C OMPOSITIO M ATHEMATICA
J. P. G LASS
Theta constants of genus three
Compositio Mathematica, tome 40, n
o1 (1980), p. 123-137
<http://www.numdam.org/item?id=CM_1980__40_1_123_0>
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123
THETA CONSTANTS OF GENUS THREE
J.P. Glass
© 1980 Sijthoff & Noordhoff International Publishers - Alphen aan den Rijn Printed in the Netherlands
Introduction
In this paper we will examine theta constants of genus three and the
polynomial equations
thatthey satisfy.
Thetotality
of these(homogeneous)
relations defines aprojective variety
and we will showthat this
variety
can be definedby
a certain collection ofquartic polynomials.
In the process we willgain
a betterunderstanding
of thisvariety and,
inparticular,
relatepoints
on thevariety
to curves ofgenus three and limits of these. The chief tool used will be the
symplectic
groupSp(3, Z)
and its action on theta constants. We will also make use of Riemann’s calculations on the moduli of non-hyperelliptic
curves of genus three. In themain,
the resultsdepend
onlong
andcomplicated calculations,
most of which have been omitted.The reader is referred to
[7]
for details.Finally,
this work would not have beenpossible
without thehelp
of P.Swinnerton-Dyer (my
research
supervisor),
J.H.Conway
and S. Norton.’1. Preliminaries
We shall
only
beconsidering
theta functions of genus three withhalf-integer
characteristics. Thatis,
infinite series of the form:where z E
C’;
T ESf3
theSiegel
upper halfplane
of dimensionthree;
E, E’ E
Z3;
exp is theexponential function;
and t denotes transpose.This function is
analytic
in both the z and the T variables. In’ This paper is essentially a summary of the author’s Ph.D. thesis [7].
0010-437X18010110123- 16 $00.20/0
particular,
we shall be interested in theta constants, which are theta functions evaluated at z = 0. Thesymbol [,]
is called the charac- teristic of the function and isdesignated
odd or evenaccording
to theparity
of e . E’. Thef ollowing
reduction formula is valid:As a result we can restrict our attention to characteristics which consist of
only
zeroes and ones. Then there will be 36 even theta functions and 28 odd ones. These functions are even or oddaccording
to the
parity
of their characteristic. Hence the 28 odd theta constants all vanishidentically
in T and we are left with the 36 even ones, none of which vanishesidentically.
It is this set of 36 functions which will be at the centre of ourinvestigations.
There is an
important
group calledSp(3, Z)
and defined to be be:where a,
b,
c, d are 3 x 3integral
matrices. This group has itsprincipal
congruencesubgroups;
for n apositive integer:
as well as
Igusa’s
group:where for a matrix
A, Ao
denotes itsprincipal diagonal.
It is easy tosee that when n is even these two conditions are
equivalent
to:These definitions lead to the transformation formula for theta constants
([1]
p.227).
In fact in its mostgeneral
form itapplies
totheta functions and involves a transformation of the z
variable,
butwe will not
require
this. The formula is:where and in the obvious
context, E denotes the characteristic
[;,];
the rest of the notation of(1.3) being explained
below:(a) Sp(3, Z)
acts as a group ofbiholomorphic
transformations ongiving
an action of the group on the characteristics.(c) K(M)
is aneighth
root ofunity, depending
on Mwhere the E and E’ on the left of the terms are
transposed -
we will beconsistently negligent
aboutthis,
because it isalways unambiguous.
(e) 0[,E](,r)
is the theta constant0[§,](0, T).
The
operation
definedby (1.4)
has the property that M preservesevenness and oddness of the characteristic E. We shall often write theta characteristics as E instead of the ofhcial notation
[:,].
The 36 even thêta constants
(with
reducedcharacteristic)
define aprojective embedding
of thequotient
manifoldW31r(4, 8) (see [2]
p.(189).
The groupr(l)
acts on the set of reduced characteristicsby
formula
(1.4)
because of([3]
p.89):
We would like to be able to define an action of
r(l)
on the thetaconstants as a result of the transformation law
(1.3).
This is notpossible
in any obvious sense because of thesign ambiguity
inherent in the square root of
det(cT
+d).
However we can find anaction on the
P35 having
the thêta constants ascoordinates; by putting
the coordinates of
p35
and the 36 even theta constants in a fixedcorrespondence
andwriting:
where,
of course, if the reduction of a g - i mod 2changes
thesign
ofthe
appropriate theta,
then we introduce thatchange
ofsign.
