3
with infection age dependent infectivity depends only on the mean of the random infectivity function
[
11
], the deterministic limit of the model with random susceptibility depends on the distribution of
this random susceptibility function in a much more complicated way. To see this, suppose that we
wish to compute the average susceptibility of the individuals at some time
t
. This average can be
obtained by summing the contributions of individuals that have not been infected on the interval
[0
, t
), and of individuals that have been infected at some time
s∈
[0
, t
) and have not yet been
reinfected again on the interval [
s, t
). But the probability that such an individual has not been
reinfected by time
t
depends on the full trajectory of their susceptibility, as well as on the trajectory
of the force of infection, on the interval [
s, t
) (see
(3.5)
below). This explains why the deterministic
limit is more complex than that in [
11
], and shows that, in their 1932-33 model, Kermack and
McKendrick implicitly assumed that the only random component of the susceptibility function
is the time of recovery (see the discussion in Section 5.2). As a consequence, we obtain a strict
generalization of the model in [24,25] as the deterministic limit of our stochastic model.
Since in our model there is a flux of new susceptibles, due to waning of immunity, one expects
that under certain conditions, there may be a stable endemic equilibrium. We manage to study
the existence, uniqueness and some stability properties of an endemic equilibrium (as well as the
stability or instability of the disease–free equilibrium) in our deterministic limit. We identify a
threshold, which is the harmonic mean of the large time limit of the susceptibility (which is 1 in
Figure 1, but may be less than 1 in our general model). If the basic reproduction number
R0
(defined below by
(4.1)
) is smaller than this threshold, then the process converges to the disease-free
equilibrium. We also show that under appropriate assumptions, if
R0
is larger than the threshold,
and the model converges as
t→ ∞
to some limit, then this limit is the unique endemic equilibrium,
which is fully characterized. We conjecture that under appropriate assumptions, when
R0
is larger
than the threshold, any solution of the deterministic limit starting with a non zero force of infection
at time t= 0 does converge to the endemic equilibrium.
Let us comment on the method used to prove our law of large numbers result. One key argument
is based upon a coupling of the processes which count the numbers of infections of the various
individuals up to time
t
with i.i.d. counting processes, where the renormalized force of infection
is replaced by its deterministic limit. This approach, for which the inspiration came from [
8
], is
an application of ideas from the theory of propagation of chaos, see Sznitman [
33
]. Note both
that we were unable to adapt the methodology of [
11
] to the setting of the present paper, and
that the assumptions made here on the random infectivity function are weaker than those made in
[
11
]. Recently, the methodology of the present paper has been applied to the model in [
11
], thus
resulting in the same result under weaker assumptions, see [
13
]. We also note that our approach
differs significantly from the techniques classically used for age-structured population models, as
in [
27
,
22
,
35
,
16
,
17
,
9
]. In these papers, the authors describe the model as a branching process
(sometimes with interaction), which becomes an infinite dimensional Markov process if one adds all
the age structure in the present state of the system, in which the lifespan, birth rate and death rate
depend on the ages of all individuals in the population. The state of such a model is then described
by the empirical measure of the ages of the individuals. These works combine infinite-dimensional
stochastic calculus and measure-valued Markov processes analysis in order to prove the convergence
of the model. In contrast, our stochastic models are non Markovian, and their deterministic limit
does have a memory.
Using random infectivity and susceptibility functions allows us to build a very general model
which is both versatile and tractable. It captures the effect of a progressive loss of immunity, and
this loss is allowed to be different from one individual to another. The integral equations that we
obtain to describe the large population limit of our model are both compact and extremely general,
since most epidemic models with homogeneous mixing and a closed population can be written in
this form. The effect of the variability of susceptibility on the endemic threshold has received very
little attention in the literature, despite some profound implications which we outline in the present