1 Introduction
It is well known that the eigenvalues and eigenfunctions of the Laplacian play an important role in global differential geometry since they reveal important relations between geometry of the manifold and analysis. Among the eigenvalue problems of the Laplacian, the biharmonic operator eigenvalue problems are interesting projects because these problems root in physics and geometric analysis. In this paper, we investigate the lower bounds of the first eigenvalues for the buckling problem and clamped plate problem on manifolds. There is a lot of research on these problems; see, for example, [1‐6], among others.
Let M be an n-dimensional compact connected Riemannian manifold with smooth boundary ∂M. We consider the biharmonic operator eigenvalue problem for the famous buckling problem
and clamped plate problem
where \(\Delta^{2}\) is the bi-Laplace operator, and n⃗ denotes the outer unit normal vector field of the boundary ∂M. Equation (1.1) describes the critical buckling load of a clamped plate subjected to a uniform compressive force around its boundary. It is known that the spectrum of this eigenvalue problem is real and purely discrete: Equation (1.2) describes the characteristic vibrations of a clamped plate. The spectrum of this eigenvalue problem is also real and purely discrete:
$$ \textstyle\begin{cases} \Delta^{2}f=-\Lambda\Delta{f}\quad \mbox{in }M, \\ f|_{\partial\Omega}=\frac{\partial f}{\partial\vec{n}}|_{\partial M}=0, \end{cases} $$
(1.1)
$$ \textstyle\begin{cases} \Delta^{2}f=\Gamma f\quad \mbox{in }M, \\ f|_{\partial\Omega}=\frac{\partial f}{\partial\vec{n}}|_{\partial M}=0, \end{cases} $$
(1.2)
$$0< \Lambda_{1}\leq\Lambda_{2}\leq\cdots\leq \Lambda_{k}\leq\cdots\uparrow +\infty. $$
$$0< \Gamma_{1}\leq\Gamma_{2}\leq\cdots\leq \Gamma_{k}\leq\cdots\uparrow +\infty. $$
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By the results of Li and Yau [7] and the variational characterization for eigenvalues, we can obtain lower bounds for eigenvalues of problems (1.1) and (1.2) on \(M \subset R^{n}\) (see Levine and Protter [8]), respectively, where \(\omega_{n}\) denotes the volume of a unit ball in \(\mathbb{R}^{n}\). Recently, Chen et al. [1] have investigated the first eigenvalues of problems (1.1) and (1.2) on n-dimensional compact connected Riemannian manifolds with Ricci curvature bounded from below by \((n-1)\). They proved that where \(\lambda_{1}\) denotes the first eigenvalue of the Dirichlet eigenvalue problem. For more research, we refer the readers to [4, 5, 9‐13].
$$\frac{1}{k}\sum_{i=1}^{k} \Lambda_{i}\geq\frac{n}{n+2}\frac{4\pi ^{2}}{(\omega_{n}V(M))^{\frac{2}{n}}}k^{\frac{2}{n}},\qquad \frac{1}{k}\sum_{i=1}^{k} \Gamma_{i}\geq\frac{n}{n+4}\frac{16\pi ^{4}}{(\omega_{n}V(M))^{\frac{4}{n}}}k^{\frac{4}{n}}, $$
$$\Lambda_{1}>n,\qquad \Gamma_{1}>n\lambda_{1}, $$
2 Preliminaries
In this section, we recall some preliminary knowledge, such as the Reilly formula, for later use.
Lemma 2.1
(Reilly’s formula [14])
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Let
M
be an
n-dimensional compact connected Riemannian manifold with smooth boundary
∂Ω. For every
\(f\in C^{\infty}(\bar {\Omega})\), we have
where Δf, ∇f, and
\(\nabla^{2}f\)
are the Laplacian, gradient, and Hessian of
f, Ric is the Ricci curvature of
M, Δ̄f
and ∇̄f
are the Laplacian and gradient of
f
in
∂M, and
σ
and
H
are the second fundamental form and the mean curvature of
∂M
with respect to the inner unit normal vector field
n⃗
on
∂M.
