c 2012, glenn e. lahodny jr. - tdl
TRANSCRIPT
Persistence or Extinction of Disease in Stochastic Epidemic Models andDynamically Consistent Discrete Lotka-Volterra Competition Models
by
Glenn E. Lahodny Jr., M.S.
A Dissertation
In
Mathematics and Statistics
Submitted to the Graduate Facultyof Texas Tech University in
Partial Fulfillment ofthe Requirements for the Degree of
Doctor of Philosophy in Applied Mathematics
Approved
Linda Allen(Co-chair)
Lih-Ing Roeger(Co-chair)
Ed Allen
Peggy Gordon MillerDean of the Graduate School
August, 2012
c©2012, Glenn E. Lahodny Jr.
Texas Tech University, Glenn E. Lahodny Jr., August 2012
ACKNOWLEDGEMENTS
First, I would like to acknowledge the faculty in the department of Mathematics
and Statistics at Texas Tech University. It was a privilege and a pleasure to learn
from and work with such wonderful professors. I will never forget the experiences I
had in this department and at Texas Tech University. The staff in the Mathematics
and Statistics department also deserve special thanks for their hard work, kindness,
and willingness to assist in any matter.
I would also like to thank my advisors, Drs. Linda Allen and Lih-Ing Roeger, for
taking the time to mentor me. Thank you both for your hard work, suggestions,
kindness, and always taking the time to help. Thanks to Dr. Edward Allen for all of
his helpful comments, teaching me about stochastic differential equations, taking
time to write recommendation letters, and serve as a committee member.
Thanks to my parents, Glenn and Janice Lahodny, for the love, encouragement,
and support you have given me. I am very fortunate to have parents who are so
supportive and caring despite the circumstances, and I love you both very much.
To my fiancee, Megan Trenck, thank you for being the incredible person that you
are. You are a kind, beautiful, and intelligent women and you have been the most
positive influence in my life since we’ve met. Thank you for all of your love and
support over the years. I love you very much and look forward to a long, happy life
together.
Last, I would like to thank Mrs. Ramona Pelkey for pushing me to be a better
student, work hard, and always do my best. Without your influence, I am certain
that I would not have the education and opportunities that I do today.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
TABLE OF CONTENTS
Acknowledgements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ii
Abstract . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . v
List of Figures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . vii
1. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
2. Dynamically Consistent Discrete Lotka-Volterra Competition Models . . 4
2.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2.2 Discrete Lotka-Volterra Competition Models . . . . . . . . . . 9
2.2.1 Existence and Local Stability of Equilibria . . . . . . . . . 9
2.2.2 Monotonicity, Positive Invariance, and Global Stability . . 11
2.3 Numerical Examples . . . . . . . . . . . . . . . . . . . . . . . 19
2.4 Discussion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21
3. Extinction or Persistence of Disease in Stochastic Epidemic Models . . . 22
3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22
3.2 Mathematical Methods . . . . . . . . . . . . . . . . . . . . . . 24
3.3 Single Infectious Group . . . . . . . . . . . . . . . . . . . . . . 27
3.4 Multiple Infectious Groups . . . . . . . . . . . . . . . . . . . . 29
3.4.1 SEIR Model . . . . . . . . . . . . . . . . . . . . . . . . . . 30
3.4.2 Vector-Host Model . . . . . . . . . . . . . . . . . . . . . . 33
3.4.3 Stage-Structured Model . . . . . . . . . . . . . . . . . . . 37
3.4.4 Treatment Model . . . . . . . . . . . . . . . . . . . . . . . 40
3.5 Discussion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 48
4. Stochastic Multi-Patch Epidemic Models . . . . . . . . . . . . . . . . . 51
4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51
4.2 Multi-Patch SIS, SIR, and SIRS Models without Demographics 52
4.2.1 Deterministic Models . . . . . . . . . . . . . . . . . . . . . 53
4.2.2 Markov Chain Models . . . . . . . . . . . . . . . . . . . . 59
4.2.3 Stochastic Differential Equation Models . . . . . . . . . . . 62
4.2.4 Numerical Examples . . . . . . . . . . . . . . . . . . . . . 67
4.3 Multi-Patch SIS, SIR, and SIRS Models with Demographics . . 76
4.3.1 Deterministic Models . . . . . . . . . . . . . . . . . . . . . 76
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4.3.2 Markov Chain Models . . . . . . . . . . . . . . . . . . . . 83
4.3.3 Stochastic Differential Equation Models . . . . . . . . . . . 84
4.3.4 Numerical Examples . . . . . . . . . . . . . . . . . . . . . 85
4.4 Discussion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 86
Bibliography . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 89
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ABSTRACT
Two distinct topics are considered in this dissertation. The first topic concerns
nonstandard finite-difference (NSFD) schemes for the Lotka-Volterra competition
model, and the second topic concerns the persistence or extinction of disease in
stochastic epidemic models.
A problem of interest in numerical analysis is to derive a discrete-time model
which can be used to approximate the solution of an ordinary differential equation
(ODE) or system of ODEs. These discrete models can be constructed by applying
finite difference schemes to a given ODE. The goal is to derive a discrete model
which preserves the properties of the corresponding continuous model. In Chapter
2, the Lotka-Volterra competition model is introduced and some well-known
properties of the model are stated. A general class of discrete-time competition
models constructed from a NSFD scheme is considered. Sufficient conditions are
derived such that the elements of this class of difference equations are dynamically
consistent with the Lotka-Volterra competition model. The discrete models are
shown to preserve the positivity of solutions, existence and stability conditions of
the equilibrium points, boundedness of solutions, and monotonicity of the
Lotka-Volterra system.
The second topic concerns thresholds for epidemic models. In deterministic
epidemic theory, the basic reproduction number, R0, and type reproduction
numbers, Ti, are well-known thresholds used to determine whether a disease will
persist or become extinct. For stochastic epidemic models, there are similar
thresholds which are used to estimate the probability of disease persistence or
extinction. Typically, the deterministic and stochastic thresholds are discussed
separately. In Chapter 3, some deterministic (ODE) epidemic models from the
literature are considered. The basic reproduction number and type reproduction
numbers are calculated for each of these models and a corresponding
continuous-time Markov chain (CTMC) model is derived. For each of the CTMC
models, a stochastic threshold is computed as well as the probability of disease
persistence or extinction. In addition, a new relationship is illustrated between the
deterministic and stochastic thresholds.
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Factors such as spatial heterogeneity, connectivity, and dispersal of individuals
through worldwide travel can significantly affect disease dynamics. The effects of
these factors have been studied for several infectious diseases including influenza,
severe acute respiratory syndrome (SARS), and tuberculosis. In these studies, the
population is split into several groups or patches and dispersal is allowed between
these patches. In Chapter 4, deterministic and stochastic multi-patch epidemic
models with and without demographics are derived and analyzed. As in Chapter 3,
the basic reproduction number is calculated for the deterministic models. Two types
of stochastic multi-patch models are explored: CTMC models and stochastic
differential equation (SDE) models. For the CTMC models, the stochastic threshold
is computed as well as the probability of disease persistence or extinction.
Numerical examples illustrate the differences between the deterministic and
stochastic patch models.
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LIST OF FIGURES
2.1 Four approximate solutions to the Lotka-Volterra competition model
in the phase plane. For figure (a), the step size is h = 0.5 and for figure
(b), the step size is h = 0.1. . . . . . . . . . . . . . . . . . . . . . . . 20
2.2 Four approximate solutions to the Lotka-Volterra competition model
as a function of time. Parameter values and initial conditions are the
same as in Figure 2.1 with a step size of h = 0.1. . . . . . . . . . . . . 21
3.1 The ODE solution and one sample path of the CTMC SEIR model.
Parameter values are Λ = 1, d = 0.005, β = 0.25, ν = 0.1, γ = 0.05,
and α = 2d = 0.01 with initial conditions S(0) = 200, E(0) = 0,
I(0) = 2, and R(0) = 0. The disease persists with probability 1−P0 =
0.926. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33
3.2 The ODE solution and one sample path of the CTMC vector-host
model. Parameter values are Λ = 0.5, d = 0.005, γ = 0.1, Γ = 500,
µ = 0.5, and βm = βh = 0.2 with initial conditions S(0) = 100,
I(0) = 2, M(0) = 1000, and V (0) = 0. The disease persists with
probability 1− P0 = 0.970. . . . . . . . . . . . . . . . . . . . . . . . . 37
3.3 The ODE solution and one sample path of the CTMC staged-progression
model. Parameter values are Λ = 1, d = 0.005, β1 = 0.4, β2 = 0.1,
ν1 = 0.2, ν2 = 0.05, d1 = 0.02, and d2 = 0.01 with initial conditions
S(0) = 200, I1(0) = 1, I2(0) = 1, and R(0) = 0. The disease persists
with probability 1− P0 = 0.917. . . . . . . . . . . . . . . . . . . . . . 42
3.4 The ODE solution and one sample path of the CTMC treatment model.
Parameter values are Λ = 1, d = 0.005, β1 = 0.1, β2 = 0.04, βT =
0.25β2, r1 = r2 = 0.05, p = 0.5, q = 0.1, ν1 = 0.5, ν2 = 0.1, and
d1 = d2 = 1.5d ν1 = 0.2, ν2 = 0.05, d1 = 0.02, and d2 = 0.01. The
reproduction numbers are R1 = 2.58 and R2 = 5.08. The disease
persists with probability 1− P0 = 0.936. . . . . . . . . . . . . . . . . 49
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4.1 The ODE solution and one sample path for the CTMC two-patch SIS
model. Parameter values are β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4,
ds12 = ds21 = 0.1, and di12 = di21 = 0.1 with initial conditions S1(0) =
199, I1(0) = 1, S2(0) = 200, and I2(0) = 0. An outbreak occurs with
probability 1− P0 = 0.6590. The locally stable endemic equilibrium is
(S1, I1, S2, I2) ≈ (68, 132, 161, 39). . . . . . . . . . . . . . . . . . . . . 69
4.2 The ODE solution and one sample path for the CTMC three-patch SIS
model. Parameter values are β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4,
β3 = 0.1, γ3 = 0.4, dskj = dikj = 0.1 for k 6= 3 and j 6= 3, and ds13 =
ds31 = di13 = di31 = 0 with initial conditions S1(0) = 149, I1(0) = 1,
S2(0) = 150, I2(0) = 0, S3(0) = 150, and I3(0) = 0. An outbreak
occurs with probability 1 − P0 = 0.6491. The locally stable endemic
equilibrium is (S1, I1, S2, I2, S3, I3) ≈ (53, 97, 126, 24, 144, 6). . . . . . . 71
4.3 The ODE solution and one sample path for the CTMC two-patch SIS
model. Parameter values are β1 = 0.8, γ1 = 0.1, β2 = 0.3, γ2 = 0.4,
α1 = α2 = 0.5, ds12 = ds21 = 0.1, and di12 = di21 = 0.1 with initial
conditions S1(0) = 195, I1(0) = 5, S2(0) = 185, and I2(0) = 15. . . . . 72
4.4 The ODE and SDE solutions for the two-patch SIS model. Parameter
values are β1 = 0.8, γ1 = 0.1, β2 = 0.3, γ2 = 0.4, α1 = α2 = 0.5, ds12 =
ds21 = 0.1, and di12 = di21 = 0.1 with initial conditions S1(0) = 195,
I1(0) = 5, S2(0) = 185, and I2(0) = 15. . . . . . . . . . . . . . . . . . 72
4.5 Solution of the ODE and one sample path for the CTMC two-patch
SIRS model. Parameter values are β1 = 0.8, γ1 = 0.1, β2 = 0.2,
γ2 = 0.4, ν1 = ν2 = 0.1, α1 = α2 = 0.4, and dskj = dikj = drkj = 0.1 for
k, j = 1, 2 with initial conditions S1(0) = 195, I1(0) = 5 R1(0) = 0,
S2(0) = 185, I2(0) = 15, and R2(0) = 0. . . . . . . . . . . . . . . . . . 73
4.6 The ODE and SDE solutions for the two-patch SIRS model. Parameter
values are β1 = 0.8, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, ν1 = ν2 = 0.1,
α1 = α2 = 0.4, and dskj = dikj = drkj = 0.1 for k, j = 1, 2 with initial
conditions S1(0) = 195, I1(0) = 5 R1(0) = 0, S2(0) = 185, I2(0) = 15,
and R2(0) = 0. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 74
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4.7 Solutions of the ODE and SDE nine-patch SIS models. Parameter
values are βj = 0.3, γj = 0.2 for j = 2, 4, 6, 8, βj = 0.2, γj = 0.4, for
j = 1, 3, 7, 9, β5 = 0.6, and γ5 = 0.3 with initial conditions S5(0) = 95,
I5(0) = 5, and Sj(0) = 100, Ij(0) = 0 for j 6= 5. . . . . . . . . . . . . . 75
4.8 Solutions of the ODE and SDE nine-patch SIS models. Parameter
values are βj = 0.1, γj = 0.4 for j = 1, 2, 3, 4, 7, βj = 0.1, γj = 0.2
for j = 5, 6, 8, and β9 = 0.5 and γ9 = 0.1 with initial conditions
S9(0) = 99, I9(0) = 1, and Sj(0) = 100, Ij(0) = 0 for j 6= 9. . . . . . . 76
4.9 The ODE solution and one sample path for the CTMC two-patch SIS
model with demographics. Parameter values are Λ1 = Λ2 = 2, µ1 =
µ2 = 0.01, β1 = 0.5, γ1 = 0.2, β2 = 0.2, γ2 = 0.5, and dskj = dikj = 0.1
for all k, j = 1, 2 with initial conditions S1(0) = 199, I1(0) = 1, S2(0) =
200, and I2(0) = 0. An outbreak occurs with probability 1−P0 = 0.4265. 87
4.10 Solution of the ODE and SDE two-patch SIS models with demograph-
ics. Parameter values are Λ1 = Λ2 = 2, µ1 = µ2 = 0.01, β1 = 0.5,
γ1 = 0.2, β2 = 0.2, γ2 = 0.5, and dskj = dikj = 0.1 for k, j = 1, 2 with
initial conditions S1(0) = 195, I1(0) = 5, S2(0) = 195, and I2(0) = 5. . 87
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CHAPTER 1
INTRODUCTION
Most ordinary differential equations (ODEs) or systems of ODEs cannot be solved
analytically. Therefore, numerical methods such as Euler’s method or Runge-Kutta
methods are used to solve the equation or system. These numerical methods can be
derived by applying finite difference schemes to the ODE or system of ODEs
resulting in a corresponding difference equation or system of difference equations.
Ideally, the resulting difference equation should have the same properties as the
differential equation. A differential equation and its corresponding difference
equation are said to be dynamically consistent if they have the same properties [52].
Properties of interest may include the existence of periodic solutions, stability of
equilibrium points, or bifurcations.
Liu and Elaydi [52] applied a nonstandard finite-difference (NSFD) scheme to the
Lotka-Volterra competition system and derived a dynamically consistent system of
difference equations which preserves many properties of the ODE system. Using a
NSFD scheme similar to that of Liu and Elaydi, Roeger and Lahodny [63] also
derived a dynamically consistent discrete competition model. In Chapter 2, the
Lotka-Volterra competition system is introduced and some well-known properties of
the system are stated. A general class of difference equations is considered.
Conditions are stated to guarantee that the members of this class are dynamically
consistent with the Lotka-Volterra competition model.
A problem of major interest in mathematical epidemiology is to determine
whether an outbreak of an infectious disease will result in an epidemic. For
deterministic epidemic models, a well-known threshold is the basic reproduction
number, R0. This threshold is defined as the expected number of secondary
infections resulting from the introduction of one infectious individual into a
completely susceptible population [3]. In general, if R0 ≤ 1, the disease will become
extinct and if R0 > 1, the disease persists. Of course, the basic reproduction
number is an expectation. Thus, even if R0 > 1, there is a nonzero probability that
the disease will become extinct. For instance, if an outbreak begins with only one
infectious individual, there is a chance that individual will recover or die before they
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
can infect a susceptible individual. The benefit of using stochastic epidemic models
is that the probability of disease extinction or persistence can be calculated. For
stochastic epidemic models, there is a threshold similar to the basic reproduction
number which is used to predict whether a disease will persist.
In Chapter 3, several epidemic models from the literature are introduced. For
each of these models, the basic reproduction number is calculated and a
corresponding continuous-time Markov chain (CTMC) model is described. Using
the theory of multi-type branching processes, a stochastic threshold is derived to
predict the probability of disease extinction and a new relationship between the
deterministic and stochastic thresholds is illustrated. For specific models, analytical
expressions for the probability of disease extinction are derived. The content in
Chapter 3, co-authored with Linda J.S. Allen, has been published in The Journal of
Biological Dynamics [8].
Infectious diseases in humans or domestic and wild animals such as influenza,
tuberculosis, SARS, and foot-and-mouth disease can be easily transmitted from
region to region. Factors such as spatial connectivity and the dispersal of
individuals through travel can significantly affect the likelihood that a disease will
persist in a given region. For instance, a disease may not be prevalent in rural areas,
but if individuals from an urban center travel to these more remote regions, then
the disease may be more likely to persist. Alternatively, the reverse may be the case
where the disease is present in rural areas and is spread to urban areas [68]. Thus,
dispersal and environmental heterogeneity should be accounted for in epidemic
models.
The role of dispersal on disease dynamics has been examined for general epidemic
models [5, 24, 41, 72] and models focused on particular diseases such as tuberculosis
[25], malaria [33], and influenza [42, 66]. Many of these models involve dividing a
region into multiple patches and allowing dispersal of susceptible or infectious
individuals between these patches [5, 41, 42, 72].
The role of movement also has important implications for disease control. For
instance, it may be possible to stop the spread of a disease by conducting border
checks and restricting the movement of infectious individuals or restricting the
movement to and from high-risk patches where a disease is more prevalent. Ruan,
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Wang, and Levin [65] showed that the spread of SARS can be contained by
implementing border screening for infectious individuals. On the other hand,
screening at the borders is only effective in identifying individuals exhibiting
symptoms. Gao and Ruan [33] state that the dispersal of exposed or latent
individuals can contribute to the spread of disease and that ineffective border
screening may adversely affect disease transmission.
In Chapter 4, stochastic multi-patch epidemic models that are analytically
tractable are developed. These models are used to examine how dispersal between
patches and the location of an outbreak affect the probability of disease persistence
or extinction. These results have important implications for disease control.
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CHAPTER 2
DYNAMICALLY CONSISTENT DISCRETE LOTKA-VOLTERRA
COMPETITION MODELS
In this chapter, the Lotka-Volterra competition model is introduced and a general
class of discrete-time competition models derived from a NSFD scheme is
considered. Sufficient conditions are stated so that the elements of this class of
discrete models are dynamically consistent with the Lotka-Volterra competition
model. The discrete models are shown to preserve the positivity of solutions,
existence and stability conditions of equilibrium points, boundedness of solutions,
and monotonicity of the continuous Lotka-Volterra competition system.
In Section 2.1, the Lotka-Volterra competition model is introduced and some
well-known properties of the model are stated. In addition, dynamically consistent
discrete-time competition models constructed by Liu and Elaydi [52] and Roeger
and Lahodny [63] are discussed. In Section 2.2, a general class of discrete-time
competition models is considered and sufficient conditions are derived to ensure that
the elements of this class of difference equations preserves the properties of the
Lotka-Volterra competition system. In Section 2.3, explicit discrete models are
given and numerical results illustrate dynamical consistency. Finally, in Section 2.4,
the results are summarized and possible future work is presented.
