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(3b−a2

9

)3

. Then the following assertions hold:

Case 1: When △ > 0, (19) has one real root and one pair of conjugate virtual roots;

Case 2: When △ = 0, (19) has three real roots, at least two of which are repeated roots;

Case 3: When △ < 0, (19) has three different real roots.

Moreover, the roots of (19) are

z1 =3

ρ1+3 ρ2+ a

3, z2 = ψ√3

ρ1+ ¯ψ√3 ρ2+ a

3, z3 = ¯ψ√3

ρ1+ ψ√3 ρ2+ a

3, where ρ1 =−2a3− 9ab + 27c

54 +

△, ρ2 =−2a3− 9ab + 27c

54 −√

△, ψ = −1 2+ i

3 2 and i2 =−1.

By Lemma 2, if △ ≤ 0, the basic reproduction number R0 = max{|z1|, |z2|, |z3|}; if

△ > 0, we obtain the reproduction number R0 = z1. We conclude our local stability in the following theorem.

Theorem 2. For the disease transmission model (5) (equivalently, (6)), if R0 < 1, then the disease-free equilibrium ξ0 (x0) is locally asymptotically stable. On the other hand, if R0 > 1, then ξ0 (x0) is unstable.

4 Global stability analysis

In this section, the qualitatively global analysis of model (6) (equivalently, (5)) is pre-sented. We first show that setn+m := [0, 1]n+m is positive invariant.

Lemma 3. Set n+m is positively invariant under the flow determined by equation (6).

That is, x(t)∈ △n+m for all t > 0 and x(0)∈ △n+m.

Proof. Denote the boundaries of set n+m by ∂△n+m. Then it consists of the two parts

∂△1n+m and ∂△2n+m, where

∂△1n+m :={x ∈ △n+m: xk = 0 for some k}, and

∂△2n+m :={x ∈ △n+m: xk = 1 for some k}.

Then to prove that n+m is positively invariant, it suffices to prove that the assignment vector at any boundary point of the vector field yielded by equation (6) is tangent or pointing into the set n+m. Since n+m is a rectangle in Rn+m, the “outer normals”

at boundaries ∂△1n+m and ∂△2n+m are ⃗n1k := −ek and ⃗n2k := ek, respectively, where ek denotes the standard unit vector in Rn+m. Moreover, we compute that

(I). For x∈ ∂△1n+m with xk = 0 for some k = 1, . . . , n + m:

˙

x· ⃗n1k =









[

αkΘ(x1) + qk

n+m

j=n+1

βjxj ]

, for k = 1,· · · , n,

−rk

n j=1

Φ(x1), for k = n + 1, 2,· · · , n + m.

Thus, ˙x· ⃗n1k ≤ 0 for all k = 1, . . . , n + m.

(II). For x∈ ∂△2n+m with xk = 1 for some k = 1, . . . , n + m:

˙

x· ⃗n2k =







−γ, for k = 1, · · · , n,

−µk, for k = n + 1, 2,· · · , n + m.

Thus, ˙x· ⃗n2k < 0 for all k = 1, . . . , n + m.

By (I) and (II), we have that the assignment vector at any boundary point of the vector field yielded by equation (6) is tangent or pointing into the set n+m. Hence, the proof of Lemma3 is complete.

Next, we show that DFE ξ0 defined in (7) is globally asymptotically stable in model (5) if R0 < 1. Equivalently, equilibrium x0 = 0∈ Rn+m is globally asymptotically stable

in model (6) if R0 < 1. (For simplification, we also call x0 to be a DEF for model (6).) Before it, we first show that no equilibrium lies in n+m expect x0 and recall a general qualitative analytic result in the differential equations proposed by Lajmanovich and Yorke [12].

Lemma 4. The only equilibrium for (6) in ∂n+m, the boundary of n+m, is DFE x0.

Proof. Suppose the statement of Lemma 4 is false. Then there exists an equilibrium

¯

x := (¯x1,· · · , ¯xn+m) for (6) in ∂ n+m −{x0}. Then by definition, ¯xk = 0 for some k∈ {1, · · · , n + m}.

(I). If k∈ {1, · · · , n}, then by (6), since dxdtk = 0, we have that αkΘ( ¯x1)+qkn+m

j=n+1βjx¯j = 0. Hence Θ( ¯x1), ∑n+m

j=n+1βjx¯j = 0. Consequently, ¯xj = 0 for all j = 1, . . . , n + m, i.e.,

¯

x = x0(= 0), a contradiction.

