Consider the eigenvalue problem

where $\Omega \subset \mathbb{R}^2$ is a bounded domain. Denote by $\{\lambda_n\}$ the sequence of the corresponding eigenvalues,

and let $\varphi_n$ be an eigenfunction associated with $\lambda_n$. Let $\mu(\varphi_n)$ be a number of nodal domains of $\varphi_n$. Courant’s theorem asserts that $\mu(\varphi_n) \leq n$ for any $n$. This result was refined by Å. Pleijel as follows.

Theorem (Section 5 in ). Let $j_{0,1}$ be the first zero of the Bessel function $J_0$. Then

The upper bound $\frac{4}{j_{0,1}^2}$ is not sharp, as it was proved, e.g., by Bougain . Moreover, it was conjectured by Polterovich  that

In fact, this conjectured upper bound is achieved for rectangles $\Omega = (0,a) \times (0,b)$ such that $\frac{a^2}{b^2}$ is irrational; see, e.g., . However, it seems that, apart such rectangles, the Pleijel constant $Pl(\Omega)$ have not been found explicitly for any other domain $\Omega$. At least, the question of finding such domains was explicitly posed by Bonnaillie-Noël et al in Section 6.1 of .

The aim of the present post is to obtain the explicit expression for $Pl(B)$, where $B$ is a unit disk (ball) in $\mathbb{R}^2$. Disk is the second most natural candidate for such tryings (after irrational rectangles), since we explicitly know all of its eigenvalues and eigenfunctions, and we know that its eigenfunctions have some good multiplicity properties. Our main result is the following.

Theorem.

where $\theta=\theta(x)$ is the solution of the transcendental equation

Proof. Let $B := \{x \in \mathbb{R}^2:~ |x| < 1\}$. By a separation of variables, it is not hard to see that any eigenfunction (up to rotation) can be expressed in the form

and $\lambda_{\nu,k} = j_{\nu,k}^2$ is the eigenvalue associated with $\varphi_{\nu,k}$. Here $j_{\nu,k}$ is the $k$-th zero of the $\nu$-th Bessel function $J_\nu$. Any eigenvalue $\lambda_{0,k}$ has multiplicity $1$ (associated eigenfunction is radial), while any other eigenvalue has multiplicity $2$ (associated eigenfunctions are $\varphi_{\nu,k}$ and its rotation). Clearly, $\mu(\varphi_{0,k}) = k$ and $\mu(\varphi_{\nu,k}) = 2 \nu k$ for $\nu \in \mathbb{N}$.

Note that $\lambda_{\nu,k}$ is represented by two indexes $\nu,k$, and it is not straightforwardly clear how to put $\lambda_{\nu,k}$ explicitly in the increasing order as $\lambda_n$. However, since we are interested in the behavior as $n \to \infty$, we use the Weyl law which, for $\Omega=B$, can be read as

Hence, noting that for any $\lambda_n$ there exists a unique pair $(\nu_n,k_n)$ such that $\lambda_n = \lambda_{\nu_n,k_n}$, we get

Recalling that $\mu(\varphi_{\nu,k}) = (2 \nu + \sigma(\nu)) k$, where $\sigma(0)=1$ and $\sigma(\nu)=0$ for $\nu \in \mathbb{N}$, we then deduce that

Extracting a subsequence (still denoted by ${n}$) which delivers the value $Pl(B)$, omitting (for simplicity) subindex for $(\nu_n,k_n)$, and noting that $n \to \infty$ iff $\nu + k \to \infty$, we obtain

All we need now is to study the behavior of $j_{\nu,k}$ as $\nu + k \to \infty$. Let us immediately note that the sequence $\varphi_{0,k}$ cannot be a maximizing sequence for $Pl(B)$ since otherwise the inequality $j_{0,k} > k \pi - \frac{\pi}{4}$ (see Eq. (1.2) in ) yields

but we will see later that $Pl(B) > 0$. Thus, we always assume that $\nu \in \mathbb{N}$, and hence $\mu(\varphi_{\nu,k}) = 2 \nu k$ and

\begin{equation}\label{1} Pl(B) = \lim_{\nu + k \to \infty} \frac{8 \nu k}{j_{\nu,k}^2}. \end{equation}