2.1 Introduction
The Lotka-Volterra competition model has the form:
x = x(r1 − a11x− a12y),
y = y(r2 − a21x− a22y),(2.1)
where x and y are the population densities of two competing species, r1 and r2 are
the intrinsic growth rates, and a12 and a21 are the interspecific coefficients. The
“dot” notation denotes differentiation with respect to t, x = dx/dt. Assume that
ri > 0 and aij > 0 for i, j = 1, 2. The properties of system (2.1) are well-known [3]:
1. The positive cone, R2+, is positively invariant. If the initial conditions (x0, y0)
are positive, then the solutions remain positive for all forward time.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
2. There are at most four nonnegative equilibria: the extinction equilibrium
E0 = (0, 0), the single-species equilibria E1 = (r1/a11, 0) and E2 = (0, r2/a22),
and the coexistence equilibrium
E3 =
(r1a22 − r2a12
a11a22 − a12a21
,r2a11 − r1a21
a11a22 − a12a21
).
The coexistence equilibrium lies in R2+ provided that
a11
a21
<r1
r2
<a12
a22
ora11
a21
>r1
r2
>a12
a22
.
3. The stability properties of the equilibria are:
(a) E0 is always unstable
(b) E1 is locally asymptotically stable ifa11
a21
<r1
r2
(c) E2 is locally asymptotically stable ifr1
r2
<a12
a22
(d) E3 is locally asymptotically stable if and only if (iff)
a11
a21
>r1
r2
>a12
a22
.
Moreover, if E3 is stable, it is globally asymptotically stable.
4. The system is competitively monotone.
5. The solutions are eventually bounded in the set S = [0, r1/a11]× [0, r2/a22].
The set S is positively invariant.
The term “dynamically consistent” was first used by Liu and Elaydi [52]. If a
discrete system has the same properties as the corresponding continuous system,
then the discrete and continuous systems are said to be dynamically consistent.
Properties of interest may include positivity of solutions, existence and stability of
equilibrium points, periodicity of solutions, and bifurcations. A formal definition is
given by Mickens [54].
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Definition 2.1. (Mickens, [54]) Consider the differential equation
dx
dt= f(x, t, λ) (2.2)
and a discrete model of it given by
xk+1 = F (xk, tk, h, λ). (2.3)
We assume that f is such that the proper existence-uniqueness theorem holds; λ
represents the parameters defining the system; the time step-size is h = ∆t with
tk = hk, k an integer; and xk is an approximation to x(tk). Let the differential
equation and/or its solutions have property P . The discrete model, given by
equation (2.3), is dyamically consistent with equation (2.2), with respect to property
P , if it has and/or its solutions also have property P .
The following example illustrates the application of finite-difference schemes to a
one-dimensional ODE in order to derive a dynamically consistent difference
equation.
Consider the decay equation
x = −ax, (2.4)
where a > 0. The solution of this equation is well-known, x(t) = x0e−at. A forward
Euler scheme for (2.4) isxn+1 − xn
h= −axn,
where h = ∆t, tn = hn, and xn is an approximation of x(tn). It follows that
xn+1 = xn(1− ah),
and so
xn = x0(1− ah)n.
Note that the solution of the differential equation, x(t) = x0e−at, and the solution of
the difference equation, xn = x0(1− ah)n, do not necessarily have the same
properties. For instance, if h = 2/a, the solution xn = x0(1− ah)n oscillates between
positive and negative x0 while x(t) = x0e−at decreases monotonically to zero. Only
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
if h is sufficiently small, 0 < h < 1/a, will the solution xn = x0(1− ah)n decrease
monotonically to zero. Alternatively, a backward Euler scheme for (2.4) is
xn+1 − xnh
= −axn+1.
Solving for xn+1,
xn+1 =xn
1 + ah.
It follows that
xn =x0
(1 + ah)n. (2.5)
Since ah > 0, the solution xn = x0/(1 + ah)n decreases monotonically to zero
regardless of the choice for h. Thus, (2.5) preserves positivity and monotonicity of
the soluion to (2.4). For additional examples in one dimension, see [11, 31, 62, 64].
Liu and Elaydi [52] constructed the following NSFD scheme for the
Lotka-Volterra system (2.1):
X − xφ
= r1x− a11xX − a12yX,
Y − yφ
= r2y − a21xY − a22yY,(2.6)
where X = xn+1, x = xn, and φ = h+O(h2).
The NSFD scheme of Liu and Elaydi leads to the system of difference equations
X = x
(1 + φr1
1 + φ(a11x+ a12y)
),
Y = y
(1 + φr2
1 + φ(a21x+ a22y)
).
(2.7)
Cushing et al. [28] showed that the system of difference equations (2.7) preserves
many properties of the differential equation system (2.1) including positivity of
solutions, existence and stability conditions of equilibrium solutions, monotonicity,
and boundedness of solutions.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Following the discretization example (2.6), Roeger and Lahodny [63] constructed
the following NSFD scheme for system (2.1):
X − xφ1
= r1[(1 + θ1)x− θ1X]− a11x[(1 + θ11)X − θ11x]
−a12y[(1 + θ12)X − θ12x],Y − yφ2
= r2[(1 + θ2)y − θ2Y ]− a21x[(1 + θ21)Y − θ21y]
−a22y[(1 + θ22)Y − θ22y],
(2.8)
where φi > 0, θi ≥ 0, and θij ≥ 0 for i, j = 1, 2. In the special case that φ1 = φ2,
θi = 0, and θij = 0 for all i, j = 1, 2, this system is reduced to (2.6).
The NSFD scheme of Roeger and Lahodny leads to the system of difference
equations
X = x · 1 + φ1r1 + φ1(r1θ1 + a11θ11x+ a12θ12y)
1 + φ1(r1θ1 + a11θ11x+ a12θ12y) + φ1(a11x+ a12y),
Y = y · 1 + φ2r2 + φ2(r2θ2 + a21θ21x+ a22θ22y)
1 + φ2(r2θ2 + a21θ21x+ a22θ22y) + φ2(a21x+ a22y),
(2.9)
where X = xn+1, x = xn, φi > 0, θi ≥ 0, and θij ≥ 0 for i, j = 1, 2.
If θ11 ≥ θ12 and θ22 ≥ θ21, then the system of difference equations (2.9) preserves
the positivity of solutions, existence and stability conditions for each equilibrium
solution, and monotonicity [63]. Note that (2.9) can be written as
X = x · F1(x, y) + φ1r1
F1(x, y) + φ1(a11x+ a12y),
Y = y · F2(x, y) + φ2r2
F2(x, y) + φ2(a21x+ a22y),
(2.10)
where
F1(x, y) = 1 + φ1(r1θ1 + a11θ11x+ a12θ12y),
F2(x, y) = 1 + φ2(r2θ2 + a21θ21x+ a22θ22y).
Similarly, (2.7) can be written as (2.10), where F1(x, y) = F2(x, y) = 1. The system
of difference equations (2.9) is a complicated system with many parameters. The
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
goal is to find other, more simplistic, functions F1 and F2 such that a system of the
form (2.10) is dynamically consistent with the Lotka-Volterra competition system
(2.1). In the next section, a generalized discrete competition model of the form
(2.10) is explored.
2.2 Discrete Lotka-Volterra Competition Models
Consider a discrete Lotka-Volterra competition model of the form:
X = x · F1(x, y) + φ1r1
F1(x, y) + φ1(a11x+ a12y),
Y = y · F2(x, y) + φ2r2
F2(x, y) + φ2(a21x+ a22y),
(2.11)
where X = xn+1, x = xn, and φi > 0 for i, j = 1, 2.
To ensure that solutions of (2.11) remain in the positive cone, R2+, assume that
the functions F1 and F2 are positive-valued for all (x, y) ∈ R2+.
2.2.1 Existence and Local Stability of Equilibria
A discrete competition system of the form (2.11) is shown to be dynamically
consistent with the Lotka-Volterra competition system (2.1) with respect to the
existence and stability conditions for each equilibrium regardless of the choice of the
functions F1 and F2.
Note that (2.11) can be written as
X = x+φ1x(r1 − a11x− a12y)
F1(x, y) + φ1(a11x+ a12y),
Y = y +φ2y(r2 − a21x− a22y)
F2(x, y) + φ2(a21x+ a22y).
The following lemma states that the discrete system (2.11) has the same
equilibrium solutions as the Lotka-Volterra competition system (2.1).
Lemma 2.1. The discrete competition system (2.11) is dynamically consistent with
the continuous system (2.1) with respect to the equilibrium points.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Proof. To find the equilibria of (2.11), set X = x and Y = y. It follows that
x(r1 − a11x− a12y) = 0,
y(r2 − a21x− a22y) = 0.
The solutions of this system are the equilibrium solutions of the Lotka-Volterra
competition model (2.1).
The next lemma determines the stability of the equilibrium points for the discrete
model (2.11).
Lemma 2.2. The discrete competition system (2.11) is dynamically consistent with
the continuous system (2.1) with respect to the local stability of the equilibrium
points E0, E1, and E2.
Proof. The Jacobian matrix for (2.11) evaluated at E0 is
J(E0) =
1 +r1
F1(0, 0)0
0 1 +r2
F2(0, 0)
.Since the eigenvalues are both greater than one, E0 is unstable. At E1,
J(E1) =
1− r1
F1(E1) + r1
− a12(r1/a11)
F1(E1) + r1
0 1 +r2 − a21(r1/a11)
F2(E1) + a21(r1/a11)
.The eigenvalues of this matrix are the diagonal entries. Thus, the equilibrium E1 is
locally asymptotically stable provided that r2 − a21(r1/a11) < 0. That is,
a11
a21
<r1
r2
.
Similarly, the equilibrium E2 is locally asymptotically stable if
r1
r2
<a12
a22
.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
The following theorem states that the stability condition for the coexistence
equilibrium E3 of the discrete system is the same as for the continuous system.
Systems (2.1) and (2.11) are dynamically consistent with respect to the local
stability of all equilibrium points.
Theorem 2.1. The coexistence equilibrium E3 of (2.11) is locally asymptotically
stable if and only if a11a22 − a12a21 > 0.
Proof. The Jury conditions [3] state that an equilibrium point (x, y) of a
two-dimensional system is locally asymptotically stable if
|trace(J(x, y))| < 1 + det(J(x, y)) < 2.
At the coexistence equilibrium E3 = (x, y),
J(E3) =
1− a11x
F1 + a11x+ a12y− a12x
F1 + a11x+ a12y
− a21y
F2 + a21x+ a22y1− a22y
F2 + a21x+ a22y
.Clearly trace(J) > 0. So |trace(J)| < 1 + det(J) iff 1 + det(J)− trace(J) > 0. Now
1 + det(J)− trace(J) =(a11a22 − a12a21)xy
(F1 + a11x+ a12y)(F2 + a21x+ a22y).
which is positive iff a11a22 − a12a21 > 0. Moreover, 1 + det(J) < 2 iff 1− det(J) > 0.
Now
1−det(J) =a11x
F1 + a11x+ a12y+
a22y
F2 + a21x+ a22y− (a11a22 − a12a21)xy
(F1 + a11x+ a12y)(F2 + a21x+ a22y).
It is straightforward to show that this expression is positive. By the Jury conditions,
the equilibrium E3 is locally asymptotically stable iff a11a22 − a12a21 > 0.
2.2.2 Monotonicity, Positive Invariance, and Global Stability
Conditions are derived so that the discrete system (2.11) is a competitive
monotone system. Let X = X(x, y) and Y = Y (x, y).
Lemma 2.3. Suppose that
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
(i)∂F1
∂xand f1(x, y) = x(r1 − a11x− a12y) have opposite signs for all (x, y) ∈ R2
+,
(ii)∂F2
∂xand f2(x, y) = y(r2 − a21x− a22y) have the same sign for all (x, y) ∈ R2
+.
If 0 ≤ x1 ≤ x2 and y ≥ 0 is fixed, then for system (2.11)
X(x1, y) ≤ X(x2, y) and Y (x1, y) ≥ Y (x2, y).
Proof. Fix y ≥ 0 and for i = 1, 2 set
D1i = F1(xi, y) + φ1(a11xi + a12y),
D2i = F2(xi, y) + φ2(a21xi + a22y).
Then
X(x2, y)−X(x1, y) = (x2− x1) +φ1x2(r1 − a11x2 − a12y)
D12
− φ1x1(r1 − a11x1 − a12y)
D11
.
This expression is nonnegative iff
D11D12(x2 − x1) + φ1D11x2(r1 − a11x2 − a12y)− φ1D12x1(r1 − a11x1 − a12y) ≥ 0.
Applying a computer algebra system such as Maple, the above inequality holds iff
φ21r1a12y(x2 − x1) + φ1r1(F1(x1, y)x2 − F1(x2, y)x1) + φ1a11x1x2(F1(x2, y)− F1(x1, y))
+φ1a12y(F1(x2, y)x2 − F1(x1, y)x1) + F1(x1, y)F1(x2, y)(x2 − x1) ≥ 0.
Since x2 ≥ x1,
φ1r1(F1(x1, y)x2 − F1(x2, y)x1) + φ1a11x1x2(F1(x2, y)− F1(x1, y))
+φ1a12y(F1(x2, y)x2 − F1(x1, y)x1)
≥ φ1r1(F1(x1, y)x1 − F1(x2, y)x1) + φ1a11x21(F1(x2, y)− F1(x1, y))
+φ1a12y(F1(x2, y)x1 − F1(x1, y)x1)
≥ φ1(F1(x2, y)− F1(x1, y))x1(a11x1 + a12y − r1)
= −φ1(F1(x2, y)− F1(x1, y))f1(x1, y) ≥ 0.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Similarly,
Y (x1, y)− Y (x2, y) =φ2y(r2 − a21x1 − a22y)
D21
− φ2y(r2 − a21x2 − a22y)
D22
.
This expression is nonnegative iff
φ2D22y(r2 − a21x1 − a22y)− φ2D21y(r2 − a21x2 − a22y) ≥ 0.
Applying a computer algebra system such as Maple, the above inequality holds iff
φ22r2a21y(x2 − x1) + φ2r2y(F2(x2, y)− F2(x1, y)) + φ2a21y(x2F2(x1, y)− x1F2(x2, y))
+φ2a22y2(F2(x1, y)− F2(x2, y)) ≥ 0.
Since x2 ≥ x1,
φ2r2y(F2(x2, y)− F2(x1, y)) + φ2a21y(x2F2(x1, y)− x1F2(x2, y))
+φ2a22y2(F2(x1, y)− F2(x2, y))
≥ φ2(F2(x1, y)− F2(x2, y))(a21x1 + a22y − r2)
= −φ2(F2(x1, y)− F2(x2, y))f2(x1, y) ≥ 0.
By a symmetric argument, the following lemma is not difficult to prove.
Lemma 2.4. Suppose that
(i)∂F1
∂yand f1(x, y) = x(r1 − a11x− a12y) have the same sign for all (x, y) ∈ R2
+,
(ii)∂F2
∂yand f2(x, y) = y(r2 − a21x− a22y) have opposite signs for all (x, y) ∈ R2
+.
If 0 ≤ y1 ≤ y2 and x ≥ 0 is fixed, then for system (2.11)
X(x, y1) ≥ X(x, y2) and Y (x, y1) ≤ Y (x, y2).
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Proof. Fix x ≥ 0 and for i = 1, 2 set
E1i = F1(x, yi) + φ1(a11x+ a12yi),
E2i = F2(x, yi) + φ2(a21x+ a22yi).
Then
Y (x, y2)− Y (x, y1) = (y2 − y1) +φ2y2(r2 − a21x− a22y2)
E22
− φ2y1(r2 − a21x− a22y1)
E21
.
This expression is nonnegative iff
E21E22(y2 − y1) + φ2E21y2(r2 − a21x− a22y2)− φ2E22y1(r2 − a21x− a22y1) ≥ 0.
Applying a computer algebra system such as Maple, the above inequality holds iff
φ22r2a21x(y2 − y1) + φ2r2(F2(x, y1)y2 − F2(x, y2)y1) + φ2a22y1y2(F2(x, y2)− F2(x, y1))
+φ2a21x(F2(x, y2)y2 − F2(x, y1)y1) + F2(x, y1)F2(x, y2)(y2 − y1) ≥ 0.
Since y2 ≥ y1,
φ2r2(F2(x, y1)y2 − F2(x, y2)y1) + φ2a22y1y2(F2(x, y2)− F2(x, y1))
+φ2a21x(F2(x, y2)y2 − F2(x, y1)y1)
≥ φ2r2y1(F2(x, y1)− F2(x, y2)) + φ2a22y21(F2(x, y2)− F2(x, y1))
+φ2a21xy1(F2(x, y2)− F2(x, y1))
= −φ2(F2(x, y2)− F2(x, y2))f2(x, y1) ≥ 0.
Similarly,
X(x, y1)−X(x, y2) =φ1x(r1 − a11x− a12y1)
E11
− φ1x(r1 − a11x− a12y2)
E12
.
This expression is nonnegative iff
φ1E12x(r1 − a11x− a12y1)− φ1E11x(r1 − a11x− a12y2).
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Applying a computer algebra system such as Maple, the above inequality holds iff
φ21r1a12x(y2 − y1) + φ1r1x(F1(x, y2)− F1(x, y1)) + φ1a12x(y2F1(x, y1)− y1F1(x, y2))
+φ1a11x2(F1(x, y1)− F1(x, y2)) ≥ 0.
Since y2 ≥ y1,
φ1r1x(F1(x, y2)− F1(x, y1)) + φ1a12x(y2F1(x, y1)− y1F1(x, y2))
+φ1a11x2(F1(x, y1)− F1(x, y2))
≥ φ1(F1(x, y1)− F1(x, y2))(a11x1 + a12y − r1)
= −φ1(F1(x, y1)− F1(x, y2))f1(x, y1) ≥ 0.
Theorem 2.2. Suppose that conditions (i) and (ii) in Lemmas 2.3 and 2.4 hold. If
0 < x1 ≤ x2 and 0 < y2 ≤ y1, then for system (2.11)
X(x1, y1) ≤ X(x2, y2) and Y (x1, y1) ≥ Y (x2, y2).
That is, the discrete system (2.11) is a competitive monotone system.
Proof. Applying the previous two lemmas,
X(x1, y1) ≤ X(x2, y1) ≤ X(x2, y2)
and
Y (x1, y1) ≥ Y (x2, y1) ≥ Y (x2, y2).
Note that the conditions in Theorem 2.2 are sufficient but not necessary. Indeed,
the discrete system (2.11) preserves monotonicity if F1 and F2 are positive constants
or if F1 and F2 are positive linear functions of x and y, respectively. That is, if
F1(x, y) = a1x+ b1 and F2(x, y) = a2y + b2, where a1, a2, b1, and b2 are positive
constants.
Theorem 2.3. For the discrete model (2.11), the set S = [0, r1/a11]× [0, r2/a22] is
positively invariant.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Proof. Let X = X(x, y) and Y = Y (x, y) in (2.11) and suppose (x, y) ∈ S. That is,
0 ≤ x ≤ r1/a11 and 0 ≤ y ≤ r2/a22. Since F1 and F2 are positive-valued for all
(x, y) ∈ R2+, both X and Y are positive. Moreover,(
X − r1
a11
)−(x− r1
a11
)= X − x
= x
(F1 + φ1r1
F1 + φ1(a11x+ a12y)
)− x
≤ x
(F1 + φ1r1
F1 + φ1a11x
)− x
= x
(1 +
φ1(r1 − a11x)
F1 + φ1a11x
)− x
= x
(φ1(r1 − a11x)
F1 + φ1a11x
)= −φ1a11x
(x− r1/a11
F1 + φ1a11x
).