(II). If k ∈ {n + 1, · · · , n + m}, then by (6), since dxdtk = 0, we have that Φ( ¯x1) = 0 and hence ¯xj = 0 for all j = 1, . . . , n. Moreover, for j = n + 1, . . . , n + m, since dxdtj = 0, we have that ¯xj = 0. Thus, ¯x = x0(= 0), a contradiction.

By (I) and (II), we conclude that the only equilibrium for (6) in ∂n+m, is the DFE x0. It completes the proof of Lemma 4.

Lemma 5. ( [12]) Consider the system dx

dt = Ax + H(x), (20)

where A is an ¯m× ¯m matrix and H(x) is continuously differentiable in a region D ∈ Rm¯. Suppose that the following assumptions hold:

(A1) The compact convex set C ⊂ D is positively invariant under the flow determined by equation (20).

(A2) lim

→0

∥H(x)∥

∥x∥ = 0.

(A3) There exist some r > 0 and eigenvector ν ∈ Rm¯ of AT such that ν · x ≥ r∥x∥ for all x∈ C.

(A4) ν· H(x) ≤ 0 for all x ∈ C.

(A5) {0} is the largest positively invariant set for (20) contained in set M := {x ∈ C : ν· H(x) = 0}.

Then either (i) x = 0 is globally asymptotically stable in C, or (ii) for any initial value x˜0 ∈ C − {0}, the solution ϕ(t, ˜x0) of (20) satisfies lim inft→∞∥ϕ(t, ˜x0)∥ ≥ m, where m > 0 is independent of ˜x0. Moreover, there exists a nontrivial equilibrium x of (20) in C.

Theorem 3. If R0 < 1, then x0 is globally asymptotically stable in n+m. On the other hand, if R0 > 1, then there exists an epidemic equilibrium x(> 0) in n+m. Moreover, for any initial value ˜x0 ∈ △n+m− {x0}, the solution ϕ(t, ˜x0) of (6) satisfies lim inft→∞∥ϕ(t, ˜x0)∥ ≥ m, where m > 0 is independent of ˜x0.

Proof. Notice first that equation (6) can be rewritten in the form of (20):

dx

and

Then (i) by Lemma 3, n+m is a positive invariant (compact) set for equation (6) in Rn+m; (ii) Since each term of H(x) has degree equal to 2, we have that lim

x→0

∥H(x)∥

∥x∥ = 0.

(iii) Let A1 := AT + aI where a = max{γ, µn+1,· · · , µn+m}. Then A1 is a nonnegative, irreducible matrix. Hence, by Perron-Frobenius theorem, there exists an eigenvalue λ∈ R of A1 such that λ = ρ(A1)(> 0). Moreover, it has a corresponding eigenvector ν > 0.

Consequently, λ− a is an eigenvalue of AT and ν is its corresponding eigenvector. Then for all x∈ △n+m = [0, 1]n+m, we have that ν· x ≥ ν0∥x∥1 ≥ ν0∥x∥2 where ν0 > 0 takes (22). This means that initial value starting at point x will leave M immediately under the flow determined by (21). Hence, we conclude that the largest invariant set for (21) contained in M is {0}. Thus, all assumptions in Lemma 5 hold and hence either one of the following cases hold: Case 1: Equilibrium x (= 0) is globally asymptotically stable

in n+m. Case 2: For any initial value ˜x0 ∈ △n+m− {x0}, the solution ϕ(t, ˜x0) of (6) satisfies lim inft→∞∥ϕ(t, ˜x0)∥ ≥ m, where m > 0 is independent of ˜x0. Moreover, there exists a nontrivial equilibrium x of (6) in n+m. In fact, by Lemma 4, x(> 0) is an epidemic equilibrium. By Theorem 2, Case 1 occurs iff R0 < 1 and Case 2 occurs iff R0 > 1. This completes the proof of Theorem3.

Theorem 4. If R0 > 1, then there exists a unique endemic equilibrium x(> 0) of (6) such that x is globally asymptotically stable in n+m− {x0}.

Proof. Note that the existence of the endemic equilibrium x(> 0) is guaranteed by Theorem 3. Then we aim to show that such endemic equilibrium is unique and globally asymptotically stable.