Thisaction
corresponds
to that ofr(l)
onYe3.
Theproof
that this action isgenuine
is not difficult(see [7] Chap. 2).
Thef ollowing
theorempicks
out two
important subgroups.
THEOREM 1.1:
(a) If
M= (f ))
EF(2)
thenexp(cPE(M» =::tl for
all reduced evencharacteristics E
if
andonly if
M Er(2, 4).
(b)
Let M Er(2),
then we have theidentity
for
all reduced even characteristics E andfor
some non-zero constantC
if
andonly if M OE ± T(4, 8) (i.e.
either M or -M is inF(4, 8».
The
proof
isessentially
contained in[1]
partII,
p. 232.2. The
permutation representation
It is a well-known fact that
r(I)/r(2)
isisomorphic
to the sym-plectic
groupSp(3, F2),
which we shall refer to asS6(2). By
formulae(1.4)
and(1.5),
the groupr(1)/r(2)
acts on the 28odd,
reduced characteristics and the 36 even, reduced characteristics. It can be shown that these twopermutation representations
areequivalent
torepresentations
ofS6(2)
to be described below. Theproof
is a con-sequence of the fact that
S6(2)
hasunique subgroups
of indices 28 and 36 up toconjugacy. (See [7] Chap.
2 fordetails).
The group
S6(2)
can bethought
of in thefollowing
way: thesymmetric
groupSg
sits inside as asubgroup
of index 36. A con-venient notation for a set of coset
representatives
is obtainedby taking
the numbers(l, 2, ..., 8)
andpicking
out subsets of four with theircomplements,
so that12M
is the same as## (and
these areindependent
oforder),
thusgiving i(â)
= 35objects.
Theseobjects
arecalled bifid maps
(this terminology
seems to haveoriginated
withCayley)
in the group and form a set of cosetrepresentatives
of58
inS6(2).
Once
again
consider the set(l, 2, ..., 8)
and also theobjects ij
where
i 0 j
bothbelong
to the set, of which there are 28. ThenS6(2)
acts on the 28
objects by
therecipe:
(a)
apermutation
ESg sends ij
toi"ja’
(b)
a bifid map«é"d fixes ij
if iand j
lie onopposite
sides of the bar in the bifid map, and otherwisecomplements ij
in either the numera- tor or the denominator(whichever
isappropriate).
Now construct 36
objects
from(1, 2,..., 8) by taking
the!d) objects
lë’2d together
with thesymbol
00. There is a deliberate confusion herebetween the bifid maps and these
objects
because the action to bedefined here is
really S6(2)
on its cosets moduloSg.
Define the action ofS6(2)
on the 36objects
as follows:(a) 00
is fixedby
all ofSg,
but the bifid map9&Cd
send 00 to theobject efgh.
(b)
o- ESg
sends theobject gkd
to""’d;
whereas if$fl%
is a bifidmap and an
object,
in the case that{a, {3, y,,bl splits
as 3 :1 overthe bar in
’efëghd
the latter isfixed,
but if itsplits
2: 2 we havegenerically
We now have
permutation representations
ofS6(2)
on both 28 and 36 letters in thishighly
convenient form.Corresponding
to these arethe actions of
F(I)IF(2)
on theodd,
reduced theta characteristics and even, reduced theta characteristicsrespectively.
As mentionedbefore,
these actions areisomorphic
in theirrespective pairs.
3.
Equations
between thêta constantsThe book
[3] (p. 49) gives
aprocedure
forfinding degree
fourrelations between theta constants, and we shall follow this. There are
three basic types of
relations, involving
linear combinations of thefollowing objects, respectively (1)
fourth powers of theta constants(2) products
of squares of theta constants(3)
tetrads of distinct theta constants. The coefficients arealways
:L- 1. Thepermutation
part of the action(1.6)
now hasexplicit
form when weidentify
the 36 even, reduced characteristics with theobjects 00, =.
We will write down the relations asequations
in these latter-mentionedobjects.
Now recall that the thêta constants embed
W31F(4, 8)
inp35.
Hence theequations above,
takentogether,
define avariety
which we shallcall
V3. Also,
thetotality
ofhomogeneous
relations in the theta constants defines a smallervariety,
which we shall callS3.
It is clearthat the group action
(1.6)
preserves relations between the theta constants.Moreover,
it is obvious from theoriginal
définition of thequartics
listed above thatthey
also arepreserved by r(l). (See [3]
p.49 for the
original
form of thesequartics).