It follows that
X − r1
a11
=
(x− r1
a11
)(1− φ1a11x
F1(x, y) + φ1a11x
)≤ 0,
and so 0 ≤ X ≤ r1/a11. Similarly, 0 ≤ Y ≤ r2/a22. By induction, the set S is
positively invariant.
Lemma 2.5. Solutions of the discrete model (2.11) are eventually bounded. That is,
lim supn→∞
xn ≤r1
a11
and lim supn→∞
yn ≤r2
a22
.
Proof. As in the proof of Theorem 2.3,(X − r1
a11
)−(x− r1
a11
)≤ φ1x
(r1/a11 − xF1 + φ1a11x
).
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
The right-hand side is negative iff x > r1/a11. It follows that if x > r1/a11, then(X − r1
a11
)<
(x− r1
a11
).
That is, X is closer to r1/a11 than x. Similarly, if y > r2/a22 then Y is closer to
r2/a22 than y. Thus, if (x0, y0) lies outside of the set S, then trajectories approach
the boundary of S. On the other hand, if (x0, y0) ∈ S, then (xn, yn) ∈ S for all
n > 0. In either case, solutions eventually lie in S. That is,
lim supn→∞
xn ≤r1
a11
,
lim supn→∞
yn ≤r2
a22
.
The preceding results have established that if F1 and F2 are positive-valued
functions for all (x, y) ∈ R2+, then a discrete competition system of the form (2.11)
and the Lotka-Volterra competition model (2.1) are dynamically consistent with
respect to the positive invariance of R2+, the existence and local stability conditions
of the equilibrium solutions E0, E1, E2, and E3, positive invariance of the set
S = [0, r1/a11]× [0, r2/a22], and the boundedness of solutions within the set S.
Furthermore, if the functions F1 and F2 satisfy the following conditions:
(i)∂F1
∂xand f1 have opposite signs for all (x, y) ∈ R2
+,
(ii)∂F2
∂xand f2 have the same sign for all (x, y) ∈ R2
+,
(iii)∂F1
∂yand f1 have the same sign for all (x, y) ∈ R2
+,
(iv)∂F2
∂yand f2 have opposite signs for all (x, y) ∈ R2
+,
then the systems (2.11) and (2.1) are both competitive monotone systems.
A theorem by Smith [69] is used to establish the global stability of the coexistence
equilibrium, E3. A 2× 2 matrix J is called K-positive if J11 > 0, J12 < 0, J21 < 0,
and J22 > 0 for all (x, y) ∈ R2+ [63].
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Theorem 2.4. (Smith, [69]) Suppose a map P : S → S is continuously
differentiable and satisfies the following:
(a) S contains order intervals and is ≤K-convex,
(b) det(DP (x)) > 0 for x ∈ S; the map is orientation preserving,
(c) DP (x) is K-positive in S,
(d) P is injective.
Then P is a competitive map and P nx is eventually componentwise monotone for
all x ∈ S. In this case, if an orbit has compact closure in S, then it converges to a
fixed point of P .
Consider the map P defined by P (x, y) = (X(x, y), Y (x, y)). By Theorem 2.3,
P : S → S is a map from the compact, connected set S into itself.
Lemma 2.6. If conditions (i) and (ii) from Lemmas 2.3 and 2.4 hold, the Jacobian
matrix J is K-positive in R2+.
The preceding result follows directly from Theorem 2.2. The following lemma
shows that the discrete map is orientation preserving. That is, the determinant of
the Jacobian matrix is always positive.
Lemma 2.7. Suppose the two conditions (i) from Lemma 2.3 and Lemma 2.4 hold
and ∂F1/∂y = ∂F2/∂x = 0. Then det(J) > 0 for all (x, y) ∈ R2+.
Proof. For ease of notation, denote the partial derivatives of F1 and F2 with respect
to x and y by F1x, F1y, F2x, and F2y, respectively. The result follows easily using a
computer algebra system such as Maple. The determinant of the Jacobian matrix is:
det(J) =1
[F1 + φ1(a11x+ a12y)]2[F2 + φ2(a21x+ a22y)]2· φ1F
22F1x(−f1)
+φ2F21F2y(−f2) + (F1F2 + φ1a12yF2 + φ2a21xF1)(F1 + φ1r1)(F2 + φ2r2)
+φ1φ2[r1F1F2y(−f2) + r2F2F1x(−f1) + φ1r1a12yF2y(−f2) + φ2r2a21xF1x(−f1)
+xyF1xF2y(−f1)(−f2) + a21xF2F1x(−f1) + a12yF1F2y(−f2) + F1yF2x(−f1)(f2)
+a21yF1y(−f1)(φ2r2 + F2) + a12xF2x(−f2)(φ1r1 + F1)].
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
The only possible non-positive terms are
φ1φ2[F1yF2x(−f1)(f2) + a21yF1y(−f1)(φ2r2 + F2) + a12xF2x(−f2)(φ1r1 + F1)].
Since F1y = F2x = 0, these terms equal zero and det(J) > 0.
In order to apply Smith’s theorem, the map P must be injective. As noted by
Smith, since S = [0, r1/a11]× [0, r2/a22] is compact and connected, it is enough to
show that there exists (x, y) ∈ P (S) ⊂ S such that P−1(x, y) is a single point.
Consider the point (0, 0) ∈ P (S). Since all nonzero points in S are mapped to
nonzero points in S, it follows that P−1(0, 0) = (0, 0), a single point. Applying
Theorem 2.4, we have the following result.
Theorem 2.5. Suppose that the conditions of Lemma 2.7 hold. Then all solutions of
the discrete system (2.11) converge to one of the equilibria. Thus, if the coexistence
equilibrium E3 is locally asymptotically stable, it is also globally stable in R2+.
2.3 Numerical Examples
In this section, discrete competition models of the form (2.11) are compared to
Euler’s method. Applying Euler’s method to the Lotka-Volterra competition system
(2.1) leads to the system of difference equations:
X = x[1 + h(r1 − a11x− a12y)],
Y = y[1 + h(r2 − a21x− a22y)].(2.12)
In order for this system to preserve the positivity of solutions, the step size, h > 0,
must be sufficiently small. That is,
h(a11x+ a12y − r1) ≤ 1,
h(a21x+ a22y − r2) ≤ 1,
for all (x, y) ∈ R2+. However, for any h > 0 there exists (x, y) ∈ R2
+ such that these
inequalities are not satisfied. Thus, Euler’s method does not preserve the positivity
of solutions for (2.1). On the other hand, if the initial conditions are relatively
small, then Euler’s method yields a good approximation.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Consider a discrete competition model of the form (2.11). As stated in Section
2.3, it is difficult to find explicit functions F1 and F2 that satisfy the hypotheses of
Theorem 2.2. A trivial example is to choose F1 and F2 to be positive constants. In
the special case where F1 = F2 = 1, (2.11) is the discrete model constructed by the
NSFD scheme of Liu and Elaydi (2.6).
Let us now compare several discrete models of the form (2.11) to Euler’s method.
The solution of (2.1) is approximated using four distinct numerical methods. The
numerical methods used are Euler’s method (2.12), the discrete model of Liu and
Elaydi (2.7), the discrete model of Roeger and Lahodny (2.9), and a discrete model
of the form (2.11) where F1(x, y) = F2(x, y) = 0.2. Consider the parameter values
r1 = 2, r2 = 3, a11 = 0.02, a12 = 0.01, a21 = 0.02, and a22 = 0.03. For the discrete
models of Liu and Elaydi and Roeger and Lahodny, let φ1 = φ2 = φ = h. For these
values, a11a22 − a12a21 > 0, and so the coexistence equilibrium E3 = (75, 50) lies in
R2+ and is globally asymptotically stable. For each of these discrete models with an
initial condition of (x0, y0) = (5, 5), solutions approach the equilibrium E3. The
solutions of the four discrete models are graphed in the phase plane in Figure 2.1
and as a function of time in Figure 2.2. It should be noted that for a fixed time t,
the numerical method does not converge for F1(x, y) = F2(x, y) = 0.2.
Figure 2.1. Four approximate solutions to the Lotka-Volterra competition model inthe phase plane. For figure (a), the step size is h = 0.5 and for figure (b), the stepsize is h = 0.1.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Figure 2.2. Four approximate solutions to the Lotka-Volterra competition model asa function of time. Parameter values and initial conditions are the same as in Figure2.1 with a step size of h = 0.1.
2.4 Discussion
A general class of the discrete-time competition models was considered. Provided
that F1 and F2 are positive-valued functions for all (x, y) ∈ R2+, the discrete model
(2.11) preserves the positivity of solutions, existence and local stability conditions
for each equilibrium, and the boundedness of solutions within the set
S = [0, r1/a11]× [0, r2/a22]. If additional restrictions are imposed on the functions
F1 and F2, the discrete model also preserves the monotonicity of the system (2.1)
and the global stability of the coexistence equilibrium. However, it is difficult to
find explicit functions F1 and F2 which satisfy these conditions.
Since the discrete models discussed here are for the Lotka-Volterra competition
model, discrete versions of the Lotka-Volterra predator-prey and cooperative
systems could also be considered in the future.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
CHAPTER 3
EXTINCTION OR PERSISTENCE OF DISEASE IN STOCHASTIC EPIDEMIC
MODELS
3.1 Introduction
The basic reproduction number, R0, is defined as the expected number of
secondary infections caused by one infectious individual during their infectious
period [10, 40]. This is a well-known threshold for deterministic epidemic models
which is used to determine whether a disease will persist. In general, if R0 > 1, the
disease persists and if R0 ≤ 1, the disease dies out. The basic reproduction number
can be calculated using the next-generation matrix approach of Diekmann et al. [29]
and van den Driessche and Watmough [70, 71]. This method involves linearizing the
system of ordinary differential equations (ODEs) about the disease-free equilibrium
(DFE). Heesterbeek and Roberts [39, 61] derived equivalent thresholds relating to
the control of a specific infectious group i known as type reproduction numbers, Ti.The type reproduction numbers can also be used to predict disease persistence
(Ti > 1) or extinction (Ti < 1).
Continuous-time Markov chain models are the stochastic counterpart of the ODE
model. For CTMC models, time is continuous and the random variables are
discrete. Similar to the basic reproduction number for deterministic epidemic
models, in stochastic epidemic theory there is a threshold which is used to predict
the probability of disease persistence or extinction for the CTMC model. The
stochastic threshold is similar to the basic reproduction number. In fact, Allen and
van den Driessche [9] showed that the stochastic threshold is equivalent to the basic
reproduction number R0. The theory behind the stochastic threshold depends on
continuous-time branching processes. Whittle [73] derived an expression for the
probability of disease persistence for a susceptible-infectious-recovered (SIR) model
provided that the population size is sufficiently large and a small number of
infectious individuals are present. If the initial number of infectious individuals is
I(0) = i, the probability of disease persistence is
1−(
1
R0
)i. (3.1)
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
The result of Whittle is only valid under certain assumptions. In particular, it is
assumed that infectious individuals give ‘birth’ to new infectious individuals
independently of others and that each individual has the same probability of giving
birth. These two assumptions are fundamental in Galton-Watson branching process
theory [16, 38, 44, 55, 60]. Provided that there is a large population size and a small
number of infectious individuals, these assumptions may be realistic and the
approximation (3.1) of Whittle is a good approximation.
Of course, this approximation is only valid for epidemic models with one
infectious class. If there are multiple infectious classes, the probability of disease
persistence depends on the number of infectious individuals in each class. In
particular if there are n infectious classes, Ij(0) = ij infectious individuals in class j
for j = 1, . . . , n, and the probability of extinction for class j is qj, then a well-known
result from multitype branching processes [4, 16, 38, 60] states that the probability
of disease persistence is approximately
1− qi11 qi22 · · · qinn . (3.2)
However, this approximation is only valid under certain restrictions. There have
been several applications of branching process theory to obtain estimates for the
probability of extinction for populations, genetics, cellular processes, and epidemics
on networks [19, 20, 23, 30, 36, 44, 48, 57, 59, 74].
Typically, the deterministic and stochastic thresholds are discussed separately.
The goals of this chapter are to review some classic results on the thresholds for
epidemic models and illustrate a relationship between the deterministic and
stochastic thresholds. Furthermore, these thresholds are calculated for some
well-known epidemic models from the literature. In Section 3.2, some useful
methods and results from probability theory, branching process theory, and the
theory of continuous-time Markov chains will be discussed. In Section 3.3, the
dynamics of an epidemic model with one infectious class will be summarized and
Whittle’s approximation (3.1) for the probability of disease persistence is derived.
In Section 3.4, the deterministic and stochastic thresholds are calculated for
epidemic models with multiple infectious classes and new expressions are derived for
the probability of disease persistence.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
3.2 Mathematical Methods
A common method for calculating the basic reproduction number is the
next-generation matrix approach. This method will be discussed here briefly. For
more details on the next-generation matrix approach, see Diekmann et al. [29] and
van den Driessche and Watmough [70, 71].
Let ~I = (I1, . . . , In)T denote the vector of infectious individuals so that Ij is the
number of infectious individuals in class j. Linearizing the system of differential
equations about the DFE gives
d~I
dt= J~I = (F − V )~I,
where J = F − V is the Jacobian matrix evaluated at the DFE. The matrix F
contains all terms which represent new infections and the matrix V contains all
remaining terms such as the rates of recovery, death, or transition between
infectious classes. The next-generation matrix is the matrix FV −1 and the basic
reproduction number is the spectral radius of this matrix [70, 71]. That is,
R0 = ρ(FV −1).
Sufficient conditions were stated by van den Driessche and Watmough [70, 71] to
guarantee that the DFE is locally asymptotically stable if R0 < 1. The basic
reproduction number may be interpreted biologically as the asymptotic
per-generation growth rate [29, 43].
The type reproduction numbers may also be calculated from the next-generation
matrix using the method of Heesterbeek and Roberts [39, 61]. This method will be
described breifly. Let K = FV −1 denote the next-generation matrix, ej denote the
jth unit column vector, and Pj denote the n× n matrix with all zero entries except
for the diagonal element pjj = 1. In the first generation, the number of infections of
type j is eTj Kej = kjj. In the second generation, the number of infections of type j
is eTj K[(I− Pj)K]ej, where I is the n× n identity matrix. In generation n, the
number of infections of type j is eTj K[(I− Pj)K]n−1ej. In general, the type
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
reproduction number for the control of a single infectious group Ij is
Tj = eTj K∞∑k=1
[(I− Pj)K]kej = eTj K[I− (I− Pj)K]−1ej,
provided that ρ((I− Pj)K) < 1 and K is irreducible [39, 61]. In the case of one
infectious group, n = 1, the type reproduction number equals the basic reproduction
number, T1 = R0. If there are n = 2 infectious groups, there is a type reproduction
number for each group. They are
T1 = k11 +k12k21
1− k22
,
T2 = k22 +k12k21
1− k11
.
The assumption that K is irreducible requires k12k21 6= 0, and in order for Ti to
exist, kjj < 1 for j = 1, 2.
Roberts and Heesterbeek [61] illustrated that 1−R0 and 1− Ti are either both
positive, negative, or equal to zero. Allen and Lahodny [8] showed that for two
infectious groups, one of the following relationships holds:
Ti < R0 < 1 or Ti > R0 > 1 or Ti = R0 = 1. (3.3)
This relationship between Ti and R0 makes sense biologically. The inequality
T1 > R0 > 1 implies that if the basic reproduction number is greater than one, then
more effort is needed to control a single infectious group than to control both
groups. These deterministic thresholds can be extended to models with periodic or
heterogeneous environments [17, 18, 43].
Next we summarize some results from the theory of multitype branching
processes. The focus will be on results relating to the probability of extinction
[16, 44, 45, 55, 60]. For more details on branching processes and their applications,
consult the following references [16, 30, 36, 38, 44, 45, 48, 55].
Let ~I(t)|t ∈ [0,∞) be a collection of discrete random vectors where~I(t) = (I1(t), . . . , In(t))T . For simplicity, the same notation is used for the random
variables as for the deterministic variables. Assume that individuals of type i give
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
‘birth’ to individuals of type j and that the number of offspring produced by a type
i individual is independent of the number of offspring produced by other type i
individuals or individuals of type j 6= i. Let Yjinj=1 denote the offspring random
variables for a type i individual. That is, Yji is the number of type j offspring
produced by one type i individual for i = 1, . . . , n. Denote the probability that one
type i individual produces kj type j individuals as
Pi(k1, . . . , kn) = ProbY1i = k1, . . . , Yni = kn.
Given Ii(0) = 1 and Ij(0) = 0 for j 6= i, define the offspring probability generating
function (pgf) for type i as
fi(x1, . . . , xn) =∞∑
kn=0
· · ·∞∑k1=0
Pi(k1, . . . , kn)xk11 · · · xknn .
Note that fi always has a fixed point at ~1 = (1, . . . , 1). That is, fi(1, . . . , 1) = 1 for
i = 1, . . . , n.
Assume that each offspring pgf fi is not simple. That is, fi is not a linear function
of the variables xj and fi(0, . . . , 0) 6= 0. Explicitly,
fi(x1, . . . , xn) 6=n∑j=1
ajxj.
The expectation matrix M = [mji] is a nonnegative n× n matrix such that the
element mji is the expected number of type j offspring produced by a type i
individual. That is,
mji =∂fi∂xj
∣∣∣∣~x=~1
.
Assume that the matrix M is irreducible.
Under the assumptions that fi is not simple and M is irreducible, the spectral
radius of the expectation matrix, ρ(M), determines whether the probability of
extinction is less than or equal to one [16, 38, 60]. If ρ(M) ≤ 1, the probability of
disease extinction is one
limt→∞
Prob~I(t) = ~0 = 1.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
If ρ(M) > 1, there exists a unique fixed point (q1, . . . , qn) ∈ (0, 1)n of the offspring
pgfs, fi(q1, . . . , qn) = qi for i = 1, . . . , n, such that the probability of disease
extinction is
P0 = limt→∞
Prob~I(t) = ~0 = qi11 · · · qinn < 1,
where ij = Ij(0) [16, 60]. This expression follows from the assumption that the
offspring random variables Yji are independent.
3.3 Single Infectious Group
Consider the classic SIR epidemic model where S, I, and R denote the number of
susceptible, infectious, and recovered individuals, respectively. Let N = S + I +R
denote the total population size. The model consists of three ODEs:
S = Λ− dS − βSI
N,
I =βSI
N− (d+ γ + α)I,
R = γI − dR,
where S(0) > 0, I(0) > 0, and R(0) = 0. The parameter Λ is the immigration/birth
rate, βSI/N is the rate at which susceptible individuals are infected, d is the natural
death rate, γ is the recovery rate, and α is the disease-related death rate. The DFE
is (S, 0, 0) = (Λ/d, 0, 0). The basic reproduction number for the SIR model is
R0 =β
d+ γ + α.
The same basic reproduction number applies to SIS and SIRS models as well. This
formula for the basic reproduction number follows directly from the differential
equation for I when S ≈ N . If R0 ≤ 1, then solutions approach the DFE and if
R0 > 1, then solutions approach a unique endemic equilibrium [49].
The corresponding CTMC SIR model can be defined in terms of the transitions
that occur in the stochastic process ~X(t) = (S(t), I(t), R(t)), t ∈ [0,∞) during some
infinitesimally small time ∆t, and the corresponding transition probabilities,
Prob ~X(t+ ∆t) = ~b| ~X(t) = ~a = P (~a,~b)∆t+ o(∆t).
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The random variables S, I, and R are discrete-valued and continuous in time. For
simplicity, the same notation is used for the random variables and the deterministic
variables. The transitions and rates are given in Table 3.1.
Table 3.1. Transitions and rates for the CTMC SIR epidemic model.
