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GLOBAL SOLUTIONS OF THE COOPERATIVE CROSS-DIFFUSION SYSTEMS
GLOBAL SOLUTIONS OF THE COOPERATIVE CROSS-DIFFUSION SYSTEMS
The Pure and Applied Mathematics. 2015. Feb, 22(1): 75-90
Copyright © 2015, Korean Society of Mathematical Education
  • Received : December 13, 2014
  • Accepted : January 27, 2015
  • Published : February 28, 2015
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SEONG-A, SHIM

Abstract
In this paper the existence of global solutions of the parabolic cross-diffusion systems with cooperative reactions is obtained under certain conditions. The uniform boundedness of W 1,2 norms of the local maximal solution is obtained by using interpolation inequalities and comparison results on differential inequalities.
Keywords
1. INTRODUCTION
This article deals with the following quasilinear parabolic system in population dynamics which is called cooperative cross-diffusion system.
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where α 12 , α 21 , d, ai, bi, ci are positive constants for i = 1, 2. The initial functions u 0 , v 0 are not constantly zero. In the system (1.1) u and v are nonnegative functions which represent the population densities of two species in a cooperative relationship. d 1 and d 2 are the diffusion rates of the two species, respectively. a 1 and a 2 denote the intrinsic growth rates, b 1 and c 2 account for intra-specific cooperative pressures, b 2 and c 1 are the coefficients for inter-specific competitions. α 11 and α 22 are usually referred as self-diffusion , and α 12 , α 21 are cross-diffusion pressures. By adopting the coefficients αij ( i , j = 1, 2) the system (1.1) takes into account the pressures created by mutually interacting species. For more details on the backgrounds of this model, the readers are refered to Okubo and Levin [7] .
Pao [8] in 2005, and Delgado et al. [4] in 2008 have obtained some results on the existence of global solutions of the elliptic cross-diffusion systems with cooperative reactions. In this paper the existence of global solutions of the parabolic cross-diffusion systems with cooperative reactions is obtained under certain conditions. To state results on the system (1.1) we use the following notation throughout this paper.
Notations. Let ­ Ω be a region in
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. The norm in Lp (Ω­) is denoted by |·| Lp(Ω­) , 1 ≤ p ≤ ∞, where | f | Lp(­Ω) = ( Ω | f ( x )| p dx ) 1/p , if 1 ≤ p ≤ ∞, and | f | L(Ω) = sup {| f ( x )| : x ∈ Ω}. The usual Sobolev spaces of real valued functions in Ω with exponent k ≥ 0 are denoted by
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, 1 ≤ p ≤ ∞. And
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represents the norm in the Sobolev space
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.
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we shall use the simplified notation ||·|| k,p for
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and |·| p for |·| Lp(Ω) . ­
The local existence of solutions to (1.1) was established by Amann [1] , [2] , [3] . According to his results the system (1.1) has a unique nonnegative solution u (·, t ), v (·, t ) in
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, where T ∈ (0,∞] is the maximal existence time for the solution u, v . The following result is also due to Amann [2] .
Theorem 1.1. Let u 0 and v 0 be in
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. The system (1.1) possesses a unique nonnegative maximal smooth solution
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for 0 ≤ t < T , where p > n and 0 < T ≤ ∞. If the solution satisfies the estimates
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then T = +∞. If, in addition, u 0 and v 0 are in
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then
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, and
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Here we state the main results of this paper. Throughout this this paper we assume the condition
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which means the inter-specific competition pressures are greater than the intra-specific cooperative pressures.
Theorem 1.2. Suppose that the initial functions u 0 , v 0 are in
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. Also assume the condition (1.2). Let ( u ( x,t ), v ( x,t )) be the maximal solution to the system (1.1) as in Theorem 1.1 Then there exist positive constant
  • M0=M0(||u0||1, ||v0||1,a1,a2,b1,b2,c1,c2)
such that
  • sup{||u(·,t)||1, ||v(·,t)||1:t∈ [0,T)} ≤M0
For the boundedness results of L 2 and W 1,2 norms of the maximal solution to the system (1.1) we assume the following condition in Theorem 1.3, Theorem 1.4
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Theorem 1.3. Suppose that the initial functions u 0 , v 0 are in
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. Also assume the condition (1.2) and (1.3). Let ( u ( x , t ), v ( x , t )) be the maximal solution to the system (1.1) as in Theorem 1.1. Then there exist a positive constant M 1 = M 1 (|| u 0 || 1 , || v 0 || 1 , di , ai , bi , ci , i = 1, 2) such that
  • sup{||u(·,t)||2, ||v(·,t)||2:t∈ [0,T)} ≤M1.