Thisimplies
thatF(l)
preserves both
S3
andV3.
We wish toinvestigate
thepossible configurations
ofvanishing
coordinates onV3
and for this purpose weonly
need thepermutation
part of theF(l)
action.DEFINITION:
(a)
Atriple
of distinct even characteristics is called even(resp.
odd)
if the vector sum of the three is even(resp. odd)
in the usualdot-product
sense. This isequivalent
to the existence of an element ofS6(2) sending
thetriple
to(oo, X, Y)
where the numerators of X and Y intersectevenly (resp. oddly).
(b)
A set of coordinates inP35
is called avanishing
set if thereexists a
point
on V3having precisely
those coordinatesequal
to zero.It is clear that
S6(2)
isdoubly-transitive
on the 36-set(Sg
is thestabiliser of
oo)
hence the first twovanishing
coordinates may be chosen in asingle
way.LEMMA 3.1: l
(a)
Thevanishing of 00
andlël-à together implies
thevanishing of
acoordinate
oddly-related
to these two in the senseof
thedefinition.
(b)
Thevanishing of 00
and’ë’-d
and"é" implies
thevanishing of
either
{abc}
or{ fgh );
where{abc}
standsfor
the sextetof
coordinates :(m, abcd, abce, abcf, abcg, abch).
(c) If
avanishing
set contains more than six coordinates but doesn’t contain a set(with
nineelements) of
theform (abc)
Ulfgh}
then it contains a
complete
setof
theform (ab);
where(ab)
standsfor
the set
(-, abxy) of
16 coordinatesfor
a, bfixed
and x, y variable.(d) If
avanishing
setstrictly
contains a setof
theform {ab}
then itcontains at least 18 coordinates
and,
moreover, contains a standard 9-set(abc)
Utfghl.
The
proofs depend
onchoosing
the correctequations
to work with.For
example,
in(a)
useequations
oftype (3)
and for(b)
useequations
of type
(2).
In order to find the structure of the
larger vanishing
sets, we haveto recode the coordinates. This is because the number of different
possibilities
becomes far toolarge
to cope with in the present nota- tion. This"super-notation"
and its uses were discoveredby
J.H.Conway.
Pick out the
following
nine coordinates and relabel them as fol- lows :Note that these nine coordinates
actually
form a9-set; namely {123}
U(456).
Nowsplit
the numbers1,..., 9
into three blocks:The
remaining
27 coordinates are codedby
a choice of one numberfrom each of the three blocks. If we choose 9
(from
the thirdblock)
then we define:
On the other
hand,
we define:where i’ and i" form the
complement
of i in(1, 2, 3)
andj’, j"
thecomplement of j
in(4, 5, 6).
We can now think of the residual 27 coordinates as
points
of a cubein
3-space, by letting (1,
2,3); (4, 5, 6); (7, 8, 9)
be coordinates on the three coordinate axes. Before we can makegeneral geometric
state-ments about
vanishing
sets vis à vis thecube,
we will need thef ollowing
result.PROPOSITION 3.1: The
full
groupof automorphisms of
the cube canbe realised
by
elementsof S6(2)
whichfix
the set([1], [2], ..., [9]).
The
proof
of thisproposition
isstraightforward.
We are now in a
position
to prove thefollowing
lemma.LEMMA 3.2:
Suppose that, in
the newnotation,
the coordinates[1], ..., [9]
all vanish.Then,
on thecube, if
any two collinearpoints vanish,
so does the thirdpoint
on that line.Moreover, if
anypoint
vanishes then two
of
the three linespassing through it
also vanish.PROOF: Because of the
proposition,
weonly
have to prove these results once on the cube. For thecollinearity result,
take the line[148], [248], [348]
which coordinates in the oldlanguage
are$$, iiÔ,
#$ respectively.
Now, exhypothesi,
4568 = 7568 = 0 and 00=0. Then the linearquartic
codedby (568) gives
the result.For the second part, suppose 1248 = 0 =
[347].
The three linesthrough
it are:[347], [247], [147]; [347], [357], [367]; [347], [348], [349]
which in old coordinates are
respectively: 1248, 1348, 2348; 1248, 1258, 1268; 1248, 3568,
3478. Now consider thebiquadratic equations (without
their squarepowers):
Using
the knownvanishings
we getNow combine this with the
collinearity
result and we haveproved
theoriginal
claim.Q.E.D.
