Applied Mathematics, 2011, 2, 1068-1075
doi:10.4236/am.2011.29148 Published Online September 2011 (http://www.SciRP.org/journal/am)
Copyright © 2011 SciRes. AM
Positive Solutions to the Nonhomogenous p-Laplacian
Problem with Nonlinearity Asymptotic to at
Innity in
1p
u
N
Li Wang
School of Mathematics and Statistics, Huazhong Normal University, Wuhan, China
E-mail: wangli.423@163.com
Received March 20, 2011; revised June 6, 2011; accepted June 13, 2011
Abstract
In this paper, we study the following problem


2
1,
|| in ,
, 0 in ,

p
N
p
pN N
uVxuu Kxfuhx
uW u
 

(*)
where , the potential is a positive bounded function,
1pN

Vx
,
pN
hL
11
1, 1, 0, pNh
pp
 
0,h

f
s is nonlinearity asymptotical to 1
p
s
at infinity, that is,
~fs Os1p
as
s
. The aim of this
paper is to discuss how to use the Mountain Pass theorem to show the existence of positive solutions of the present
problem. Under appropriate assumptions on and , we prove that problem (*) has at least two positive
solutions even if the nonlinearity
, , hVK f

f
s does not satisfy the Ambrosetti-Rabinowitz type condition:
 
0
1
0d, 0 ,0
u
Fufssf uuu
p
 
.
Keywords: Positive Solutions, p-Laplacian, Nonlinearity Asymptotic, Mountain Pass Theorem
1. Introduction and Preliminaries
In this paper, we study the following problem
  

2
1,
in ,
, 0 in ,

p
p
pN N
uVxuu Kxfuhx
uW u
 

(1.1)
where


2
div, ,
11
1, 1, 0, 0,
ppN
puuuhL
pNh h
pp
 
 
and the function and
, VK
f
satisfy the following
conditions:

1
V
, , aA
:
N
V
, 0B
is continuous and there exist
such that

1
aVx A
x

.
1
F
,ft C
, if

0ft0.t
2
F
+1
0
lim 0
p
t
ft .
t
3
F
There exists
, 1qpp
,such that
lim 0
q
n
ft , where Np
pNp
.
t

4
F

1
+
lim 1,
p
t
ft l
t
 .
1
K
Kis a positive continuous bounded function and
there exists > 0 such that
0
R
 

0
1
sup:0 inf:.
p
fs Vx
sx
Kx
s

 R

 





Throughout this paper, we define the following
Weighted Sobolev space


1, :d
N
p
pN p
Wu uVxux




L. WANG1069
WClearly, . W is a Hilbert space with its
scalar product and norm are given by

1,
pN
W
 

21
p
,
andd ,
N
N
pp
pp
uvuu vVxuvx
uuVxux




d
because of
it is equivalent to the standard
1
V
1,
p
N
W
:IW
norm. So, We associate with (1.1) the func-
tional defined by
 
 
1d
dd






N
NN
pp
IuuVxux
p
,
K
xFu xhxux
(1.2)
where
 
0d
u
F
uftt. By
1
V and

1
K
there
exists such that
00C
 
0
K
xCVx, for all
N
x. (1.3)
Thus, I is well defined on W and with
1, ICW
 
 
21
, d
dd,






N
NN
pp
I
uvu uvVxuvx
K xfuvxhxvx
for all . We also use the notation: vW


1
d for all 1,.
N
tt
t
uux t

Under the conditions

1
F
and

2
F
, we are able to
prove
I
has a Mountain Pass geometry. Namely setting


 


0,1 ,,00,and10CW I
 
  ,
we have and



[0,1]
inf max0.
t
cIt


The value is called the Mountain Pass level
for
c
I
. Ekeland’s variational principle implies that there
exists a Cerami sequence at c, namely a sequence
such that

u
nW
 

*
and 10
as ,
nnn
W
IucI uu
n


(1.4)
where denotes the dual space of . At this point,
to get an existence result, it clearly suffices to show that
is bounded and then that
n has a strongly
convergent subsequence whose limit is a non-trivial
critical point of
*
W W

n
u u
I
. These two steps consist the heart of
the proofs of Theorems 1.1 below.
For problems like (1.1) as p = 2, in most works, the
following superlinear condition of

f
t, the so-called
Ambrosetti-Rabinowitz type condition is assumed
 
0
1
0d, 0 ,0
u
Fufssf uuu
p
 
.
(1.5)
Our equation does not satisfy (1.5) under assumption
of
4
F
. The difficulty to prove that is bounded
is linked to the fact that we are considering an non-
linearity asymptotically problem.

