Figures & data
Figure 1. Period-doubling bifurcations in the disease-free Equation (Equation15(15)
(15) ), where d=0.5, b=0.1, on the horizontal axis
and on the vertical axis
![Figure 1. Period-doubling bifurcations in the disease-free Equation (Equation15(15) St+1=(re−bSt+(1−d))St.(15) ), where d=0.5, b=0.1, on the horizontal axis 20≤r≤140 and on the vertical axis 20≤S≤120.](/cms/asset/458ec9bc-1481-4334-b62e-f0dfd2d4190d/tjbd_a_1537449_f0001_ob.jpg)
Figure 2. Bifurcation diagram for SIR model: As increases from values less than 1 to values greater than 1, the model dynamics changes from disease extinction to disease persistence on a locally asymptotically stable period 2 population cycle.
![Figure 2. Bifurcation diagram for SIR model: As R0 increases from values less than 1 to values greater than 1, the model dynamics changes from disease extinction to disease persistence on a locally asymptotically stable period 2 population cycle.](/cms/asset/a8057d19-1520-4ded-a8ac-9e5fdbefdc68/tjbd_a_1537449_f0002_ob.jpg)
Figure 3. Model (Equation7(7)
(7) ) with
has a locally asymptotically stable endemic period-2 population cycle when
.
![Figure 3. Model (Equation7(7) St+1=g(Nt)+(1−d)Stϕ(It)It+1=(1−d)St(1−ϕ(It))+(1−γ)(1−d)ItRt+1=γ(1−d)It+(1−d)Rt,(7) ) with g(Nt)=rNte−bNt has a locally asymptotically stable endemic period-2 population cycle when b=0.1, γ=d=0.5, β=0.05andr=e4.](/cms/asset/1ddbf452-a84b-470f-a3ce-2bd05c31cb86/tjbd_a_1537449_f0003_oc.jpg)
Figure 4. Susceptible and recovered disease-free populations of Model (Equation19(19)
(19) ) undergo period-doubling bifurcations as r is varied between 20 and 140, where p=0.78, d=0.5 and b=0.1.
![Figure 4. Susceptible and recovered disease-free populations of Model (Equation19(19) St+1=(1−p)r(St+Rt)e−b(St+Rt)+(1−d)StRt+1=pr(St+Rt)e−b(St+Rt)+(1−d)Rt.(19) ) undergo period-doubling bifurcations as r is varied between 20 and 140, where p=0.78, d=0.5 and b=0.1.](/cms/asset/f17cee84-473f-4112-ae54-de4b76e79488/tjbd_a_1537449_f0004_oc.jpg)
Figure 5. Bifurcation diagram for ISAv Model (Equation20(20)
(20) ): As
increases from values less than 1 to values greater than 1, the model dynamics changes from disease extinction to disease persistence on a periodic or chaotic population cycle.
![Figure 5. Bifurcation diagram for ISAv Model (Equation20(20) St+1=rSte−bSt+dˆSt(θϕI(It)+θˆϕV(Vt))It+1=dˆ(St(θϕˆI(It)+θˆϕˆV(Vt))+μˆIt)Vt+1=dˆV(Vt+δIt),(20) ): As R0 increases from values less than 1 to values greater than 1, the model dynamics changes from disease extinction to disease persistence on a periodic or chaotic population cycle.](/cms/asset/5982e742-6aab-4728-a59f-d68e3efb4dd2/tjbd_a_1537449_f0005_ob.jpg)
Figure 6. Model (Equation20(20)
(20) ) with
has a locally asymptotically stable period 4 population cycle when
and all the other parameter values are kept fixed at their current values in Figure .
![Figure 6. Model (Equation20(20) St+1=rSte−bSt+dˆSt(θϕI(It)+θˆϕV(Vt))It+1=dˆ(St(θϕˆI(It)+θˆϕˆV(Vt))+μˆIt)Vt+1=dˆV(Vt+δIt),(20) ) with g(St)=rSte−bSt has a locally asymptotically stable period 4 population cycle when βI=0.056 and all the other parameter values are kept fixed at their current values in Figure 5.](/cms/asset/5d8fe59e-4683-4549-ba47-c8ecf92141c9/tjbd_a_1537449_f0006_oc.jpg)