mathcal {S}_2\). The schematic diagram of the model is presented in Fig. 1.
Like many multi-strain pathogens, dengue has been studied for evidence of immune response and cross-protection after infection with one serotype. Most studies concur that infection with any of the four serotypes induces lifetime immunity to that serotype and confers at least short-term cross-protection against all other serotypes. Several studies (Coudeville and Garnett 2012; Recker et al. 2009; Reich et al. 2013) argue that including the period of cross-protection and increased transmissibility from individuals suffering from DHF or DSS in secondary infections are of particular importance to reproduce the multi-annual patterns observed in surveillance of dengue cases. The work of Reich et al. (2013) provided strong evidence for substantial cross-protection for an average duration of 1.88 years after the primary infection. After this period has elapsed, individuals will enter a period during which the effect of ADE may appear in a secondary infection. This effect is inversely correlated with the concentration of non-neutralizing antibodies and may become inapparent over time due to the decline of antibody concentration to sufficiently low levels. Thus, high antibody concentrations are assumed to be protective, low concentrations are irrelevant in the context of ADE, and medium concentrations are associated with the ADE phenomenon. We assumed that following the period of partial protection associated with the risk of ADE, individuals are fully susceptible to other serotypes. The effect of ADE also appears as increased viral titres in human blood, which in turn influences the likelihood of a mosquito becoming infected after a bloodmeal (Carrington and Simmons 2014). We assumed higher human-to-mosquito transmissibility of the secondary infection during the partial protection period, compared to the primary infection.
To investigate the effect of vaccine on the dynamics of dengue infection, we implemented tetravalent (all serotypes) vaccination in our model for individuals with no prior exposure to dengue serotypes. We consider two scenarios in which vaccination is implemented either for the susceptible population, or for newborns only. We assumed that the vaccine-induced immunity provides some degree of protection to each serotype. Since vaccination primes the individual’s immune response to all serotypes, we assumed that vaccinated individuals are subject to the ADE effect after the period of full protection has elapsed if infection occurs.
Dengue Dynamics in the Vector Population
We model dengue dynamics with a system of ordinary differential equations, where all variables depend on time t. First, we develop the subsystem for the mosquito population. The total mosquito population is denoted by V. The recruitment (birth) in the mosquito population is given by the function \(\hat{b}(t)\). We elaborate on this birth function and its expression in Eq. (13) when we revisit the subsystem for the mosquito population. Assuming that all mosquitoes are born susceptible and die at the rate \(\hat{\mu }\), the dynamics of dengue in susceptible mosquitoes are governed by
$$\begin{aligned} \dot{S}_V =\hat{b}(t)-\left( F_{V}^{1}+F_{V}^{2}+F_{V}^{A1}+F_{V}^{A2}\right) S_V- \hat{\mu } S_V, \end{aligned}$$
(1)
where \(F_{V}^{1}+F_{V}^{2}+F_{V}^{A1}+F_{V}^{A2}\) is the force of infection for the vector population, describing that a susceptible mosquito can acquire dengue \(\mathcal {S}_1\) or \(\mathcal {S}_2\) from infectious individuals. The term for the force of infection in the mosquito population will be explicitly defined in Sect. 2.3.
Since mosquitoes infected by individuals experiencing DHF or DSS (i.e. the effect of ADE with high viral titres) may become infectious in a significantly shorter incubation period compared to mosquitoes that acquire dengue from infectious individuals with mild form of infection (Carrington and Simmons 2014), we assumed two different extrinsic incubation periods \(1/\hat{\alpha }\) and \(1/\hat{\alpha }_{_A}\). For the exposed classes in the mosquito population, we obtain the system
$$\begin{aligned} \dot{E}_V^{1}= & {} F_{V}^{1} \, S_V-(\hat{\alpha } + \hat{\mu }) E_V^{1}, \quad \dot{E}_V^{A1} = F_{V}^{A1} \, S_V-(\hat{\alpha }_{_A} +\hat{\mu }) E_V^{A1},\nonumber \\ \dot{E}_V^{2}= & {} F_{V}^{2} \, S_V-(\hat{\alpha } + \hat{\mu }) E_V^{2}, \quad \dot{E}_V^{A2} = F_{V}^{A2} \, S_V-(\hat{\alpha }_{_A}+ \hat{\mu }) E_V^{A2}, \end{aligned}$$
(2)
where index A indicates whether infection was acquired from a human with high viral titres that is associated with the ADE phenomenon.