n
u
There are a few works on asymptotically linear prob-
lems on unbounded domains. The first result is due to
Stuart and Zhou [1]. They study a problem of the type of

, ,
N
uVxu fux  (1.6)
assuming that it has a radial symmetry. Thanks to this
assumption, the problem is somehow set in and
possesses a stronger compactness. Moreover in [2], a
problem of the form

,,
N
uKxu fxux 
is studied, where is a constant and
0K
,
f
xs
is
asymptotically linear in s and periodic in
N
x. Sub-
sequently, taking advantages of some techniques intro-
duced in [3], an extended study of radially symmetric
problems on was done in [4]. Jeanjean et al. in [5]
discussed (1.6) under some different conditions of
N
Vx and
f
u, it gives results that (1.6) has a posi-
tive solution. Recently, under the assumptions
1
V as
0
with 02
k
and is
smooth and there exist

2: :KK
0

N
,
such that

0
1x
k
Kx

, Ambrosetti et al. in [6] proved that
problem


1
in,
, 0 in , 3,

N
NN
uVxu Kxfu
uH uN
 

(1.7)
has a bound state for
p
fu u with 2
2
N
pN

and

24
, 0,
22
1, .



N
NN (1.8)
Moreover, it is also proved in [6] that, if
p
f
uu
in (1.7), then the restriction of 2
2
N
pN
 is nece-
ssary to get a ground state (i. e. a least energy solution) of
(1.7). Liu et al. in [7] showed that (1.7) has a bound state
and ground state solution if
f
is asymptotically linear
at infinity and other assumptions of and
,VK
f
.
Similar to [8,9] considered the problem
 

1
in ,
, 0, 3,
N
uu Kxfuhx
uHu N
 

(1.9)
Copyright © 2011 SciRes. AM
L. WANG
1070
with

lim
t
ft l
t
 
. It studied the problem by the
case and to obtain the multiple posi-
tive solutions in these two cases.
ll
Our result is motivated by some work on the existence
of positive solutions for asymptotically linear Schrod-
inger equations as well as by some ideas used for
bounded domain problems. Positive solutions of nonlin-
ear elliptic problems on a bounded domain have been
much studied (see, for example [3,10,11,12]). But to our
best knowledge, it seems that there few results about (1.1)
which is a p-laplacian equation with nonlinearity as-
ymptotic to 1
p
u at infinity in
N
. In this paper, we
shall extend the results of [9] to the more general case.
As is known, to seek a weak solution of (1.1) is equiva-
lent to find a nonzero critical point of
I
in , so by
the Ekeland’s variational principle [13], we can get a
weak solution 0 for
W
u
Np
hL
suitably small easily.
Moreover, 0 is the local minimizer of u
I
and
. However, under our assumptions it seems
difficult to get a second solution (different from 0) of
(1.1) by applying the Mountain Pass theorem. Since we
lose the (AR) condition, we must overcome the difficulty
of the lack of a priori bound in W for Palais-Smale se-
quences. On the other hand, once a (PS) sequence is
bounded in , it also has some difficulties to show this
sequence converges to a different solution from 0.
When , it seems difficult to get the boundness
result of , so we only discuss the case

00Iu
l
u
l
W

n
u
u

W
and obtain Theorem 1.1:
Theorem 1.1. Suppose that

pN
hL
,11
1
pp

,1,,. Let pN 0h0h
 
11 4
,VF F,

1
K
be hold and *
l
with

*infd: ,
()d1.
N
N
pp
p
uVxuxuW
Kxux

 

(1.10)
Then there exists such that problem (1.1) has
at least two positive solutions satisfying
and if
0d