Description State transition ∆ ~X(t) Rate
Birth of S (S, I, R)→ (S + 1, I, R) ΛDeath of S (S, I, R)→ (S − 1, I, R) dSInfection (S, I, R)→ (S − 1, I + 1, R) βSI/NRecovery (S, I, R)→ (S, I − 1, R + 1) γIDeath of I (S, I, R)→ (S, I − 1, R) (d+ α)IDeath of R (S, I, R)→ (S, I, R− 1) dR
To derive a stochastic threshold for disease extinction, the Markov process
summarized in Table 3.1 is approximated near the DFE. The dynamics of I are
considered when the susceptible population size S is approximately S = Λ/d and
the initial number of infectious individuals I(0) is small. Assume that S(t) = S,
R(t) = 0, and the events associated with I(t) are independent. The assumption that
the events are independent leads to a branching process [16, 38, 44, 55, 60]. An
approximation for the probability of disease extinction
P0 = limt→∞
ProbI(t) = 0,
can be obtained from the offspring probability generating function (pgf) for I.
The offspring pgf for infectious individuals is defined when the initial number of
infectious individuals is one, I(0) = 1. The probability of a successful transmission
for an infectious individual is β/(β + d+ γ + α) which leads to a total of two
infectious individuals, x2, and the probability of a death or recovery is
(d+ γ + α)/(β + d+ γ + α) which results in zero infectious individuals, x0 = 1. The
offspring pgf for I is
f(x) =βx2 + d+ γ + α
β + d+ γ + α.
For other examples of constructing offspring pgfs, see [16, 38, 44, 48, 55]. The
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
expected number of offspring per infectious individual is given by
m = f ′(1) =2β
β + d+ γ + α.
For a small initial number of infectious individuals, the branching process either hits
zero (disease extinction) or increases rapidly (disease persistence). The occurrence
of these outcomes depends on the value of m. If m ≤ 1, then
limt→∞
ProbI(t) = 0 = 1,
and if m > 1, there exists a unique fixed point q ∈ (0, 1) of the offspring pgf f ,
f(q) = q, such that
P0 = limt→∞
ProbI(t) = 0 = qi,
where i = I(0) is the initial number of infectious individuals [16, 38, 44, 55, 60]. The
three cases in which m < 1, m = 1, and m > 1 are called the subcritical, critical,
and supercritical cases, respectively.
For the SIR model, it is easy to see that R0 < 1 (R0 = 1 or R0 > 1) if and only if
m < 1 (m = 1 or m > 1). Moreover, in the supercritical case m > 1, the fixed point
of the offspring pgf is q = 1/R0. Therefore, the approximation of Whittle [73] is
valid. For I(0) = i and R0 > 1, the probability of disease persistence is given by
1− (1/R0)i.
In the next section, epidemic models with multiple infectious groups are
considered. Deterministic and stochastic thresholds for disease extinction are
calculated.
3.4 Multiple Infectious Groups
In this section, some well-known deterministic epidemic models are considered.
These models include SEIR, vector-host, treatment, and stage-structured models
[26, 70]. The corresponding CTMC models are derived and offspring pgfs are
defined for the infectious groups. The probability of disease extinction is given for
each model and numerical examples are presented for each model.
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3.4.1 SEIR Model
The classic SEIR model is similar to the SIR model with the exception that there
is an exposed or latent group E, where 1/ν is the average latent period. The model
consists of four ODEs:
S = Λ− dS − βSI
N,
E =βSI
N− νE − dE,
I = νE − (d+ γ + α)I,
R = γI − dR.
The basic reproduction number is calculated using the next-generation matrix
approach for the E and I groups [70, 71]. The next-generation matrix is
FV −1 =
βν
(ν + d)(d+ γ + α)
β
d+ γ + α
0 0
.The basic reproduction number is the spectral radius of this matrix,
R0 =βν
(ν + d)(d+ γ + α).
Since FV −1 is reducible, the type reproduction numbers cannot be defined. Thus, it
is not possible to control the disease by controlling only E or I. Both E and I must
be controlled in order to achieve disease extinction. The dynamics of the SEIR
model are well-known [53]. If R0 ≤ 1, the DFE (S, 0, 0, 0) = (Λ/d, 0, 0, 0) is globally
asymptotically stable and if R0 > 1, a unique endemic equilibrium exists and is
globally asymptotically stable [53].
For the CTMC model, let ~X(t) = (S(t), E(t), I(t), R(t)) be a discrete random
vector. The state transitions and rates for the CTMC SEIR model are given in
Table 3.2.
Offspring pgfs for the multitype branching process can be defined for the variables
E and I. Assume that S(0) = S, R(0) = 0, and the initial population size N(0) ≈ S
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Table 3.2. Transitions and rates for the CTMC SEIR epidemic model.Description State transition Rate
Birth of S (S,E, I, R)→ (S + 1, E, I, R) ΛDeath of S (S,E, I, R)→ (S − 1, E, I, R) dSInfection (S,E, I, R)→ (S − 1, E + 1, I, R) βSI/NE becomes I (S,E, I, R)→ (S,E − 1, I + 1, R) νEDeath of E (S,E, I, R)→ (S,E − 1, I, R) dERecovery (S,E, I, R)→ (S,E, I − 1, R + 1) γIDeath of I (S,E, I, R)→ (S,E, I − 1, R) (d+ α)IDeath of R (S,E, I, R)→ (S,E, I, R− 1) dR
is sufficiently large. Given E(0) = 1 and I(0) = 0, the offspring pgf for E is
f1(x1, x2) =νx2 + d
ν + d
and given E(0) = 0 and I(0) = 1, the offspring pgf for I is
f2(x1, x2) =βx1x2 + d+ γ + α
β + d+ γ + α.
The expectation matrix for this branching process is
M =
0β
β + d+ γ + αν
ν + d
β
β + d+ γ + α
.The pgfs f1 and f2 are not simple and the matrix M is irreducible. According to the
Jury conditions [3], ρ(M) < 1 iff
trace(M) < 1 + det(M) < 2. (3.4)
The second inequality in the Jury conditions (3.4) is clearly satisfied since
det(M) < 0. The first inequality is satisfied iff R0 < 1. That is,
ρ(M) < 1 iff R0 < 1. (3.5)
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
If R0 > 1, the fixed point of the offspring pgfs is calculated by setting fi(q1, q2) = qi
for i = 1, 2 and solving for qi. The unique solution (q1, q2) ∈ (0, 1)2 is
q1 =ν
ν + d
1
R0
+d
ν + d, (3.6)
q2 =1
R0
. (3.7)
The probability of disease extinction is approximately P0 = qi11 qi22 , where E(0) = i1
and I(0) = i2. In the case I(0) = 1 and E(0) = 0, the same result as Whittle [73] is
obtained for the probability of disease persistence. The probability q1 can be
interpreted epidemiologically. Given one exposed individual, that individual either
dies with probability d/(ν + d) or survives with probability ν/(ν + d) to become
infectious. Then the infectious individual successfully transmits the disease with
probability q2 = 1/R0. Note that q2 < q1. This makes sense biologically since the
disease is more likely to persist if individuals are already infectious rather than just
exposed to the disease.
A numerical example illustrates that the approximate probability of disease
extinction, P0, is in close agreement with an estimate obtained from simulation of
sample paths. Consider the parameter values Λ = 1, d = 0.005, β = 0.25, ν = 0.1,
γ = 0.05, and α = 2d = 0.01. For these values, R0 = 3.66 and ρ(M) = 1.35. The
stable endemic equilibrium for the deterministic model is
(S, E, I, R) = (48.5, 7.21, 11.1, 111).
There is a disease outbreak before the stabilization at the endemic equilibrium. The
results are given in Figure 3.1.
Using the formulas (3.6) and (3.7) for the fixed point of the offspring pgfs,
(q1, q2) = (0.3076, 0.2730). The probability of disease extinction, P0, is compared to
the estimate obtained from examining the proportion of sample paths (out of
10,000) for which the sum E(t) + I(t) hits zero (disease extinction) prior to reaching
an endemic size of 20. If the sum E(t) + I(t) is greater than 20, it is considered an
outbreak. The results are given in Table 3.3.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
0 50 100 150 2000
20
40
60
80
100
120
140
160
180
200
Time t
S, E
, I, R
SEIR
Figure 3.1. The ODE solution and one sample path of the CTMC SEIR model.Parameter values are Λ = 1, d = 0.005, β = 0.25, ν = 0.1, γ = 0.05, and α = 2d =0.01 with initial conditions S(0) = 200, E(0) = 0, I(0) = 2, and R(0) = 0. Thedisease persists with probability 1− P0 = 0.926.
3.4.2 Vector-Host Model
Consider a vector-host model where S is the number of susceptible hosts, I is the
number of infectious hosts, H = S + I is the total number of hosts, M is the
number of susceptible vectors, and V is the number of infectious vectors. Other
vector-host models have been used to model malaria and dengue fever, where
Table 3.3. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC SEIR model. Parameter valuesare Λ = 1, d = 0.005, β = 0.25, ν = 0.1, γ = 0.05, and α = 2d = 0.01 with initialconditions S(0) = 200, E(0) = e0, I(0) = i0, and R(0) = 0.
e0 i0 P0 Approx.
1 0 0.3076 0.30850 1 0.2730 0.28631 1 0.0840 0.08902 0 0.0946 0.09320 2 0.0745 0.0741
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
mosquitoes are the vector [27, 32]. A simple vector-host model has the form:
S = Λ− dS + γI − βhSV
H,
I =βhSV
H− (d+ γ)I,
M = Γ− µM − βmMI
H,
V =βmMI
H− µV.
The transmission rate from vector to host is βhSV/H and from host to vector is
βmMI/H. The parameters βh and βm are defined as βh = ab and βm = ac, where a
is the number of bites per vector per unit time, b is the per-bite vector to host
transmission probability, and c is the per-bite host to vector transmission
probability. The DFE is (S, 0, M , 0) = (Λ/d, 0,Γ/µ, 0). The basic reproduction
number is the spectral radius of the next-generation matrix,
FV −1 =
0βhµ
βmd+ γ
M
H0
.That is,
R0 =
√βhβm
µ(d+ γ)
M
H=
√βhβm
µ(d+ γ),
where βm = βmM/H. The type reproduction numbers are the square of the basic
reproduction number [61],
Ti = R20
for i = 1, 2. The same amount of control is needed for either the vector or host
population. Note that the inequalities in (3.3) are valid.
For the corresponding CTMC model, let ~X(t) = (S(t), I(t),M(t), V (t)) be a
discrete random vector. The transitions and corresponding rates for the CTMC
vector-host model are given in Table 3.4.
Assume that S(0) = S = H and M(0) = M are sufficiently large. Given I(0) = 1
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Table 3.4. State transitions and rates for the CTMC vector-host model.Description State transition Rate
Host birth (S, I,M, V )→ (S + 1, I,M, V ) ΛDeath of S (S, I,M, V )→ (S − 1, I,M, V ) dSHost infection (S, I,M, V )→ (S − 1, I + 1,M, V ) βhSV/HHost recovery (S, I,M, V )→ (S + 1, I − 1,M, V ) γIDeath of I (S, I,M, V )→ (S, I − 1,M, V ) dIVector birth (S, I,M, V )→ (S, I,M + 1, V ) ΓDeath of M (S, I,M, V )→ (S, I,M − 1, V ) µMVector infection (S, I,M, V )→ (S, I,M − 1, V + 1) βmMI/HDeath of V (S, I,M, V )→ (S, I,M, V − 1) µV
and V (0) = 0, the offspring pgf for I is
f1(x1, x2) =βmx1x2 + d+ γ
βm + d+ γ,
and given I(0) = 0 and V (0) = 1, the offspring pgf for V is
f2(x1, x2) =βhx1x2 + µ
βh + µ.
The expectation matrix for this branching process is
M =
βm
βm + d+ γ
βhβh + µ
βm
βm + d+ γ
βhβh + µ
.The offspring pgfs are not simple and the matrix M is irreducible. The spectral
radius of M is
ρ(M) =βm
βm + d+ γ+
βhβh + µ
.
It is simple to verify that ρ(M) < 1 iff R0 < 1.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
If R0 > 1, the unique fixed point (q1, q2) ∈ (0, 1)2 of the offspring pgfs is given by
q1 =(βh + µ)(d+ γ)
βh(βm + d+ γ)=
βm
βm + d+ γ
1
T1
+d+ γ
βm + d+ γ, (3.8)
q2 =µ(βm + d+ γ)
βm(βh + µ)=
βhβm + µ
1
T1
+µ
βh + µ. (3.9)
The expression for q1 can be interpreted epidemiologically. Given one infectious
host, that host can either transmit the disease to a susceptible vector with
probability βm/(βm + d+ γ) or die or recover before transmission with probability
(d+ γ)/(βm + d+ γ). If the transmission is successful, then the probability of
transmission from host to host is 1/T1. Similarly, the probability q2 has an
epidemiological meaning. Given one infectious vector, that vector can either
transmit the disease to a susceptible host with probability βh/(βh + µ) or die with
probability µ/(βh + µ). If the transmission is successful, then the probability of
transmission from an infectious vector to a susceptible vector is 1/T1.
Using the formulas for q1 and q2, if I(0) = i0 and V (0) = v0, the probability of
disease extinction is
P0 = qi01 qv02 =
(d+ γ
βh
)i0 ( µ
βm
)v0 ( βh + µ
βm + d+ γ
)i0−v0.
The same expression, except for notation, was obtained by Bartlett [21].
The probability of disease extinction, P0, is illustrated in a numerical example.
Consider the parameter values Λ = 0.5, d = 0.005, γ = 0.1, Γ = 500, µ = 0.5, and
βm = βh = 0.2. For these values, R0 = 2.76, Ti = 7.62, and ρ(M) = 1.24. The DFE
and endemic equilibrium for the ODE model are given by S = 100, M = 1000, and
(S, I , M , V ) = (17.5, 83.3, 750, 250). One sample path of the CTMC vector-host
model for which an outbreak occurs is illustrated in Figure 3.2.
Using the formulas (3.8) and (3.9) for the fixed point of the offspring pgfs,
(q1, q2) = (0.1746, 0.7518). The probability of disease extinction, P0, is compared to
the estimate obtained from examining the proportion of sample paths (out of
10,000) for which the sum I(t) + V (t) hits zero (disease extinction) prior to reaching
an endemic size of 50. The results are given in Table 3.5.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
0 50 1000
10
20
30
40
50
60
70
80
90
100
110
Time t
S, I
SI
0 50 1000
200
400
600
800
1000
1200
Time t
M, V
MV
Figure 3.2. The ODE solution and one sample path of the CTMC vector-host model.Parameter values are Λ = 0.5, d = 0.005, γ = 0.1, Γ = 500, µ = 0.5, and βm = βh =0.2 with initial conditions S(0) = 100, I(0) = 2, M(0) = 1000, and V (0) = 0. Thedisease persists with probability 1− P0 = 0.970.
3.4.3 Stage-Structured Model
Consider a stage-structured model with m stages of infection:
S = Λ− dS −m∑k=1
βkSIkN
,
I1 =m∑k=1
βkSIkN
− (ν1 + d1)I1,
Ii = νi−1Ii−1 − (νi + di)Ii, i = 2, 3, . . . ,m,
R = νmIm − dR,
Table 3.5. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC vector-host model. Parametervalues are Λ = 0.5, d = 0.005, γ = 0.1, Γ = 500, µ = 0.5, and βm = βh = 0.2 withinitial conditions S(0) = 100, I(0) = i0, M(0) = 1000, and V (0) = v0.
i0 v0 P0 Approx.
1 0 0.1746 0.17620 1 0.7518 0.75731 1 0.1312 0.13422 0 0.0305 0.03320 2 0.5652 0.5619
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
where N = S +∑m
i=1 Ii +R. Susceptible individuals are infected and then progress
through m stages of infection before recovery, νm = γ. Natural death or
disease-related death may occur in each stage of the infection, di = d+ αi. The
DFE is S = Λ/d. This model, except for notation, was considered by van den
Driessche and Watmough [70]. The basic reproduction number was calculated by
van den Driessche and Watmough [70]. The next-generation matrix is FV −1 where
F =
β1 β2 · · · βm
0 0 · · · 0...
.... . .
...
0 0 · · · 0
,
and
V −1 =
1
ν1 + d1
0 · · · 0
ν1
(ν1 + d1)(ν2 + d2)
1
ν2 + d2
· · · 0
......
. . ....
ν1ν2 · · · νm−1
(ν1 + d1)(ν2 + d2) · · · (νm + dm)
ν2 · · · νm−1
(ν2 + d2) · · · (νm + dm)· · · 1
νm + dm
.
Thus,
R0 =β1
ν1 + d1
+β2ν1
(ν1 + d1)(ν2 + d2)+ · · ·+ βmν1 · · · νm−1
(ν1 + d1) · · · (νm + dm).
For the corresponding CTMC stage-structured model, let~X(t) = (S(t), I1(t), . . . , Im(t), R(t)) be a discrete random vector. The state
transitions and rates are given in Table 3.6.
Assume that S(0) = S is sufficiently large and R(0) = 0. Given Ii(0) = 1 and
Ij(0) = 0 for j 6= i, the offspring pgf for Ii is
fi(x1, . . . , xm) =βix1xi + νixi+1 + di
βi + νi + di, i = 1, . . . ,m− 1.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Table 3.6. State transitions and rates for the CTMC stage-structured model.Description State transition Rate
Birth of S S → S + 1 ΛDeath of S S → S − 1 dS
Infection (S, I1)→ (S − 1, I1 + 1)m∑k=1
βkSIk/N
Death of Ij Ij → Ij − 1 djIjProgression (Ij, Ij+1)→ (Ij − 1, Ij+1 + 1) νjIjRecovery (Im, R)→ (Im − 1, R + 1) νmImDeath of R R→ R− 1 dR
Given Im(0) = 1 and Ij(0) = 0 for j = 1, . . . ,m− 1, the offspring pgf for Im is
fm(x1, . . . , xm) =βmx1xm + νm + dmβm + νm + dm
.
The expectation matrix for this branching process is an m×m matrix
M =
2β1
β1 + ν1 + d1
β2
β2 + ν2 + d2
· · · βmβm + νm + dm
ν1
β1 + ν1 + d1
β2
β2 + ν2 + d2
· · · 0
0ν2
β2 + ν2 + d2
· · · 0
......
. . ....
0 0 · · · βmβm + νm + dm
.
In the case of two infectious groups, m = 2, the expectation matrix is
M =
2β1
β1 + ν1 + d1
β2
β2 + ν2 + d2ν1
β1 + ν1 + d1
β2
β2 + ν2 + d2
.The 2× 2 matrix M satisfies ρ(M) < 1 iff the Jury conditions (3.4) are satisfied. It
is a tedious but straightforward calculation to derive conditions for the second
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
inequality of the Jury conditions:
det(M) < 1 iffβ1
ν1 + d1
< 1.
Moreover, conditions for the first inequality of the Jury conditions are
trace(M) < 1 + det(M) iff R0 < 1.
Thus
ρ(M) < 1 iff R0 < 1.
Unfortunately, even in the case m = 2, if R0 > 1 an analytical expression for the
fixed point (q1, q2) of the offspring pgfs cannot be obtained. The fixed point and
probability of extinction are calculated numerically.
Consider the parameter values Λ = 1, d = 0.005, β1 = 0.4, β2 = 0.1, ν1 = 0.2,
ν2 = 0.05, d1 = 0.02, and d2 = 0.01. For these values, R0 = 3.33 and ρ(M) = 1.52.
