
Schechter Minimax Systems and Critical Point Theory (Springer, 2009)
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11. Fucˇ´ık Spectrum: Resonance |
Proof of Theorem 11.1. By (11.9) and (11.61), we have |
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(11.62) |
2P(x, t) ≤ W0(x), x , t R. |
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In view of Lemma 11.8, this implies |
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(11.63) |
G(u) ≥ −2 |
P(x, u)dx ≥ −B0 = − W0(x)dx, u S,1. |
I claim that |
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(11.64) |
G(v) → −∞ as v → ∞, v N −1. |
Assume this for the moment. Then there is an R > 0 sufficiently large that (3.4) holds with A = N −1 ∩ ∂ BR and B = S,1. Moreover, for this choice of A and B, A links B [hm] by Lemma 11.10. We can now apply Theorem 3.4 to conclude that there is a
sequence {uk } D such that |
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(11.65) |
G(uk ) |
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c, |
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(1 |
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uk |
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D )G (uk ) |
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0, |
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+ |
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and from (11.56) we readily estimate c by |
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(11.66) |
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−B0 ≤ c ≤ B1. |
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From (11.65) we find |
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(11.67) |
I (uk , a, b) − 2 |
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P(x, uk )dx →c, |
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(11.68) |
I (uk , a, b) − ( p(·, uk ), uk ) →0, |
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(11.69) |
(I (uk , a, b), v) |
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2( p( , uk ), v) |
→ |
0, |
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Assume that |
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(11.70) |
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ρk = uk D → ∞, |
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and let u˜k = uk /ρk . Then u˜k D =2 |
1. Thus, there is a renamed subsequence such that |
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u˜k → u˜ weakly in D, strongly in L |
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( ), and a.e. in . As a consequence, (11.59) and |
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(11.68) imply |
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(11.71) |
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b u+ 2. |
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˜ |
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This shows that u˜ ≡ 0. Moreover, (11.69) implies |
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(11.72) |
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(u, a, b) |
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Thus, u˜ is a solution of (11.5) and satisfies |
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(11.73) |
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I (u˜, a, b) = 0. |
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11.3. Existence |
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137 |
If we combine this with (11.71), we see that u˜ D = 1. |
Consequently, u˜k → u˜ |
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strongly in D. Combining (11.67) and (11.68), we obtain |
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(11.74) |
H (x, uk) dx → −c. |
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Let ± = {x : ±u˜(x) > 0}, 0 = {x : u˜ (x) = 0}. Then uk (x) → ±∞ for x ±. By (11.9) and (11.13),
−c = lim H (x, uk) dx
≤H+(x) dx
+
+H−(x) dx
−
+W0(x) dx
0
< − B1,
contradicting (11.66). Thus, (11.70) does not hold. Once we know that the sequence {uk } is bounded in D, we can use standard techniques [122] to obtain a solution of
(11.75) G(u) = c, −B0 ≤ c ≤ B1, G (u) = 0,
which is a solution of (11.2).
It thus remains to prove (11.64). Let {vk } N −1 be a sequence such that ρk =vk D → ∞. Let v˜k = vk /ρk . Then v˜k D = 1 and there is a renamed subsequence
such that v˜k → v˜ in D and a.e. in . Since |
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(11.76) |
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|F(x, t)| ≤ C(t2 + |t|) |
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by (11.7), we have |
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(11.77) |
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|F(x, vk )/ρk2| ≤ C(v˜k2 + |v˜k |/ρk ) |
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and, consequently, |
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(11.78) |
2 |
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+ 2 |
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k → |
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by (11.6). This means that |
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G(vk )/ρk2 |
= v˜k 2D − 2 |
F(x, vk )dx/ρk2 |
→ v˜ 2D − a v˜− 2 − b v˜+ 2
≤(λ −1 − a) v˜− 2 + (λ −1 − b) v˜+ 2.
Since both a and b are greater than λ −1, this will always be positive since v˜ ≡ 0. Thus, (11.64) holds, and the proof of Theorem 11.1 is complete.