We can now make
simple geometric
observations about the cube to determine allvanishing
setscontaining [1],..., [9]
and hence allvanishing
sets.Suppose [1],..., [9]
all vanishalong
with onepoint
of thecube,
which we may take to be a cornerpoint. Then, repeatedly using
lemma
3.2,
we see thatonly
three cases occur: either one whole facevanishes,
or twoadjacent
facesvanish,
or three faces which meet in apoint
vanish.Coupling
this with lemma3.1,
we are able to enunciate thefollowing.
THEOREM 3.1: The
only possible vanishing
sets have thefollowing
sizes :
To finish off this section we shall describe one technical result essential in the
sequel.
Notsurprisingly,
theequations defining
V3give
more information about the fourth powers of coordinates than the coordinates themselves. Thatis,
if we denoteby 0’
theregular
map from
P35
to itself which raises each coordinate to its fourth power, then we will be able to work moreeasily
with thevariety 0’(V3). Fortunately,
it turns out that thequotient
groupr(2)1±r(4, 8)
is transitive on the fibresof 04
when restricted to V3. Hence in orderto compare V3 and
S3
we may look at theirimages
under 04 . Theproof
of thistransitivity depends
uponsplitting
into two cases:multiplication
of coordinatesby
± 1(governed by equations
of type(3))
andmultiplication by
i. Theequations
of types 2 and 3greatly
restrict the
possible configurations
ofmultiplications
of coordinatesby
fourth roots ofunity.
It remains to be shown that thepossibilities
are cut down to
precisely
thosegenerated by
the groupf(2)/±r(4,8).
For
example, F(2,4)/--ÈF(4,8)
is the group whichmultiplies
coor-dinates
by ± 1,
and has order22°.
An element of this groupqcting
onan
equation
of type three either fixes each term, ormultiplies
all threeby -1.
Hence theproduct
of any two terms’sign changes
must beidentically
1. This can all be translated to the vector spaceF36
where the group generates asubspace
and thissubspace
is cut outby hyperplanes
of the form: a sum of 8 coordinatesequals
zero(cor- responding
to apair
of terms of anequation).
See[7] Chapter
3 fordetails. Of course this
proof only
works forpoints
on V3 with no zerocoordinates;
for as soon as coordinatesvanish,
the groups involved getsmaller;
but then theequations change and,
infact, everything
works out as
expected.
4. Classification of the
points
of V3In this final section our aim is to prove that V3 =
S3 and,
in theprocess, we shall
classify
thepoints
ofS3
vis à vis thepoints
of W3.The
analysis proceeds
as follows: first we look atpoints
with no zerocoordinates,
thenpoints
with one zero coordinateand, finally, points
with six or more zero coordinates.
Our first concern is with
non-hyperelliptic
curves of genus 3 and these are allnon-singular plane quartics.
Thebackground
to our workderives from the papers of Riemann
[4,5]
and theirsequel by
Weber[6].
In these papersthey
describe therelationship
between the 28bitangents
of aplane quartic
and the 28 odd reduced characteristics.After some
long
calculationsthey
arrive at a sextet ofcomplex
numbers which serve as "moduli" for
plane quartics.
In thesequel
acertain fixed
pairing
of the coordinates Xi inp35
with the 36 evenreduced characteristics is used
(we
shall not bother to write it downexplicitly). Following
Weber([6]
p.108)
we define thefollowing.
Let
(x,, ..., x36)
be apoint
of V3 with the property that none of the coordinates is zero. Now define ninecomplex
numbers:We note that if T E
lit’3
represents anon-hyperelliptic
curve then thecorresponding point (0[l#](T), ...)
of V3 has novanishing
coordinates(by
a combination of the Riemannvanishing
theorem and Riemann-Roch).
The
proof
of thefollowing
theorem involveswriting
down hordes ofskilfully
chosen rational functions of the a,making
use of theequations defining
V3, andmultiplying
lots ofexpressions together.
THEOREM 4.1: Given
(xi, ..., X36)
in V3 with all x;# 0, every ratiox§lxf
is a rationalfunction of
the nine constants ai,a), aN defined by (4.1).
In
fact,
there are formulae which express thea’!
as functions of theai,
ai (see [6]
p. 108 et.seq.)
