Groupe de travail
d’analyse ultramétrique
R OBERT R UMELY
Capacity theory on algebraic curves and canonical heights
Groupe de travail d’analyse ultramétrique, tome 12, n
o2 (1984-1985), exp. n
o22, p. 1-17
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CAPACITY
THEORY
ON ALGEBRAIC CURVES AND CANONICAL HEIGHTSby
Robert RUMELY(Y. AMICE,
G.CHRISTOL,
P.ROBBA)
12e
année, 1984/85,
n°22,
17 p.13
mai1985
This note outlines a
theory
ofcapacity
for adelic sets onalgebraic
curves. Itwas motivated
by
a paper of D. CANTOR where thetheory
wasdeveloped
forP~ .
Complete proofs
of all assertions aregiven
in amanuscript [R],
which Ihope
topublish
in theSpringer-Verlag
Lecture Notes in Mathematics series.The
capacity
is a measure of the size of a set which is definedgeometrically
but has arithmetic consequences.
(It
goes under several names in theliterature, including
"Transfinitediameter", "Tchebychev constant",
, and "Robbinsconstant",
,depending
on thecontext.)
The introduction to Cantor’s paper contains several niceapplications,
which I encourage the reader to see. I havemainly
been concern-ed with
generalizations
of thefollowing
theorem of Fekete andSzegö [F-S].
T?IEOREI. - Let E be a
compact
set inC ,
stable undercomplex conjugation.
Then,
(A)
If thelogarithmic capacity is 1 ,
there is aneighborhood
U ofE which contains
only
a finite number ofcomplete
Galois orbits ofalgebraic
inte-(B)
Ify(s) ~ 1 ,
then everyneighborhood
of E containsinfinitely
many com-plete
Galois orbits ofalgebraic integers.
Some
examples
ofcapacities
are : for a circle ordisc,
its radiusR ;
for a linesegment, 2014
of itslength ;
for twosegments I- b , - 3’’]
uMb - a) ;
for a
regular
n-gon inscribed in a circle of radiusR,
The
capacity y(E)
in the theorem should moreproperly
be called the"logarith-
mic
capacity
of E withrespect
to thepoint ~
n. Thegeneral
definition of ca-pacity
will begiven
below. Ofequal significance
with/(E)
is the Green’s func- tionE) .
Recall that thisis anonnegative function,
harmonic inE ,
with value 0 on E and a
logarithnic pole
at , such thatI
is bounded in a
neighborhood
of ~. TheFekete-Szegö
theorem isproved by
cons-tructing
monicpolynomials
whose normalizedlogarithm P~ I
closely approximates G(z, ~
;E) .
Thealgebraic integers
in the theorem arethe roots of the
polynomials.
(")
RobertRUMELY, Department
ofMathematics, University
ofGeorgia, ATHENS,
GA30602 (Etats-Unis).
The condition in the
Fekete-Szegö
theorems that the members bealgebraic integers
is a restriction on their
conjugates
at finiteprimes, just
aslying
in aneighborhood
of E is a restriction at the archimedean
prime.
CANTORgeneralized
the classicaltheory
in several directions,First,
he gave an adelicforraulation, placing
allthe
primes
on anequal footing. Second,
he defined thecapacity
of an adelic setwith
respect
to severalpoints,
notjust
one, which gave thetheory
smooth behaviorunder
pullbacks by
rational functions,(In
the classicaltheory
overC ,
ifF(z)
is a monic
polynomial
ofdegree
n , then~(F (E))
=’{(E) l/n .) Thirdly,
he for-mulated versions of the
theory
withrationality
conditions : forexample,
in theFekete-Szegö theorem,
ifR ,
then the numbersproduced
inpart (B)
could betaken to be
totally
real.(This special
case wasoriginally proved by
R.ROBINSON.)
There were some errors in the
proofs
of therationality,
but no doubt the resultsare true. Cantor’s definition of the
capacity
of a set withrespect
to severalpoints
wasquite novel, involving
the value as a matrix game of a certain symme- tric matrix constructed from Green’s functions.The
functoriality properties
of Cantor"scapacity suggested
that it should bepossible
to extend thetheory
to all curves. Indoing
so, I havegiven
a differentapproach
to theoriginal results,
and found someinteresting connections
with Néron ’ s canonicalheights.
