POSITIVE SOLUTIONS FOR PREDATOR-PREY EQUATIONS WITH NONLINEAR DIFFUSION RATES
IN KVUNG AHN
1.
Introduction
In this paper, we will investigate the existence of positive solutions to the predator-prey interacting system
-
~(x, u)~u= uf(x,
u,v) -
~(x,v)~v= vg(x,u,v)
au an +
IW= 0 on an an av +
O'V= o.
in n
(1)
in a bounded region n in Rn with smooth boundary, where
~and
~
are strictly positive functions, serving as nonlinear diffusion rates, and
Ko, 0'> 0 are constants. Assume that the growth rates f,
9are Cl monotone functions. The variables
u,v may represent the pop- ulation densities of the interacting species in problems from ecology, microbiology, etc.
In [12], the solutions of the equations
{
-~u: uM(x,u,v)
-~v
- vN(x,
u,v) in n
under the boundary conditions
~:=
~:= 0 are investigated in the competition and symbiosis cases, using the monotone-iteration scheme.
For the predator-prey case, the variational approach was used in [4] for the first time.
Received June 17, 1993. Revised November 29,1993.
AMS Subject Classification 35J60.
This work was partially supported by GARC-KOSEF.
In [5], [6] and [7], necessary and sufficient conditions for the existence of positive solutions of the elliptic system
{
- dldu = uM(u,v) - d
2dv = vN(u, v)
u=v=O on 80
with constant diffusion rates have been established for all the possible cases of monotonicities associated with the functions M and N. For those works, index theory ([5], [7]) and decomposed operators ([6]) have been employed to prove the existence of positive solutions.
Therefore, the problems of the existence of positive solutions for the nonlinear interacting systems with constant diffusion rates are to a large degree solved. However, in many chemical and biological systems, the diffusion rates indeed depend on the densities u and v. Thus we need to stu.dy the readion-diffusion systemS .with no:iilinear diffusion rate from this point of view.
To attack our problem, we first give some a priori estimates on solutions to the system (1) to have the compactness of the correspond- ing operators for the nonlinear elliptic equations. We then handle the linearization to equations.
In section 2, we provide a sequence of lemmas which will be used to prove the results in section 3. In section 3, we will give suffi- cient and necessary conditions for existence of positive solutions of (1) for the predator-prey interaction. The existence of positive solutions can be characterized by the spectral· property of a certain operator of Schrodinger type.
2. Preliminaries
In this paper we will consider problems in the space X = C(fi), where n is a bounded region in Rn and let r(T) denote the spectral radius of a linear operator T.
Let I = I(x, e). Then I
EF ifand only if I E C(fi
XR+) and (Fl) I E
Clin e, fe(x,e) < ° in n x R+, and for some N
ER+, Ife(x,e)1 :5 N where (x,e)
En x [0, eo].
(F2) I(x, 0) > ° and I(x, e) < 0, where (x,e) En x (eo, 00) for some
constant eo > 0.
(F9)
f(x,~)is concave down on the set of (x, 0 where f(x, 0 < O.
Let <p = <p(x,O. Then <p
EG if and only if <p
EC(fi
XR+) and <p is Cl-function in
~which in addition satisfies
(GI)
<p(x,~) ~6 > 0 for some constant 6 and
~ ER+, x
EO.
( G
2) <p is nondecreasing and concave down in
~ ER +.
LEMMA 1.
Let f
EF and
<p EG. Then 'P J~x,u~ is decreasing in u
X,B for x EO.
Proof. We consider bounded regions OJ,
j =1,2,3, 0
1 ={x E
o : f(x,ut}
~0 and f(X,U2) > O},
O2= {x
EO:f(x,ut} <
o and f(x,u2)
~ A}, 03= {x
EO;f(x,ut} < 0 and !(X,U2) 50}.
Then 0 = 0
1U 0
2U03.
For
x E0
1or
x EO
2 ,it is easy to see the monotonicity of ~.
