1. Introduction
Let
x0 ∈ [0,2
π) and
k ∈
N be fixed. We consider the following two-point boundary value problems:
()
()
where
h ∈
L1(0,2
π) is given and
g : (0,2
π) ×
R →
R is a Caratheodory function; that is,
g(
x,
u) is continuous in
u ∈
R, for a.e.
x ∈ (0,2
π), is measurable in
x ∈ (0,2
π) for all
u ∈
R, and satisfies, for each
r > 0, the fact that there exists an
ar ∈
L1(0,2
π) such that
()
for a.e.
x ∈ (0,2
π) and all |
u| ≤
r. Concerning the growth condition of the nonlinear term
g to (
1) and (
2), we assume that
- (H)
there exist constants −1 < β ≤ 0, r0 > 0, and a, b, c, d ∈ L1(0,2π), a, b ≥ 0 and a(x) ≤ 2k + 1 for a.e. x ∈ (0,2π) with strict inequality on a positive measurable subset of (0,2π), such that for a.e. x ∈ (0,2π) and all u ≥ r0
()
-
and for a.e. x ∈ (0,2π) and all u ≤ −r0
()
- (G)
there exist constants −1 < β ≤ 0, r0 > 0, and a, b, c, d ∈ L1(0,2π), a, b ≥ 0 and a(x) ≤ 2k − 1 for a.e. x ∈ (0,2π) with strict inequality on a positive measurable subset of (0,2π), such that for a.e. x ∈ (0,2π) and all u ≥ r0
()
-
and for a.e. x ∈ (0,2π) and all u ≤ −r0
()
respectively, and a generalized Landesman-Lazer condition
()
for all
v ∈
N(
L)\{0}, may be satisfied. Here
N(
L) denotes the subspace of
L1(0,2
π) spanned by sin
kx and cos
kx,
β ∈
R,
, and
. Under assumptions and either with or without the Landesman-Lazer condition
()
for all
v ∈
N(
L)\{0}, the solvability of the problem (
1) has been extensively studied if the nonlinearity
g(
x,
u) has at most linear growth in
u as |
u| →
∞ (see [
1–
13] for the case
x0 = 0 and [
14–
16] for the general case) or grows superlinearly in
u in one of directions
u →
∞ and
u → −
∞ and may be bounded in the other (see [
8,
17] for the case
x0 = 0 and [
14] for the general case when
k = 0). Based on the well-known Leray-Schauder continuation method (see [
18,
19]), we obtain solvability theorems to (
1) (resp., (
2)) when
g(
x,
u) satisfies (
H) (resp., (
G)) and either (
8) with −1 <
β < 0 or (
9) with
β = 0 is satisfied, which extends the results of [
15] for the nonresonance case, and has been established in [
9] for the case
x0 = 0 and
g(
x,
u) grows sublinearly in
u as |
u| →
∞ with −1 <
β ≤ 1. Unfortunately, it is still unknown when
k ∈
N,
g(
x,
u) grows linearly in
u as |
u| →
∞ and the assumption of (
8) is replaced by
()
for all
v ∈
N(
L)\{0} with
β > 0. In the following we will make use of real Banach spaces
Lp(0,2
π),
C[0,2
π] and Sobolev spaces
W2,1(0,2
π) and
H1(0,2
π). The norms of
Lp(0,2
π),
C[0,2
π] and
H1(0,2
π) are denoted by
and
, respectively. By a solution of (
1), we mean a periodic function
u :
R →
R of period 2
π which belongs to
W2,1(0,2
π) and satisfies the differential equation in (
1) a.e.
x ∈ (0,2
π).
2. Existence Theorems
For each v ∈ W2,1(0,2π) with v(0) − v(2π) = v′(0) − v′(2π) = 0 and k ∈ N, we write , , and v⊥ = ∑0≤j≠kPjv. Here Pjv denotes the projection of v on the eigenspace of d2/dx2 spanned by sinjx and cosjx for j ∈ N ∪ {0}. Just as an application of [11, Lemma 2] or [1, Lemma 2.2], we can modify slightly the proof of [15, Lemma 1] to obtain the next lemma.
Lemma 1. Let k ∈ N ∪ {0} and Γ be a nonnegative L1(0,2π)-function such that for a.e. x ∈ (0,2π), Γ(x) ≤ 2k + 1 with strict inequality on a positive measurable subset of (0,2π). Then there exists a constant K1 > 0 such that
()
whenever
p ∈
L1(0,2
π) with 0 ≤
p(
x) ≤
Γ(
x) for a.e.
x ∈ (0,2
π) and
u ∈
W2,1(0,2
π) is a periodic function of period 2
π with
u(0) −
u(2
π) =
u′(0) −
u′(2
π) = 0.