138 |
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11. |
Fucˇ´ık Spectrum: Resonance |
Proof of Theorem 11.2. By (11.15) and (11.61) we have |
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(11.79) |
−2P(x, t) ≤ W0(x), |
x , t R. |
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Consequently, |
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(11.80) |
G(u) ≤ −2 |
P(x, u) dx ≤ B0, |
u S,2. |
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Moreover, I claim that |
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(11.81) |
G(w) → ∞ as w → ∞, w M . |
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Assuming this, we note that there is an R > 0 sufficiently large that |
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(11.82) |
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≤ A |
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sup G |
inf G |
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where A = M ∩ ∂ BR and B = S,2. This is not quite (3.4). To correct the situation, we let G1 = −G. Then (11.82) becomes
(11.83) |
sup |
G1 ≤ |
inf G |
1. |
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A |
B |
We know from Lemma 11.11 that A links B [hm]. Consequently, we may apply Theorem 3.4 to conclude that there is a sequence {uk } D such that (11.65) holds with G replaced by G1. Now c satisfies the estimates
(11.84) |
inf |
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≤ c ≤ sup G1 |
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M∩BR |
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(11.85) |
inf |
G ≤ −c ≤ sup G. |
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BR |
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By (11.14), (11.56), and (11.80), we see that c satisfies (11.66) as well. Thus, for the given sequence, (11.65), (11.67)–(11.69) hold with c replaced by −c, while c satisfies (11.66). If we assume that (11.70) holds, we can reason as in the proof of Theorem 11.1 that there is a renamed subsequence of {u˜k } converging in D to a function u˜ D and a.e. in . Moreover, the function u˜ satisfies (11.72) and (11.73). Also, (11.74) holds with c replaced by −c. But then (11.15) and (11.16) imply
(11.86)
c = lim H (x, uk)dx ≥ |
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H+(x)dx + |
H−(x)dx − W0(x) dx > B1. |
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0 |
This contradiction shows that the ρk are bounded, and we can now employ standard techniques to obtain a solution of
(11.87) |
G(u) = c1, −B1 ≤ c1 ≤ B0, G (u) = 0. |
This produces the desired result.
11.4. Notes and remarks |
139 |
It therefore remains only to prove (11.81). Let {wk } M be a sequence such that
ρk = wk D → ∞. Let w˜ k = wk /ρk . Then we have w˜ k D |
1, and there is a |
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= 2 |
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renamed subsequence such that w˜ k → w˜ weakly in D, strongly in L |
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(11.88) |
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a w− 2 |
b w+ 2. |
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k → |
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Consequently, |
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G(wk )/ρ2 |
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≥ |
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− ˜ D |
+1 − |
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+1 − |
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which is positive since both a and b are less than λ +1. This completes the proof of the theorem.
11.4 Notes and remarks
The presentation given here is from [124]. Further work was done in [102].
Chapter 12
Rotationally Invariant Solutions
12.1 Introduction
In this chapter (and the next) we study periodic solutions of the Dirichlet problem for the semilinear wave equation. In this chapter we study radially symmetric solutions for the problem
(12.1) |
u := utt − u = f (t, x, u), |
t R, x BR , |
(12.2) |
u(t, x) = 0, t R, x ∂ BR, |
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(12.3) |
u(t + T, x) = u(t, x), t R, x BR, |
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where |
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(12.4) |
BR = {x Rn : |x| < R}. |
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In this case we have |
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f (t, x, u) = f (t, |x|, u), |
x BR. |
Our basic assumption is that the ratio R/ T is rational. Thus, we can write
(12.5) 8R/ T = a/b,
where a, b are relatively prime positive integers. We show that
(12.6) n ≡ 3 (mod(4, a))
implies that the linear problem corresponding to (12.1)–(12.3) has no essential spectrum. If
(12.7) |
n ≡ 3 |
(mod(4, a)), |
then the essential spectrum of the linear operator consists of precisely one point:
(12.8) |
λ0 = −(n − 3)(n − 1)/4R2. |
M. Schechter, Minimax Systems and Critical Point Theory, DOI 10.1007/978-0-8176-4902-9_12, © Birkhäuser Boston, a part of Springer Science+Business Media, LLC 2009
142 |
12. Rotationally Invariant Solutions |
This shows that the spectrum has at most one limit point. We can then consider the nonlinear case
(12.9) |
f (t, r, s) = μs + p(t, r, s), |
where μ is a point in the resolvent set, r = |x|, and |
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(12.10) |
| p(t, r, s)| ≤ C(|s|θ + 1), s R, |
for some number θ < 1. Our main theorem is
Theorem 12.1. If (12.6) holds, then (12.1)–(12.3) has a weak rationally invariant solution. If (12.7) holds and λ0 < μ, assume, in addition, that p(t, r, s) is nondecreasing in s. If μ < λ0, assume that p(t, r, s) is nonincreasing in s. Then (12.1)–(12.3) has a weak rotationally invariant solution.
Our proof of this theorem will make use of Theorem 10.2. For the definition of essential spectrum, cf., e.g., [126] and [106].