Suppose x
EO.Note that 'P(x,ttt> < 'P(X,U2) and
~< J(X,U2) by
3 ttl - tt2 UI - tt2
the assumptions (F3) and (G2). Since f(x, ut} s f(x, U2) 5 0, one
must have J(:c,ud . 'P(X,U2) <
~. 'P(x,u d . Therefore we have that
ttl U2 - tt2 ttl
for x
E0
3, ~'P(x,ttd -
~~= 'P(x,ud
X UI UI X U2 tt2<
O.Thus for
UI
'P X,U2
tt2 -x
E0, 'P X,tt J«x,tt» is decreasing in u.
LEMMA
2. Let P > 0 be a constant. Assume
<p EG. Also let
o 1= h
~0, h E CO(fi) where
0:'E (0,1). Consider
{
- <p(x,
u)~u+ Pu
= hon ou +
IW= 0 on 00. (2)
Then (2) has
aunique positive solution
uE C2,O(n). Moreover, the solution operator S such that u = Sh is compact in K or C(fi), where K is the positive cone ofC(n).
Proof. The positiveness of solutions to (2) for
h ~0 follows from the strong maximum principle. First we show that the nonnegative solution to (2) is unique when 0 ShE CO(fi). Let u and
't!be two distinct nonnegative solutions of (2). Without loss of generality, let minxEo(u(x)-v(x)) < O. Let u(xo)-v(xo) = minxEo(u(x)-v(x)) < O.
Assume Xo
'E00. Then by the minimality of u - v at xo, we have
a(tt-a~(xo)
SOand K[U(XO) - v(xo)] <
O.Thus the boundary condition
(4) becomes [8uJ:o) - 8vJ:o)]+I\;[u(xo)-v(xo)] < 0, which is a contradi~tion.
Thus Xo (j. an. Since u and v are solutions of (2), we have
- <p(x, u)<p(x, v
)~(u - v) + P(u<p(x, v) - Vlp(X, u» (3)
=h(x)(<pex, v) - cp(x, u))
Observe that at Xo EO, -cp(xo, u(xo»<p(xo,
v(xo»~(u(xo)-v(xo»s 0 by the minimizing property of Xo. Also we have
p.[u(xo)cp(xo, u(xo»- v(xo)cp(xo, u(xo»] < 0 since the nondecreasing function <p > 0 is con- cave down. Hence the left side of (3) is negative. Since v(xo) > u(xo) and h(xo)
~0, the right side of (3) is nonnegative, which is a contra- diction. Therefore we must have u = v.
Next we shall prove the existence of a solution. First we can show the a priori bound in a space C
2,Q(fi) of every solution to (2), where a E (0,1) and then find a fixed point of the following equation
{
-~u = :0:~)
~: + I\;U = 0 on ao.
Let u be a solution of equation (2) for x
E0, i.e., u is a fixed point of equation (4). Denote Green's function under the Robin boundary condition
:~+
1\;.= 0 by G
R.Then
( (h-PU(Y»)
u(x) = ln GR(X,y) <p(y,u(y» dy. (5) Since IIPull oo s IIhll oo by a general maximum principle, we can esti- mate:
LIGR h -<pPu I (6)
SIlGRIILn'n-t1lh - PUIlLn .8-
1< K1211hlloo8-1 = K
2l1hll oo.
{I aG
Rh - Pu I (7)
ln
aXjcp
s :"'111 h - PUIlLm L r~ < 211 h lloo 8- 1 N =Kllhll~
where N = J
1!!.::.!lm.1 and r = IIx - yll. Thus (6), (7) imply
r m-l
(8) So applying the elliptic regularity to (4) and the fact lIV'ull
oo :::;Mllhll
oo ,we have u E W
2,m(S1) where m > n and by (8)
(9) for some constant C. Since m > n, the Sobolev imbedding theorem implies
(10) where some
aE (0,1). On the other hand, the Schauder estimate ([2]) gives
lIullc2,o :::;
C1(n, a)(lIull
oo+ 6-
1·lIh - Pullc
o ). (11)Therefore lIullc2... is also bounded.
