AbstractLet $$\Omega {\subset } {\mathbb {R}}^2$$
Ω
⊂
R
2
be a bounded planar domain, with piecewise smooth boundary $$\partial \Omega $$
∂
Ω
. For $$\sigma >0$$
σ
>
0
, we consider the Robin boundary value problem $$\begin{aligned} -\Delta f =\lambda f, \qquad \frac{\partial f}{\partial n} + \sigma f = 0 \text{ on } \partial \Omega \end{aligned}$$
-
Δ
f
=
λ
f
,
∂
f
∂
n
+
σ
f
=
0
on
∂
Ω
where $$ \frac{\partial f}{\partial n} $$
∂
f
∂
n
is the derivative in the direction of the outward pointing normal to $$\partial \Omega $$
∂
Ω
. Let $$0<\lambda ^\sigma _0\le \lambda ^\sigma _1\le \ldots $$
0
<
λ
0
σ
≤
λ
1
σ
≤
…
be the corresponding eigenvalues. The purpose of this paper is to study the Robin–Neumann gaps $$\begin{aligned} d_n(\sigma ):=\lambda _n^\sigma -\lambda _n^0 . \end{aligned}$$
d
n
(
σ
)
:
=
λ
n
σ
-
λ
n
0
.
For a wide class of planar domains we show that there is a limiting mean value, equal to $$2{\text {length}}(\partial \Omega )/{\text {area}}(\Omega )\cdot \sigma $$
2
length
(
∂
Ω
)
/
area
(
Ω
)
·
σ
and in the smooth case, give an upper bound of $$d_n(\sigma )\le C(\Omega ) n^{1/3}\sigma $$
d
n
(
σ
)
≤
C
(
Ω
)
n
1
/
3
σ
and a uniform lower bound. For ergodic billiards we show that along a density-one subsequence, the gaps converge to the mean value. We obtain further properties for rectangles, where we have a uniform upper bound, and for disks, where we improve the general upper bound.