Thus it is the a;,a)
which serve as "the moduli". These f ormulaeonly
determine thea’i
up tomultiplication
of all three of them
by -1 but,
because the rational functions in the above theorem are invariant underthis,
it does us no harm.In Weber’s
development
of thetheory,
anon-hyperelliptic
curve isput into a normal form
namely,
the rationalisation ofwhere
el, e2, e3
are linear functions of the coordinates tl, t2, t3 in p2.They
are definedby
theequations:
The strategy
is, given
P on V3 with no zerocoordinates,
to definethe a
by (4.1)
and reverse Weber’s steps togive
a curve. This isalmost
possible,
in the sense that all the necessary conditions areopen so that at worst we come out with a limit of curves. Let us now
give
the details. Define a rational mapwhere 1,=, (tiei)"’
stands for the rationalised version of that curve(a quartic);
theei
are definedby (4.3); and,
as mentionedpreviously,
theai,
ai
determine thea ’;2.
Set X =
«/1«(6).
It is clear that the Zariski closureX
of X is anirreducible
variety.
Now define a Zariski open subset Uof X by
thefollowing
open conditions:(1)
thecurve 1]=1 (tiç)1/2
isnon-singular.
Call thisquartic
C.(2)
the seven lines tl= 0, t2
= 0, t3 = 0,tl + t2 + t3 = 0,
altI + a2t2 + a3t3 =0, a 1 t
1 +a 2’t2
+a3t3
=0, a ï t
1 +a 2 t2
+a3t3
= 0 and allbitangents
toC.
(3)
each subset of three lines from the seven in(2)
has the pro-perty : the
points
of intersection with C do not lie on asingle
conic.The last condition is the
only
one that isn’tobviously
open. This condition isimportant
becausegeometrically
it means that the other 21bitangents
can be constructed out of these seven. Toverify
theopenness, reduce first to the case where all
triples
of lines arelinearly independent-being
an open condition this isacceptable.
Thus it remains to prove that: if aquartic
in p2 has t1 =0, t2
=0, t3
= 0 asbitangents
thenthe condition that their
points
of intersection lie on a conic is a closedone. The
proof
of this isstraightforward. (See [7] Chap.
4 fordetails).
Finally,
take P on V3 with no zerocoordinates,
form the a;,a ), a
by (4.1)
and thus apoint
ofX by (4.4).
Now U isstrongly
dense inX
hence we obtain a sequence of
non-hyperelliptic
curves such thattheir ai,
a), a’!
convergestrongly
to those for P(the ai needing
ascintilla of
analysis). Invoking
theorem4.1,
and thetransitivity
des-cribed at the end of section
3,
we haveproved
THEOREM 4.2:
Any poirt
Pof
V3 with no zero coordinates is the strong limit in V3of
a sequenceof points corresponding
to non-hyperelliptic
curves. Inparticular,
P is inS3.
Hyperelliptic
curves of genus threealways
haveprecisely
onevanishing
theta constantand,
as we shall see now, the reverse is also true. In thehyperelliptic
case there is a very obvious choice for the modulinamely,
the five un-normalisedbranch-points. By choosing
aspecial
canonicalhomology basis,
these five branchpoints
can beexpressed
as rational functions of even theta constants in thathomology
basis. Moreprecisely, given
fivecomplex
numbers Ikl, lk2, À3, A4, Às distinct from0, 1
and eachother,
define ahyperelliptic
Riemann surface of genus 3 as a two-sheeted branched cover of P’ in the standard way. On it there is the
f ollowing
canonicalhomology
basis:
the dashes
indicating
that thepath
is in the lower sheet. It is then asimple
matter to compute the values(being half-periods)
of theAbel-Jacobi
map 0
at the branchpoints.
All theta functions con-sidered in this
paragraph
are evaluated at the T EW3
definedby
theabove canonical
homology
basis. Now examine thepullbacks
of thetheta functions
O[:,](cf>(P), T). Knowing
the valuesof 0
at branchpoints
as we do we can work out at which branchpoints
anyparticular
thêta vanishes. Look forpairs
of thetas whosequotient
hasa double zero at 0 and a double
pole
at 00(i.e.
the branchpoints
above0,oo).
These are constantmultiples
of thecovering
map zand,
plugging
in values like P =z-’(,kl)
we get, forexample
In the book
[3]
p. 186 it is shown that for the above canonicalhomology
basis0[’,O’,](O,,r)=O.