Let v E C
2,O(0) and define T : C
2,O(0) -. C
2,O(0) such that
u= Tv is a solution of (4). Then T is continuous, compact and bounded.
Therefore the Schauder fixed point theorem provides a fixed point u such that Tu = u.
The compactness of the solution operator S in C(O) such that
u=
Shfollows from (9), (10) and (11) by the Ascoli-Arula theorem.
COROLLARY.
Let P > ° and
T> ° be constants. Suppose a( x)
EC
1(0) and a(x)
~6
0> 0, Consider for a E (0,1),
{
~a(x)~u
+ Pu = h(x),
an +
TU =0, on an. (12)
Then (12) has a unique solution u in C
2(0) and the solution operator T such that u = Th is a compact operator in X = C(O).
The following is well-known. We record this to use in the proof of
other results.
LEMMA 3. Suppose a E C 1 (fi) and a(x) ;::: Co > 0 and b(x) E
£=(n). Let
T> 0 be a constant. Then there exists u > 0, u E C2(fi), such that for a unique Al > 0
{
-
a(x)~u+ b(x)u = A1U an au +
TU =0 on an.
Moreover, Al is increasing in a( x) and a ratio :~:~.
(13)
Let X be a Banach space and let F be a strongly positive nonlinear compact operator on X such that F(O)
=O.
LEMMA 4. Assume F'(O) exists with r(F'(O» > 1. H there is no p E (0,1} in any neighborhood of whi.ch. the equation u = pF'IJ,h.C!S a solution u as lIull _
00,then F has a positive fixed point u such that Fu
=u in the positive cone K of X.
Proof. See Theorem 13.2 in [1].
LEMMA 5. Let T be a compact positive linear operator on an or- dered Banacb. space. Let u > 0 be a positive element.
(i) HTu > u, then r(T) > 1 (ii) H Tu < u, then r(T) < 1 (iii) HTu = u, then r(T) = 1.
Proof. See Lemma 2.3 in [5].
LEMMA 6. Let a(x)
~Co > 0 and b(x) E £=(n). Also let P be positive constant such that P + b(x) > 0 for x E n. Then
(i)
A1(a(x)~+ b(x)) > 0 {::} r[(
-a(x)~+ P)-l(P + b(x »] > 1 (ii) A1(a(x)6. + b(x» < 0 {::} r[( -a(x)6. + P)-l(P + b(x»} < 1 (iii)
A1(a(x)~+ b(x)) = 0 {::} r[(
-a(x)~+ P)-l(P + b(x»] = 1
where Al is the first eigenvalue under Robin boundary condition.
Proof. Let <jJ > 0 be the eigenfunction corresponding to the eigen- value A1(a(x)6.+b(x)). Then
("""",a(x)~+P)<jJ= (P+b(x
»<jJ-A1(a(x)~+b(x))<jJ. So one can see that
(-a(x)~+ P)<jJ >, =, < (P + b(x))<jJ de- pending on the sign of
A1(a(x)~+b(x)).Let T:=
(-a(x)~+p)-l(p+b(x». Then T is a positive compact operator under Robin boundary
condition in C(n) by Corollary. Therefore one may apply Lemma 5 to get the results.
Consider the following equation,
{
- lp(x,
u)~u= uf(x, u)
au an +
KU =0 on an.
in 0.
(14)
Next we shalllinearize the equation (14) at
u= O. Use Lemma 2 to define the solution operator S in C(n) by Su
=ii, where ii is the unique solution of
{
- lp(x,
ii)~ii+ Pii
=uf(x, u) + Pu
ail -
0~{"\
an +
KU =on
VH.(15)
Also we define the solution operator SL of linearization by SLW = v, where
vis the unique solution of
{
-
lp(x,o)~v+ Pv = wf(x,O) + Pw
an
Qv+
KV= ° on an. (16)
LEMMA 7. The operator S is FTechet differentiable at u = 0, and S'(O) = SL.