Notation. - Let C be a
smooth, geometrically
connectedprojective
curve definedover a number field K . If v is a
place
ofK ,
we writeK
for thecompletion
of K at
v ,
.K
will be thealgebraic
closure ofK , Kv
thealgebraic
closureof and
K
thecompletion
of thealgebraic
closure of K .Gal(K/K)
willbe the usual Galois group ; the group of continuous
automorphisms
ofK /K .
If v isnonarchimedean,
and lies over a rationalprime
p, the absolute value onK v
associated to vwill be normalized
sothat
if v isarchinedean, then x
+yi)
v =( x
+y2)~ . Thus,
we areusing
the absolute norma-lization for our absolute values. These absolute values extend in a
unique
way to absolute values onthe # , which
we continue to denoteby jxj
v . For any fieldF , C(F)
will mean the set ofpoints
of C rational overF ,
andF(C)
thefield of
algebraic
functionson ~
rational over F.Classical
theory. -
In the classicaltheory,
if E CC
is acompact set,
thenits
capacity (with respect
to thepoint ~ ~
isgiven by
theequivalent
definitions(transfinite diameter)
(Tchebychev constant)
(logarithmic capacity)
(equilibrium potential)
(Robbins constant) .
Eore a
probability
measure is a positive Measure of total mass1,
andis the Gr eexl’s function of u.nbounded
cor:ponent
of thecomplement
of E . If03B3(E) ~ 0 ,
y there is aunique probability minimizing
theintegral defining
V(E) ,
y and Green’s function isgiven by
Throughout
thefollowing,
we willimplicitly
assune thatY’(~)
0 .(This
is thecase, for
example,
if E contains a one-dimensionalcontinuum.)
Fornon-compact
sets
F,
thecapacity
and Greeii’ s function are definedby
llimits:iriportant
class of sets whosecapacities
are known are PL-domains(Polynomial
Leuniscate If is a donic
polynomial
ofdegree
n , y then the set E =C ; I I ~ R}
hascapacity ~ ~(~ ) -
This is because the Green’s function is for andV(E)
can be read off as theresidue of the Green’s function In
particular,
thecapacity
of a circle isits radius.
The
equality
of the various definitions of wasproved
andEach definition of
y(E)
is useful in a different context. Its role as theTcheby-
chev constant
gives functoriality
underpullbacks.
Its definition in terms of the measure allows the construction ofpolynomials
whoselogarithm approximates
thefunction. Its
expression
in terns ofV(E)
allows it to becomputed
for 8anysets,
and was the definition which CANTORgeneralized
in the adelictheory.
The c ano nic al dis t anc e. - In all definitions of
capacity
in the classical case, the crucialingredient
is the presence of the distance functiony~
which has apole
at co . The connection between tllegeouetric
and arithmetic sides of thetheory
cones froLi the fact that the distance function can be used to
decompose
the absolute value of apolynomial
in terws of its roots.In
constructing
atheory
ofcapacity
on curves, thestarting point
is to find si- uilar functions which can be used todecompose
the v-absolute value ofalgebraic
functions onS(K )
for everyplace
v and every curve C. I call such functions"canonical distance
functions", although
the tern should be understoodguardedly
since
they
do not ingeneral satisfy
thetriangle inequality~
outonly
a weak ver-sion of it. For any
place
v, and anypoint ç
E there is a canonical dis- which isunique
up toscaling by a constant,
satisfies thefollowing properties :
i°
(Positivity)
Forz2
eB
we have 0 [z1,z2JÇ; co ,
21 . = 0 if,
andonly if , zl = z2 .
2°
(Normalization at ~ ~
Letg(z)
eK (c)
have asimple
zeroat ~ .
