Abstract:Abstract. We prove some Liouville type results for stable solutions to the biharmonic problem ∆ 2 u = u q , u > 0 in R n where 1 < q < ∞. For example, for n ≥ 5, we show that there are no stable classical solution in R n when n+4 n−4 < q ≤ n−8 n −1 + .
“…It was shown there exists nontrivial finite Morse index solutions of (14) if and only if N ≥ 11 and θ ≥ θ JL . In [51] the nonexistence of stable solutions of (5) was examined. It was shown that there is no positive stable solutions of (5) provided either: N ≤ 8 or N ≥ 9 and 1 < θ < N N −8 + ε N where ε N is some positive, but unknown parameter.…”
Section: Theorem 2 (Fourth Order Scalar Equation)mentioning
confidence: 99%
“…Critical to our approach in the following result: Lemma 6. [51] Suppose that (u, v) is a stable smooth positive solution of (4) with p = 1. Then by Lemma 7, u is a positive stable solution of (5) and then the results of [51] imply there is some C < ∞ such that…”
We examine the elliptic system given byfor 1 < p ≤ θ and the fourth order scalar equationwhere 1 < θ. We prove various Liouville type theorems for positive stable solutions. For instance we show there are no positive stable solutions of (1) (resp. (2)) provided N ≤ 10 and 2 ≤ p ≤ θ (resp. N ≤ 10 and 1 < θ). Results for higher dimensions are also obtained. These results regarding stable solutions on the full space imply various Liouville theorems for positive (possibly unstable) bounded solutions ofwith u = v = 0 on ∂R N + . In particular there is no positive bounded solution of (3) for any 2 ≤ p ≤ θ if N ≤ 11. Higher dimensional results are also obtained.
“…It was shown there exists nontrivial finite Morse index solutions of (14) if and only if N ≥ 11 and θ ≥ θ JL . In [51] the nonexistence of stable solutions of (5) was examined. It was shown that there is no positive stable solutions of (5) provided either: N ≤ 8 or N ≥ 9 and 1 < θ < N N −8 + ε N where ε N is some positive, but unknown parameter.…”
Section: Theorem 2 (Fourth Order Scalar Equation)mentioning
confidence: 99%
“…Critical to our approach in the following result: Lemma 6. [51] Suppose that (u, v) is a stable smooth positive solution of (4) with p = 1. Then by Lemma 7, u is a positive stable solution of (5) and then the results of [51] imply there is some C < ∞ such that…”
We examine the elliptic system given byfor 1 < p ≤ θ and the fourth order scalar equationwhere 1 < θ. We prove various Liouville type theorems for positive stable solutions. For instance we show there are no positive stable solutions of (1) (resp. (2)) provided N ≤ 10 and 2 ≤ p ≤ θ (resp. N ≤ 10 and 1 < θ). Results for higher dimensions are also obtained. These results regarding stable solutions on the full space imply various Liouville theorems for positive (possibly unstable) bounded solutions ofwith u = v = 0 on ∂R N + . In particular there is no positive bounded solution of (3) for any 2 ≤ p ≤ θ if N ≤ 11. Higher dimensional results are also obtained.
“…where we used (2.3) in the last step. For the second term on the right hand side of (2.20), applying the estimate (2.3) from [15], i.e., (∆u) 2 ≥ 2 p+1 u p+1 , and the fact that ∆u < 0 from [14] or [16], we have…”
“…We use the idea of Moser and multiply (1.7) by uη 2 where η ∈ C ∞ 0 (R N ); see [16] and [17]. Note that as u ∈ L ∞ (R N ), by the regularity theory u ∈ C 4 (R N ).…”
In this paper, we prove the Lazer-McKenna conjecture for the suspension bridge model in higher dimension. We also discuss some properties of the limiting problem related to the Swift-Hohenberg equation.
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