Proof. Let ii
=Su be the unique solution of (15) and v be the
solution to (16). Assume that Ilull
oois small. Then from (15) and
(16), we have
It is easy to see that lIulloo
=O(lIulloo), and IIhlloo
=o(lIulloo) when u is small. Thus lIu - vlloo = O(lIhlloo) = o(lIulloo).
Let K = C(fi)+ be the positive cone of the ordered Banach space C(fi). We define the ordered interval [[u}, U2]]
:={u
EC(fi) :
UI ~U
~U2 for
UI,U2
EC(fin. In the next two lemmas, AI(A) denotes the first eigenvalue of an operator A under the boundary condition
~: +
KU =0.
LEMMA
8. Let I E F and e.p E G.
(i) If AI(e.p(X,O)d + l(x,O» > 0, then the equations (14) have
aunique positive solution in C2(fi).
(ii) If AI(e.p(X,O)d+ l(x,O»
~0, then
U== ° is the only nonnegative solution of (1.1,).
Proof (i) Suppose AI(e.p(X,O)d + I(x, 0» > 0.
Ifu is a positive solution of (14), then °
~u <
Coby the general maximum principle.
Choose P > 2max{suPfix[o,co]l/(x,e)l,co L}. Let [[0, CO]] denote the order interval in C(fi). We define an operator A : C(fi)
-+C(fi) by Au
=S( ul(x, u)+Pu) where S is again defined as the solution operator of the equation (2). Then A is an increasing strongly positive compact operator from [[0, CO]] to C(fi) by Lemma 2. Note that u is a positive solution of (14) if and only if
uis a fixed point of the operator A.
Itis easy to see that u == CO is an upper solution of the equation of (14).
So we have A'(u)
~u. Also note that u == ° is a solution of (14) and Lemma 7 implies that A'(u)
=A'(O)
=(-e.p(x, O)d+P)-I[f(X, O)+P].
Thus we have r(A'(O» > 1 by Lemma 6. Now applying Theorem 7.6 in [1], we have a maximal solution u in [[0, co]].
(ii) Let u be a positive solution of (14). Then we have (e.p( x, u)d + I(x,u»u
=0. This implies AI[e.p(X,u)d + I(x,u)]
=0. Then since
I
EF and
g EG, f~(~» is decreasing in u by Lemma
1.So by the last part of Lemma 3, we have AI[e.p(X,O)d+ l(x,O)] > AI[e.p(X,u)d+
I(x, u)]
=0, which is a contradiction.
Next we show that the above solution is unique. Suppose
UIand U2 are two positive solutions of (14). Let u be a maximal solution of (14).
Then
U ~ UIand
U ~ U2.IT we can show u =
UIand
U=
U2,then
Ut
= U2. Thus it suffices to show that any other positive solution
Utmust coincide with ii.. Since ii. and Ul are solutions of (14), we have .
l
[-Ul~U- - +
U~Ul]= 1- UUl [!(X,ii.) ( _) - !(x,Ud] ( )
o
0 ~x,u
~X,Ul (18)
The left integral of (18) is
fo [-Ul~ii. + ii.~Ul] = foo [-Ul: + ii. ';;: ] = foo [UlK.ii. - ii.K.Ul] = o.
Since ~ is decreasing in
Uby Lemma 1 , the right side of (18) is nonpositive. By the continuity of! and
~ g,we must have ii.
=Ul'
The following lemma is a generalization of Lemma 4 [6]. Here the diffusion rate is nonlinear. According to Lemma 8, the equation (14) has a unique positive solution. We denote it by u<p,f. Let u<pn,fn be the unique positive solution of
{
-
~n(x, u)~u= u!n(x, u)
- au an + K.U
=0 on an.
(19)
LEMMA 9.
Assume!
EF and
~EG.
(i)
(~,f)
1-+u<p,! is a continuous mapping ofG x F
-+cl,Q(n x R+) for some a
E(0,1).
(ii) H!:; ~ £; :t: !:;, for x
En, then either
U<Pl,fl> U<P2,f2 or
U<Pl,fl
== U<P2,f2 == O.