After the extrinsic incubation period has elapsed, infectious mosquitoes are able to transmit the disease and are part of the infection classes that correspond to their exposed compartments. Assuming that such mosquitoes remain infectious for the remaining part of their lifespan, the dynamics of infectious mosquitoes can be expressed by
$$\begin{aligned} \dot{I}_V^{1}= & {} \hat{\alpha } E_V^{1}-\hat{\mu } I_V^{1}, \quad \dot{I}_V^{A1} = \hat{\alpha }_{_A} E_V^{A1}-\hat{\mu } I_V^{A1},\nonumber \\ \dot{I}_V^{2}= & {} \hat{\alpha } E_V^{2}-\hat{\mu } I_V^{2}, \quad \dot{I}_V^{A2} = \hat{\alpha }_{_A} E_V^{A2}-\hat{\mu } I_V^{A2}. \end{aligned}$$
(3)
Dengue Dynamics in the Human Population
We define the force of infection for \(\mathcal {S}_1\) and \(\mathcal {S}_2\) in the human population by
$$\begin{aligned} F_H^{1}=\lambda _1 \frac{I_V^{1}+I_V^{A1}}{H}, \quad F_H^{2}=\lambda _2 \frac{I_V^{2}+I_V^{A2}}{H}, \end{aligned}$$
(4)
where H is the total human population and \(\lambda _1\) and \(\lambda _2\) are, respectively, the rates at which mosquitoes transmit \(\mathcal {S}_1\) and \(\mathcal {S}_2\) to humans. Denoting susceptible individuals by \(S_H\), the equation
$$\begin{aligned} \dot{S}_H =(1-\phi )B-\big (F_H^{1}+F_H^{2}\big )S_H-\xi S_H- \mu S_H, \end{aligned}$$
(5)
describes the dynamics of infection in humans, where B is the constant birth rate and \(\mu \) is the natural death rate. Susceptible individuals are vaccinated at a rate \(\xi \) and move to the class \(W_H\). The parameter \(\phi \) represents the vaccination coverage of newborns. If \(\phi >0\), a fraction \(\phi \) of newborns are vaccinated and recruited directly to the \(W_H\) class. We assume that vaccinated individuals will be fully protected for a period of time (\(1/\eta \)). After this period has elapsed, they move to the class of individuals with partial protection (\(X_H\)), who are subject to ADE for the rest of their lifetime. The governing equations are
$$\begin{aligned} \dot{W}_H= & {} \phi B+\xi S_H-\eta W_H-\mu \, W_H,\nonumber \\ \dot{X}_H= & {} \eta W_H-\big (p_1 F_H^{1}+p_2 F_H^{2}\big )X_H- \mu \, X_H, \end{aligned}$$
(6)
where the parameters \(0 \le p_1 \le 1\) and \(0 \le p_2 \le 1\) represent, respectively, the reduced probabilities of acquiring infection with \(\mathcal {S}_1\) and \(\mathcal {S}_2\) due to partial protection.