Theorem 1.4. Suppose that the initial functions u 0 , v 0 are in
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. Also assume the condition (1.2) and (1.3). Let ( u ( x , t ), v ( x , t )) be the maximal solution to the system (1.1) as in Theorem 1.1. Then there exist a positive constant M 2 = M 2 (|| u 0 || 1 , || v 0 || 1 , di , αij , ai , bi , ci , i = 1, 2) such that
  • sup{||u(·,t)||1,2, ||v(·,t)||1,2:t∈ [0,T)} ≤M2.
From the results of Theorems 1.2, 1.3 and 1.4 and the Sobolev embedding inequality we have positive constants M′ = M′ ( di , αij , ai , bi , ci , i = 1,2) M = M ( di , αij , ai , bi , ci , i = 1,2) such that for the maximal solution ( u, v ) of (1.1) with the conditions (1.2), (1.3)
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We also conclude that T = + ∞ from Theorem 1.1.
This paper is organized as follows. Section 2 provides preliminaries on differential equations and a few consequences of Gagliardo-Nirenberg interpolation inequality which are necessary for the proofs of Theorems 1.2, 1.3, and 1.4. And Sections 3, 4, and 5 present the proofs of Theorems 1.2, 1.3, and 1.4, respectively.
2. PRELIMINARIES
This section introduce the Gagliardo-Nirenberg interpolation inequality and its consequences. Also some preliminary results on the bounds and comparisons of differential equations and inequalities are provided.
Theorem 2.1 (Gagliardo-Nirenberg interpolation inequality). Let
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be a bounded domain with Ω in Cm. For every function u in Wm,r (Ω), 1 ≤ q , r ≤ ∞ the derivative Dju , 0 ≤ j < m , satisfies the inequality
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where
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for all a in the interval
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, provided one of the following three conditions :
  • (i)r≤q,
  • (ii),or
  • (iii)andis not a nonnegative integer.
( The positive constant C depends only on n, m, j, q, r, a. )
Proof. We refer the reader to A. Friedman [5] or L. Nirenberg [6] for the proof of this well-known calculus inequality.
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Corollary 2.1. There exist positive constants C,
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, and
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such that for every function u in
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Proof. n = 1, m = 1, r = 2, q = 1 satisfy the condition (ii) in Theorem 2.1. Letting j = 0 in this case the necessary condition on p, a for inequality (2.1) becomes
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From equation (2.5) if p = 4, then
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if
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then
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then if p = 2, then a = 13. Therefore we have inequalities (2.2), (2.3), (2.4).
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Corollary 2.2. For every function u in
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Proof. m = 2, r = 2, q = 1 satisfy the condition (ii) in Theorem 2.1.
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Theorem 2.2 (Young’s Inequality). If a and b are nonnegative real numbers and p and q are positive real numbers such that
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then
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The equality hold if and only if ap = bq .
Theorem 2.3 (Hölder’s Inequality). If
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are Lebesgue measurable and p, q ∈ [1,∞] are real numbers such that
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then
  • |fg|1≤|f|p|g|q.
Lemma 2.1 below presents a few basic inequalities that will be used for the computations in this paper.
Lemma 2.1. Let x ≥ 0, y ≥ 0. Then
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Proof . Inequalities (2.7), (2.8), (2.9) are simply proved.
To show inequalities (2.10), (2.11), let
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g ( x ) = 2 k−1 ( xk + yk ) − ( x + y ) k . Then
  • g′(x) =k2k−1xk−1−k(x+y)k−1.