The DFE value is S = 200 and the endemic equilibrium is
(S, I1, I2, R) = (53.7, 3.33, 11.1, 111). The fixed point of the offspring pgfs is
(q1, q2) = (0.1943, 0.4268). The probability of disease extinction, P0, is compared to
the estimate obtained from examining the proportion of sample paths (out of
10,000) for which the sum I1(t) + I2(t) hits zero (disease extinction) prior to
reaching an endemic size of 20. If the sum I1(t) + I2(t) is greater than 20, it is
considered an endemic. The results are given in Table 3.7. The ODE solution and
one sample path for the CTMC stage-structured model are plotted in Figure 3.3.
The initial conditions are S(0) = S = 200, I1(0) = I2(0) = 1, and R(0) = 0.
3.4.4 Treatment Model
A model for the treatment of tuberculosis (TB) was developed by Castillo-Chavez
and Feng [26]. Tuberculosis is a bacterial infection and antibiotics are used to treat
infected individuals. When treatment methods are either inadequate or incomplete,
there is a possibility that antibiotic resistance will develop [26]. The model of
Castillo-Chavez and Feng [26] considers two strains of TB, drug-sensitive and
drug-resistant strains. For this model, there are six groups: susceptible individuals
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Table 3.7. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC staged-progression model. Pa-rameter values are Λ = 1, d = 0.005, β1 = 0.4, β2 = 0.1, ν1 = 0.2, ν2 = 0.05,d1 = 0.02, and d2 = 0.01 with initial conditions S(0) = 200, I1(0) = i1, I2(0) = i2,and R(0) = 0.
i1 i2 P0 Approx.
1 0 0.1943 0.19320 1 0.4268 0.42951 1 0.0829 0.08392 0 0.0378 0.03870 2 0.1822 0.1836
S, treated individuals T , exposed individuals E1 and E2, and infectious individuals
I1 and I2. The subscript i = 1 denotes the drug-sensitive strain of tuberculosis and
i = 2 denotes the drug-resistant strain. Susceptible individuals are exposed to either
the sensitive or resistant strain and enter the exposed or latent group E1 or E2,
respectively. After some latent period, exposed individuals become infectious. There
is disease-related death for both strains, di = d+ αi. Antibiotic treatment is not
effective for the resistant strain. Thus, exposed and infectious individuals with the
sensitive strain are treated at rates r1 and r2, respectively. The treatment of
exposed individuals may be inadequate, pr2, or incomplete which results in
antibiotic resistance, qr2. Therefore treatment is only effective in some proportion of
individuals (1− p− q). Treated individuals, T , can become infected with either
strain, but are less likely to become infected with the resistant strain than
susceptible individuals, βT ≤ β1. Except for notation, the model of Castillo-Chavez
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
0 20 40 60 80 1000
50
100
150
200
Time t
S, I 1, I
2, R
SI1I2R
Figure 3.3. The ODE solution and one sample path of the CTMC staged-progressionmodel. Parameter values are Λ = 1, d = 0.005, β1 = 0.4, β2 = 0.1, ν1 = 0.2,ν2 = 0.05, d1 = 0.02, and d2 = 0.01 with initial conditions S(0) = 200, I1(0) = 1,I2(0) = 1, and R(0) = 0. The disease persists with probability 1− P0 = 0.917.
and Feng [26] has the form:
S = Λ− dS − β1SI1
N− β2SI2
N,
E1 =β1SI1
N+βTTI1
N− β2E1I2
N− (d+ ν1 + r1)E1 + pr2I1,
I1 = ν1E1 − (d1 + r2)I1,
E2 = β2S + E1 + T
NI2 + qr2I1 − (d+ ν2)E2,
I2 = ν2E2 − d2I2,
T = −βTTI1
N− β2TI2
N+ r1E1 + (1− p− q)r2I1 − dT.
Let N = S + E1 + I1 + E2 + I2 + T denote the total population size. The DFE is
given by S = Λ/d. The failure of treatment is not considered as a new infection [70].
Let ~X(t) = (E1(t), E2(t), I1(t), I2(t))T . The system of ODEs for the latent and
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
infectious groups can be linearized about the DFE:
d ~X(t)
dt= (F − V ) ~X(t),
where
F =
0 0 β1 0
0 0 0 β2
0 0 0 0
0 0 0 0
and V =
d+ ν1 + r1 0 −pr2 0
0 d+ ν2 −qr2 0
−ν1 0 d1 + r2 0
0 −ν2 0 d2
.
The next-generation matrix is
FV −1 =
β1ν1
(d+ ν1 + r1)(d1 + r2)− ν1pr2
0 ∗ 0
β2ν1ν2qr2
d2(d+ ν2)[(d+ ν1 + r1)(d1 + r2)− ν1pr2]
β2ν2
d2(d+ ν2)∗ ∗
0 0 0 0
0 0 0 0
,
where “*” denotes a nonzero entry but does not affect the value ρ(FV −1). Thus,
R0 = max
β1ν1
(d+ ν1 + r1)(d1 + r2)− ν1pr2
,β2ν2
d2(d+ ν2)
= maxR1,R2.
The threshold R1 was derived by van den Driessche and Watmough [70]. For a more
in-depth analysis of this model, see [26].
For the corresponding CTMC treatment model, let
~X(t) = (S(t), E1(t), E2(t), I1(t), I2(t), T (t))
be a discrete random vector. The state transitions and rates for the CTMC
stage-structured model are given in Table 3.8.
Assume that S(0) = S is sufficiently large and T (0) = 0. Given E1(0) = 1 and
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Table 3.8. State transitions and rates for the CTMC treatment model.Description State transition Rate
Birth of S S → S + 1 ΛDeath of S S → S − 1 dSDrug-sensitive infection (S,E1)→ (S − 1, E1 + 1) β1SI1/NDrug-resistant infection (S,E2)→ (S − 1, E2 − 1) β2SI2/NResistant to infection of E1 (E1, E2)→ (E1 − 1, E2 + 1)Latent to infectious (E1, I1)→ (E1 − 1, I1 + 1) ν1E1
Treatment of E1 (E1, T )→ (E1 − 1, T + 1) r1E1
Death of E1 E1 → E1 − 1 dE1
Death of I1 I1 → I1 − 1 d1I1
Effective treatment of I1 (I1, T )→ (I1 − 1, T + 1) (1− p− q)r2I1
Inadequate treatment of I1 (E1, I1)→ (E1 + 1, I1 − 1) pr2I1
Treatment resistance I1 (I1, E2)→ (I1 − 1, E2 + 1) qr2I1
Drug-sensitive infection of T (E1, T )→ (E1 + 1, T − 1) βTTI1/NDrug-resistant infection of T (E2, T )→ (E2 + 1, T − 1) βTTI2/NDeath of T T → T − 1 dTDeath of E2 E2 → E2 − 1 dE2
Latent to infectious (E2, I2)→ (E2 − 1, I2 + 1) ν2E2
Death of I2 I2 → I2 − 1 d2I2
I1(0) = E2(0) = I2(0) = 0, the offspring pgf for E1 is
f1(x1, x2, x3, x4) =ν1x2 + d+ r1
ν1 + d+ r1
.
Similarly, the offspring pgfs for I1, E2, and I2 are
f2(x1, x2, x3, x4) =β1x1x2 + pr2x1 + qr2x3 + d1 + (1− p− q)r2
β1 + d1 + r2
,
f3(x1, x2, x3, x4) =ν2x4 + d
ν2 + d,
f4(x1, x2, x3, x4) =β2x3x4 + d2
β2 + d2
.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Note that the offspring pgfs are not simple. The expectation matrix is
M =
0β1 + pr2
β1 + d1 + r2
0 0
ν1
ν1 + d+ r1
β1
β1 + d1 + r2
0 0
0qr2
β1 + d1 + r2
0β2
β2 + d2
0 0ν2
d+ ν2
β2
β2 + d2
=
[M1 0
∗ M2
],
where M1 and M2 are the 2× 2 matrices in the upper left and lower right corners of
M. Apply the Jury conditions (3.4) to each of the submatrices M1 and M2. Clearly,
trace(Mi) > 0 and det(Mi) < 1 for i = 1, 2. Now
1 + det(M1)− trace(M1) = 1− ν1(β1 + pr2)
(ν1 + d+ r1)(β1 + d1 + r2)− β1
β1 + d1 + r2
=(d1 + r2)(ν1 + d+ r1)− ν1(β1 + pr2)
(ν1 + d+ r1)(β1 + d1 + r2).
Thus, trace(M1) < 1 + det(M1) if and only if
ν1(β1 + pr2)
(d1 + r2)(ν1 + d+ r1)< 1.
This inequality holds iff R1 < 1. Similarly, trace(M2) < 1 + det(M2) iff R2 < 1. By
the Jury conditions, ρ(Mi) < 1 iff Ri < 1. It follows that ρ(M) > 1 iff R0 > 1.
Since the matrix M is reducible, there is not necessarily a unique fixed point
(q1, q2, q3, q4) ∈ (0, 1)4 of the offspring pgfs for R0 > 1 (ρ(M) > 1). In fact, there are
four fixed points of the offspring pgfs lying in (0, 1]4 One of the fixed points is
(q1, q2, q3, q4) = (1, 1, 1, 1) which always exists. The existence of the remaining three
fixed points depends on the values R1 and R2. If R1 > 1, the first fixed point is
q1 =ν1
ν1 + d+ r1
1
R1
+d+ r1
ν1 + d+ r1
,
q2 =1
R1
,
q3 = 1,
q4 = 1.
(3.10)
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
If R2 > 1, there are two more fixed points in (0, 1]4. The second fixed point is
q1 = 1,
q2 = 1,
q3 =ν2
d+ ν2
1
R2
+d
d+ ν2
,
q4 =1
R2
.
(3.11)
The third fixed point is
q1 =ν1q2
ν1 + d+ r1
+d+ r1
ν1 + d+ r1
,
q3 =ν2
d+ ν2
1
R2
+d
d+ ν2
,
q4 =1
R2
,
(3.12)
and q2 is the unique solution in (0, 1) of the quadratic equation Ax2 +Bx+ C = 0
where
A =β1ν1
(β1 + d1 + r2)(ν1 + d+ r1),
B = −β1ν1 + (d1 + r2)(ν1 + d+ r1)− pr2ν1
(β1 + d1 + r2)(ν1 + d+ r1),
C(q3) =pr2(d+ r1) + [qr2q3 + d1 + (1− p− q)r2][ν1 + d+ r1]
(β1 + d1 + r2)(ν1 + d+ r1).
Numerical examples will illustrate which of the three fixed points is used to
determine the probability of disease extinction. Fix the parameter values Λ = 1,
d = 0.005, βT = 0.25β2, r1 = r2 = 0.05, p = 0.5, q = 0.1, ν1 = 0.5, ν2 = 0.1, and
d1 = d2 = 1.5d. Only the transmission rates β1 and β2 will be varied. In each
example, the probability of disease extinction P0 is calculated and compared with
the numerical approximation based on the proportion of sample paths (out of
10,000) for which the infected population E1(t) + I1(t) + E2(t) + I2(t) hits zero
before reaching a size of 20. If the infected population exceeds 20, it is considered
an endemic. In each of the examples, assume S(0) = S and T (0) = 0.
For the first example, let β1 = 0.1 and β2 = 0.005. Then R1 = 2.58 and
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
R2 = 0.635. For the deterministic model, there exists a stable endemic equilibrium
(S, E1, I1, E2, I2, T ) = (69.8, 1.83, 15.9, 1.53, 20.3, 72.4). The fixed point (3.10),
(q1, q2, q3, q4) = (0.4489, 0.3883, 1, 1) is used to calculate the probability of
extinction. For a small initial number of individuals infected with the drug sensitive
strain, E1(0) and I1(0), the probability of extinction and the numerical
approximation for the branching process are calculated. The results are given in
Table 3.9. The extinction probability does not depend on the drug-resistant strain
for small initial values. Moreover, if only the drug resistant strain is present,
E1(0) = 0 and I1(0) = 0, the probability of extinction is one.
Table 3.9. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC treatment model. Parametervalues are Λ = 1, d = 0.005, β1 = 0.1, β2 = 0.005, βT = 0.25β2, r1 = r2 = 0.05,p = 0.5, q = 0.1, ν1 = 0.5, ν2 = 0.1, and d1 = d2 = 1.5d with initial conditionsS(0) = S = 200, T (0) = 0, E2(0) = 0, I2(0) = 0, E1(0) = e1, and I1(0) = i1.
e1 i1 P0 Approx.
1 0 0.4489 0.44580 1 0.3883 0.39611 1 0.1743 0.18172 0 0.2015 0.21140 2 0.1507 0.1554
For the second example, let β1 = 0.1 and β2 = 0.04. Then R1 = 2.58 and
R2 = 5.08. For the deterministic model, there exists a stable endemic equilibrium
(S, E1, I1, E2, I2, T ) = (28.7, 0, 0, 8.16, 109, 0). The fixed points
(q1, q2, q3, q4) = (0.4489, 0.3883, 1, 1),
(q1, q2, q3, q4) = (0.3922, 0.3253, 0.2351, 0.1969),
are used to calculate the probability of extinction. The proportion of sample paths
for which the total number of infectives hits zero, (Approx.a), is calculated and
compared to the probability of extinction calculated from the fixed point (3.12), Pa0.
In addition, the proportion of sample paths for which the drug sensitive strain hits
zero (Approx.b = E1(t) + I1(t) = 0) is compared to the probability of extinction
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
calculated from the point (3.11), Pb0. The results for several initial conditions are
summarized in Table 3.10. The ODE solution and one sample path of the CTMC
treatment model are plotted in Figure 3.4.
Table 3.10. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC treatment model. Parametervalues are Λ = 1, d = 0.005, β1 = 0.1, β2 = 0.04, βT = 0.25β2, r1 = r2 = 0.05,p = 0.5, q = 0.1, ν1 = 0.5, ν2 = 0.1, and d1 = d2 = 1.5d with initial conditionsS(0) = S = 200, T (0) = 0, E1(0) = e1, I1(0) = i1, E2(0) = e2, and I2(0) = i2.Probability Pa0 is calculated from fixed point (3.12) and probability Pb0 is calculatedfrom fixed point (3.11).
e1 i1 e2 i2 Pa0 Approx.a Pb0 Approx.b
1 0 0 0 0.3922 0.3893 0.4489 0.44710 1 0 0 0.3253 0.3233 0.3883 0.38801 1 0 0 0.1178 0.1270 0.1743 0.17900 0 1 0 0.2351 0.2336 1 10 0 0 1 0.1969 0.1956 1 10 0 1 1 0.0463 0.0472 1 11 0 1 0 0.0852 0.0934 0.4489 0.44760 1 0 1 0.0640 0.0688 0.3383 0.3953
For the third example, let β1 = 0.02 and β2 = 0.04. Then R1 = 0.515 and
R2 = 5.08. For the deterministic model, there exists a stable endemic equilibrium
(S, E1, I1, E2, I2, T ) = (69.8, 1.83, 15.9, 1.53, 20.3, 72.4). The fixed point (3.12),
(q1, q2, q3, q4) = (0.8307, 0.8120, 0.2351, 0.1969) is used to calculate the probability of
extinction. The results are given in Table 3.11.
3.5 Discussion
Deterministic thresholds such as the basic reproduction number or type
reproduction numbers are important in mathematical epidemiology. These
thresholds provide information about the persistence or extinction of an infectious
disease, the amount of control needed to eradicate a particular disease, and which
parameters should be adjusted in order to control the spread of disease. The
deterministic thresholds are well-known [29, 39, 61, 70, 71]. However, much less is
known about stochastic thresholds with the exception of the approximation (3.1) of
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
0 200 4000
20
40
60
80
100
120
140
160
180
200
Time t
S, E
1, I1
0 200 4000
50
100
150
Time tT,
E2, I
2
SE1I1
TE2I2
Figure 3.4. The ODE solution and one sample path of the CTMC treatment model.Parameter values are Λ = 1, d = 0.005, β1 = 0.1, β2 = 0.04, βT = 0.25β2, r1 = r2 =0.05, p = 0.5, q = 0.1, ν1 = 0.5, ν2 = 0.1, and d1 = d2 = 1.5d ν1 = 0.2, ν2 = 0.05,d1 = 0.02, and d2 = 0.01. The reproduction numbers are R1 = 2.58 and R2 = 5.08.The disease persists with probability 1− P0 = 0.936.
Table 3.11. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC treatment model. Parametervalues are Λ = 1, d = 0.005, β1 = 0.02, β2 = 0.04, βT = 0.25β2, r1 = r2 = 0.05,p = 0.5, q = 0.1, ν1 = 0.5, ν2 = 0.1, and d1 = d2 = 1.5d with initial conditionsS(0) = S = 200, T (0) = 0, E1(0) = e1, I1(0) = i1, E2(0) = e2, and I2(0) = i2.
e1 i1 e2 i2 P0 Approx.
1 0 0 0 0.8307 0.83560 1 0 0 0.8120 0.81151 1 0 0 0.6745 0.67700 0 1 0 0.2351 0.23830 0 0 1 0.1969 0.19250 0 1 1 0.0463 0.04701 0 1 0 0.1953 0.19240 1 0 1 0.1599 0.1670
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Whittle [73]. If a small initial number of infectious individuals are introduced into a
large susceptible population, then an estimate for the probability of disease
persistence or extinction can be obtained from multitype branching processes
approximations.
New expressions for the probability of extinction were derived for several
well-known models. For each of the models discussed, the estimate for the
probability of disease extinction, P0, was shown to be in strong agreement with the
numerical approximation based on computing sample paths. Furthermore, new
relationships between the deterministic and stochastic thresholds were derived.
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CHAPTER 4
STOCHASTIC MULTI-PATCH EPIDEMIC MODELS
4.1 Introduction
Infectious diseases in humans or domestic and wild animals such as influenza,
tuberculosis, SARS, and foot-and-mouth disease can be easily transmitted from
region to region. Factors such as spatial connectivity and the dispersal of
individuals through travel can significantly affect the likelihood that a disease will
persist in a given region. For instance, a disease may not be prevalent in rural areas,
but if individuals from an urban center travel to these more remote regions, there
may be outbreaks in remote areas. Alternatively, the reverse may be the case where
the disease is present in rural areas and is spread to urban areas [68]. Similarly, the
spread of disease can occur at an accelerated rate in social or environmental
‘hotspots’ such as airports, schools, or common water sources [15, 22, 47]. Thus, it
is important to account for factors such as dispersal and environmental
heterogeneity in epidemic models.
The role of dispersal on disease dynamics has been examined for general epidemic
models [5, 12, 13, 14, 24, 41, 72] and models focused on particular diseases such as
tuberculosis [25], malaria [33], and influenza [66, 42]. Many of these models involve
dividing a region into multiple patches and allowing dispersal of susceptible or
infectious individuals between these patches [5, 41, 42, 67, 72]. Allen, Kirupaharan,
and Wilson [7] considered a discrete-time two-patch SIS epidemic model. One patch
was considered high-risk, having a patch reproduction number greater than one, and
the other patch was low-risk with a patch reproduction number less than one. In
the absence of movement, the disease persisted only in the high-risk patch. When
the dispersal of susceptible and infectious individuals was allowed between the two
patches, an endemic equilibrium was reached in both patches. Furthermore, when
only infectious individuals were allowed to move between the two patches the
disease did not persist in either patch; all susceptible individuals eventually moved
into the low-risk patch and the high-risk patch became empty. Similar results were
obtained by Allen et al. [5].