$$\begin{aligned}& \int_{M}\bigl[(\Delta f)^{2}-\bigl|\nabla^{2}f\bigr|^{2}- \operatorname{Ric}(\nabla f,\nabla f)\bigr]\, \mathrm{d}V \\& \quad = \int_{\partial M}\bigl[-2(\bar{\Delta} f)\langle\nabla f, \vec{n} \rangle +(n-1)H\langle\nabla f, \vec{n}\rangle^{2}+\sigma(\bar{\nabla} f,\bar {\nabla} f)\bigr]\, \mathrm{d}A, \end{aligned}$$
Lemma 2.2
(Hessian comparison theorem)
Let
M
be an
n-dimensional complete Riemannian manifold, and let
\(x_{0}, x_{1}\in M\). Let
\(\gamma:[0, \rho(x_{1})]\rightarrow M\)
be a minimizing geodesic joining
\(x_{0}\)
and
\(x_{1}\), where
\(\rho(x)\)
is the distance function
\(\operatorname {dist}_{M}(x_{0}, x)\). Let
K
be the sectional curvature of
M, and let
\(\mu_{i} (\rho)\) (\(i=0,1\)) be the functions defined by
and
Then the Hessians of
ρ
and
\(\rho^{2}\)
satisfy
where
X
is any vector in
\(T_{x}M\)
perpendicular to
\(\gamma'(\rho(x))\).
$$\mu_{0}(\rho)= \textstyle\begin{cases} k_{0}\cdot\coth(k_{0}\cdot\rho(x))& \textit{if } \inf_{\gamma }K=-k_{0}^{2}, \\ \frac{1}{\rho(x)} & \textit{if } \inf_{\gamma}K=0, \\ k_{0}\cdot\cot(k_{0}\cdot\rho(x)) & \textit{if } \inf_{\gamma }K=k_{0}^{2} \textit{ and } \rho< \frac{\pi}{2k_{0}} \end{cases} $$
$$\mu_{1}(\rho)= \textstyle\begin{cases} k_{1}\cdot\coth(k_{1}\cdot\rho(x))& \textit{if } \inf_{\gamma }K=-k_{1}^{2}, \\ \frac{1}{\rho(x)} & \textit{if } \inf_{\gamma}K=0, \\ k_{1}\cdot\cot(k_{1}\cdot\rho(x)) & \textit{if } \inf_{\gamma }K=k_{1}^{2} \textit{ and } \rho< \frac{\pi}{2k_{1}}. \end{cases} $$
$$\begin{aligned}& \mu_{0}\bigl(\rho(x)\bigr)\cdot\|X\|^{2}\geq \nabla^{2}\rho(x) (X,X)\geq\mu _{1}\bigl(\rho(x)\bigr)\cdot \|X\|^{2}, \\& 2\rho(x)\mu_{0}\bigl(\rho(x)\bigr)\cdot\|X\|^{2}\geq \nabla^{2}\rho ^{2}(x) (X,X)\geq2\rho(x)\mu_{1} \bigl(\rho(x)\bigr)\cdot\|X\|^{2}, \\& \nabla^{2}\rho(x) \bigl(\gamma',\gamma' \bigr)=0, \qquad \nabla^{2}\rho^{2}(x) \bigl(\gamma ',\gamma'\bigr)=2, \end{aligned}$$
Thus, the following inequalities hold (cf. [15]):
$$\begin{aligned}& (n-1)\mu_{0}\bigl(\rho(x)\bigr)\geq\Delta\rho(x)\geq(n-1) \mu_{1}\bigl(\rho(x)\bigr), \end{aligned}$$
(2.1)
$$\begin{aligned}& 2(n-1)\rho(x)\mu_{0}\bigl(\rho(x)\bigr)+2\geq\Delta \rho^{2}(x)\geq2(n-1)\rho (x)\mu_{1}\bigl(\rho(x) \bigr)+2. \end{aligned}$$
(2.2)
We recall the following variational characterization for the first eigenvalues of the buckling problem and the clamped plate problem: and
$$ \Lambda_{1}(M)=\min_{\substack{f\in H_{0}^{2}(M)\\f\not\equiv0}}\frac {\int_{M}(\Delta f)^{2} \, \mathrm{d}V}{\int_{M}|\nabla f|^{2}\, \mathrm {d}V} $$
(2.3)
$$ \Gamma_{1}(M)=\min_{\substack{f\in H_{0}^{2}(M)\\f\not\equiv0}}\frac {\int_{M}(\Delta f)^{2} \, \mathrm{d}V}{\int_{M}f^{2}\, \mathrm{d}V}. $$
(2.4)
3 Main results
In this section, we give and prove our main results, that is, we estimate the lower bounds of the first eigenvalues of problems (1.1) and (1.2).