After exposure to a serotype, individuals enter the exposed classes \(E_H^1\) and \(E_H^2\), with average latency periods of \(1/\alpha _1\) and \(1/\alpha _2\) units of time, before becoming infectious. Primary infections with \(\mathcal {S}_1\) (individuals in \(I_H^1\)) and \(\mathcal {S}_2\) (individuals in \(I_H^2\)) will recover at the rates \(\gamma _1\) and \(\gamma _2\), respectively, and move to the corresponding classes \(T_H^1\) and \(T_H^2\) with full protection. The equations describing such dynamics are
$$\begin{aligned} \dot{E}_H^1= & {} F_H^{1} \, S_H-\alpha _1 E_H^1- \mu E_H^1,\nonumber \\ \dot{I}_H^1= & {} \alpha _1 E_H^1- \mu I_H^1-\gamma _1 I_H^1,\nonumber \\ \dot{T}_H^1= & {} \gamma _1 I_H^1-\rho _1 T_H^1- \mu T_H^1, \end{aligned}$$
(7)
and
$$\begin{aligned} \dot{E}_H^2= & {} F_H^{2} \, S_H-\alpha _2 E_H^2- \mu E_H^2,\nonumber \\ \dot{I}_H^2= & {} \alpha _2 E_H^2- \mu I_H^2-\gamma _2 I_H^2,\nonumber \\ \dot{T}_H^2= & {} \gamma _2 I_H^2-\rho _2 T_H^2- \mu T_H^2, \end{aligned}$$
(8)
where \(\rho _1\) and \(\rho _2\) are, respectively, the rates at which individuals in the \(T_H^1\) and \(T_H^2\) classes lose their full protection. We assume that recovery after the primary infection with a particular serotype provides lifelong immunity against that serotype. After the transient period of full protection has elapsed, individuals move to the class \(S_H^{M2}\) (or \(S_H^{M1}\)) and become susceptible to infection with \(\mathcal {S}_2\) (or \(\mathcal {S}_1\)). While this susceptibility is reduced by a factor \(q_2\) (or \(q_1\)) due to partial protection, the secondary infection (if occurs) is subject to ADE. As the partial protection wanes over time, individuals become fully susceptible and the secondary infection may occur without the ADE effect. The infection dynamics are described by the following equations:
$$\begin{aligned} \dot{S}_H^{M2}= & {} \rho _1 T_H^1- q_2 \, F_H^{2} \, S_H^{M2}- (\mu +\theta _2) S_H^{M2},\nonumber \\ \dot{S}_H^{L2}= & {} \theta _2 S_H^{M2}- F_H^{2} \, S_H^{L2}- \mu S_H^{L2},\nonumber \\ \dot{S}_H^{M1}= & {} \rho _2 T_H^2-q_1 \, F_H^{1} \, S_H^{M1}- (\mu +\theta _1) S_H^{M1},\nonumber \\ \dot{S}_H^{L1}= & {} \theta _1 S_H^{M1}-F_H^{1} \, S_H^{L1}- \mu S_H^{L1}. \end{aligned}$$
(9)
where \(\theta _2\) and \(\theta _1\) are the rates at which individuals move from the \(S_H^{M2}\) and \(S_H^{M1}\) classes to \(S_H^{L2}\) and \(S_H^{L1}\) and become fully susceptible to heterologous infections.
Individuals exposed to \(\mathcal {S}_1\) and \(\mathcal {S}_2\) as secondary infection move to the classes \(E_H^{M1}\) and \(E_H^{M2}\) with the ADE effect, or to the classes \(E_H^{L1}\) and \(E_H^{L2}\) without the ADE effect. After the exposed period has elapsed, disease progression with the secondary infection in \(I_H^{M1}\), \(I_H^{L1}\), \(I_H^{M2}\) and \(I_H^{L2}\) is identical to that with the primary infection, and recovery from secondary infection will confer full protection against both serotypes. Since vaccinated individuals have already been primed to all serotypes, infection during partial protection will be considered as secondary infection with the ADE effect. In our model, this means that new infections with \(\mathcal {S}_1\) and \(\mathcal {S}_2\) from the class \(X_H\) move to \(E_H^{M1}\) and \(E_H^{M2}\), respectively. The following equations express such dynamics mathematically as
$$\begin{aligned} \dot{E}_H^{M2}= & {} q_2\, F_H^{2}\, S_H^{M2}+p_2\, F_H^{2}\, X_H -\alpha _2 E_H^{M2}- \mu E_H^{M2},\nonumber \\ \dot{I}_H^{M2}= & {} \alpha _2 E_H^{M2}- \mu I_H^{M2}- \gamma _2 I_H^{M2},\nonumber \\ \dot{E}_H^{M1}= & {} q_1\, F_H^{1}\, S_H^{M1}+p_1 \, F_H^{1}\, X_H -\alpha _1 E_H^{M1}- \mu E_H^{M1},\nonumber \\ \dot{I}_H^{M1}= & {} \alpha _1 E_H^{M1}- \mu I_H^{M1}- \gamma _1 I_H^{M1}, \end{aligned}$$
(10)
$$\begin{aligned} \dot{E}_H^{L2}= & {} F_H^{2} \, S_H^{L2} -\alpha _2 E_H^{L2}- \mu E_H^{L2},\nonumber \\ \dot{I}_H^{L2}= & {} \alpha _2 E_H^{L2}- \mu I_H^{L2}- \gamma _2 I_H^{L2},\nonumber \\ \dot{E}_H^{L1}= & {} F_H^{1} \, S_H^{L1} -\alpha _1 E_H^{L1}- \mu E_H^{L1},\nonumber \\ \dot{I}_H^{L1}= & {} \alpha _1 E_H^{L1}- \mu I_H^{L1}- \gamma _1 I_H^{L1}, \end{aligned}$$
(11)
and
$$\begin{aligned} \dot{R}_H = \gamma _1 \big (I_H^{L1}+I_H^{M1}\big )+\gamma _2 \big (I_H^{L2}+I_H^{M2}\big )-\mu R_H, \end{aligned}$$
(12)
where \(R_H\) is the class of individuals immune against both serotypes.