(I). We show that the existence of the endemic equilibrium x is unique. Suppose that x = (x1,· · · , xn+m)T and z = (z1,· · · , zn+m )T are two distinct endemic equilibria of and z are two equilibria of (6), we have that:

(i) If k0 ∈ {1, · · · , n}, then

xk0 on the left-hand side of the first equality. Hence, (1− xk0)

(ii) If k0 ∈ {n + 1, · · · , n + m}, then

−µk0xk0 + rk0(1− xk0)Φ(x1) =−µk0zk0 + rk0(1− zk0)Φ(z1) = 0.

By timing xzk0

k0

on the left-hand side of the above first equality, we have that, after some simple reduction,

(1− xk0)Φ(zk0 xk

0

x1) = (1− zk0)Φ(z1).

But this make a contradiction with xk0 > zk0 and zk zk0 xk

0

xk for all k = 1, . . . , n + m.

By (i) and (ii), we have the result that model (6) has a unique endemic equilibrium.

(II). We show that the endemic equilibrium x is globally asymptotically stable in

n+m− {x0}. Define G and g be two real-valued functions in △n+m by

G(x) = max

1≤k≤n+m

{xk xk

}

and g(x) = min

1≤k≤n+m

{xk xk

}

. (24)

Then G(x) and g(x) are continuous and their right-hand derivatives exist along solutions of (6).

Let x(t) be a solution of (6). Then for any given t0 ≥ 0, there is some sufficiently small ϵ > 0 such that G(x(t)) = xk0x(t)

k0 , for some k0 ∈ {1, . . . , n + m} in t ∈ [t0, t0+ ϵ], and hence

G|(6)(x(t0)) = xk0(t0) xk0 , where G|(6) is define as

G|(6) = lim sup

h→0+

G(x(t + h))− G(x(t))

h .

Note that by the definition of G, we have that for t∈ [t0, t0+ ϵ], xk0(t0)

xk

0

xk(t0)

xk (or xk xk

0

xk0(t0)xk(t0)), k = 1, . . . , n + m. (25) In the following, we will show that if G(x(t0)) > 1 (i.e., xk0(t0) > xk0), then G|(6)(x(t0)) <

0. Indeed,

(i) If k0 ∈ {1, · · · , n}, then

xk0xk0(t0) xk0(t0) =

{

−γxk0(t0) + [1− xk0(t0)]

[

αk0Θ(x1(t0)) + qk0

n+m

j=n+1

βjxj(t0)

]} xk0 xk0(t0)

=−γxk0 + [1− xk0(t0)]

[

αk0Θ( xk

0

xk0(t0)x1(t0)) + qk0

n+m

j=n+1

βj

( xk

0

xk0(t0)xj(t0) )]

<−γxk0 + [1− xk0] [

αk0Θ(x1) + qk0

n+m

j=n+1

βjxj ]

(by (25), x > 0 and xk0(t0) > xk0)

= 0,

since x is an equilibrium. Hence, we have that G|(6)(x(t0)) < 0.

(ii) If k0 ∈ {n + 1, · · · , n + m}, then

xk0xk0(t0)

xk0(t0) ={−µk0xk0(t0) + rk0[1− xk0(t0)]Φ(x1(t0))} xk0 xk0(t0)

=−µk0xk0 + rk0[1− xk0(t0)]Φ( xk0

xk0(t0)x1(t0))

<−µk0xk0 + rk0[1− xk0]Φ(x1) (by (25), x > 0 and xk0(t0) > xk0)

= 0,

since x is an equilibrium. Hence, we have that G|(6)(x(t0)) < 0.

By (i) and (ii), we showed that if G(x(t0)) > 1, then G|(6)(x(t0)) < 0. By the similar argument, it can be showed that if g(x(t0)) < 1, then g|(6)(x(t0)) > 0. Moreover, if G(x(t0)) = 1, then G|(6)(x(t0)) ≤ 0, and if g(x(t0)) = 1, then g|(6)(x(t0)) ≥ 0. The proof of these assertions are omitted here since the similarity.

Define the Lyapunov candidate functions U and V in n+m by U (x) = max{G(x) − 1, 0},

V (x) = max{1 − g(x), 0}.

Then U and V are continuous and nonnegative functions in△n+m. Moreover,

By (I) and (II), the proof of Theorem 4 is complete.

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