Theorem 3.1
Let
\((M,g)\)
be an
n-dimensional compact connected Riemannian manifold with smooth boundary
∂M
and Ricci curvature bounded from below by a positive constant C. Let
\(\Lambda_{1}(M)\)
be the first eigenvalue of the buckling problem (1.1). Then, for any vector field
\(X\in\Gamma(T M)\)
such that
\(\|X\|_{\infty}=\sup_{M}|X|<\infty\) (where
\(|X|=\sqrt{g(X, X)}\)) and
\(\inf_{M}\operatorname {div}(X)>0\), we have
$$ \Lambda_{1}(M)\geq \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty }} \biggr)^{2}+C. $$
(3.1)
Proof
For any \(f\in C^{\infty}_{0}(\Omega)\), the vector field \(|\nabla f|^{2}X\) has compact support on M, and a simple calculation shows that For any \(\varepsilon>0\), it follows from Young’s inequality that Combining this inequality and (3.2) yields It follows from \(f|_{\partial M}=\frac{\partial f}{\partial\vec {n}}|_{\partial M}=0\) that \((\nabla f)|_{\partial M}=0\). Then by the divergence theorem we have This equality and (3.3) imply that is, Let Then It is obvious that when \(g'(\varepsilon)=0\), we have \(\varepsilon _{0}=(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}})^{\frac{1}{2}}\) and \(g''(\varepsilon_{0})=-4\inf_{M}\operatorname{div}X<0\), and therefore, From this equality and from (3.4) it follows that
$$\begin{aligned} \operatorname{div}\bigl(X|\nabla f|^{2}\bigr) =&2|\nabla f|X\bigl( \vert \nabla f\vert \bigr)+|\nabla f|^{2}\operatorname{div}(X) \\ \geq&-2|\nabla f|\|X\|_{\infty}\bigl\vert \nabla \vert \nabla f\vert \bigr\vert +|\nabla f|^{2}\inf_{M} \operatorname{div}(X). \end{aligned}$$
(3.2)
$$|\nabla f|\bigl\vert \nabla \vert \nabla f\vert \bigr\vert \leq \frac{|\nabla|\nabla f||^{2}}{2\varepsilon^{2}}+\frac{\varepsilon^{2}|\nabla f|^{2}}{2}. $$
$$ \operatorname{div}\bigl(X|\nabla f|^{2}\bigr)\geq-2\|X\|_{\infty} \biggl(\frac{|\nabla |\nabla f||^{2}}{2\varepsilon^{2}}+\frac{\varepsilon^{2}|\nabla f|^{2}}{2} \biggr) +|\nabla f|^{2} \inf_{M}\operatorname{div}(X). $$
(3.3)
$$ \int_{M}\operatorname{div}\bigl(X|\nabla f|^{2} \bigr)\, \mathrm{dV}= \int_{\partial M}|\nabla f|^{2}\langle X, \vec{n}\rangle\, \mathrm{dV_{\partial M}}=0. $$
$$\int_{M}\bigl\vert \nabla \vert \nabla f\vert \bigr\vert ^{2}\, \mathrm{dV}\geq\frac{\varepsilon^{2}}{\| X\|_{\infty}} \Bigl(\inf _{M} \operatorname{div}X-\varepsilon^{2}\|X \|_{\infty } \Bigr) \int_{M}|\nabla f|^{2}\, \mathrm{dV}, $$
$$ \frac{\int_{M}|\nabla|\nabla f||^{2}\, \mathrm{d}V}{\int_{M}|\nabla f|^{2}\, \mathrm{d}V} \geq\frac{\varepsilon^{2}}{\|X\|_{\infty}} \Bigl(\inf_{M} \operatorname {div}X-\varepsilon^{2}\|X\|_{\infty} \Bigr). $$
(3.4)
$$g(\varepsilon)=\varepsilon^{2}\inf_{M} \operatorname{div}X-\varepsilon^{4}\|X\| _{\infty}. $$
$$g'(\varepsilon)=2\varepsilon\inf_{M} \operatorname{div}X-4\varepsilon^{3}\|X\| _{\infty}, \qquad g''(\varepsilon)=2\inf_{M} \operatorname{div}X-12\varepsilon ^{2}\|X\|_{\infty}. $$
$$\max g(\varepsilon)= \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|^{\frac {1}{2}}_{\infty}} \biggr)^{2}. $$
$$ \frac{\int_{M}|\nabla|\nabla f||^{2}\,\mathrm{d}V}{\int_{M}|\nabla f|^{2}\,\mathrm{d}V} \geq \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}} \biggr)^{2}. $$
(3.5)
On the other hand, if \(f\in C^{\infty}_{0}(\Omega)\), then Indeed, without loss of generality, we choose the normal coordinate \((U; x^{1}, \ldots, x^{n})\) for any point \(P\in M\), and a simple calculation shows that where \(f_{j}=\frac{\partial f}{\partial x^{j}}\). From the Cauchy-Schwarz inequality it follows that Combining (3.7) and (3.8) yields which implies that on M for any \(f\in C^{\infty}_{0}(\Omega)\). Since \(C^{\infty }_{0}(\Omega)\) is dense in \(H^{2}_{0}(\Omega)\), the last relation also holds for all \(f\in H^{2}_{0}(\Omega)\).
