C OMPOSITIO M ATHEMATICA
T ADAYUKI M ATSUZAWA S HUKICHI T ANNO
Estimates of the first eigenvalue of a big cup domain of a 2-sphere
Compositio Mathematica, tome 47, n
o1 (1982), p. 95-100
<http://www.numdam.org/item?id=CM_1982__47_1_95_0>
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95
ESTIMATES OF THE FIRST EIGENVALUE OF A BIG CUP DOMAIN OF A 2-SPHERE
Tadayuki
Matsuzawa and Shukichi Tanno@ 1982 Martinus Nijhoff Publishers - The Hague Printed in the Netherlands
Let
S2
=(S2, go)
be the unit2-sphere
in the Euclidean3-space E3
and let
D(r)
denote a cup domain ofS2
which is thegeodesic
disk ofradius r centered at the south
pole Q. Let À1(r)
denote the firsteigenvalue
of the Dirichletproblem
forD(r).
For’TT/2
r ’TT, wehave
2>Bi(r)>0.
However nice estimates ofÀ1(r)
seem to be un- known. Forexample,
the value r for whichÀ1(r)
= 1 is related to thestudy
ofstability
of minimal surfaces inE4 (see [1],
p.27),
and some estimate of r for whichÀ 1(r) >
1 wasgiven
in[1].
In this note we
give
estimates ofÀi(r)
for r which is near ’TT(Theorem 1.1).
If we let r tend to ’TT, thenThis agrees with a recent result
by
S. Ozawa[5] (cf.
Remark ii in the section2).
In the section
3,
as anexample,
we calculate our estimates forr = 7T -
10-50;
Contrary
to 2-dimensional case, the firsteigenvalue
of a cupdomain of a unit
3-sphere S’
isexplicitly
calculatable(see [4],
p.154, [2],
p.201).
We express our thanks to Mr. Muto for some comments.
1. The first
eigenvalue
of a cup domainLet
(x,
y,z)
be the canonical coordinates ofE3.
ThenS2 = {(x,
y,z);
X2 + y2 + Z2 = 1}.
Put P =(0, 0, 1)
andQ
=(0, 0, -1).
We denote the 0010-437X/82070095-06$00.20/096
Laplacian
onS2 by
A. Then it is known thatsatisfies
Af + 2f = 0
onS2 - {P, QI
for any constant C.f (z)
= 0 hasjust
two solutionsfor -1 z 1,
and solutionsdepend
on C. Letr =
r(x,
y,z)
denote the distance function fromQ
onS2.
Then-
-W-e- fix- ro(6 ç-ro m-) and
consider thecorresponding
cup domalnD(ro) = {(x,
y,z)
ES2; r(x,
y,z):5 ro}.
Then we have some constantC = C(ro)
such that the solutions y =y(ro), (3
=(3(ro)
offc(z)
= 0satisfy
yj8
= -cos ro.Namely
C is determinedby (3 ;
Let z = a be the
point
wherefc(z)
takes its maximum. Thenand the maximum value is
equal
to2/(1- a2).
We define a function Fon
D(ro) by
F is a
piecewise
smoothC’-function
onD(ro) vanishing
on theboundary
ofD(ro).
Therefore the firsteigenvalue Ài(ro)
of D =D(ro)
satisfies
Since the volume element of
D(ro)
is sin r dr A d0(where
0 denotesthe rotation
parameter
around thez-axis),
we getLet D = D’ U
D",
where D’ denotes the part of D for z - a and D"corresponds
to az (3.
Thenwhere the second
equality
follows from the fact that F vanishes on z =J3
and the normal derivative of F vanishes on z = a. Theref ore weget
THEOREM 1.1: Let
D(ro)
be a cup domain inS2.
Then thefirst eigenvalue À1(ro)
is estimatedby
where
/3, C,
a and A are determinedby
thefollowing :
PROOF: The first
inequality
of(1.4)
f ollow s from a calculationapplying 0(t)
= sin t to Theorem 3 in[3].
The secondinequality
of(1.4)
is(1.3). q.e.d.