Hence the function g ( x ) has the critical value 0 at x = y which is the minimum value if k ≥ 1, and the maximum value if 0 < k ≤ 1. Thus we obtain inequalities (2.10) and (2.11).
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Theorem 2.4 (Picard’s local existence and uniqueness theorem). If f ( x, t ) is a continuous real-valued function that satisfies the Lipschitz condition
  • |f(x, t) −f(y, t)| ≤L|x−y|
in some open rectangle R = {( x, t ) | a < x < b, c < t < d } that contains the point ( x 0 , t 0 ), then the initial value problem
  • x′ =f(x, t),x(t0) =x0
has a unique solution in some closed interval I = [ t 0 ε , t 0 + ε ] where ε > 0.
Theorem 2.5. Let f ( x ) be a real-valued differentiable functions defined on an open interval ( a , b ). Then for every initial point x 0 in ( a , b ) a solution of the initial value problem
  • x′ =f(x),x(0) =x0
is either constant or strictly monotone.
Proof . The conclusion follow from the fact that f ( x ( t )) never changes sign for the solution x ( t ) of the given initial value problem. To see why this is so, suppose that x ( t ) is not a constant solution, and f ( x ( t )) changes sign. Then it would have to be f ( x ( t 1 )) = 0 at some t 1 > 0 and f ( x ( t )) ≠ 0 for t in the left of t 1 or right of t 1 . But it contradict the fact that from Theorem 2.4 the constant solution y ( t ) ≡ x ( t 1 ) is a unique solution in some closed interval [ t 1 ε , t 1 + ε ], where ε > 0.
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Corollary 2.3. Let c 1 > 0, p > 1, and c 2 , c 3 be any real numbers. Then there exists a positive constant M = M ( x 0 , p , c 1 , c 2 , c 3 ) such that the solution of the initial value problem
  • x′= −c1xp+c2x+c3,x(0) =x0≥ 0
satisfies that
  • x(t) ≤Mfor all t≥ 0.
Proof. The function f ( x ) = − c 1 xp + c 2 x + c 3 is differentiable functions on
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and falls in either of the two cases:
  • case(a)f(x) ≤ 0 for allx≥ 0
  • case(b) there exist a positive constantm = m(p,c1,c2,c3) such thatf(m) = 0,f(x) > 0 forxin some interval on the left ofm, andf(x) < 0 for allx>M.
In case (a) x′ (0) = f ( x 0 ) ≤ 0, and thus by Theorem 2.5 x ′( t ) ≤ 0 for all t ≥ 0. Hence x ( t ) ≤ x 0 for all t ≥ 0. In case (b) if 0 < x 0 < m then the solution x ( t ) cannot cross the constant solution y ( t ) ≤ m by Theorem 2.5, and thus x ( t ) ≤ m for all t ≥ 0. If x 0 m then x′ (0) = f ( x 0 ) ≤ 0, and thus by Theorem 2.5 x ′( t ) ≤ 0 for all t ≥ 0. Hence x ( t ) ≤ x 0 for all t ≥ 0. Therefore in any case there exists a positive constant M = M ( x 0 , p , c 1 , c 2 , c 3 ) such that x ( t ) ≤ M for all t ≥ 0.
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Lemma 2.2 (Gronwall’s inequality and the Comparison Principle for differential equations). Let a < b ≤ ∞, and ξ ( t ) and β ( t ) be real-valued continuous functions defined on the interval [ a, b ]. If ξ ( t ) is differentiable in ( a, b ) and satisfies the differential inequality
  • ξ′(t) ≤β(t)ξ(t),t∈ (a,b),
then ξ ( t ) is bounded by the solution of the corresponding differential equation y ′( t ) = β ( t ) y ( t ), y ( a ) = ξ ( a ), that is,
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for all t ∈ [ a, b ]. And it follows that if in addition ξ ( a ) ≤ 0, then ξ ( t ) ≤ 0 for all t ∈ [ a, b ].
Proof. We refer the reader to [2] .
Lemma 2.3. Let c 1 > 0, p > 1, and c 2 , c 3 be any real numbers. Suppose that two differentiable functions ϕ ( t ) and x ( t ) satisfy
  • ϕ′ ≤ −c1ϕp+c2ϕ+c3,ϕ(0) =ϕ0
  • x′ = −c1xp+c2x+c3,x(0) =ϕ0.