$$ \bigl\vert \nabla \vert \nabla f\vert \bigr\vert ^{2}\leq\bigl| \nabla^{2} f\bigr|^{2}. $$
(3.6)
$$ \bigl\vert \nabla \vert \nabla f\vert \bigr\vert ^{2}(P) = \sum _{q=1}^{n} \biggl[\frac{(\sum_{i=1}^{n}f_{i}f_{iq})^{2}}{\sum_{i=1}^{n}f_{i}^{2}} \biggr], $$
(3.7)
$$ \sum_{q=1}^{n} \Biggl(\sum _{i=1}^{n}f_{i}f_{iq} \Biggr)^{2} \leq \Biggl[\sum_{q=1}^{n} \Biggl(\sum_{i=1}^{n}f_{i}^{2} \Biggr) \Biggl(\sum_{i=1}^{n}f_{iq}^{2} \Biggr) \Biggr] = \Biggl(\sum_{i=1}^{n}f_{i}^{2} \Biggr) \Biggl(\sum_{i,q=1}^{n}f_{iq}^{2} \Biggr). $$
(3.8)
$$\bigl\vert \nabla \vert \nabla f\vert \bigr\vert ^{2}(P)\leq \sum_{i,q=1}^{n}f_{iq}^{2}= \bigl\vert \nabla^{2} f\bigr\vert ^{2}(P), $$
$$\bigl\vert \nabla \vert \nabla f\vert \bigr\vert ^{2}\leq\sum _{i,q=1}^{n}f_{iq}^{2}= \bigl\vert \nabla^{2} f\bigr\vert ^{2} $$
From Reilly’s formula and the equality \(f|_{\partial M}=\frac{\partial f}{\partial\vec{n}}|_{\partial M}=0\) we get Since the Ricci curvature of M is bounded from below by a constant C, this gives From this inequality and from (3.5) and (3.6) it follows that which, together with (2.3) and the arbitrariness of X, implies □
$$\int_{M} \bigl[(\Delta f)^{2}-\bigl|\nabla^{2}f\bigr|^{2}- \operatorname{Ric}(\nabla f,\nabla f) \bigr]\, \mathrm{d}V=0. $$
$$ \int_{M}\bigl|\nabla^{2}f\bigr|^{2}\,\mathrm{d}V \leq \int_{M}(\Delta f)^{2}\,\mathrm{d}V-C \int_{M}|\nabla f|^{2}\,\mathrm{d}V. $$
$$ \frac{\int_{M}(\Delta f)^{2} \,\mathrm{d}V}{\int_{M}|\nabla f|^{2}\,\mathrm{d}V} \geq \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}} \biggr)^{2}+C, $$
(3.9)
$$ \Lambda_{1}(M) \geq \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}} \biggr)^{2}+C. $$
Theorem 3.2
Assume that
\((M,g)\)
and
\(X\in\Gamma(T M)\)
satisfy the conditions of Theorem
3.1
and let
\(\Gamma_{1}(M)\)
be the first eigenvalue of the clamped plate problem (1.2). Then
where
\(\lambda_{1}(M)\)
is the first eigenvalue of the Dirichlet eigenvalue problem.