Note first that the following inequality is satisfied for all $\nu \geq 0$ and $k \in \mathbb{N}$:

\begin{equation}\label{eq:EL1} j_{\nu,k} > \nu + \frac{\nu^{1/3}}{2^{1/3}}\left(\frac{3\pi}{8}(4k-1)\right)^{2/3}, \end{equation}

see the result of  or  in combination with the upper estimate for the zeros of the Airy function from , Theorem 2. Therefore, estimating \eqref{eq:EL1} from below by the first or the second summand, we deduce that

\begin{equation}\label{eq:upper_bound} Pl(B) \leq \lim_{\nu + k \to \infty} \min\left\{ \frac{8k}{\nu}, C \left(\frac{\nu}{k}\right)^{1/3} \right\} \end{equation}

for some constant $C>0$ which does not depend on $\nu$ and $k$.

Suppose at the moment that $Pl(B) > 0$. (We will achieve this fact later.) Under this assumption, we conclude from \eqref{eq:upper_bound} that both $\nu$ and $k$ tend to infinity, and there exist $A_1, A_2 > 0$ such that

Moreover, recalling that $(\nu,k)$ is a maximizing subsequence for $Pl(B)$, we can always select a sub-subsequence (which is hence also a maximizing subsequence for $Pl(B)$) still denoted by $(\nu,k)$, such that

\begin{equation}\label{2} \lim_{\nu \to \infty}\frac{k}{\nu} = x_0 \in [A_1,A_2]. \end{equation}

That is, we have $k = \nu \, x_0 + o(k)$ for all large $\nu$.

Let us now use the result of Elbert , Section 1.5, which states that

\begin{equation}\label{3} \lim_{\nu \to \infty} \frac{j_{\nu,\nu x}}{\nu} = \frac{1}{\cos \theta(x)}, \quad x > 0, \end{equation}

where $\theta=\theta(x)$ is the solution of the (transcendental) equation

\begin{equation}\label{eq:theta} \tan \theta - \theta = \pi x, \quad \theta \in \left(0, \frac{\pi}{2}\right). \end{equation}

Combining \eqref{1}, \eqref{2}, and \eqref{3}, we see that $Pl(B) = 8 x_0 \left(\cos \theta(x_0)\right)^2$, and $x_0$ have to satisfy

\begin{equation}\label{eq:PLB} Pl(B) = 8 x_0 \left(\cos \theta(x_0)\right)^2 = 8 \, \sup_{x>0} \left\{ x \left(\cos \theta(x)\right)^2 \right\} > 0. \end{equation}

Most likely, \eqref{eq:theta} and hence \eqref{eq:PLB} cannot be solved in closed forms. However, one can convince himself that the left-hand side of \eqref{eq:theta} is strictly increasing in $\left(0, \frac{\pi}{2}\right)$, and hence the unique root of \eqref{eq:theta} and the value of $Pl(B)$ can be found with arbitrary precision via the standard numerical methods. In particular, using the build-in methods of Mathematica, we obtain

The corresponding Mathematica code can look like that:

Remark 1. The numerics suggests that the function $n \mapsto \frac{\mu(\varphi_n)}{n}$ decreases to $Pl(B)$ for large $n \in \mathbb{N}$. For instance,

Remark 2. If we consider the Neumann eigenvalues instead of the Dirichlet ones, then the result of our theorem remains valid. To show this fact, we argue in much the same way as in , Section 2.3. Namely, Neumann eigenfunctions have the form

where $j_{\nu,k}’$ is the $k$-th zero of the derivative $J_\nu’$ of the Bessel function $J_\nu$. Moreover, $\lambda_{\nu,k} = (j_{\nu,k}’)^2$ is the associated eigenvalue. It is easy to see that, in fact, $\psi_{\nu,k}$ is a restriction to $B$ of the Dirichlet eigenfunction $\varphi_{\nu,k}$ defined on a bigger ball $B_R$. Moreover,

and, clearly, $\mu(\phi_{\nu,k}) = 2 \nu k$ for $\nu,k \in \mathbb{N}$. The result is then follows directly.

Remark 3. One can obtain similar explicit expressions of Pleijel’s constant for some circular sectors, at least for those whose opening angle is $\pi/m$, $m \in \mathbb{N}$.

The PDF-version of this post can be found here.

# Bibliography

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