Then
  • ϕ(t) ≤x(t)for all t≥ 0.
And especially, if ϕ 0 ≥ 0 then there exists a positive constant M = M ( ϕ 0 , p , c 1 , c 2 , c 3 ) such that
  • ϕ(t) ≤Mfor all t≥ 0.
Proof . Let ξ = ϕ − x . Then
ξ ′ = ϕ ′ − x ≤ −c1(ϕpxp) + c2(ϕx) = ξ(−c1η + c2),
where
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Here notice that η ( t ) is a continuous function using the mean value theorem and the continuities of ϕ ( t ) and x ( t ). Now, since ξ (0) = 0 we conclude that ξ ( t ) = ϕ ( t ) − x ( t ) ≤ 0 for all t ≥ 0 from Lemma 2.2. And if ϕ 0 ≥ 0, from Corollary 2.3 there exists a positive constant M = M ( ϕ 0 , p , c 1 , c 2 , c 3 ) such that x ( t ) ≤ M for all t ≥ 0. Thus ϕ ( t ) ≤ M for all t ≥ 0.
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3.L1-BOUND OF SOLUTIONS TO (1.1)
Proof of Theorem 1.2. By taking integration over the interval [0, 1] for the first and second equations in (1.1) we have that
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Let
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The condition b 1 c 2 > b 2 c 1 implies δ > 0. It also holds that
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Thus it is shown that
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from the facts
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Using (3.1) we have
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and thus
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where
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From Hölder’s inequality
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it follows that
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and thus
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where
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Hence by the Gronwall’s type inequailty in Lemma 2.3 there exists positive constant M 0 = M 0 (|| u 0 || 1 , || v 0 || 1 , a 1 , a 2 , b 1 , b 2 , c 1 , c 2 ) satisfying
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for all t ≥ 0.
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4.L2-BOUND OF SOLUTIONS TO (1.1)
Proof of Theorem 1.3. Multiplying the first and second equations in (1.1) by u = u ( x, t ) and v = v ( x , t ), respectively, and taking integrations over [0, 1] we have that
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Using Neumann boundary conditions
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and similarly
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Using condition (1.3) that
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and
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, we have
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Thus it follows from (4.1) that
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By Young’s inequality
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holds for any ε > 0. And by applying Lemma 2.1 to inequality (2.2) and using the uniform L 1 -boundedness of u and v from Step 1, we have
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where C is a positive constant depending only on a i , b i , c i ( i, j = 1, 2). Thus (4.2) becomes
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where
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and the constants
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and
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are depending on di , ai , bi , ci ( i, j = 1, 2). And by applying Lemma 2.1 to inequality (2.4) and using the uniform L 1 -boundedness of u and v from Step 1, we have
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where
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is a positive constant depending only on ai, bi, ci ( i, j = 1, 2). And thus
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where C′ is a positive constant depending only on ai, bi, ci ( i, j = 1, 2). Thus we have
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by Lemma 2.1, where C 0 , C 1 , C 2 are positive constants di, ai, bi, ci ( i, j = 1, 2). Hence by the Gronwall’s type inequailty in Lemma 2.3 we obtain the following L 2 -bound of u and v such that
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where M 1 is a positive constant depending on || u 0 || 2 , || v 0 || 2 , di, ai, bi, ci ( i, j = 1, 2).
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5.W1,2-BOUND OF SOLUTIONS TO (1.1)
Proof of Theorem 1.4. To obtain uniform bounds of | ux | 2 and | vx | 2 for the solution of (1.1) let us denote that
  • P=d1u+α11u2+α12uv,Q=d2v+α21uv+α22v2.
We would show the uniform boundedness of | Px | 2 and | Px | 2 and then obtain the uniform bounds of | ux | 2 and | vx | 2 from it. Here we note from Theorem 1.1 that
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for 0 ≤ t < T , and
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from the Neumann boundary conditions on u, v . Now, multiplying the first equation in (1.1) by Pt and the second equation by Qt , we have
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and thus
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where C 1 is a positive constant depending on di, αij, ai, bi, ci ( i, j = 1, 2). Here we notice from the condition (1.3) that there exists a positive constant λ = λ ( αi,j , i, j = 1, 2) satisfying
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since
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for all u ≥ 0, v ≥ 0, if λ = λ ( αij , i , j = 1, 2) > 0 is small enough.