$$ \Gamma_{1}(M)\geq \biggl( \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\| _{\infty}} \biggr)^{2}+C \biggr)\lambda_{1}(M), $$
(3.10)
Proof
By (3.9) we immediately get for all \(f\in H^{2}_{0}(M)\). From the Poincaré inequality and the fact that f is nonzero with \(f|_{\partial M}=0\) it follows that where the equality holds if and only if f is the first eigenfunction of the Dirichlet eigenvalue problem. Thus, from (2.4), (3.11), and (3.12) and from the arbitrariness of X we have □
$$ \frac{\int_{M}(\Delta f)^{2} \,\mathrm{d}V}{\int_{M} f^{2}\,\mathrm{d}V} \geq \biggl( \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}} \biggr)^{2}+C \biggr)\frac{\int_{M} |\nabla f|^{2}\,\mathrm{d}V}{\int_{M} f^{2}\,\mathrm{d}V} $$
(3.11)
$$ \frac{\int_{M} |\nabla f|^{2}\,\mathrm{d}V}{\int_{M} f^{2}\,\mathrm {d}V}\geq\lambda_{1}(M), $$
(3.12)
$$\Gamma_{1}(M) \geq \biggl( \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}} \biggr)^{2}+C \biggr)\lambda_{1}(M). $$
As an application of our theorems, we can get the following results.
Corollary 3.3
Let
\((M,g)\)
be an
n-dimensional complete Riemannian manifold, and
\(B_{M}(p,r)\)
a geodesic ball with radius
\(r<\operatorname{inj}(p)\). Let
\(\kappa(p,r)=\sup\{K_{M}(x); x\in B_{M}(p,r)\}\), where
\(K_{M}(x)\)
is the sectional curvature of
M
at
x. If for
\(k>0\), \(\kappa(p,r)=k^{2}\), \(r<\frac{\pi}{2k}\), and the Ricci curvature of
\(B_{M}(p,r)\)
is bounded from below by a positive constant
C, then
$$\begin{aligned}& \Lambda_{1}\bigl(B_{M}(p,r)\bigr)\geq\bigl[(n-1)kr \cot(kr)+1\bigr]^{2}/4r^{2}+C, \\& \Gamma_{1}\bigl(B_{M}(p,r)\bigr)\geq \bigl(\bigl[(n-1)kr \cot(kr)+1\bigr]^{2}/4r^{2}+C \bigr)\lambda_{1} \bigl(B_{M}(p,r)\bigr). \end{aligned}$$
Proof
Let \(X=\nabla\rho^{2}\). Then by (2.2), (3.1), and (3.10) we have and □
$$\begin{aligned} \Lambda_{1}\bigl(B_{M}(p,r)\bigr) \geq& \biggl[ \frac{\inf_{B_{M}(p,r)}\Delta\rho ^{2}}{2\|\nabla\rho^{2}\|_{\infty}} \biggr]^{2}+C \\ \geq& \biggl[\frac{(n-1)k\inf_{B_{M}(p,r)}\cot(k\rho)}{2}+\frac {1}{2r} \biggr]^{2}+C \\ \geq& \frac{[(n-1)kr\cot(kr)+1]^{2}}{4r^{2}}+C \end{aligned}$$
$$\Gamma_{1}\bigl(B_{M}(p,r)\bigr)\geq \biggl( \frac{[(n-1)kr\cot (kr)+1]^{2}}{4r^{2}}+C \biggr)\lambda_{1}(M). $$
Corollary 3.4
Let
\(\varphi: M\hookrightarrow N\)
have a locally bounded mean curvature, that is, the number
\(h(p,r)=\sup\{|H(x)|; x\in\varphi(M)\cap B_{N}(p,r) \}\)
is finite, where
H
is the mean curvature, and let Ω be any connected component of
\(\varphi^{-1}(\overline{B_{N}(p,r)})\), where
\(p\in N\backslash\varphi(M)\)
and
\(r>0\).