The role of movement also has important implications for disease control. For
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
instance, it may be possible to stop the spread of a disease by conducting border
checks and restricting the movement of infectious individuals or restricting the
movement to and from high-risk patches where a disease is more prevalent [14]. In
the case of influenza, van den Driessche et al. [42] showed that restricting the
dispersal of infectious individuals from low to high-risk patches helps control the
disease. However, for certain parameter values, restricting the dispersal of infectious
individuals from high to low-risk patches could have negative effects on disease
control [42]. Moreover, banning all travel of infectious individuals from high to
low-risk patches could result in the low-risk patch becoming disease-free, while the
high-risk patch becomes even more disease-prevalent [42]. Similarly, Ruan, Wang,
and Levin [65] showed that the spread of SARS can be contained by implementing
border screening for infectious individuals. On the other hand, screening at the
borders is only effective in identifying individuals exhibiting symptoms. Gao and
Ruan [33] state that the dispersal of exposed or latent individuals can contribute to
the spread of disease and that ineffective border screening may adversely affect
disease transmission.
Our goals are to develop stochastic multi-patch epidemic models that are
analytically tractable and to use these models to examine how dispersal between
patches and the location of an outbreak affect the probability of disease persistence
or extinction. These results have important implications for disease control. In the
next two sections, models with multiple patches with and without demographics are
studied.
4.2 Multi-Patch SIS, SIR, and SIRS Models without Demographics
In this section multi-patch SIS, SIR, and SIRS models will be considered. In
Section 4.2.1, deterministic (ODE) multi-patch models are introduced and the
dynamics in each patch are discussed when there is no movement between patches.
Then the dynamics of the models are explored when there is movement between the
patches. Next, stochastic versions of these multi-patch models are introduced. In
Section 4.2.2, CTMC models are considered and some results from continuous-time
multitype branching process theory are used to derive an expression for the
approximate probability of disease extinction. In Section 4.2.3, SDE patch models
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are derived from the corresponding ODE models. Finally, in Section 4.2.4, the
differences between the deterministic and stochastic patch models are explored
numerically.
4.2.1 Deterministic Models
Consider a multi-patch SIS model, where n ≥ 2 is the number of patches,
Ω = 1, 2, . . . , n, and Sj(t) and Ij(t) denote the number of susceptible and
infectious individuals in patch j at time t ≥ 0, respectively. For ease of notation, let
Sj = Sj(t) and Ij = Ij(t). Denote the total population in patch j by Nj = Sj + Ij.
The model takes the form
Sj = −βjSjIjNj
+ γjIj +∑k∈Ω
(dskjSk − dsjkSj), (4.1)
Ij =βjSjIjNj
− (γj + αj)Ij +∑k∈Ω
(dikjIk − dijkIj), (4.2)
where Sj(0) > 0 and Ij(0) ≥ 0 for all j ∈ Ω. The parameters dskj ≥ 0 and dikj ≥ 0
represent the degree of movement from patch k to patch j by susceptible and
infectious individuals, respectively. The parameters βj > 0, γj ≥ 0, and αj ≥ 0
represent the rate of infection, the recovery rate, and the disease-related death rate
in patch j, respectively. This model is similar to the multi-patch SIS model of Allen,
Bolker, Lou, and Nevai [5] with the exception that there are disease-related deaths.
Summing the equations for Sj and Ij in (4.1)-(4.2), it follows that for each j ∈ Ω
Nj = −αjIj +∑k∈Ω
(dskjSk − dsjkSj + dikjIk − dijkIj). (4.3)
Let N denote the total population size in all patches,
N =∑j∈Ω
Nj. (4.4)
It follows from equation (4.3) that
N = −∑j∈Ω
αjIj. (4.5)
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Note that if there are no disease-related deaths, αj = 0 for each j ∈ Ω, then
N = N(0) is a constant.
It will be useful to introduce some notation regarding the dispersal parameters
dskj and dikj. Define the connectivity matrices as
Ds = [dskj] and Di = [dikj]. (4.6)
In the case of two patches,
Ds =
[ds11 ds21
ds12 ds22
]and Di =
[di11 di21
di12 di22
].
For each patch j ∈ Ω, define the patch reproduction number as
R0j =βj
γj + αj. (4.7)
If γj = αj = 0, then let R0j =∞. If R0j > 1, then patch j is said to be a high-risk
patch. Otherwise, it is called a low-risk patch [5].
The following theorem summarizes the dynamics in each patch when there is no
movement.
Theorem 4.1. If Ds = Di = O (zero matrices), the asymptotic solution for patch j
in the multi-patch SIS epidemic model depends on R0j.
(i) If R0j > 1, then
limt→∞
(Sj(t), Ij(t)) =
(Nj(0)
R0j,(
1− 1R0j
)Nj(0)
), αj = 0
(0, 0), αj > 0.
(ii) If R0j ≤ 1, then
limt→∞
(Sj(t), Ij(t)) =
(Nj(0), 0), αj = 0
(Cj, 0), αj > 0,
for some Cj where 0 ≤ Cj < Nj(0).
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Proof. For fixed j ∈ Ω, let ij = Ij/Nj. For simplicity, we omit the subscript j and
write i = I/N and R0 = β/(γ + α). Then
i = i[β − γ − α− (β − α)i], (4.8)
and
N = −αiN. (4.9)
The differential equation (4.8) can be expressed as
i = i(a− bi), (4.10)
where a = β − γ − α and b = β − α.
If R0 > 1 and α = 0, then N = N(0) is a constant and a, b > 0. It follows that
limt→∞
i(t) = 1− 1
R0
.
Since N is a constant, the result in part (i) follows.
If R0 > 1 and α > 0, then a, b > 0. It follows that
limt→∞
i(t) = 1− γ
β − α> 0.
Thus, i(t) is bounded below by a positive constant for sufficiently large t. It follows
from (4.9) that
limt→∞
N(t) = 0.
Thus, I(t)→ 0 and S(t)→ 0 as t→∞.
If R0 ≤ 1 and α = 0, then N = N(0) is a constant and a ≤ 0. It follows that
limt→∞
i(t) = 0.
Then part (ii) follows.
If R0 ≤ 1 and α > 0, it follows from (4.8) that
limt→∞
i(t) = 0.
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So I(t)→ 0 as t→∞. Since N(t) is decreasing, S(t)→ C for some
0 ≤ C < N(0).
Next, we define a basic reproduction number for the patch model (4.1)-(4.2). Let
F = diag[βj], (4.11)
V = diag
[γj + αj +
∑k∈Ω
dijk
]−Di, (4.12)
where Di is the dispersal matrix for infectives. The eigenvalues of F − V have
negative real part if and only if the spectral radius of FV −1 is less than one [70].
The basic reproduction number is the spectral radius of FV −1 [70],
R0 = ρ(FV −1). (4.13)
The next theorem states that if R0 < 1, the infection dies out. A result similar to
Allen et al. [5] will be applied.
Theorem 4.2. If R0 < 1, then the multi-patch SIS epidemic model (4.1)-(4.2)
satisfies I(t)→ 0 as t→∞.
Proof. Suppose R0 < 1. For each fixed j ∈ Ω,
Ij ≤
(βj − γj − αj −
∑k∈Ω
dijk
)Ij +
∑k∈Ω
dikjIk.
That is,
I ≤ (F − V )I,
where F and V are defined by (4.11) and (4.12) and I = (I1, . . . , In)T . Consider the
initial-value problem
X = (F − V )X,
X(0) = I(0).
Then X(t) = I(0)e(F−V )t. Since R0 < 1, the eigenvalues of F − V have negative real
part and since F − V has nonnegative off-diagonal elements, the solution X(t) can
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be compared with the solution I(t) [51]. By the comparison principle, since
X(t)→ 0 as t→∞, I(t)→ 0 as t→∞ [51].
Corollary 4.1. For fixed j ∈ Ω, if R0j < 1 and dijk = dikj = 0 for k 6= j, then in
model (4.1)-(4.2), Ij(t)→ 0 as t→∞ .
Proof. Fix j ∈ Ω and suppose R0j < 1. Then
Ij ≤ (βj − γj − αj)Ij < 0.
It follows that Ij is a strictly decreasing function which is bounded below by zero
and so the conclusion follows.
Consider a multi-patch SIR or SIRS model, where n ≥ 2 is the number of patches
and Ω = 1, 2, . . . , n. As before, Sj(t), Ij(t), Rj(t) denote the number of
susceptible, infectious, and recovered individuals in patch j at time t ≥ 0,
respectively. For simplicity, let Sj = Sj(t), Ij = Ij(t), and Rj = Rj(t). Let
Nj = Sj + Ij +Rj denote the total population size in patch j. The model takes the
form
Sj = −βjSjIjNj
+ νjRj +∑k∈Ω
(dskjSk − dsjkSj), (4.14)
Ij =βjSjIjNj
− (γj + αj)Ij +∑k∈Ω
(dikjIk − dijkIj), (4.15)
Rj = γjIj − νjRj +∑k∈Ω
(drkjRk − drjkRj), (4.16)
where Sj(0) > 0, Ij(0) ≥ 0, and Rj(0) = 0 for each j ∈ Ω. The notation used here is
the same as for the multi-patch SIS model (4.1)-(4.2). Here, drkj ≥ 0 represents the
degree of movement from patch k to patch j by recovered individuals and νj ≥ 0 is
the rate of loss of immunity for recovered individuals in patch j. It is assumed that
γj > 0 for each j ∈ Ω. The patch reproduction numbers remain the same as for the
SIS model,
R0j =βj
γj + αj.
In addition, Theorem 4.2 and Corollary 4.1 apply, which is stated here as a corollary.
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Corollary 4.2. (i) If R0 < 1, then in model (4.14)-(4.16), I(t)→ 0 as t→∞.
(ii) For fixed j ∈ Ω, if R0j < 1 and dijk = dikj for k 6= j, then in model
(4.14)-(4.16), Ij(t)→ 0 as t→∞.
The following theorem summarizes the dynamics of the SIR and SIRS models in
each patch when there is no movement. The connectivity matrix Dr = [drkj] is
defined as in (4.6).
Theorem 4.3. If Ds = Di = Dr = O (zero matrices), the asymptotic solution for
patch j in the SIR/SIRS epidemic model depends on R0j.
(i) If R0j > 1, then
limt→∞
(Sj(t), Ij(t), Rj(t)) =
(Sj, Ij, Rj), γj > 0, νj > 0, αj = 0
(Aj, 0, Cj), γj > 0, νj = 0, αj = 0
(0, 0, 0), γj > 0, νj > 0, αj > 0
(Bj, 0, Ej), γj > 0, νj = 0, αj > 0
where Sj = N(0)/R0, Ij = N(0)ν(R0 − 1)/R0(γ + ν),
Rj = N(0)γ(R0 − 1)/R0(γ + ν), Aj, Bj, Cj, Ej > 0, Aj + Cj = Nj(0), and
Bj + Ej < Nj(0).
(ii) If R0j ≤ 1, then
limt→∞
(Sj(t), Ij(t), Rj(t)) =
(Nj(0), 0, 0), γj > 0, νj > 0, αj = 0
(Aj, 0, Cj), γj > 0, νj = 0, αj = 0
(Bj, 0, 0), γj > 0, νj > 0, αj > 0
(Bj, 0, Ej), γj > 0, νj = 0, αj > 0
where 0 ≤ Aj, Bj < Nj(0), 0 < Cj ≤ Nj(0), 0 < Ej < Nj(0), Aj + Cj = Nj(0),
and Bj + Ej < Nj(0).
Proof. For fixed j ∈ Ω, let sj = Sj/Nj, ij = Ij/Nj, and rj = Rj/Nj. For simplicity,
omit the subscript j and write s = S/N , i = I/N , r = R/N , and R0 = β/(γ + α).
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Then s+ i+ r = 1 and r = 1− s− i. So the dynamics depend on s and i. Now
N = −αiN, (4.17)
and
s = (α− β)si+ ν(1− s− i),
i = i(βs− γ − α + αi).
Consider the SIRS model with ν > 0. Allen et al. [6] showed that the system of
differential equations for s and i has a unique globally stable positive equilibrium
(s, i) with s+ i < 1 iff β > γ + α. When β > γ + α, the equilibrium (1, 0) is a saddle
point with stable manifold on the s-axis. Also, when β ≤ γ + α, (1, 0) is globally
stable. The origin is a saddle with stable manifold the i-axis and unstable manifold
the s-axis. The preceeding result shows that for α = 0 when the population size is
constant, either the population approaches a DFE (R0 ≤ 1) or an endemic
equilibrium (R0 > 1). In the case α > 0, the population size is decreasing and either
the population becomes disease-free (R0 ≤ 1) with a reduced population size or
reaches extinction (R0 > 1). Now consider the SIR model with ν = 0. In this case,
all equilibria lie on the s-axis (i = 0). Hence, in either case R0 > 1 or R0 ≤ 1,
i(t)→ 0 which implies I(t)→ 0.
4.2.2 Markov Chain Models
Consider a corresponding CTMC multi-patch SIS, SIR, or SIRS model. Let
~X(t) = (S1(t), I1(t), . . . , Sn(t), In(t))T ,
~X(t) = (S1(t), I1(t), R1(t), . . . , Sn(t), In(t), Rn(t))T
be discrete random vectors for the corresponding CTMC SIS and SIR/SIRS models,
respectively. For simplicity, the same notation is used for the random variables and
the deterministic variables. The state transitions and rates for the CTMC SIS and
SIR/SIRS models are given in Tables 4.1 and 4.2.
As in Section 3.2, under certain restrictions, offspring pgfs for the multitype
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Table 4.1. State transitions and rates for the CTMC multi-patch SIS epidemic model.Description State transition Rate
Infection in patch j (0, . . . , Sj − 1, Ij + 1, . . . , 0) βjSjIj/Nj
Recovery in patch j (0, . . . , Sj + 1, Ij − 1, . . . , 0) γjIjDeath of Ij (0, . . . , Ij − 1, . . . , 0) αjIjSusceptible dispersal from j to k (0, . . . , Sj − 1, . . . , Sk + 1, . . . , 0) dsjkSjInfectious dispersal from j to k (0, . . . , Ij − 1, . . . , Ik + 1, . . . , 0) dijkIj
Table 4.2. State transitions and rates for the CTMC multi-patch SIR/SIRS epidemicmodel.
Description State transition Rate
Infection in patch j (0, . . . , Sj − 1, Ij + 1, . . . , 0) βjSjIj/Nj
Recovery in patch j (0, . . . , Ij − 1, Rj + 1, . . . , 0) γjIjDeath of Ij (0, . . . , Ij − 1, . . . , 0) αjIjLoss of immunity in patch j (0, . . . , Sj + 1, Ij, Rj − 1, . . . , 0) νjRj
Susceptible dispersal from j to k (0, . . . , Sj − 1, . . . , Sk + 1, . . . , 0) dsjkSjInfectious dispersal from j to k (0, . . . , Ij − 1, . . . , Ik + 1, . . . , 0) dijkIjRecovered dispersal from j to k (0, . . . , Rj − 1, . . . , Rk + 1, 0, . . . , 0) drjkRj
branching processes can be defined for each random variable Ij, j ∈ Ω. Assume that
individuals of type j, Ij, give ‘birth’ to individuals of type k, Ik, and that the
number of offspring produced by a type j individual does not depend on the number
of offspring produced by other individuals of type j or k 6= j. Moreover, assume
that the initial population in each patch is sufficiently large, Sj(0) ≈ Nj(0). Then
continuous-time multitype branching process theory can be used to approximate the
probability of extinction.
As in Chapter 3, the method of Allen and Lahodny [8] is applied. Let
Sj(0) ≈ Nj(0), Ij(0) = 1 and Ik(0) = 0 for all k 6= j. The offspring pgf for Ij is
fj(x1, . . . , xn) =
βjx2j + γj + αj +
∑k∈Ω\j
dijkxk
βj + γj + αj +∑
k∈Ω\j
dijk. (4.18)
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The term βj/(βj + γj + αj +∑
j∈Ω\j dijk) represents the probability that a
susceptible individual becomes infectious which results in two type j infectious
individuals, x2j . The term (γj + αj)/(βj + γj + αj +
∑j∈Ω\j d
ijk) represents the
probability that an infectious individual is lost due to recovery or death resulting in
zero infectious individuals, x0j . The term dijk/(βj + γj +αj +
∑j∈Ω\j d
ijk) represents
the probability of movement from patch j to k resulting in one type k infectious
individual and zero type j infectious individuals, xkx0j . The offspring pgfs for Ij are
the same for the SIS, SIR, and SIRS models.
The expectation matrix M = [mkj] is a nonnegative n× n matrix such that
mkj =
2βj
βj + γj + αj +∑
k∈Ω\j
dijk, k = j
dijk
βj + γj + αj +∑
k∈Ω\j
dijk, k 6= j.
(4.19)
Explicitly, the expectation matrix has the form:
M =
2β1
A1
di21
A2
· · · din1
Andi12
A1
2β2
A2
· · · din2
An...
.... . .
...
di1nA1
di2nA2
· · · 2β2
An
,
where Aj = βj + γj + αj +∑
k∈Ω\j dijk for j = 1, . . . , n. Note that if dijk > 0, then
M is irreducible.
Applying branching process theory and properties of M -matrix theory, it can be
shown that the spectral radius of the expectation matrix M determines whether the
probability of extinction is less than or equal to one [4, 9]. Let
D = diag
βj + γj + αj +∑
k∈Ω\j
dijk
, (4.20)
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an n× n diagonal matrix. It follows that
[M− I]D = F − V (4.21)
where I is the n× n identity matrix and F and V are defined as in (4.11) and
(4.12), respectively. Applying the theory of branching processes [16, 30, 38, 45, 60],
it follows that the continuous-time multitype branching process is subcritical,
critical, or supercritical if the spectral abscissa (the real part of the largest
eigenvalue) of F − V is less than, equal to, or greater than zero. This is equivalent
to R0 < 1 (= 1, > 1) which is in turn equivalent to ρ(M) < 1 (= 1, > 1) [9].
For fixed j ∈ Ω, assume that Nj(0) is sufficiently large, aj ∈ N is sufficiently
small, R0 > 1 (ρ(M) > 1), and M is irreducible. If in the ODE model there is a
significant increase in the number of infectives (an outbreak), then given
Sj(0) ≈ Nj(0) and Ij(0) = aj the probability of an outbreak is approximately
1− qa11 · · · qann ,
where qi = fi(q1, . . . , qn) and qi ∈ (0, 1).
Unfortunately, the size of Nj(0) and aj may depend on the particular parameter
values and obtaining analytical expressions for qi is not possible in most cases. For a
single isolated patch j ∈ Ω with Di = O, M = [mjj] = diag[2βj/(βj + γj + αj)]. It is
easy to verify that mjj > 1 if and only if R0j > 1 and that
qj = 1/R0j = (γj + αj)/βj. The latter result is due to Whittle [73]. To check the
general result about probability of extinction, we compute the proportion out of
10,000 sample paths where the infective population “hits” zero and compare it with
the estimate P0 calculated from the fixed point of the pgfs.
4.2.3 Stochastic Differential Equation Models
In this section, we derive Ito stochastic differential equation (SDE) multi-patch
SIS, SIR, and SIRS models corresponding to the deterministic models. It is first
necessary to define a Wiener process and Ito stochastic integration.
A Wiener process is a continuous stochastic process, W (t)|t ≥ 0, such that
1. W (0) = 0,
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2. For 0 ≤ t1 ≤ t2 <∞, W (t2)−W (t1) ∼ N(0, t2 − t1),
3. For 0 ≤ t0 ≤ t1 ≤ t2 <∞, the increments W (t1)−W (t0) and W (t2)−W (t1)
are independent [1, 58].