Proof. (i) The argument is similar to that in Lemma 4 [6]. Here we just give a simple modification for the uniform boundedness of {u<pn,fn}' Note that since fn
-+f and
~n -+ ~,there exists K > 0 such that
lI u<pn,fnfn(x,
u<pn,!n)+ PU<pn,fn 1100 :5 K
Therefore, as in the proof of Lemma 2 with h n
=u<pn,fnf(x,u<pn,fn) +
PU<pn,fn' we have
lIu<pn,fnllw2.m(0):5 N by (9), and so there exists a
subsequence {u<pn,fn} such that
u<pn,!n ~U in W
2,m(n).Also we have
by the Sobolev imbedding theorem,
lIu<pn,fnIIcl, .. (o):5 M where M is
a positive constant. Thus there exists a subsequence of
{u<pn,fn},say
{U'Pn,fn}
again, such that
u'Pn,fn -+ itin Cl,a(fi) for some a E (0,1).
As in the proof of Lemma 2, we conclude that
itis a solution. Then the positiveness of
u'Pn,fnimplies
it> 0. So by the uniqueness of solution,
it=
u'P,f.Therefore
u'Pn,fn -+ u'P,fin Cl,a(fi).
(ii) Suppose .h.
'Pl> h...
'P2If we assume .xl(CPl(X,O)~ + Il(X, 0» <
-0, then by Lemma 8,
U'Pl,ft==
u'P2,h== 0. SQ suppose
.xl(CPl(X,O)~+
f
1(0» x, >. ° Th en
U'Pl,h> . ° S· lnce
-uUA =
U'Pl(Z,U)ft(Z,u)>
- U'P2 Z,U 'h z,u)u'P2,h
is a lower solution of (14). Also note that
U=
Cois an upper solution. Thus there exists a solution
'itof (14) such that
u'P2,h :::;'it :::; Co.
By the uniqueness of positive solution of the equation (14),
'it=
u'P1>ft.So we have
u'P1>ft ;::: u'P2,h.Apply the strong maximal principle to get
U'Pl,fl>
u'P2,h.3. Existence Theorem
for u,v > 0 for u,v > 0 on ail
!,,(x,U,v) < °
g,,(x,u,v) < °
In this section, we consider the system (1):
-CP(x,u)~u
= u!(x,u,v)
-~(x,v)~v
=vg(x,u,v)
au \
an +KU =0 an av +uv = 0
For the predator-prey interaction, we make the following assump- tions on the system.
(HI) !,
9E Cl(fi
XR+
xR+) satisfy
{
!u(x,u,v) < 0 gu(x,u,v) > 0
Moreover, lv, gu f. 0 and all partial derivatives are uniformly bounded on fi
XR+
XR+.
(H2) There exist positive constants Cl, C
2such that
{
l(x,u,O) < 0 for
U> Cl g( x, 0, v) < 0 for v > C
2g(x, Cl, C
2 )< 0
(20) (H3) Let cp(x,u), t/J(x,v) E C(n x R+) and 'P(x,'), t/J(x,') E G.
The assumption (H!) describes how these species u, v interact with each other, while the assumption (H2) indicates that the model under consideration is logistic.
Let Al,.. (A), Al,a(A) denote the first eigenvalues of an operator A under the boundary conditions :~ +
K'= ° and :~ + a· = 0, respec-
tively.
By Lemma
8,if Al, ..('P(x,0)6 + j(x,O,O)) > ° where j
EF and
'P E
G, then the equation
{
-
cp(x,u)~u= uj(x,u,O)
au an +
KU =° on an
has a unique positive solution. Denote this positive solution by
UQ.Similarly, if
Al,a(t/J(X,O)~+g(x,O,O))> ° where 9
EF and t/J
EG,
then
{
- t/J(x,v)6v
=vg(x,O,v)
an av + av
=° on an
has a unique positive solution
VQ.According to the Lemma 9, we may define the operator T : C(n)
---+C(n) as follows. For v
EC(n), by Lemma 8, u
=Tv is the unique positive solution to the equation
{
- 'P(x,
u)~u= uj(x, u, v)
an au +
KU =° on an
if Al,..('P(x,0)6 + j(x,O,v)) > ° where j
EF and cp
EG.