(1)
If
\(\kappa(p,r)=k^{2}<\infty\)
and the Ricci curvature of Ω is bounded from below by a positive constant
C, choose
Then
$$r< \min \biggl\{ \operatorname{inj}(p), \frac{\pi}{2k}, \cot^{-1} \bigl[h\bigl(p,\operatorname {inj}(p)\bigr)/(m-1)k\bigr]/k \biggr\} . $$
$$\begin{aligned}& \Lambda_{1}(\Omega)\geq\bigl[(m-1)k\cot(kr)-h(p,r) \bigr]^{2}/4+C, \\& \Gamma_{1}(\Omega)\geq \bigl(\bigl[(m-1)k\cot(kr)-h(p,r) \bigr]^{2}/4+C \bigr)\lambda_{1}(\Omega). \end{aligned}$$
(2)
If
\(\lim_{r\rightarrow\infty}\kappa(p,r)=\infty\)
and the Ricci curvature of Ω is bounded from below by a positive constant
C, let
Choose
\(r=\max_{s>0}r(s)\). Then
$$r(s)=\min \bigl\{ \pi/2\sqrt{\kappa(p,s)},\cot^{-1}\bigl[h(p,s)/(m-1) \kappa (p,s)\bigr]/\kappa(p,s) \bigr\} , \quad s>0. $$
$$\begin{aligned}& \Lambda_{1}(\Omega)\geq \bigl(\bigl[(m-1)\sqrt{\kappa(p,r)}\cot\bigl( \sqrt{\kappa (p,r)}r\bigr)-h(p,r)\bigr]^{2}/4+C \bigr), \\& \Gamma_{1}(\Omega)\geq \bigl(\bigl[(m-1)\sqrt{\kappa(p,r)}\cot\bigl( \sqrt{\kappa (p,r)}r\bigr)-h(p,r)\bigr]^{2}/4+C \bigr) \lambda_{1}(\Omega). \end{aligned}$$
Proof
By the proof of Theorem 4.3 of [15], if \(\rho(x)=\operatorname {dist}_{N}(p,x)\) and \(f=\rho\circ\varphi: M\rightarrow\mathbb{R}\), then applying (2.1), we have Since \(\|\nabla f\|\leq1\), the estimates follow from Theorems 3.1 and 3.2. □
$$\operatorname{div}(\nabla f)\geq(m-1)k\cot(kr)-h(p,r)>0 \quad \mbox{if } \kappa (p,r)=k^{2}. $$
Remark 3.5
If, in (3.5), \(|\nabla f|\) is replaced by f, then which, together with (3.11), implies
$$\frac{\int_{M} |\nabla f|^{2}\,\mathrm{d}V}{\int_{M} f^{2}\,\mathrm {d}V}\geq \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty}} \biggr)^{2}, $$
$$ \Gamma_{1}(M)\geq \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty }} \biggr)^{2} \biggl( \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty }} \biggr)^{2}+C \biggr). $$
(3.13)
Remark 3.6
Using a similar argument as in Theorems 3.1 and 3.2 and Corollary 3.3, we can investigate the following two biharmonic operator eigenvalue problems: and We get and where \(p_{1}\) and \(q_{1}\) are the first eigenvalues of these two problems.
$$\textstyle\begin{cases} \Delta^{2}u=-p\Delta u \quad \mbox{in } \Omega, \\ u|_{\partial\Omega}=\frac{\partial^{2} u}{\partial\vec {n}^{2}}|_{\partial\Omega}=0 \end{cases} $$
$$\textstyle\begin{cases} \Delta^{2}u=qu \quad \mbox{in } \Omega, \\ u|_{\partial\Omega}=\frac{\partial^{2} u}{\partial\vec {n}^{2}}|_{\partial\Omega}=0. \end{cases} $$
$$\begin{aligned}& p_{1}(M)\geq\sup \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty }} \biggr)^{2}+C, \\& q_{1}(M)\geq \biggl(\sup \biggl(\frac{\inf_{M}\operatorname{div}X}{2\|X\|_{\infty }} \biggr)^{2}+C \biggr)\lambda_{1}(M) \end{aligned}$$
$$\begin{aligned}& p_{1}\bigl(B_{M}(p,r)\bigr)\geq \biggl( \frac{[(n-1)kr\cot (kr)+1]^{2}}{4r^{2}}+C \biggr), \\& q_{1}\bigl(B_{M}(p,r)\bigr)\geq \biggl( \frac{[(n-1)kr\cot (kr)+1]^{2}}{4r^{2}}+C \biggr)\lambda_{1}(M), \end{aligned}$$
Acknowledgements
This work was supported by the National Science Foundation of China (No. 11201400).
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The authors declare that they have no competing interests.
Authors’ contributions
All authors contributed equally to the writing of this paper. All authors read and approved for the final manuscript.