12.2 The spectrum of the linear operator
In proving Theorem 12.1, we shall need to calculate the spectrum of the linear operatorapplied to periodic rotationally symmetric functions. Specifically, we shall need
Theorem 12.2. Let L0 be the operator
(12.11) |
L0u = ut t − urr − r −1(n − 1)ur |
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applied to functions u(t, r ) in C∞( ) satisfying |
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(12.12) |
u(T, r ) = u(0, r ), ut (T, r ) = ut (0, r ), 0 ≤ r ≤ R, |
(12.13) |
u(t, R) = u R (t, 0) = 0, t R, |
where = [0, T ] × [0, R]. Then L0 is symmetric on L2( , ρ), where ρ = r n−1. Assume that 8R/ T = a/b, where a, b are relatively prime integers [i.e., (a, b) = 1]. Then L0 has a self-adjoint extension L having no essential spectrum other than the point λ0 = −(n − 3)(n − 1)/4R2. If n ≡ 3 (mod(4, a)), then L has no essential spectrum. If n ≡ 3 (mod(4, a)), then the essential spectrum of L is precisely the point λ0.
Proof. Let ν = (n − 2)/2 and let γ be a positive root of Jν (x) = 0, where Jν is the Bessel function of the first kind. Set
(12.14) |
ϕ(r ) = Jν (γ r/ R)/r ν . |
Then |
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(12.15) |
ϕ + (n − 1)ϕ /r = (x2 Jν + x Jν − ν2 Jν )/r ν+2 = −γ 2 Jν / R2. |
12.2. The spectrum of the linear operator |
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(12.16) |
ψ(t, r ) = ϕ(r )e2π ikt/ T , |
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then |
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(12.17) |
L0ψ = [(γ / R)2 − (2π k/ T )2]ψ. |
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Let γ j be the j th positive root of Jν (x) = 0, and set |
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(12.18) |
ψ j k (t, r ) = r −ν Jν (γ j r/ R)e2π ikt/ T . |
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Then ψ j k (t, r ) is an eigenfunction of L0 with eigenvalue |
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(12.19) |
λ j k = (γ j / R)2 − (2π k/ T )2. |
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It is easily checked that the functions ψ j k , when normalized, form a complete orthonormal sequence in L2( , ρ). We shall show that the corresponding eigenvalues (12.19) are not dense in R. It will then follow that L0 has a self-adjoint extension L with spectrum equal to the closure of the set {λ j k } (cf., e.g., [126]). Now
(12.20) |
γ |
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j + |
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j → ∞ |
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O(β−3) as β |
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(12.21) |
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β j = π |
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j + |
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=β2j − τk2 − (μ − 1)/4 + O(β−j 2)
where τk = 2kπ R/ T . (We may assume k ≥ 0.) Now
(12.22) β j − τk = π |
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ν − |
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− ak/4b |
= π [(4 j + n − 3)b − ak]/4b. |
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Since the expression in the brackets is an integer, we see that either β j = τk or
(12.23) |
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Thus, |
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(12.24) |
j, k |
λ j k = −(μ − 1)/4R |
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= λ0 |
lim |
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β j =τk
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12. Rotationally Invariant Solutions |
and |
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|λ j k | = ∞. |
(12.25) |
j, k |
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β j =τk
If n − 3 is not a multiple of (4, a), then
(12.26) |
β j − τk = π((4 j + n − 3) − |
can never vanish. |
To see this, note that if (b, k) = |
Hence, β j = τk . If b = (b, k), then
ak/b)/4
b, then ak/b is not an integer.
(12.27) (n − 3) = ak − 4 j j, k = k/b.
Thus, in this case we always have β j = τk and |λ j k | → ∞ as j, k → ∞. On the other hand, if n ≡ 3(mod(4, a)), then there are an infinite number of positive integers j, k such that
(12.28) n − 3 = ak − 4 j.
Hence, the point λ0 is a limit point of eigenvalues. Consequently, it is in σe(L). This completes the proof.
12.3 The nonlinear case
We now turn to the problem of solving (12.1)–(12.3). If one is searching for rotationally invariant solutions, the problem reduces to
(12.29) |
Lu = f (t, r, u), u D(L) |
where L is the self-adjoint extension of the operator L0 given in Theorem 12.2. Under the hypotheses of that theorem, the spectrum of L is discrete. We assume that
(12.30) |
f (t, r, s) = μs + p(t, r, s), |
where μ is a point in the resolvent set of L and p(t, r, s) is a Carath´eodory function on× R such that
(12.31) |
| p(t, r, s)| ≤ C(|s|θ + 1), s R, |
for some number θ < 1. We have
Theorem 12.3. Let f (t, r, s) satisfy (12.30) and (12.31), and assume the hypotheses of Theorem 12.2. If
(12.32) |
n ≡ 3 |
(mod(4, a)), |
make no further assumptions. If |
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(12.33) |
n ≡ 3 |
(mod(4, a)) |
and λ0 |
< μ, assume that p(t, r, s) is nondecreasing in s. If (12.33) holds and |
μ < λ0, assume that p(t, r, s) is nonincreasing in s. Then (12.29) has at least one
weak solution.