REMARK.
By Lemma 9, it is easy to see that T is a continuous operator and T is strictly monotone. In case that u is a prey for v, T is decreasing in
v.Replacing u by Tv in the other equation, we have
{
-
t/J(x,v)~v= vg(x,Tv,v)
- - + an av av = ° on an
According to Lemma 2, we define the operator A : C(n)
-+C(n) by considering the equation
{
- 'l/J(x,w)t:.w + Pw
=vg(x,Tv,v) + Pv
aw an +
qW= ° on an. (21)
We denote it by w = Av = (-'l/J(x,·)t:.· +p.)-l[vg(X, Tv, v) + Pv]
where P is constant. Note that the operator A has a fixed point
vin the positive cone K if and only if (Tv, v) is a nonnegative solution of (1).
THEOREM
1. Assume that (H1)-(H3) hold. If >"l,D'('l/J(X,O)t:. + g(x, uo,O» > 0, then A has
apositive fixed point in K.
Proof To show this, we apply Lemina 4. Denote Ae = 8A. IT Ae(ve)
=Ve, 8
E(0,1], ve
EK, then we have
-'l/J(x, ~)t:.ve
=8veg(x,Tve,ve) + (8 -l)Pve. (22) Suppose ve t=
0.Let ve( xo) = maxxEo ve(x) > ° for some
Xo En.
Then
Xomust be in n by the boundary condition of (21), and at
Xothe left side of (22) is nonnegative and (8 - l)Pve(xo)
~0. Thus we must have g( Xo, Tve( xo), ve(xo» 2: 0. Suppose u, v are prey and predator, respectively. Since g( x, Tv, v)
~g( x , Cb v) in v E K where Cl is a priori bound for u, we have ° S g(xo, Tve(xo), ve(xo» S g(xo, Cb ve(xo». Thus by the assumption (H2), ve(xo) S C
2 •Thus there is an a priori bound for the positive fixed points of Ae. Next observe A'(O)
=(-'l/J(x, O)t:. + P)-l(g(x, Uo, 0) + P) by Lemma 7, where (-'l/J(x,O)t:. + P)-l is a linear operator under boundary con- dition :~ +
q. =0. Since >"l,D'('l/J(X,O)t:. + g(x,uo,O» > 0, Lemma 6 implies r(A'(O» > 1. Note that A is strongly positive compact opera- tor from C(n) to C(n) by Lemma 2. Thus A has a positive fixed point v in K by Lemma 4.
THEOREM
2. Suppose the conditions (H1)-(H3) hold.
(a) If >"l,K(cp(X,O)t:. + !(x,O,O» SO, then (1) has no positive solu-
tion.
(b) Suppose
A1,u(1/1(X,0)~+ g(x,O,O» > 0. (therefore there exists a solution (0, vo) with Vo > 0.) Then the system (1) has a positive solution if and only if Al,,,(CP(X,
o)~+ f(x, 0, vo» > 0.
(c) Suppose
A1,u(1/1(X,0)~+g(x,0,0»:$0. Then the system (1) has a positive solution if and only if Al,,,(CP(X,
O)~+ f(x, 0, 0» > ° (thus
there must be a solution (uo,O) with Uo > 0) and
A1,.,.(1/1(X,0)~+ g(x, Uo, 0» > 0.
Proof. (a) Suppose (u, v) is a positive solution of the system (1).
Then u t ° and (cp( x,
u)~+ f( x, u, v»u = O. As in the proof of Lemma 8 (ii), Lemma 1 and Lemma 3 implies
A1,,,(CP(X,0)~+ f(x,O,O» >
A1,,,( cp( x,
u)~+ f(x, u, 0» > Al,,,(cp(x,
u)~+ f(x, u, v») = 0, a contra- diction. Thus the system has no positive solution.