1001
, uuW

00Iu Iu p
hd
.
2. Existence of Minimum Positive Solution
In this section, we prove the existence of minimum posi-
tive solution for
  

2
1,
in ,
, 0 in ,

p
N
p
pN N
uVxuu Kxfuhx
uW u


(2.1)
by Ekeland’s variational method. To this end, we need
some lemmas.
Lemma 2.1. Assume that ,
 
11 4
,VF F
1
K
with l
hold and 0p
. Let

11
, 1
pN
hL pp

and

be a bounded
n
uW
(PS) sequence of
I
.Then has a strongly conver-
gent subsequence in W.

n
u
Proof. It is sufficient to prove that for any 0
,
there exist
0
RR
(is given by
0
R
1
K
) and
0n
such that for all

RR
and
nn

{:|| }d
pp
n
xx RuVxux.


(2.2)
For given by
0
R
1
K
, define







10 0
0
0
12
,,, :sup:
12
12
,
12
p
p
R
CRaR R
RaR
R
RaR











,
(2.3)






20 0
0
0
12
(,,,):sup:
12
12
,
12
R
CRaR R
RaR
R
RaR











,
(2.4)
where ,
and are given by
a
1
V. Then, by
1
V, (2.3) and (2.4), we have, for all ,
0
RR

10
,,, for 2.R aVxR,

all 
p
RC x1 (2.5)
and

20
1,,,, for all 2.RCRaVxxR

 (2.6)
Let
:0N
Rx
,1 be a smooth function such
that

0, 0,
1, 2,
R
x
R
xxR

(2.7)
and, for some constant (independent of ),
00CR

0, for all .
R
C
xx
R
  (2.8)
Then, by (2.5), for all n
and , we have
0
RR



1
10
{: ||2}
1
10 0
dd
2d
2d
21 ,,,.
NN
N
N
pp
nRn RnR
pp
p
nRn R
p
pp
p
nn
xR xR
p
pp
n
ux uu
uu x
C
ux ux
R
CRaC u

















 




d
x
(2.9)
Copyright © 2011 SciRes. AM
L. WANG1071
This implies that

1
11
01 0
212 ,,,p
ppp
nR n
uCCRa





,u
(2.10)
for all and . By
n0
RR0p
, for any
0
,there exists such that

0
R

R


02 0
, for all ,
,,,
p
p
C
RR
CC Ra
R



(2.11)
where


1
1
1
p
p
Cp
p




 . By (1.4),

*0
nn
W
Iu u
as , so for any
n 0
, there
exists such that

0n
 

1
11
010
212 ,,,
for all.
nn
p
wppp
Iu u
CC Ra
nn





(2.12)
Hence, it follows from (2.10) and (2.12) that
 
*
,,
nnRn nR
W
Iu uIuu



(2.13)
for all

nn
and . Note that
0
RR
 











1
1
,d
d
dd
d.
N
N
NN
N
pp
nnRnnRnR
nnR nR
pp
p
nRnRn nR
nnR nR
I
uuuuVxu x
Kxfu uhxux
uVxux uux
Kxfu uhxux


 



 



(2.14)
For

RR
, using (2.6) and (2.11), we have,




02 0
20
,,
p
CC R

,
,,,,forall 2,
p
aC
RR
CRaVxxR
C



,
that is,
 
0,forall2,
p
p
CVxxR
C
R
 (2.15)
Therefore, from (2.8) and (2.15), we get, for all
and
n

RR
,


  
1
0
d
dd
dd
dd
.



N
NN
NN
NN
p
nnR
pp
p
nnR
p
pp
nn
p
pp
nn
p
n
uu x
uxC ux
C
uxC ux
R
uxC Vxu
C
u




 
 
 



x
(2.16)
By (F1), (K1) and (2.7), there exists
0,1
such
that, for all n
and
0
RR

dd.
p
nnR nR

NN
K
xfu
uVxu x
x

(2.17)
Since
N
p
hL
, and n
uC for some constant
C > 0, it follows from (2.7) there exists such
that

0
R
R
,for .
NnRRn
p
p
hxudx hxuRR


(2.18)
Combining (2.13), (2.14) and (2.16)-(2.18), for all
nn
and
RR
, we see that


 


1
|,
d
dd
d
d.