12.3. The nonlinear case |
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Proof. Since μ is in the resolvent set of L, there is a δ > 0 such that |
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(12.34) |
|λ j k − μ| ≥ δ j, k, |
where the λ j k are given by (12.19). Each u L2( , ρ) can be expanded in the form
(12.35) u = α j k ψ j k (t, r ),
where the ψ j k are given by (12.18). Let N0 be the subspace of those u L2( , ρ) for which α j k = 0 if β j = τk (cf. the proof of Theorem 12.2). For u N0,
(12.36) |
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α j k ψ j k (t, r ), |
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β j = τk |
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k for which |
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L ( , ρ) consisting of those u for which |
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u 2E = |
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finite. With this norm, E becomes a separable Hilbert space. Note that E |
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N0 into L |
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D(|L| |
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( , ρ) is compact [we use (12.25) |
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for this purpose]. Let |
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(12.38) |
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G(u) = ([L − μ]u, u) − 2 |
P(t, r, u)ρdtdr, u E, |
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where |
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P(t, r, s) = |
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(12.39) |
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p(t, r, σ )dσ, |
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and then |
scalar product is that of L2( , ρ). |
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One checks readily that G is a |
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C1-functional on E with |
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(12.40) |
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(G (u), v)/2 = ([L − μ]u, v) − ( p(u), v), |
u, v E, |
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where we write p(u) in place of p(t, r, u). This shows that u is a weak solution of (12.29) iff G (u) = 0. Let N be the subspace of E spanned by the ψ j k corresponding
to those λ j k |
< μ and let M denote the subspace of E spanned by the rest. Thus, |
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M = N in E. Assume first that N ∩ N0 = {0}. Then |
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(12.41) |
u 2E = |
(μ − λ j k )|α j k |2, u N. |
Thus, |
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G(v) = − v 2E − 2 |
P(t, r, v)ρdtdr |
≤− v 2E + C (|v|1+θ + |v|)ρdtdr
≤ − v 2E + C ( v 1+θ + v ) → −∞, v E → ∞, v N.
146 |
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12. |
Rotationally Invariant Solutions |
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If w M, |
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(12.42) |
G(w) ≥ δ w 2 − C( w 1+θ + w ) ≥ −K , |
w M. |
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We can now make use of Theorem 10.2. If Q is a large ball in N, then |
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(12.43) |
∂ Q G ≤ |
M |
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sup |
inf G |
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By Example 1 of Section 10.3, ∂ Q links M weakly. Moreover, if {uk } |
E is a |
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sequence such that vk = Puk → v = Pu weakly on N and wk |
= (I − P)uk → |
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w = ( |
I |
− P)u strongly in M, where P is the |
projection of E onto N, then |
{ |
u |
k } has |
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2 |
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a renamed subsequence that converges strongly in L ( , ρ). |
The reason is that |
{vk } |
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has such a subsequence because the embedding of E N0 in L |
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( , ρ) is compact. |
Thus, G (un ) → G (u) weakly in E. Hence, all of the hypotheses of Theorem 10.2 are satisfied, and we can conclude that there is a sequence {uk } satisfying (10.3). Write uk = vk + wk + yk , where vk N, wk M N0, yk N0. Then
(12.44) |
(G (uk ), vk )/2 = ([L − μ]uk , vk ) − ( p(uk ), vk ) |
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and, consequently, |
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(12.45) |
vk 2E ≤ G (uk ) vk E /2 |
+ C vk ( uk θ + 1) |
in view of (12.31) and (12.37). Similarly, |
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(12.46) |
wk 2E ≤ G (uk ) wk E /2 |
+ C wk ( uk θ + 1). |
If N0 = {0}, then it follows from (12.45) and (12.46) that uk E is bounded and consequently there is a renamed subsequence that converges weakly in E and strongly in L2( , ρ) to a function u. Thus, G (uk ) → G (u) weakly. But G (uk ) → 0. Consequently G (u) = 0 and the proof for this case is complete. If N0 = {0}, we note that
(12.47) yk 2E ≤ G (uk ) yk ) E /2 + C yk ||( uk θ + 1)
as well. Again, this together with (12.45) and (12.46) implies that uk ||E is bounded and has a renamed subsequence that converges weakly in E and such that uk = vk +wk converges strongly in L2( , ρ). Now
(12.48) |
(G (uk ), yk − y)/2 = ([L − μ](yk − y), yk − y) |
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−( p(uk ) − p(uk + y), yk − y) |
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+( p(uk + y) − p(u), yk − y) |
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+([L − μ]y, yk − y), |
where yk |
→ y weakly in E and L2( , ρ) and uk → u weakly in E and strongly in |
L2( , ρ). By hypothesis |
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(12.49) |
( p(uk ) − p(uk + y), yk − y) ≥ 0 |