REMARK i: Our
inequalities (1.4)
are most effective for ro= v. One merit of(1.4)
is that it enables us to calculateapproximated
values ofÀ 1(ro),
ro =*= ’TT.2. C alculation of A =
A(ro)
Here we calculate98
We
put
u =(1
+z)/(l - z),
a =(1
+a)/(1- a)
and b =(1
+(3)/(1- 0).
Then,
dz = 2dui(u
+1)2
andContinuing
calculations andapplying
we obtain the
following
PROPOSITION 2.1: For a =
(1
+a)/(l - a )
and b =(1
+p)/(1 - 0),
The last term of
(2.1)
is estimatedby
thefollowing
PROPOSITION 2.2: For a > 0 we have
Next we
study
the behavior ofA(ro)
as r0 --> 1r. We put 8 = 1- a andp = 1 -
{3.
Then we getetc.
By Propositions
2.1 and 2.2 we obtainand hence for ro --- > ir,
Therefore Theorem 1.3
implies
COROLLARY 2.3: Let
DE(P)
be anE-neighborhood of
apoint
P inS2.
Then thefirst eigenvalue Àt,E of S2- DE(P) satisfies
PROOF: We put E=1T-ro. Then
1+cosro=E2/2+...,
andÀi,e = À1(ro). Thus, (2.3)
follows from(2.2). q.e.d.
REMARK ii. A result of S. Ozawa
[5]
is stated asfollows;
Let(N, g)
be a compact 2-dimensional Riemannian manifold and let
DE(p)
be anE-neighborhood
of apoint
p of N. Then the firsteigenvalue À1,E
of(N, g) - DE(p)
satisfieswhere
Vol(N, g)
denotes the volume of(N, g).
Hisproof depends
onabstract
analysis,
and it is difficult to get thegeometric shape
of aneigenfunction corresponding
toAI,,,.
To get anapproximated shape
ofan
eigenf unction
thefollowing
observation is useful.Any
2-dimen-sional Reimannian manifold
(N, g)
islocally
conformal to(S2, go).
LetU be a
neighborhood
of p in N andlet §
be a conformal map from U intoU* = ÇbU
inS2.
We put P= e(p).
If Eo issufficiently small,
forany E Eo we have some
g = u(E)
such that theboundary
of an100
E-neighborhood DE(p)
of p in N ismapped by 0
intoDE+u (P ) - DE_,(P)
inS2.
The converse is also true. In the 2-dimensional case wehave another
special
propertythat,
forconformally
related metrics go andg* = hgo (h : positive function)
theLaplacians à
and A* cor-responding
to go andg* satisfy A*=(l/h)A/
for each functionf.
Therefore,
in an infinitesimaldomain,
h looks like a constant, and a function similar to F in the section 1 can be constructed in N.3. An
example;
ro= w - lo-50
As an
example
we calculate our estimate ofÀ1(ro)
for ro = 11’ -10-o.
Estimate in the introduction
corresponds
toREFERENCES
[1] J. L. BARBOSA and M. DO CARMO: Stability of minimal surfaces and eigenvalues of
the Laplacian. Math. Zeit. 173 (1980) 13-28.
[2] I. CHAVEL and E. A. FELDMAN: Spectra of domains in compact manifolds. Journ.
Funct. Anal. 30 (1978) 198-222.
[3] A. DEBIARD, B. GAVEAU et E. MAZET: Temps de sortie des boules normales et minoration local de 03BB1. Compt. Rend. Acad. Sci. Paris 278 (1974) 795-798.
[4] S. FRIEDLAND and W. K. HAYMAN: Eigenvalue inequalities for the Dirichlet problem on spheres and the growth of subharmonic functions. Comm. Math. Helv.
51 (1976) 133-161.
[5] S. OZAWA: The first eigenvalue of the Laplacian of two-dimensional Reimannian manifold (preprint; Department of Mathematics, Tokyo University, Japan).
(Oblatum 9-11-1981 & 29-VI-1981) Department of Mathematics Tokyo Institute of Technology Ohokayama, Meguro, Tokyo, Japan