N
N
NN
N
N
pp
nnRnR nR
p
nnR
nR nR
pp
p
nR nRn
p
nR
d
I
uuuVxu x
uu x
Kxf xuxhxux
uVxuxu
Vxu x
 




 


 



That is,
 
3
d1 d
2.
NN
pp
nR nR
n
ux Vxu
uC
 


 


x
(2.19)
From
0,1
and (2.7), it is easy to see that (2.19)
implies (2.2).
In the following, we give a property of variational
functional I defined by (1.1):
Lemma 2.2. If (V1), (F1)-(F3), (K) hold,
1
pN
hx L
and
N
Kx L
. Then there exist
,, 0d
such that
0Iu
 for p
hd
.
u
Proof. It follows from (F1)-(F3) that for any 0
,
there exist
,1qpp
and such that
for all s > 0,

,Cq
0
 
1
1,
p.
q
F
ssCqs
p

 (2.20)
By the Sobolev embedding and (1.3), we have
 
 
 

 


1
0
1
0
1
45
1
45
1d
dd.
11
,d
11 d
,d
1,||
1,.
N
NN
N
N
N
pp
ppq
p
pp
q
p
pp q
p
pq
p
IuuVxux
p
KxFu xhxux
uKxuCquxCh
pp
uCVxux
pp
CCqVx uxChu
uCuCquChu
p
uCuCquCh
p













 


 






u
(2.21)
Copyright © 2011 SciRes. AM
L. WANG
1072
Taking
4
1
2Cp
and setting
 
1
5
1,
2
p
q
g
ttCq
p
 t0 for t, we see that there
exists 0
such that 0t
 
max
g
tgd

0
. Then it
follows from (2.21) that there exists
such that

|| ||0
u
Iu
 for p
hd
.
Theorem 2.1. Assume that (V1), (F1)-(F4), (K1) hold,
, ,


pN
hx L

0hx
0hx
. Let

u:BuW
 ,if p
hd
,,d
is given by
Lemma 2.2, then there exists
1,
0
p
N
uW such that



0inf:0,IuIu uB

and is a positive solution of problem (1.1).
0
Proof. Since , and
u


pN
hx L

0hx

0hx
, we can choose a function W
such that
 
d0
Nhxxx
.
(2.22)
For , we have
0t
 
 

d
dd
d0,

N
NN
N
ppp
pp
t
ItVx x
p
K
xFtxthxxx
tthx xx
p







 

for small enough. Hence
0t

0
: 0cIuuB: inf
. By the Ekeland’s vari-
ational principle, there exists
n
uB
such that



00
1
1) ,
1
2) forall .
n
nn
cIu cn
I
wIu wuwB
n

 
Then by a standard procedure, see for example [14],
we can show that is a bounded (PS) sequence of I.
Hence Lemma 2.1 implies that there exists

n
u
1,
0
p
N
uW such that
00Iu
and
.

00
0Iuc
3. Existence of Second Solution
Next we prove that problem (1.1) has a Mountain Pass
type solution. For this purpose, we use a variant version
of Mountain Pass theorem ([13] Chapter IV), which
allows us to find a so-called Cerami type (PS) sequence.
The properties of this kind of (PS) sequence are very
helpful in showing its boundedness. The following
lemma shows that I deed in (1.1) has the so-called
Mountain Pass geometry.
Lemma 3.1. Let ,
 
11 4
,VF F

1
K
be hold and
*
l
with *
given by (1.10). Then there exists
vW
with v
,
is given by Lemma 2.2, such
that
Iv 0
.
Proof. By the definition of *
and *
l
, we can
choose a nonnegative function W
such that 0


d1and
d.
p
pp
x
Vxxl


*
N
N
Kx


Therefore, by (F4) and Fatou’s lemma, we deduce that
 
1
lim It lim d
1
lim( )d
11
0.
N
N
p
pp
tt
p
t
p
Ft
K
xx
p
tt
hxtx
t
l
pp






So the lemma is proved by taking 0
vt
with
large enough.
01t
From Lemma 2.2 and Lemma 3.1, there is a sequence
n
uW such that


*
lim
 and lim10.
nnn
W
nn
cI uu

Iu

(3.1)
For this sequence
n
u, let n
n
n
u
wu
.
Clearly, n is bounded in and there is a wWwW
such that, up to a subsequence,
*
weakly in ,
a.e. in ,
strongly in () for <.