Given apoint
P on V3 with onevanishing
coordinate(the
onecorresponding
toB[;°;],
and called X25 inour fixed
ordering)
define 5 constants,using
the formulae for the Ài described above:Using
theequations
for V3 with0[’,",]
= 0 we can show that: for thepoint
P, every ratiox1/x1 (jO 25)
can beexpressed
as a rationalfunction of the An. This is
just
like theorem 4.1 and isproved
in thesame way. Now the Ai in
(4.5)
define ahyperelliptic
curve and henceits theta constants for our
special
canonicalhomology
basis. Thus04(p) = 04 (point
fromhyperelliptic curve)
andby
thetransitivity
result from the end of section 3 we have
proved
that:THEOREM 4.3:
Any point
Pof
V3 withprecisely
onevanishing
coordinate is a
point of S3 corresponding
to ahyperelliptic
curve.It remains for us to consider the
points
of V3 with several zero coordinates(vide
theorem3.1).
Because allvanishing
6-sets areequivalent
under the group, we may concentrate on the six coor-dinates F =
(0[ ]É]]0[ (1]]0[ ](]] 0[É((]0[1]]]0[(]]]).
Recall the formula:where
TT2 E 7If2, T E 7If1.
It motivates the definition of thecomposite
map:
where the first map is the
Segre embedding
with coordinates orderedso that the
split
on thediagonal (mentioned above)
isrespected;
andthe second map is the
identity
map where we set the six coordinates of Yequal
to zero. The theta constants of genera one and two define varieties inp2
andp9
ofrespective
dimensions one and three. Call themS,
andS2 respectively.
In each case theequations defining
themare easy to write down:
SI
isjust
the curve x4 -y4 _z4
= 0: whereasS2
is definedby
30quartics.
These 30quartics
aregenerated by
aprocedure quoted
in the book[3]
p. 43.Take a
point
P of V3 with the coordinates of Yequal
to zero.Letting 02
be theregular
map from p35 to itself which squares eachcoordinate,
1 claim.PROPOSITION 4.1: There is a
point Q
inS2
xSI
such that(}2(p) = (}2( cP( Q».
Henceby transitivity
on thefibres of
02(see
endof
section3)
we have that Pbelongs
to thesubvariety O(S2
xSI) of S3,
or to oneof
its translates underr( 1 ).
The
proof
of thisproposition
is not difficult. Once we haveQ
in 2 with therequired
property it is asimple
matter to findequations implying
thatQ
is inS2
xSi.
The rest of theproof
involvesa
counting
argument,namely,
to show that there areenough biquadratic equations (those
of type2),
with the coordinates of Yequal
to zero, toimply
all the"interchanges" required by
theSegre embedding
(at the 0’-Ievel which issufficient).
The
higher vanishing
sets allgive points
which translate under the group action intospecial
subvarieties ofI>(S2
xS,).
These sub- varieties are the obvious ones obtainedby killing
coordinates inS2
andSI.
This
completes
our aim: to prove that V3 =S3 and,
at the same timeclassify points
ofS3.
Added in
proof
1 now believe that Theorem 4.2 can be
improved
upon in thefollowing
sense.Namely,
that to apoint
with novanishing
coor-dinates in V3 there
actually corresponds
anon-hyperelliptic
curve.The choice of the said curve
being obvious,
thedifficulty
lies inshowing
that it isnon-singular.
1 am indebted to Mr. Patrick Du Valfor
showing
me thisproof.
A papercontaining
the result and itsproof
has been
accepted
forpublication.
REFERENCES
[1] J.I. IGUSA: On the Graded Ring of Theta Constants. I and II, American Journal of Mathematics 86, 88; 1964, 1966.
[2] J.I. IGUSA: Theta Functions. Springer Verlag. 1972.
[3] H. RAUCH and H. FARKAS: Theta functions with Applications to Riemann Surfaces. Williams and Wilkins. 1974.
[4] B. RIEMANN: ’Zur Theorie der Abelsche Functionen für den Fall p = 3’. Gesam- melte Werke. 1st. Auflage.
[5] B. RIEMANN: ’Ausdrücke der Klassenmoduln bei p = 3 durch Thetaquotienten fur
die Nullwerthe der Argumente’. Nachträge to Riemann’s Werke.
[6] H. WEBER: Theorie der Abelschen Functionen vom Geschlecht drei. Berlin 1876.
[7] J.P. GLASS: Theta Constants of Genus Three. Thesis. Cambridge University. 1977.
(Oblatum 2-111-1978 & 20-XI-1978) School of Mathematics
University of New South Wales
Sydney 2033
Australia