C OMPOSITIO M ATHEMATICA
J ÜRGEN J OST
On the existence of harmonic maps from a surface into the real projective plane
Compositio Mathematica, tome 59, n
o1 (1986), p. 15-19
<http://www.numdam.org/item?id=CM_1986__59_1_15_0>
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15
ON THE EXISTENCE OF HARMONIC MAPS FROM A SURFACE INTO THE REAL PROJECTIVE PLANE
Jürgen
Jost@ Martinus Nijhoff Publishers, Dordrecht - Printed in the Netherlands
The
problem
ofrepresenting
thehomotopy
classes of maps of a closed Riemann surface Y- to the realprojective plane
P(endowed
with aRiemannian
metric) by
harmonic maps has been studied in detail in[3],
we use that reference as
background (with
thetopological
assertionscompleted by [1]).
In thepresent
note, we prove thefollowing
THEOREM : Let 03B8:
03C01(03A3) ~ 03C01(P)
be a non-zerohomomorphism.
(a) If
0 isnonorientable,
anyhomotopy
classrepresenting
0 contains aminimum
of
the energy.( b ) If
0 isorientable,
then at least two(of
theinfinitely many) homotopy
classesrepresenting
0 contain a minimumof
the energy.( c) If
P is endowed with its standard R P(2)
metricof
constantpositive
curvature,
then, given
xo~ 03A3,
po EP,
there are at least twoharmonic maps
inducing
0 andmapping
xo into po.REMARKS:
(i) (a)
is newonly
for the casesince otherwise 0 induces
only
onehomotopy
class. In anycase, 0
as ina)
canalways
berepresented by
a map from 1 onto a closedgeodesic
inP,
cf.[1],
and hence alsoby
a harmonic map. It is notclear, however,
whether - for anarbitrary
metric on P - such a map is energyminimizing.
(ii) Despite
the above Theorem and several nonexistenceresults,
cf.[3],
there is still a number of
homotopy
classes where the existencequestion
is open, most
notably
for oriented maps from nonorientable surfaces into P(except
those coveredby (b)).
The
proof
of the results is obtainedby modifying
theargument
of[4] (cf.
also
[2];
akey
idea is due to Wente[6]).
The idea is to construct a map v with16
where
is the energy
of v,
andEo
denotes the infimum of the energy over all mapsinducing
0. As in[4]
or[5],
we find a map : 03A3 ~ P withSince B is
nontrivial,
û is not a constant map, and hence we can findsome
x1 ~ 03A3
withLet k: U - C be a conformal chart on some
neighbourhood
U ofû(xl )
with
k((x1))
= 0. -By Taylor’s theorem,
k Où ) aB(xl, E)
is a linear map up to an error of orderO( f. 2),
i.e.for x E
aB(Xl’ E).
We now look at conformal maps of the form
The restriction of such a map to a circle
03C1(cos 03B8
+ i sin0)
in C isgiven by
where w = u + iv.
Therefore,
we can choose a and b in such a way that w restricted to this circle coincides with anyprescribed
nontrivial linear map. This map isnonsingular
ifW.l.o.g.
(otherwise
weperform
an inversion at the unitcircle).
Hence w can be extended as a conformal map from the interior of the circle
p (cos 0
+ i sin0)
onto the exterior of itsimage. (If equality
holdsin
(4),
then thisimage
is astraight
line coveredtwice,
and the exterior is thecomplement
of this line in thecomplex plane).
We are now in a
position
to define v.On 03A3BB(x1, c)
weput v
= û.On
B(xl, E - E2),we
choose a conformal map w into the extendedcomplex plane C
as above that coincides on~Bx1, ~ - ~2) with
thelinear map
(1/(1 - ~)) d(k 0 )(x1).
Weidentify C
withS2
via stereo-graphic projection
and letbe the standard
projection,
normalizedby 03C0(0)=(x1). (We
have ofcourse identified the conformal structure on P with the standard
RP(2)
structure, so that 03C0:
S2 ~
P isconformal).
We thenput v
= 03C0 ° w onB(xl, E - E2).
Finally,
onB(xl, E)BB(xl, E - E2)
weinterpolate
between û and03C0 ° w.
Introducing polar
coordinates(r,~),
we defineand
and
finally
It is
straightforward
to calculate(cf. [4]
and[5; 4.5]).
18
Therefore
The first term contributes
(cf. (3))
since
d(x1) ~ 0,
the second one at mostsince 03C0 o w is conformal of
degree 2,
and the third one is controlledby (5).
Altogether
and if we choose E small
enough, v
satisfies(1),
and theproof
ofa)
andb)
iscomplete, arguing
as in[4]
andobserving
that û and v exhaustenough homotopy classes,
cf.[3].
For the
proof
ofc)
we fixxo OE E
and po E P and minimize the energyonly
among maps u with(6)
does not constitute arestriction,
sinceby assumption
theisometry
group of the
image
istransitive,
and hence any w: E - P can be transformed into a mapsatisfying (6)
andhaving
the same energy,simply by composition
with anisometry
of P that mapsw(xo)
onto po.Therefore,
we can work in thecategory
ofhomotopy
classes with basepoint,
and theargument
of theproof
of(a), (b)
then shows that theminimum of energy is attained in at least two
classes,
since nowattaching
of a
sphere
leads to a new class in any case.This proves
(c).
Acknowledgement
1
gratefully acknowledge
thesupport
of my workby
the Centre forMathematical
Analysis
in Canberra and the SFB 72 in Bonn.References
[1] F. ADAMS: Maps from a surface to the projective plane. Bull. London Math. Soc. 14
(1982) 533-534.
[2] H. BREZIS and J.M. CORON: Large solutions for harmonic maps in two dimensions.
Comm. Math. Phys. 92 (1983) 203-215.
[3] J. EELLS and L. LEMAIRE: On the construction of harmonic and holomorphic maps between surfaces. Math. Ann. 252 (1980) 27-52.
[4] J. JosT: The Dirichlet problem for harmonic maps from a surface with boundary onto a 2-sphere with non-constant boundary values. J. Diff. Geom. 19 (1984) 393-401.
[5] J. JOST: Harmonic maps between surfaces. Springer Lecture Notes in Math., 1062 (1984).
[6] H. WENTE: A general existence theorem for surfaces of constant mean curvature. Math.
Z. 120 (1971) 277-288.
(Oblatum 27-VIII-1984) Mathematisches Institut Ruhruniversitât Postfach 102148 D-4630 Bochum BRD