N
qN
nl
oc
W
L pqp
ww
ww
ww
n
n(3.2)
For the above w, we have the following lemma.
Lemma 3.2. Let
11 4
,VF F,
1
K
hold,
0,
pl, *
for *
given by (1.10). If
n
u
 
as , then w given by (3.2) is a
nontrivial nonnegative solution of
n
  
21, .
pp
pu
Proof.
Le
x V
The p
xuxuxlKxuu W
 
roof of this lemma is similar to that of ([
that w is nontrivial, that is
(3.3)
7]
mma 2.4). For the sake of completeness, we give a
simple proof here.
Step 1. We claim 0w
.
By contradiction, if 0w
, we claim that


1
li
n
(3.4) is tru
m supd1.
N
np
n
p
n
Kx wx
u

(3.4)
e, then it leads to a contradiction
fu
If
immediately. Indeed, since n
u, it follows from
(3.1) that
Copyright © 2011 SciRes. AM
L. WANG1073


,1
p
nn n
Iu uuo
,
that is
 



1
1
1d
1d
N
N
pnp
nn
p
n
np
n
p
n
fu
owKxw
u
fu
Kxw x
u


,
x
where, and in what follows, denotes a quantity
3.4) h

1o
. Cle
which goes to zero as n arly, this contradicts
with (3.4). Hence w
Step 1 is proved. So we
only need to prove (olds.
In fact, by

1
0 and
K
, there is a constant such
th

0,1
at
 

0
1
sup: 0inf:.
p
fs Vx
sx
Kx
s



 





R
(3.5)
This yields, for all n,


0
0
1
{:|| }
{:|| }
d
d
p
n
n
p
xx R
n
p
n
xx R1
.
u
Kx w x
u
Vxw x


(3.6)
On the other hand, since the embedding
strongly in
f

1, pB

p
LB is compact, n
ww
a subsequence,ists
0
R
W

p
LB
0
R
. Passing to
0
R
p
there ex
0
R
g
LB such that, for all n,

a.
nR
wgx0.B
By
e. in

14
,
F
F, there exists such that
60C

6
1 for all .
p
ft Ct
t (3.7)
Then, for all n,



0
6
1
6
0
a.e. in .
p
np
nn
p
n
p
R
fu
K
xwCKxw
u
CK gCB


(3.8)
Noting that a.e. in , we get
0
n
ww N


0
10 a.e. in .
np
nR
p
n
fu
K
xw B
u (3.9)
It follows from (3.8), (3.9) and the dominated con-
vergence theorem that


0
{:|| }
limd 0.
np
n
p
xx R
nn
fu
Kxw x
u

(3.10)
Hence, (3.4) is deduced from (3.6) and (3.10).
that is,
Let
Step 2. we show that w is nonnegative,
0. w

min 0,
nn
x wx
 ,
f
w

n
wx is also bounded
in W. In
u, then

 
1
,
1,
nn
p
n
Iuw x
o
u
that is,



1d1
N
pp
n
nn
p
n
fu
wKxwxo
u

 
. (3.11)
By (F),
1
0ft
for all . It follows from (3.11)
th
0t
at

lim 1wo. Thus 0a.e. in
p
w
N
x
n
n
and 0w.
Step 3. We prove w solves (3.3).
prove that for any By Lemma 3.1, it is sufficient to
0N
C
,