Now, we revisit our subsystem for dengue dynamics in the mosquito population. Recruitment into the mosquito population is modelled by the non-autonomous (seasonal-dependent) birth term (Wearing and Rohani 2006)
$$\begin{aligned} \hat{b}(t)=k H \hat{\mu } (1-a \cos (2 \pi t)), \end{aligned}$$
(13)
where k is the average number of mosquitoes per person and a is the amplitude of seasonal fluctuation. In the absence of seasonality, recruitment to the vector population is proportional to the total human population. We define the force of infection functions \(F_{V}^{1}\), \(F_{V}^{A1}\), \(F_{V}^{2}\) and \(F_{V}^{A2}\) in the mosquito subsystem as
$$\begin{aligned} F_{V}^{1}= & {} \hat{\delta }_1 \frac{I_H^1+I_H^{L1}}{H}, \quad F_{V}^{A1}=\hat{\delta }_1 \frac{\sigma _1 I_H^{M1}}{H}, \nonumber \\ F_{V}^{2}= & {} \hat{\delta }_2 \frac{I_H^2+I_H^{L2}}{H}, \quad F_{V}^{A2}=\hat{\delta }_2 \frac{\sigma _2 I_H^{M2}}{H}, \end{aligned}$$
(14)
where \(\hat{\delta }_1\) and \(\hat{\delta }_2\) are the transmission rates of \(\mathcal {S}_1\) and \(\mathcal {S}_2\), respectively, from humans to mosquitoes and \(\sigma _1\) and \(\sigma _2\) represent the enhanced transmissibility due to the ADE effect. Summarizing the above, the joint systems (1)–(3) and (5)–(12) with the functions (4) and (14) give a system of differential equations for the dynamics of dengue in the mosquito and human populations. Variables and parameters of the model are listed in Tables 1 and 2.
Table 1 Serotype-specific variables are labelled with indices 1 and 2 that correspond to \(\mathcal {S}_1\) and \(\mathcal {S}_2\)
Table 2 Serotype-specific parameters are labelled with indices 1 and 2 that correspond to \(\mathcal {S}_1\) and \(\mathcal {S}_2\)
Standard arguments from the theory of ordinary differential equations guarantee that the system for dengue dynamics in the mosquito and human populations admits a unique solution. For the total human population H, there is a globally attracting equilibrium \(\bar{H}=B/ \mu \), that is, \(\lim _{t \rightarrow \infty } H(t)=B/ \mu \). The dynamics of the total mosquito population is given by
$$\begin{aligned} \dot{V}=\hat{b}(t)- \hat{\mu } V. \end{aligned}$$
Considering \(H=\bar{H}\) and the constant recruitment term \(\hat{b}(t)=k \bar{H} \hat{\mu }\) (without seasonal variation) in the vector population, the equation \(\hat{b}(t)- \hat{\mu } {V}=0\) has a unique solution \(\bar{V}=k \bar{H}\), and the total mosquito population converges, that is, \(\lim _{t \rightarrow \infty } V(t)=\bar{V}\).