Wiener processes are needed to define the Ito stochastic integral of a random
function. Let f(t,X(t)) be a random function on [a, b]× X(t)|t ≥ 0 such that∫ b
a
E(f 2(t))dt <∞
[1, 58]. If a = t0 < t1 < · · · < tm = b is a partition of [a, b], ∆t = (b− a)/m, and
∆W (ti) = W (ti+1)−W (ti), then the Ito stochastic integral of f is defined as
∫ b
a
f(t)dW (t) = limm→∞
m−1∑i=0
f(ti)∆W (ti),
where the convergence is in the mean square sense [1, 58]. It is now possible to
define an Ito SDE.
An Ito SDE on the interval [0, T ] has the form
dX(t) = f(t,X(t))dt+ g(t,X(t))dW (t), (4.22)
where W (t) is a Wiener process. The functions f and g are called the drift and
diffusion coefficients, respectively [1, 58]. The notation dW (t) in equation (4.22) is
slightly abusive since Wiener processes are nowhere differentiable. Equation (4.22)
is used for notational convenience for the solution X(t) of
X(t) = X(0) +
∫ t
0
f(s,X(s))ds+
∫ t
0
g(s,X(s))dW (s), (4.23)
where t ∈ [0, T ] [1, 58]. The first integral is a Riemann integral and the second
integral is an Ito stochastic integral [1, 58]. The notation X(t) is also for
convenience since X(t) denotes a sample path X(t) = X(t, ω), where ω is an
element of the sample space of X. For more information on the theory and
applications of SDEs, see [1, 4, 58].
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Next, a procedure will be applied to construct an equivalent Ito SDE model from
a given deterministic model. This procedure, illustrated in [1, 2, 4], is often referred
to as the diffusion approximation method by Kurtz [50] or the chemical Langevin
equation by Gillespie [34]. Given the transitions and rates in Tables 4.1 and 4.2, the
corresponding SDE model has the form
d ~X(t) = ~f( ~X, t)dt+G( ~X, t)d ~W (t), (4.24)
where ~f( ~X, t) = E(∆ ~X(t)) is the drift vector, G( ~X, t) is a diffusion matrix which
satisfies GGT = Σ = E(∆ ~X(t)(∆ ~X(t))T ), and ~W (t) is a vector of independent
Wiener processes.
First consider a SDE two-patch SIS model. The drift vector has the same form as
the deterministic model
~f( ~X, t) =
−β1S1I1
N1
+ γ1I1 − ds12S1 + ds21S2
β1S1I1
N1
− γ1I1 − α1I1 − di12I1 + di21I2
−β2S2I2
N2
+ γ2I2 + ds12S1 − ds21S2
β2S2I2
N2
− γ2I2 − α2I2 + di12I1 − di21I2
,
and the diffusion matrix is given by
G =
[G11 O G13
O G22 G23
],
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
where
Gjj =
−
√βjSjIjNj
√γjIj 0√
βjSjIjNj
−√γjIj −
√αjIj
, j = 1, 2,
G13 =
[−√ds12S1
√ds21S2 0 0
0 0 −√di12I1
√di21I2
],
G23 =
[√ds12S1 −
√ds21S2 0 0
0 0√di12I1 −
√di21I2
].
The explicit form of the stochastic two-patch SIS model is
dS1 =
(−β1S1I1
N1
+ γ1I1 − ds12S1 + ds21S2
)dt−
√β1S1I1
N1
dW1
+√γ1I1dW2 −
√ds12S1dW7 +
√ds21S2dW8,
dI1 =
(β1S1I1
N1
− γ1I1 − α1I1 − di12I1 + di21I2
)dt+
√β1S1I1
N1
dW1
−√γ1I1dW2 −
√α1I1dW3 −
√di12I1dW9 +
√di21I2dW10,
dS2 =
(−β2S2I2
N2
+ γ2I2 + ds12S1 − ds21S2
)dt−
√β2S2I2
N2
dW4
+√γ2I2dW5 +
√ds12S1dW7 −
√ds21S2dW8,
dI2 =
(β2S2I2
N2
− γ2I2 − α2I2 + di12I1 − di21I2
)dt+
√β2S2I2
N2
dW4
−√γ2I2dW5 −
√α2I2dW6 +
√di12I1dW9 −
√di21I2dW10.
Two-patch SIR/SIRS models of the form (4.24) can be constructed in a similar
manner. For the SDE two-patch SIRS model, the drift vector is the same as the
right-hand side of the ODE model (4.14)-(4.16) and the diffusion matrix is
G =
[G11 O G13 G14 G15
O G22 G23 G24 G25
],
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
where
Gjj =
−
√βjSjIjNj
0√νjRj 0
−
√βjSjIjNj
−√γjIj 0 −
√α1I1
0√γjIj −
√νjRj 0
, j = 1, 2,
G13 =
−√ds12S1
√ds21S2
0 0
0 0
,
G23 =
√ds12S1 −
√ds21S2
0 0
0 0
.The 3× 2 submatrices G14, G24, G15, and G25 have a similar form. The stochastic
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
two-patch SIR/SIRS model has the following explicit form:
dS1 =
(−β1S1I1
N1
+ ν1R1 − ds12S1 + ds21S2
)dt−
√β1S1I1
N1
dW1
+√ν1R1dW3 −
√ds12S1dW9 +
√ds21S2dW10,
dI1 =
(β1S1I1
N1
− γ1I1 − α1I1 − di12I1 + di21I2
)dt+
√β1S1I1
N1
dW1
−√γ1I1dW2 −
√α1I1dW4 −
√di12I1dW11 +
√di21I2dW12,
dR1 = (γ1I1 − ν1R1 − dr12R1 + d221R2)dt+
√γ1I1dW2 −
√ν1R1dW3
−√dr12R1dW13 +
√dr21R2dW14,
dS2 =
(−β2S2I2
N2
+ ν2R2 + ds12S1 − ds21S2
)dt−
√β2S2I2
N2
dW5
+√ν2R2dW7 +
√ds12S1dW9 −
√ds21S2dW10,
dI2 =
(β2S2I2
N2
− γ2I2 − α2I2 + di12I1 − di21I2
)dt+
√β2S2I2
N2
dW5
−√γ2I2dW6 −
√α2I2dW8 +
√di12I1dW11 −
√di21I2dW12,
dR2 = (γ2I2 − ν2R2 + dr12R1 − dr21R2)dt+√γ2I2dW6 −
√ν2R2dW7
+√dr12R1dW13 −
√dr21R2dW14.
4.2.4 Numerical Examples
The dynamics of the ODE, CTMC, and SDE multi-patch models will be
illustrated in several numerical examples. The first set of examples considers
two-patch and three-patch SIS epidemic models without disease-related deaths of
the form (4.1)-(4.2). We apply branching process theory to derive the probability of
disease persistence and illustrate the significance of the location of the outbreak. In
the second set of examples we illustrate the difference in extinction behavior
between the deterministic and stochastic models with disease-related deaths. These
latter examples illustrate the effects of finite-time extinction. In a third and final
example, we illustrate a stochastic nine-patch model representative of the analogous
deterministic model of Allen et al. [5].
Consider a two-patch SIS epidemic without disease-related deaths. If
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
ds12 + ds21 > 0, then there exists a unique DFE for the ODE model given by
(S1, 0, S2, 0) =
(ds21N
ds12 + ds21
, 0,ds12N
ds12 + ds21
, 0
), (4.25)
where N = N(0). According to Theorem 4.2, the DFE (4.25) is globally
asymptotically stable if R0 < 1, where R0 is defined as in (4.13) [70]. The
next-generation matrix is
FV −1 =1
γ1γ2 + γ1di21 + γ2di12
[β1(γ2 + di21) β1d
i21
β2di12 β2(γ1 + di12)
]
and the basic reproduction number R0 equals
β1(γ2 + di21) + β2(γ1 + di12) +√
[β1(γ2 + di21)− β2(γ1 + di12)]2 + 4β1β2di12di21
2(γ1γ2 + γ1di21 + γ2di12).
For the corresponding CTMC two-patch model, the offspring pgfs for I1 and I2 are
given by (4.18) and the expectation matrix is given by (4.19). It is straightforward
to show that R0 < 1 iff ρ(M) < 1. If R0 > 1, then the probability of disease
persistence is given by equation (3.2). Unfortunately, if R0 > 1, an analytical
expression for the unique fixed point (q1, q2) ∈ (0, 1)2 of the offspring pgfs cannot be
calculated. The fixed point and probability of disease extinction are found
numerically.
Consider the parameter values β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, and
dskj = dikj = 0.1 for k, j = 1, 2 with a total population size of N = 400. For these
values, R01 = 5, R02 = 0.5, R0 = 2.83, and ρ(M) = 1.45. Patch 1 is a high-risk
patch and patch 2 is low-risk. According to Theorem 4.1, in the absense of dispersal
the disease persists in patch 1 and dies out in patch 2. However, when dispersal is
allowed the disease persists in both patches. For the deterministic model, there
exists a locally stable endemic equilibrium (S1, I1, S2, I2) ≈ (68, 132, 161, 39). This
result is consistent with the results of Allen and Kirupaharan [7]. In Table 4.3, the
probability of disease extinction P0 is calculated and compared to the approximation
obtained from the proportion of sample paths (out of 10,000) for which the sum
I1(t) + I2(t) hits zero (disease extinction) before time t = 150. The solution of the
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
ODE and one sample path for the CTMC model are plotted in Figure 4.1.
Table 4.3. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC two-patch SIS model. Parametervalues are β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, ds12 = ds21 = 0.1, and di12 = di21 = 0.1with initial conditions I1(0) = i1, S1(0) = 200− i1, I2(0) = i2, and S2(0) = 200− i2.
i1 i2 P0 Approx.
1 0 0.3410 0.34060 1 0.8055 0.80621 1 0.2747 0.27732 0 0.1163 0.11710 2 0.6489 0.6495
Figure 4.1. The ODE solution and one sample path for the CTMC two-patch SISmodel. Parameter values are β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, ds12 = ds21 = 0.1,and di12 = di21 = 0.1 with initial conditions S1(0) = 199, I1(0) = 1, S2(0) = 200, andI2(0) = 0. An outbreak occurs with probability 1 − P0 = 0.6590. The locally stableendemic equilibrium is (S1, I1, S2, I2) ≈ (68, 132, 161, 39).
Consider a three-patch SIS epidemic without disease-related deaths. Suppose that
the patches are arranged in a strip so there is no direct dispersal between patches
one and three. Consider the parameter values β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4,
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
β3 = 0.1, γ3 = 0.4, and dskj = dikj = 0.1 for k 6= 3 and j 6= 3 with a total population
size of N = 450. For these values, R01 = 5, R02 = 0.5, R03 = 0.25, R0 = 2.77, and
ρ(M) = 1.43. Patch 1 is a high-risk patch and patches 2 and 3 are low-risk. For the
deterministic model, there exists a locally stable endemic equilibrium,
(S1, I1, S2, I2, S3, I3) ≈ (53, 97, 126, 24, 144, 6). In Table 4.4, the probability of
disease extinction P0 is calculated and compared to the approximation obtained
from the proportion of sample paths (out of 10,000) for which the sum
I1(t) + I2(t) + I3(t) hits zero before time t = 150. The solution of the ODE and one
sample path for the CTMC model are plotted in Figure 4.2.
Table 4.4. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC three-patch SIS model. Parametervalues are β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, β3 = 0.1, γ3 = 0.4, dskj = dikj = 0.1for k 6= 3 and j 6= 3, and ds13 = ds31 = di13 = di31 = 0 with initial conditions I1(0) = i1,S1(0) = 150− i1, I2(0) = i2, S2(0) = 150− i2, I3(0) = i3, and S3(0) = 150− i3.
i1 i2 i3 P0 Approx.
1 0 0 0.3509 0.35890 1 0 0.8407 0.84220 0 1 0.9613 0.96311 1 1 0.2836 0.2901
The results in Tables 4.3 and 4.4 illustrate that the location of an outbreak plays
an important role in the persistence of a disease. The probability of disease
extinction is significantly higher if an outbreak occurs in a low-risk patch.
The next set of examples illustrates differences between the extinction dynamics
of deterministic and stochastic multi-patch models with disease-related mortality. In
particular, these examples show that there is finite-time extinction for the stochastic
(CTMC and SDE) models, and for the deterministic models the infectious
population asymptotically approaches zero without ever hitting zero. The difference
in extinction behavior between deterministic and stochastic models is well-known.
When population sizes are small in deterministic models, they can rebound but this
is not the case in stochastic models because extinction occurs for small population
sizes. In 1991, Mollison [56] coined the term “atto-fox” to denote the fraction of one
fox (10−18 of a fox), an unrealistically small fraction reached by the predator
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Figure 4.2. The ODE solution and one sample path for the CTMC three-patch SISmodel. Parameter values are β1 = 0.5, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, β3 = 0.1,γ3 = 0.4, dskj = dikj = 0.1 for k 6= 3 and j 6= 3, and ds13 = ds31 = di13 = di31 = 0 withinitial conditions S1(0) = 149, I1(0) = 1, S2(0) = 150, I2(0) = 0, S3(0) = 150, andI3(0) = 0. An outbreak occurs with probability 1 − P0 = 0.6491. The locally stableendemic equilibrium is (S1, I1, S2, I2, S3, I3) ≈ (53, 97, 126, 24, 144, 6).
population in a deterministic predator-prey system.
Consider a two-patch SIS epidemic with a relatively high rate of disease-related
mortality compared to the rate of recovery. Consider the parameter values β1 = 0.8,
γ1 = 0.1, β2 = 0.3, γ2 = 0.4, α1 = α2 = 0.5, and dskj = dikj = 0.1 for k, j = 1, 2 with
an initial population size of N(0) = 400. For these values, R01 = 4/3, R02 = 1/3,
R0 = 1.17, and ρ(M) = 1.075. There are significant differences between the
dynamics of the deterministic and stochastic models. For the ODE model, the total
population size in both patches asymptotically approaches zero. For the CTMC
model, the number of infectious individuals hits zero in a finite amount of time. In
the absence of infectious individuals, the number of susceptible individuals remains
constant and is not driven to zero. The solution of the ODE and one sample path
for the CTMC model are plotted in Figure 4.3. Using the same parameter values
and initial conditions, a similar result holds for the SDE two-patch SIS model. The
results are plotted in Figure 4.4.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Figure 4.3. The ODE solution and one sample path for the CTMC two-patch SISmodel. Parameter values are β1 = 0.8, γ1 = 0.1, β2 = 0.3, γ2 = 0.4, α1 = α2 = 0.5,ds12 = ds21 = 0.1, and di12 = di21 = 0.1 with initial conditions S1(0) = 195, I1(0) = 5,S2(0) = 185, and I2(0) = 15.
Figure 4.4. The ODE and SDE solutions for the two-patch SIS model. Parametervalues are β1 = 0.8, γ1 = 0.1, β2 = 0.3, γ2 = 0.4, α1 = α2 = 0.5, ds12 = ds21 = 0.1,and di12 = di21 = 0.1 with initial conditions S1(0) = 195, I1(0) = 5, S2(0) = 185, andI2(0) = 15.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Next consider a two-patch SIRS model with disease-related deaths. Consider the
parameter values β1 = 0.8, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, ν1 = ν2 = 0.1,
α1 = α2 = 0.4, and dskj = dikj = drkj = 0.1 for k, j = 1, 2 with an initial population
size of N(0) = 400. For these values, R01 = 1.6, R02 = 0.25, R0 = 1.36, and
ρ(M) = 1.15. Again, the total population asymptotically approaches zero for the
deterministic model. For the CTMC model, the number of infectious individuals
hits zero in a finite amount of time. In the absense of infectious individuals,
susceptible individuals remain susceptible and recovered individuals lose their
immunity driving the number of recovered individuals in each patch to zero. The
solution of the ODE and one sample path for the CTMC model are plotted in
Figure 4.5. A similar result holds for the SDE model, graphed in Figure 4.6.
Figure 4.5. Solution of the ODE and one sample path for the CTMC two-patch SIRSmodel. Parameter values are β1 = 0.8, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, ν1 = ν2 = 0.1,α1 = α2 = 0.4, and dskj = dikj = drkj = 0.1 for k, j = 1, 2 with initial conditionsS1(0) = 195, I1(0) = 5 R1(0) = 0, S2(0) = 185, I2(0) = 15, and R2(0) = 0.
In two final examples, ODE and SDE nine-patch SIS models without
disease-related mortality are simulated and compared. Consider a nine-patch SIS
model where the patches are arranged in a 3× 3 grid and dispersal only occurs
between two patches if they share an adjacent edge. The patches are numbered
consecutively from left to right and top to bottom with the patch in the (1, 1)
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Figure 4.6. The ODE and SDE solutions for the two-patch SIRS model. Parametervalues are β1 = 0.8, γ1 = 0.1, β2 = 0.2, γ2 = 0.4, ν1 = ν2 = 0.1, α1 = α2 = 0.4, anddskj = dikj = drkj = 0.1 for k, j = 1, 2 with initial conditions S1(0) = 195, I1(0) = 5R1(0) = 0, S2(0) = 185, I2(0) = 15, and R2(0) = 0.
position being patch 1 and the patch in the (3, 3) position being patch 9. The
deterministic model is the same as the nine-patch SIS model discussed by Allen et al.
[5]. The focus of this investigation will be on the corresponding stochastic models.
The dispersal rates for susceptible individuals are small and the infectious dispersal
rates are much larger. For j = 2, 4, 6, 8, let βj = 0.3 and γj = 0.2. For j = 1, 3, 7, 9,
let βj = 0.2 and γj = 0.4. For the center patch, j = 5, let β5 = 0.6 and γ5 = 0.3. If
two patches j and k share an edge, then dskj = dsjk = 0.01 and dikj = dijk = 0.1.
Assume that the initial population size in each patch is 100, Sj(0) + Ij(0) = 100 for
j = 1, . . . , 9, so the total population size is N = 900. For these values, the patch
reproduction numbers are R0j = 1.5 for j = 2, 4, 6, 8, R0j = 0.5 for j = 1, 3, 7, 9, and
R05 = 2. The basic reproduction number is R0 = 1.27. For the ODE and SDE
nine-patch models, the disease persists in all patches. In the high-risk patches, there
is a greater number of infectives and a reduced number of susceptibles. Susceptible
individuals move to the low risk patches [5]. The solution of the ODE model and a
sample path of the SDE model are plotted in Figure 4.7. In the branching process
approximation of the CTMC model, with a small number of infectious individuals
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
there is a positive probability of disease extinction without an outbreak in any
patch, provided ρ(M) > 1. This probability can be computed from the fixed point of
the offspring pgfs. In this example, we did not compute this probability.
Figure 4.7. Solutions of the ODE and SDE nine-patch SIS models. Parameter valuesare βj = 0.3, γj = 0.2 for j = 2, 4, 6, 8, βj = 0.2, γj = 0.4, for j = 1, 3, 7, 9, β5 = 0.6,and γ5 = 0.3 with initial conditions S5(0) = 95, I5(0) = 5, and Sj(0) = 100, Ij(0) = 0for j 6= 5.
Now consider a nine-patch SIS model with parameter values βj = 0.1, γj = 0.4 for
j = 1, 2, 3, 4, 7, βj = 0.1, γj = 0.2 for j = 5, 6, 8, and β9 = 0.5 and γ9 = 0.1. If two
patches j and k share an edge, then dsjk = dskj = 0.01, and dijk = dikj = 0.1. Again,
suppose that Sj(0) + Ij(0) = 100 for j = 1, . . . , 9 so the total population size is
N = 900. For these values, the patch reproduction numbers are R0j = 0.25 for
j = 1, 2, 3, 4, 7, R0j = 0.5 for j = 5, 6, 8, and R09 = 5. The basic reproduction
number is R0 = 2.01. Suppose at outbreak occurs in patch 9, a high-risk patch.
Choose the initial conditions I9(0) = 1, S9(0) = 99, and for all j 6= 9, Sj(0) = 100
and Ij(0) = 0. For the ODE and SDE nine-patch models, the results are similar.