The terms
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in (5.1) ae estimated in terms of P and Q from inequality (2.7) in lemma 2.1.
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Now we observe using Young’s inequality that
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hold for any ε > 0. Similar estimates are applied to the terms
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,
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,
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,
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and so on. Using these inequalities and inequalities (2.8), (2.9) in lemma 2.1 we obtain that
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where C 2 , C 3 , C 4 are positive constant depending on di, αij, ai, bi, ci ( i, j = 1, 2). Thus we have
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for any ε > 0. Here we choose a small ε > 0 so that
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and thus
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where C 5 is a positive constants depending on di, αij, ai, bi, ci ( i, j = 1, 2). Now we observe that
  • P=d1u+α11u2+α12uv≥α11u2,Q=d2v+α21uv+α22v2≥α22v2,
and thus
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where C 6 is a positive constant depending only on di, αij , ai, bi, ci ( i, j = 1, 2). Applying the inequalities (2.6) and (2.3) to the function P = d 1 u + α 11 u 2 + α 12 uv we have
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Here using the uniform boundedness of the L 1 norm of P , we have
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where C 7 , C 8 , C 9 , C 10 are positive constants depending on di, αij, ai, bi, ci ( i, j = 1, 2). Similar estimates are obtained also for Q . Hence we have
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where C 11 , C 12 , C 13 are positive constants depending on di, αij, ai, bi, ci ( i, j = 1, 2). Hence by the Gronwall’s type inequailty in Lemma 2.3 we obtain the following W 1,2 -bound of P and Q such that
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where
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is a positive constant depending on || u 0 || 2 , || v 0 || 2 , di, αij, ai, bi, ci ( i, j = 1, 2).
In order to obtain estimates for ux and vx , we notice that
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where
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Here we note that | A |, the determinant of A , is bounded below by the positive constant d 1 d 2 , and | A | is of class O ( u 2 + v 2 ) as u → ∞ and v → ∞, we have the inequality
  • |ux| + |vx| ≤C14(|Px| + |Qx|) for everyx∈ [0, 1] × [0,∞)
for some constant C 14 depending only on di, αij , ( i, j = 1, 2). Therefore we obtain the following W 1,2 -bound of u and v such that
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where M 2 is a positive constant depending on || u 0 || 2 , || v 0 || 2 , di, αij, ai, bi, ci ( i, j = 1, 2).
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References
Amann H. 1989 Dynamic theory of quasilinear parabolic equations, III. Global Existence Math Z. 202 219 - 250    DOI : 10.1007/BF01215256
Amann H. 1990 Dynamic theory of quasilinear parabolic equations, II. Reaction-diffusion systems Differential and Integral Equations 3 (1) 13 - 75
Amann H. 1993 Non-homogeneous linear and quasilinear elliptic and parabolic boundary value problems Function spaces, differential operators and nonlinear analysis (1992), Teubner-Texte Math. Friedrichroda 133 9 - 126
Delgado M. , Montenegro M. , Suárez A. 2009 A Lotka-Volterra symbiotic model with cross-diffusion J. Differential Equations 246 2131 - 2149    DOI : 10.1016/j.jde.2008.10.032
Friedman A. 1969 Partial differential equations Holt, Rinehart and Winston New York
Nirenberg L. 1959 On ellipic partial differential equations Ann. Scuo. Norm. Sup. Pisa 13 (3) 115 - 162
Okubo A. , Levin L.A. 2001 Interdisciplinary Applied Mathematics 2nd Edition Springer-Verlag New York Diffusion and Ecological Problems: Modem Perspective
Pao C.V. 2005 Strongly coupled elliptic systems and applications to Lotka-Volterra models with cross-diffusion Nonlinear Anal. 60 1197 - 1217    DOI : 10.1016/j.na.2004.10.008