21
1
d
d.
N
N
pp
p
wwVxw
lKx wx


x

(3.12)
Using (3.1) and n
u, we have


1
,Iu
1
n
p
n
o
u for any
that is,

0N
C
,




21
1
1
d
d1.
N
N
pp
nn
np
n
p
n
wwVxw
fu
Kxwx o
u

x


(3.13)
Since weakly in as we see
th
n
wwW n,
at




21
1
1
d
d1.
N
N
pp
np
n
p
n
wwVxw
fu
Kxwx o
u

x


(3.14)
So, Step 3 is complete provided that


11
1dd

NN
npp
n
p
n
fu
K
.xwxlKxwx
u

(3.15)
In fact, by (3.7) and (1.3) we have




11
1
1
1
78
d
d.
N
N9
p
np
p
n
p
n
p
p
nn
fu
Kxw x
u
CVxwxCw C

(3.16)
that is,
p
p


1
1
1
p
np
p
n
p
n
fu
Kx w
u

is bounded in

1
p
N
p
L.
Copyright © 2011 SciRes. AM
L. WANG
1074
Let
0 and x



0
:
:0.
N
N
xw
xwx
 
 
Noting that
n
n
n
u
ww
u

a.e. andn
u,
then n
u a.e. in x
 . Hence by (F), we have
4



11
11
1p
n
u (3.17)
a.e. in.



pp
npp
pp
n
fu
Kxw Kxlw
x
Since a.e. in, it follows fro
that
0
n
w 0
x m (3.7)



11
1

n
11
0
0
a.e. in.



pp
p
p
n
p
u
pp
n
f
K
xw
u
x
Thus, (3.16)–(3.18) imply that
Kxlw
(3.18)




11
11
1n
p
n
u
1
weakly in.


pp
npp
pp
p
N
p
fu
Kxw Kxlw
L
. (3.19)
From and

0N
C

N
KL
, we
that
know

1
pN
KL
, then (3.19) leads to (3.15).
If
Lemma 3.3. 0p
, *
l
and

11
,VK
ld, then.3) haontrivial non-
,
ho problemy n
e solutions.
(3s no an
negativ
Proof. Since l*
isstant , there a con0
suc
f
h
that ** l

.
By the definition o *
in (1.10), thists a
t
ere ex
vW
such tha

d1
p
Kxv x
and N
*
p*
v


.

0N
C ie maySince s dense in w assume
Now, let
R > 0 be suchat
W,

0N
vC
th
supp
R
v
define
B
and

p
f d
N
p
uVxu x



:Kx
u
 
1,
0
in
d1,
N
R
pp
R
xuWB

Then, and

1,
0.
p
R
vW B
*.
p
Rvl


(3.20)
compactness of the embedding By the

1, p
0
R
WB

p
R
LB, it is nifficult to see that there
exists
ot d
1,
0
p
R
R
wW Bwith and 0
R
w
d1
N
p
R
K
xw x
such that
 
21, .
pp
p
RR R
wVxw R RR
wKxw xB

Since positive continuous
function,finition of
0
R
w
by the de
and K(x) is a
R
, we have that

20.
p
pRRR
wVxw w

From
1
V, we get

20
p
R
Vxw w
for all
0w and
R
R


1
12
0d
pp
R
Vxw .
by th
R
R R
www

Thuse strong maximum principle in [15], we
have
0, ; 0, .
R
RR
n
If
w
wxBxR
 
0uW
is a nonnegative solution of (3.3), then
integrating by parts.




1
2
|| d
R
p
pR
BwV
xw wux


1
2
2
2
1
1
d
d
dd
dd
d.
R
R
RR
RR
R
p
RR
B
R R
p
R
B
p
p
RR
RR
BB
p
pRR
R
BB
p
R
B
Kxwux
wux
ww
uSVx wwux
nn
ww
lKx wu xuS
nn
lKx wu x









Using ,0uWu
andwe may choose R > 0
large enough such that , thus the
above calculation shows that
0u
,

1d0
R
p
R
BlKxwu x
Rl
in contradiction
w). This comp
Proof of Theorem 1.1. Clearly, if
ith (3.20lete the proof.
n
u, as
3.2 and 3.3 we get a
n, from Lemmas contradic-
tion. Hence,
u is boumma
n
2.1 we see that problem (2.1) positive solution
1
uW
nded in . Then by Le
h
W
as a
with
0Iu . So, the pr
1
eorem 2.1.
4. Referenc
A. Stua S. Zhou, “A Variational Problem
Related to
oof is complete by
es
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No. 17, 1996, p
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ishing at Infinity,” Journal of the European Mathematical
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