Non-negative initial conditions give rise to non-negative solutions of the system, and therefore the solutions are bounded and thus exist for all times. When the human population is at the disease-free state (i.e. \(F_{V}^{1}+F_{V}^{2}+F_{V}^{A1}+F_{V}^{A2}=0\)), the subsystem for mosquito dynamics admits a unique equilibrium, at which \(S_V(t) \equiv \bar{V}\) and all other classes are at zero states (i.e. the disease-free equilibrium). When there is no infection in the human population, the unique steady state is globally stable. Similarly, when the mosquito population is at the disease-free state (i.e. \(F_{H}^{1}+F_{H}^{2}=0\)), the subsystem for human population admits a unique equilibrium with
$$\begin{aligned} S_H(t)\equiv & {} \frac{(1-\phi ) B}{\xi +\mu }, \qquad W_H(t) \equiv \frac{\phi B}{\eta +\mu }+\frac{\xi (1-\phi ) B}{(\xi +\mu )(\eta +\mu )},\nonumber \\ X_H(t)\equiv & {} \frac{\eta \phi B}{(\eta +\mu )\mu }+\frac{\eta \xi (1-\phi ) B}{(\xi +\mu )(\eta +\mu )\mu }, \end{aligned}$$
and all other classes are at zero states, which is the disease-free equilibrium. With no infection in the mosquito population, the unique steady state is globally stable.
The Modified Model
We modify the original model to incorporate the possible difference in the enhanced transmissibility of human to mosquito due to the ADE effect in vaccinated individuals. We include the classes \(Y_H^{1}\) and \(Y_H^{2}\) for vaccinated individuals exposed to \(\mathcal {S}_1\) and \(\mathcal {S}_2\), respectively, and introduce \(Z_H^{1}\) and \(Z_H^{2}\) for the corresponding infection classes. The parameters \(\kappa _1\) and \(\kappa _2\) represent the enhanced transmissibility factors. With these modifications, the system (10) for the dynamics of the human population is expressed by
$$\begin{aligned} \dot{E}_H^{M2}= & {} q_2\, F_H^{2}\, S_H^{M2} -\alpha _2 E_H^{M2}- \mu E_H^{M2},\nonumber \\ \dot{I}_H^{M2}= & {} \alpha _2 E_H^{M2}- \mu I_H^{M2}- \gamma _2 I_H^{M2},\nonumber \\ \dot{E}_H^{M1}= & {} q_1\, F_H^{1}\, S_H^{M1} -\alpha _1 E_H^{M1}- \mu E_H^{M1},\nonumber \\ \dot{I}_H^{M1}= & {} \alpha _1 E_H^{M1}- \mu I_H^{M1}- \gamma _1 I_H^{M1},\nonumber \\ \dot{Y}_{H}^{2}= & {} p_2 \, F_H^{2} \, X_H -\alpha _2 Y_H^{2}- \mu Y_H^{2},\nonumber \\ \dot{Z}_{H}^{2}= & {} \alpha _2 Y_H^{2}- \mu Z_H^{2}- \gamma _2 Z_H^{2},\nonumber \\ \dot{Y}_{H}^{1}= & {} p_1 \, F_H^{1} \, X_H -\alpha _1 Y_H^{1}- \mu Y_H^{1},\nonumber \\ \dot{Z}_{H}^{1}= & {} \alpha _1 Y_H^{1}- \mu Z_H^{1}- \gamma _1 Z_H^{1},\nonumber \\ \end{aligned}$$
and we revise the Eq. (12) to
$$\begin{aligned} \dot{R}_H = \gamma _1 \big (I_H^{L1}+I_H^{M1}+Z_H^{1}\big )+\gamma _2 \big (I_H^{L2}+I_H^{M2}+Z_H^{2}\big )-\mu R_H, \end{aligned}$$
for the class of individuals recovered from both serotypes. The force of infection terms in Eq. (14) for serotypes acquired from infectious humans with the ADE effect is also redefined as
$$\begin{aligned} F_V^{A1}=\hat{\delta }_1 \frac{\sigma _1 I_H^{M1}+\kappa _1\, Z_H^{1}}{H},\quad F_V^{A2}=\hat{\delta }_2 \frac{\sigma _2 I_H^{M2}+\kappa _2\, Z_H^{2}}{H}. \end{aligned}$$