Proof. Just as in [20, Lemma 1], we can modify slightly the proof of [11, Lemma 2] or [1, Lemma 2.2] to obtain the fact that there exists a constant K1 > 0 such that
()
whenever
p ∈
L1(0,2
π) with 0 ≤
p(
x) ≤
Γ(
x) for a.e.
x ∈ (0,2
π) and
u ∈
W2,1(0,2
π) with
u(0) −
u(2
π) =
u′(0) −
u′(2
π) = 0. Let us extend
u(
x) and
p(
x) 2
π periodically in
x to all of
R and then use the same notations for the periodic extensions as for the original functions. In this case, we have
and
()
Since
,
p(
x) ≥ 0 for a.e.
x ∈ (0,2
π), and
for all
v,
w ∈
W2,1(0,2
π) with
v(0) −
v(2
π) =
v′(0) −
v′(2
π) = 0 and
w(0) −
w(2
π) =
w′(0) −
w′(2
π) = 0, we have
and
()
Combining (
12) with (
13), we have
()
Lemma 2. Let k ∈ N and Γ be a nonnegative L1(0,2π)-function such that for a.e. x ∈ (0,2π), Γ(x) ≤ 2k − 1 with strict inequality on a positive measurable subset of (0,2π). Then there exists a constant K2 > 0 such that
()
whenever
p ∈
L1(0,2
π) with 0 ≤
p(
x) ≤
Γ(
x) for a.e.
x ∈ (0,2
π) and
u ∈
W2,1(0,2
π) is a periodic function of period 2
π with
u(0) −
u(2
π) =
u′(0) −
u′(2
π) = 0. Here
and
for each
v ∈
W2,1(0,2
π) with
v(0) −
v(2
π) =
v′(0) −
v′(2
π) = 0.
Theorem 3. Let k ∈ N ∪ {0} and g : (0,2π) × R → R be a Caratheodory function satisfying (H). Then for each h ∈ L1(0,2π) problem (1) has a solution u, provided that either (8) with −1 < β < 0 or (9) with β = 0 holds.
Proof. Let α ∈ R be fixed and 0 < α < 2k + 1. We consider the boundary value problems
()
for 0 ≤
t ≤ 1, which becomes the original problem when
t = 1. Since 0 <
α < 2
k + 1, we observe from Lemma
1 that (
17) has only a trivial solution when
t = 0. To apply the Leray-Schauder continuation method, it suffices to show that solutions to (
17) for 0 <
t < 1 have an a priori bound in
H1(0,2
π). To this end, let
θ :
R →
R be a continuous function such that 0 ≤
θ ≤ 1,
θ(
u) = 0 for |
u| ≤
r0, and
θ(
u) = 1 for |
u| ≥ 2
r0. We define
,
()
and
g2(
x,
u) =
g(
x,
u)
−
g1(
x,
u). Then
g1,
g2 : (0,2
π)
×
R →
R are Caratheodory functions, such that for a.e.
x ∈ (0,2
π) and
u ∈
R,
u ≠ 0
()
()
If
u is a possible solution to (
17) for some 0 <
t < 1, then using (
19), (
20), and Lemma
1, we have
()
which implies that
()
for some constants
C1,
C2 > 0 independent of
u. It remains to show that solutions to (
17) for 0 <
t < 1 have an a priori bound in
H1(0,2
π). We argue by contradiction and suppose that there exists a sequence {
un} of periodic functions with period 2
π and a corresponding sequence {
tn} in (0,1) such that
un is a solution to (
17) with
t =
tn and
for all
n. Let
; then
for all
n ∈
N, and by (
22) we have
as
n →
∞. Since
and
for all
n ∈
N, we have a bounded sequence {
Pkvn} in
H1(0,2
π). For simplicity, we may assume that
vn converges to
v in
H1(0,2
π) for some
v ∈
N(
L) with
. In particular,
vn →
v in
C[0,2
π]. Clearly,
v(·−
x0) ∈
N(
L) and
. It follows that
un(
x) →
∞ for each
x ∈
R with
v(
x) > 0, and
un(
x)→−
∞ for each
x ∈
R with
v(
x) < 0. Since
and
, we have
()
Multiplying each side of (
17) by
Pkvn(
x −
x0), and then integrating them over [0,2
π] when
u =
un and
t =
tn, we get
()
By (
19) and the assumption of −1 <
β ≤ 0, we have
()
for a.e.
x ∈ (0,2
π). Combining (
22) with (
25), we get that
is bounded from below by an
L1(0,2
π)-function independent of
n. By (
20) and the assumption of −1 <
β ≤ 0, we have
()
for a.e.
x ∈ (0,2
π), In particular,
is bounded from below by an
L1(0,2
π)-function independent of
n, which implies that
is also so,
, and
()
for all
n ∈
N with
un(
x −
x0) ≠ 0. Here sign(
w) = 1 if
w > 0, sign(
w) = 0 if
w = 0, and sign(
w) = −1 if
w < 0. Applying Fatou’s lemma to the integral
, we have
()
which is a contradiction when either (
8) with −1 <
β < 0 or (
9) with
β = 0 is satisfied. Hence, the proof of this theorem is complete.
By slightly modifying the proof of Theorem 3, we can apply Lemma 2 to obtain an existence theorem to (2) when condition (H) is replaced by (G) and either (8) with −1 < β < 0 or (9) with β = 0 is satisfied, which has been established in [20] for the case x0 = 0 when (9) with β = 0 is satisfied and in [9] for the case x0 = 0 when (8) with β = −1 is satisfied.
Theorem 4. Let k ∈ N and g : (0,2π) × R → R be a Caratheodory function satisfying (G). Then for each h ∈ L1(0,2π) problem (2) has a solution u, provided that either (8) with −1 < β < 0 or (9) with β = 0 holds.
Conflicts of Interest
There are no conflicts of interest involved.