The disease persists in patch 9, the high-risk patch, but there is a significant
reduction in the total population size. There is very little infection in the low-risk
patches. See Figure 4.8. Although it is not clear in the SDE model, in the
branching process approximation of the CTMC model, with ρ(M) > 1, there is a
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positive probability of disease extinction.
Figure 4.8. Solutions of the ODE and SDE nine-patch SIS models. Parameter valuesare βj = 0.1, γj = 0.4 for j = 1, 2, 3, 4, 7, βj = 0.1, γj = 0.2 for j = 5, 6, 8, andβ9 = 0.5 and γ9 = 0.1 with initial conditions S9(0) = 99, I9(0) = 1, and Sj(0) = 100,Ij(0) = 0 for j 6= 9.
4.3 Multi-Patch SIS, SIR, and SIRS Models with Demographics
In this section multi-patch SIS, SIR, and SIRS models with demographics will be
considered. The development and analysis of these models is similar to the analysis
of the multi-patch models without demographics. However, there are some
significant differences in that with immigration and births, disease-related deaths
cannot drive the total population to extinction.
4.3.1 Deterministic Models
Consider a multi-patch SIS model with demographics, where n ≥ 2 is the number
of patches and Ω = 1, 2, . . . , n. The notation is the same as for the multi-patch
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SIS model without demographics (4.1)-(4.2). The model takes the form
Sj = Λj − µjSj −βjSjIjNj
+ γjIj +∑k∈Ω
(dskjSk − dsjkSj), (4.26)
Ij =βjSjIjNj
− (γj + αj + µj)Ij +∑k∈Ω
(dikjIk − dijkIj), (4.27)
with Sj(0) > 0 and Ij(0) ≥ 0 for all j ∈ Ω. The parameters Λj > 0 and µj > 0
represent the immigration rate and natural death rate in patch j, respectively.
Summing the equations for Sj and Ij in (4.26)-(4.27), it follows that for each
j ∈ Ω
Nj = Λj − µjNj − αjIj +∑k∈Ω
(dskjSk − dsjkSj + dikjIk − dijkIj). (4.28)
Let N denote the total population size in all patches,
N =∑j∈Ω
Nj. (4.29)
It follows from equation (4.28) that
N =∑j∈Ω
(Λj − µjNj − αjIj) >∑j∈Ω
Λj −∑j∈Ω
(µj + αj)Nj ≥∑j∈Ω
Λj − mjN, (4.30)
where mj = maxj∈Ω(µj + αj). Thus, N is always positive, it is impossible to drive
the total population to zero.
For each patch j ∈ Ω, define the patch reproduction number as
R0j =βj
γj + µj + αj. (4.31)
The following theorem summarizes the dynamics in each patch when there is no
movement or disease-related death.
Theorem 4.4. Let Ds = Di = O (zero matrices) and suppose αj = 0. Then
(i) If R0j ≤ 1, then
limt→∞
(Sj(t), Ij(t)) =
(Λj
µj, 0
).
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
(ii) If R0j > 1, then
limt→∞
(Sj(t), Ij(t)) =
(Nj
R0j
, Nj −Nj
R0j
)where Aj +Bj = Λj/µj.
Proof. For fixed j ∈ Ω, let ij = Ij/Nj. For simplicity, omit the subscript j and write
i = i/N and R0 = β/(γ + µ). Then
N = Λ− µN, (4.32)
and
i = i
(β − γ − Λ
N− βi
). (4.33)
The solution of (4.32) is
N(t) =Λ
µ+
(N(0)− Λ
µ
)e−µt.
Since µ > 0,
limt→∞
N(t) =Λ
µ.
Thus, for all 0 < ε < µ there exists T sufficiently large so that for t ≥ T
Λ
µ(1 + ε/µ)≤ N(t) ≤ Λ
µ(1− ε/µ).
Then equation (4.33) is bounded for t ≥ T :
i(β − γ − µ− ε− βi) ≤ i ≤ i(β − γ − µ+ ε− βi).
If R0 ≤ 1, then β − γ − µ ≤ 0. Thus,
i ≤ i(ε− βi).
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Since ε > 0, by the comparison principle, the limit i = limt→∞ i(t) is bounded:
0 ≤ i ≤ ε
β.
Since ε > 0 is arbitrary, i(t)→ 0. Thus,
limt→∞
(S(t), I(t)) =
(Λ
µ, 0
).
If R0 > 1, then β − γ − µ > 0 and β > 0. By the comparison principle, if R0 > 1
and ε is sufficiently small, then the limit i = limt→∞ i(t) is bounded:
β − γ − µ− εβ
≤ i ≤ β − γ − µ+ ε
β.
Since ε is arbitrary, i(t)→ 1− 1/R0. Thus,
limt→∞
(S(t), I(t)) =
(N
R0
, N − N
R0
).
Next, a basic reproduction number is defined for the patch model (4.26)-(4.27).
Let
F = diag[βj], (4.34)
V = diag
[γj + αj + µj +
∑k∈Ω
dijk
]−Di, (4.35)
where Di is the dispersal matrix for infectives. The basic reproduction number is
the spectral radius of FV −1 [70],
R0 = ρ(FV −1). (4.36)
The next theorem states that if R0 < 1, then the infection dies out. The proof is
similar to the proofs of Theorem 4.2 and Corollary 4.1.
Theorem 4.5. (i) If R0 < 1, then the multi-patch SIS epidemic model with
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demographics (4.26)-(4.27) satisfies I(t)→ 0 as t→∞.
(ii) For fixed j ∈ Ω, if R0j < 1 and dijk = dikj = 0 for k 6= j, then in model
(4.26)-(4.27), Ij(t)→ 0 as t→∞.
Consider a multi-patch SIR or SIRS model with demographics, where n ≥ 2 is the
number of patches and Ω = 1, 2, . . . , n. The notation is the same as for the
multi-patch SIR or SIRS model without demographics. The model takes the form
Sj = Λj − µjSj −βjSjIjNj
+ νjRj +∑k∈Ω
(dskjSk − dsjkSj), (4.37)
Ij =βjSjIjNj
− (γj + αj + µj)Ij +∑k∈Ω
(dikjIk − dijkIj), (4.38)
Rj = γjIj − µjRj − νjRj +∑k∈Ω
(drkjRk − drjkRj), (4.39)
where Sj(0) > 0, Ij(0) ≥ 0, and Rj(0) = 0 for each j ∈ Ω. The patch reproduction
numbers remain the same as for the SIS model with demographics,
R0j =βj
γj + µj + αj.
In addition, Theorem 4.5 applies which is stated here as a corollary.
Corollary 4.3. (i) If R0 < 1, then the multi-patch SIR or SIRS epidemic model
with demographics (4.37)–(4.39) satisfies I(t)→ 0 as t→∞.
(ii) For fixed j ∈ Ω, if R0j < 1 and dijk = dikj = 0 for k 6= j, then in model
(4.37)–(4.39), Ij(t)→ 0 as t→∞.
The next theorem summarizes the dynamics of the SIR and SIRS models with
demographics in each patch when there is no movement or disease-related death.
The following results will be used in the proof of Theorem 4.6. Consider the
following systems:
x = f(t, x), (4.40)
y = g(y), (4.41)
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where f and g are continuous and locally Lipschitz in x in Rn and solutions exist for
all positive time. The equation (4.40) is said to be asymptotically autonomous with
limit equation (4.41) if f(t, x)→ g(x) as t→∞ uniformly for x in Rn [37].
Corollary 4.4. ([37], p. 851) If solutions of system (4.40) are bounded and the
equilibrium e of the limit system (4.41) is globally asymptotically stable, then any
solution x(t) of system (4.40) satisfies x(t)→ e as t→∞.
Theorem 4.6. Let Ds = Di = Dr = O (zero matrices) and suppose αj = 0. Then
(i) If R0j ≤ 1, then
limt→∞
(Sj(t), Ij(t), Rj(t)) =
(Λ
µ, 0, 0
).
(ii) If R0j > 1, then
limt→∞
(Sj(t), Ij(t), Rj(t)) = (S, I , R),
where S, I , R > 0 and S + I + R = Λ/µ.
Proof. For fixed j ∈ Ω, let sj = Sj/Nj, ij = Ij/Nj, and rj = Rj/Nj. For simplicity,
omit the subscript j and write s = S/N , i = I/N , r = R/N , and R0 = β/(γ + α).
Then s+ i+ r = 1 and r = 1− s− i. So the dynamics depend on s and i. First,
N = Λ− µN. (4.42)
It follows that
limt→∞
N(t) =Λ
µ.
The differential equations for s and i are:
s =Λ
N(1− s)− βsi+ ν(1− s− i),
i = i
(βs− γ − Λ
N
).
(4.43)
Since N(t)→ Λ/µ as t→∞, system (4.43) is asymptotically autonomous with the
limit system
s = µ(1− s)− βsi+ ν(1− s− i),i = i(βs− γ − µ).
(4.44)
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
By Corollary 4.4, the limiting equilibrium of (4.43) is the same as the limiting
equilibrium of (4.44). Applying Dulac’s criterion [3] to (4.44) with a Dulac function
D(s, i) = 1/i, shows that there are no periodic solutions in the interior of R2+.
Indeed, let
f(s, i) =s
i=
µ(1− s) + ν(1− s− i)i
− βs,
g(s, i) =i
i= βs− γ − µ.
It follows that∂f
∂s+∂g
∂i= −µ+ ν
i− β.
This expression is negative in the interior of R2+. The i-nullclines of (4.44) are i = 0
and s = 1/R0, and the s-nullcline is
i =(µ+ ν)(1− s)
βs+ ν.
If R0 > 1, then there exists a globally asymptotically stable endemic equilibrium:
s =1
R0
,
i =(µ+ ν)(R0 − 1)
β +R0ν,
r =(β −R0)(R0 − 1)
R0(β +R0ν).
If R0 ≤ 1, then the only equilibrium is (1, 0, 0). By way of contradiction, suppose
that solutions do not approach this equilibrium. That is, the ω-limit set of (4.44)
does not contain (1, 0, 0). By the Poincare-Bendixon criterion [46], the positive orbit
of (4.44) is periodic or the ω-limit set is periodic, a contradiction since there are no
periodic solutions in R2+. Thus, (1, 0, 0) is a stable equilibrium.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
4.3.2 Markov Chain Models
Consider a corresponding CTMC multi-patch SIS, SIR, or SIRS model with
demographics. Let
~X(t) = (S1(t), I1(t), . . . , Sn(t), In(t))T ,
~X(t) = (S1(t), I1(t), R1(t), . . . , Sn(t), In(t), Rn(t))T
be discrete random vectors for the SIS and SIR/SIRS models respectively. For
simplicity, the same notation is used for the deterministic variables and stochastic
random variables. The transitions and corresponding rates for ~X(t) are listed in
Tables 4.5 and 4.6.
Table 4.5. State transitions and rates for the CTMC multi-patch SIS epidemic modelwith demographics.
Description State transition Rate
Immigration in patch j (0, . . . , Sj + 1, . . . , 0) Λj
Death of Sj (0, . . . , Sj − 1, . . . , 0) µjSjInfection in patch j (0, . . . , Sj − 1, Ij + 1, . . . , 0) βjSjIj/Nj
Recovery in patch j (0, . . . , Sj + 1, Ij − 1, . . . , 0) γjIjDeath of Ij (0, . . . , Ij − 1, . . . , 0) (αj + µj)IjSusceptible dispersal from j to k (0, . . . , Sj − 1, . . . , Sk + 1, . . . , 0) dsjkSjInfectious dispersal from j to k (0, . . . , Ij − 1, . . . , Ik + 1, . . . , 0) dijkIj
Let Sj(0) ≈ Nj(0), Ij(0) = 1, and Ik(0) = 0 for all k 6= j. The offspring pgf for Ij
is similar to the branching process without demographics. That is,
fj(x1, . . . , xn) =
βjx2j + γj + αj + µj +
∑k∈Ω\j
dijkxk
βj + γj + αj + µj +∑
k∈Ω\j
dijk. (4.45)
The offspring pgfs for Ij are the same for the SIS, SIR, and SIRS models.
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Table 4.6. State transitions and rates for the CTMC multi-patch SIR/SIRS epidemicmodel with demographics.
Description State transition Rate
Immigration in patch j (0, . . . , Sj + 1, . . . , 0) Λj
Death of Sj (0, . . . , Sj − 1, . . . , 0) µjInfection in patch j (0, . . . , Sj − 1, Ij + 1, . . . , 0) βjSjIj/Nj
Recovery in patch j (0, . . . , Ij − 1, Rj + 1, . . . , 0) γjIjDeath of Ij (0, . . . , Ij − 1, . . . , 0) (αj + µj)IjDeath of Rj (0, . . . , Rj − 1, 0, . . . , 0) µjRj
Loss of immunity in patch j (0, . . . , Sj + 1, Ij, Rj − 1, . . . , 0) νjRj
Susceptible dispersal from j to k (0, . . . , Sj − 1, . . . , Sk + 1, . . . , 0) dsjkSjInfectious dispersal from j to k (0, . . . , Ij − 1, . . . , Ik + 1, . . . , 0) dijkIjRecovered dispersal from j to k (0, . . . , Rj − 1, . . . , Rk + 1, . . . , 0) drjkRj
The expectation matrix M = [mkj] is a nonnegative n× n matrix such that
mkj =
2βj
βj + γj + αj + µj +∑
k∈Ω\j
dijk, k = j
dijk
βj + γj + αj + µj +∑
k∈Ω\j
dijk, k 6= j.
(4.46)
4.3.3 Stochastic Differential Equation Models
Consider the corresponding SDE multi-patch SIS, SIR, and SIRS models with
demographics. Given the transitions and rates in Tables 4.5 and 4.6, the
corresponding SDE models have the form (4.24). The explicit form of the stochastic
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
two-patch SIS model is
dS1 =
(Λ1 − µ1S1 −
β1S1I1
N1
+ γ1I1 − ds12S1 + ds21S2
)dt+
√Λ1dW1
−√µ1S1dW2 −
√β1S1I1
N1
dW5 +√γ1I1dW6 −
√ds12S1dW13 +
√ds21S2dW14,
dI1 =
(β1S1I1
N1
− γ1I1 − α1I1 − µ1I1 − di12I1 + di21I2
)dt+
√β1S1I1
N1
dW5
−√γ1I1dW6 −
√α1I1dW9 −
√µ1I1dW10 −
√di12I1dW15 +
√di21I2dW16,
dS2 =
(Λ2 − µ2S2 −
β2S2I2
N2
+ γ2I2 + ds12S1 − ds21S2
)dt+
√Λ2dW3
−√µ2S2dW4 −
√β2S2I2
N2
dW7 +√γ2I2dW8 +
√ds12S1dW13 −
√ds21S2dW14,
dI2 =
(β2S2I2
N2
− γ2I2 − α2I2 − µ2I2 + di12I1 − di21I2
)dt+
√β2S2I2
N2
dW7
−√γ2I2dW8 −
√α2I2dW11 −
õ2I2dW12 +
√di12I1dW15 −
√di21I2dW16.
Stochastic two-patch SIR/SIRS models with demographics of the form (4.24) can be
constructed in a similar manner.
4.3.4 Numerical Examples
Consider a two-patch SIS epidemic with demographics and disease-related deaths.
The unique DFE for the ODE model given by
(S1, 0, S2, 0) =
(Λ1(µ2 + ds21) + Λ2d
s21
µ1µ2 + µ1ds21 + µ2ds12
, 0,Λ1d
s12 + Λ2(µ1 + ds12)
µ1µ2 + µ1ds21 + µ2ds12
, 0
). (4.47)
According to Theorem 4.5, this DFE is globally asymptotically stable if R0 < 1,
where R0 is given by (4.36) [70]. For this example, the next-generation matrix is
FV −1 =1
A1A2 − di12di21
[β1A2 β1d
i21
β2di12 β2A1
],
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
where A1 = γ1 + α1 + µ1 + di12 and A2 = γ2 + α2 + µ2 + di21 and the basic
reproduction number R0 equals
β1A2 + β2A1 +√
(β1A2 − β2A1)2 + 4β1β2di12di21
2(A1A2 − di12di21)
.
Consider the following parameter values for the two-patch SIS model with
demographics: Λ2 = Λ2 = 2, µ1 = µ2 = 0.01, β1 = 0.5, γ1 = 0.2, β2 = 0.2, γ2 = 0.5,
and dskj = dikj = 0.1 for k, j = 1, 2. For these values, R01 = 2.38, R02 = 0.39,
R0 = 1.73, and ρ(M) = 1.25. Patch 1 is a high-risk patch and patch 2 is low-risk. In
Table 4.7, the probability of disease extinction P0 is calculated and compared to the
approximation obtained from the proportion of sample paths (out of 10,000) for
which the sum I1(t) + I2(t) hits zero (disease extinction) before time t = 150. The
solution of the ODE and one sample path for the CTMC model are plotted in
Figure 4.9. Using the same parameter values, the solution of the ODE and SDE
models are plotted in Figure 4.10.
i1 i2 P0 Approx.
1 0 0.5735 0.57480 1 0.9008 0.90301 1 0.5166 0.51862 0 0.3289 0.32150 2 0.8114 0.8119
Table 4.7. Probability of disease extinction P0 and numerical approximation (Ap-prox.) based on 10,000 sample paths of the CTMC two-patch SIS model with demo-graphics. Parameter values are Λ1 = Λ2 = 2, µ1 = µ2 = 0.01, β1 = 0.5, γ1 = 0.2,β2 = 0.2, γ2 = 0.5, and dskj = dikj = 0.1 for k, j = 1, 2 with initial conditions I1(0) = i1,S1(0) = 200− i1, I2(0) = i2, and S2(0) = 200− i2.
4.4 Discussion
Multi-patch epidemic models with and without demographics have been derived.
For the deterministic models, in the absense of dispersal, the dynamics in each
patch depend on the patch reproduction number. In addition, a basic reproduction
number was defined for the system. If R0 < 1, the disease is driven to extinction.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
Figure 4.9. The ODE solution and one sample path for the CTMC two-patch SISmodel with demographics. Parameter values are Λ1 = Λ2 = 2, µ1 = µ2 = 0.01,β1 = 0.5, γ1 = 0.2, β2 = 0.2, γ2 = 0.5, and dskj = dikj = 0.1 for all k, j = 1, 2 withinitial conditions S1(0) = 199, I1(0) = 1, S2(0) = 200, and I2(0) = 0. An outbreakoccurs with probability 1− P0 = 0.4265.
Figure 4.10. Solution of the ODE and SDE two-patch SIS models with demographics.Parameter values are Λ1 = Λ2 = 2, µ1 = µ2 = 0.01, β1 = 0.5, γ1 = 0.2, β2 = 0.2,γ2 = 0.5, and dskj = dikj = 0.1 for k, j = 1, 2 with initial conditions S1(0) = 195,I1(0) = 5, S2(0) = 195, and I2(0) = 5.
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Texas Tech University, Glenn E. Lahodny Jr., August 2012
However, if R0 > 1, the disease may or may not persist depending on the dispersal
rates. Furthermore, stochastic multi-patch epidemic models were constructed and
branching process theory was used to determine the probability of disease
persistence or extinction. The relationship between the basic reproduction number,
R0, and the spectral radius of the expectation matrix, ρ(M), with respect to the
threshold value one has been illustrated in Chapter 3 for the case of two patches.
Numerical results show the effects of dispersal and the location of an outbreak on
the probability of disease persistence or extinction. In addition, the numerical
results illustrate a difference between the deterministic and stochastic multi-patch
models with regard to finite-time extinction.
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