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Let $$A_R\subset \mathbb {R}^N$$ A R ⊂ R N , $$N\ge 2$$ N ≥ 2 , be an annulus with inner radius R and outer radius $$R+1$$ R + 1 . We are concerned with the elliptic Neumann problem $$\begin{aligned} {\left\{ \begin{array}{ll} \varepsilon ^2\Delta u+f(u)=0 & \text {for}\ x\in A_R,\\ \frac{\partial u}{\partial n}=0 & \text {for}\ x\in \partial A_R, \end{array}\right. } \end{aligned}$$ ε 2 Δ u + f ( u ) = 0 for x ∈ A R , ∂ u ∂ n = 0 for x ∈ ∂ A R , where $$\varepsilon >0$$ ε > 0 is a small constant. In particular, the Allen-Cahn equation $$f(u)=u-u^3$$ f ( u ) = u - u 3 and the scalar field equation $$f(u)=-u+u^p$$ f ( u ) = - u + u p , $$p>1$$ p > 1 , are studied. We establish sharp asymptotic formulas of the Morse index of n-mode radial solutions as $$R\rightarrow \infty $$ R → ∞ . In the case of the scalar field equation the first n eigenvalues of the linearization around n-mode solutions of the one-dimensional problem $$\begin{aligned} {\left\{ \begin{array}{ll} \varepsilon ^2u''-u+u^p=0 & \text {for}\ 0<x<1,\\ u'(0)=u'(1)=0 \end{array}\right. } \end{aligned}$$ ε 2 u ′ ′ - u + u p = 0 for 0 < x < 1 , u ′ ( 0 ) = u ′ ( 1 ) = 0 become important. We show that, as $$\varepsilon \rightarrow 0$$ ε → 0 , the first $$\ell $$ ℓ eigenvalues converge to $$-(p+3)(p-1)/4$$ - ( p + 3 ) ( p - 1 ) / 4 and the other $$n-\ell $$ n - ℓ eigenvalues converge to 0, where $$\ell $$ ℓ is the number of the local maximum points of an n-mode solution u(x) on [0, 1].
Let $$A_R\subset \mathbb {R}^N$$ A R ⊂ R N , $$N\ge 2$$ N ≥ 2 , be an annulus with inner radius R and outer radius $$R+1$$ R + 1 . We are concerned with the elliptic Neumann problem $$\begin{aligned} {\left\{ \begin{array}{ll} \varepsilon ^2\Delta u+f(u)=0 & \text {for}\ x\in A_R,\\ \frac{\partial u}{\partial n}=0 & \text {for}\ x\in \partial A_R, \end{array}\right. } \end{aligned}$$ ε 2 Δ u + f ( u ) = 0 for x ∈ A R , ∂ u ∂ n = 0 for x ∈ ∂ A R , where $$\varepsilon >0$$ ε > 0 is a small constant. In particular, the Allen-Cahn equation $$f(u)=u-u^3$$ f ( u ) = u - u 3 and the scalar field equation $$f(u)=-u+u^p$$ f ( u ) = - u + u p , $$p>1$$ p > 1 , are studied. We establish sharp asymptotic formulas of the Morse index of n-mode radial solutions as $$R\rightarrow \infty $$ R → ∞ . In the case of the scalar field equation the first n eigenvalues of the linearization around n-mode solutions of the one-dimensional problem $$\begin{aligned} {\left\{ \begin{array}{ll} \varepsilon ^2u''-u+u^p=0 & \text {for}\ 0<x<1,\\ u'(0)=u'(1)=0 \end{array}\right. } \end{aligned}$$ ε 2 u ′ ′ - u + u p = 0 for 0 < x < 1 , u ′ ( 0 ) = u ′ ( 1 ) = 0 become important. We show that, as $$\varepsilon \rightarrow 0$$ ε → 0 , the first $$\ell $$ ℓ eigenvalues converge to $$-(p+3)(p-1)/4$$ - ( p + 3 ) ( p - 1 ) / 4 and the other $$n-\ell $$ n - ℓ eigenvalues converge to 0, where $$\ell $$ ℓ is the number of the local maximum points of an n-mode solution u(x) on [0, 1].
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