(b) (<=) Since
A1,.,.(1/1(X,0)~+g(x,uo,0»>
A1,u(1/1(X,0)~+g(x,0,0» > 0, A has a positive fixed point v in K by Theorem 1. Note that u
=Tv > ° because if Tv == 0, then by uniqueness, Vo
=v.
But
Al,,,(CP(X,O)~+ f(x,O,vo» > ° implies Tv = Tvo > 0, a con-
tradiction. Therefore (Tv, v) is a positive solution of the system (1).
(=}) Let (u,v) be the positive solution of (1). Since g(x,u,v)
~g(x,O,v), we have
-1/1(x,vo)~vo:$vOg(x,u,vo). So Vo is a lower so- lution of -1/1(x,
v)~v= vg(x, u, v). Thus Vo
:$v. So we have ° =
A1,,,(CP(X,
u)~+ f(x, u, v» < Al,,,(CP(X,
O)~+ f(x, 0, v») < Al,,,(CP(X, 0)
~
+ f(x, 0, vo». Therefore A1,,,(cp(x,
O)~+ f(x, 0, vo» > 0.
(c) Again, since A1,.,.( 1/1(x,
O)~+ g(x, Uo, 0» > 0, there exists a fixed point v of A by Theorem 1. Then u = Tv > ° since if Tv == 0,
then v = Vo. Thus, by using Lemma 1 and Lemma 3, we have
°
= A1,u(1/1(X,v)~+ g(x,O,v» :::;
A1,.,.(1/1(X,0)~+ g(x,O,O» :::; 0, a contradiction. For the necessity, let u be a positive solution with v = v of the system (1). If v = 0, then u = Uo. If v > 0, then Uo > u by the monotonicity of T. (See Remark.) Thus we have uo
~u > O.
If
A1,,,(CP(X,0)~+ f(x,O,O» :::; 0, we have a contradiction by (a). If A1,u( 1/1( x,
O)~+ g( x, Uo, 0»
:$0, then °
=A1,u( 1/1( x,
v)~+ g( x,
tt,v» <
A1,u(1/1(x, 0) + g(x, u, 0» < A1,u(
~(x,0) + g(x, Uo, 0» :::; 0, a contradic- tion again.
References
1. H. Amann, Fixed point equations and nonlinear eigenvalue problems in ordered Banach spaces,SIAM Rev. 18 (1976), 620-709.
2. D. Gilharg and N. Trudinger, Elliptic partial differential equations of second order, Springer-Verlag, New York (1983).
3. J.A. Goldstein and C-Y Lin, Singular parabolic boundary value problems in one space dimension, J.of Differential Equations 68 (1987),429-443.
4.C. Keller andR. Lui, Ezistence of steady-state solutions to predator-prey equa- tions in a heterogeneous environment,J. Math. Anal. Appl. 123 (1987),306-326.
5. L. Li, Coexistence theorems of steady-state for predator-prey interacting sys- tems, Trans. Amer. Math. Soc. 305 (1988), 143-166.
6. L. Li and A. Ghoreishi, 281-295, J. Appl. Anal. 14(4) (1991).
7. L. Li and R. Logan, Positive solutions to general elliptic competition models, J.of Diff.&;Integ Eqs. 4 (1991), 817-834.
8. C.·Y. Lin, Degenerate nonlinear parabolic boundary value problems, Nonlinear Analy. Theory, Methods&;Appl. 13(11) (1989), 1303-1315.
9. G. F. Roach, Green's junctions, Van Nostrand Reinhold Company (1970).
10. J. Smoller,Shock waves and reaction-diffusion equations, Springer-Verlag, New York (1983).
11.J. Wloka,. Partial differential equations, Cambridge University Press (1987).
12.KoZygourakisand R. Aris, Weakly coupled systems of nonlinear elliptic bound- ary value problems, Nonlinear Anal. 6(6) (1982), 555-569.