Thenthere is a constant
c > 0
such that for anyz2 E C(K ) B (~ ~
3° (Symmetry)
4° (Continuity) [Zl’ Z2]Ç
is continuous as a function of two variables. If vis
archimedean, log[z1, z2],
is harmonic in each variableseparately;
if v isnonarchimedean, log[ zl ’ Z2],
islocally
constant in eachvariable, provided
~2 °
5°
(Decomposition
offunctions)
Iff( z)
EK (C)
has zeros andpoles (with
nulv
tiplicity)
ata1’
... ,an
and’1’
... ,’n respectively,
then there is aconstant
cf
so that for all Z E wheref(z)
isdefined,
6°
(Galois invariance) If C
is defined over EC(K ) ,
then forall
7°
(Weak triangle inequality)
There is a constant IIdepending only
on C andv such that
z2]03B6, [Z2 ’ z3JÇ) .
isdean and C has
nondegenerate
reduction at v , y then M = 1 .Properties 2° ,
4° weak version of5°
characterizeZ2B: .
One canshow that for any
Z2
~C(K )
there is a functionfez)
~ K(C)
whoseonly poles
are
at 03B6
and whose zeros all lie in aprespecified
ball aboutz2. Furthernore,
after
fixing
auniformizing parameter g(z) at §
asin property
2° call such anf(z)
normalized ifl f(z)
=1 ,where
n =deg(f) .
ThenThe existence of the limit is a consequence of a naxinun nodulus
principle
foralgebraic
functions on curves. Thesymmetry
coues from Weilreciprocity.
Property
5°suggests
a connection with Neron’s canonical localheight pairing ;
and in fact Neron’s
pairing
and the canonical distance can be defined in terns of each other. Recall that Néron’spairing
is areal-valued,
bilinear functionv on divisors of
degree
0 inC(K ) having coprine support.
It has theproperty
that if D’ =
div(f )
for some functionf(z) , then, writing log v
x for the lo-garithu
to the basep(v) ,
wherep(v)
is the rationalprime lying
below v( t aking p(v)
= e if v= ~ ),
we haveTt is continuous in both
variable~.,
and thus can beregarded
asextending
func- tional evaluation tononprincipal
divisors.(It
should be noted that there is sone variation in the literatureconcerning
the normalization of Néron’spairing.
Herewe are
requiring
it toapproach
on thediagonal,
and to take rational values if v isnonarchinedean).
Thefollowing
clean formulation for the relation betweenthe canonical distance and Neron’s
pairing
was shown to neby
B. GROSS : There isa constant
C, depending
on the choice ofuniforuizing parameter g(z) at
such that
This
expression
allows the finerproperties
of Néron’spairing given by
inter-section
theory,
to be transferred to the canonical distance.The facts and formulas above arose frou a
study
of the classicaltheory
whosegoal
was first toput
thepoint ~
on anequal footing
with thepoints
ofand then to find
analogues
for all v and all C . In a number of casesspecial
formulas turned up which
suggested considering [z1,z2]03B6
as a distance. Since these formulas alsogive
noreinsight
into the nature of the canonicaldistance,
yit seeus worth
presenting
then. In all cases, we obtain anexpression
of the formwhere
((zl ’ z2))v
iscontinuous, nonnegative,
andbt)’lnded,
with asimple
zeroalong
thediagonal.
Special formulas for the canonical distance. -
The formulas are more or lessexplicit, depending
on the genus of e .Genus 0 :
projective
line.- Archimedean case. 0n one has the
spherical
chordalmetric, given
forz2 E 2.- by
Note that , is invariant when both
z1
andz2
areinverted,
andis
uniforuly
bounded aboveby
1 . When theplane
is identified with asphere
ofdiameter 1
by stereographic projection,
it is thelength
of the chord fromzl
to
z2 .
For notationalcompatibility
with curves ofhigher
genus, writeObserve
z2]~
=IZ1 - z2|, while
for03B6 ~ ~,
wheref(z): (1
+I çI2)i/(z - ,) .
Weemphasize
that[zl’
isonly
determined up to
scaling by
a constantc(~)
foreach ~ .
-
Nonarchimedean
case. For finiteprimes
theappropriate analogue
of the chordal metric is thep-adic spherical distance, given
forz. , z2
eK by
and
again putting ((zl ’ z2))V = Bzl ’ z211v ’
we haveFrom these
expressions properties
1°-7° followeasily.
All curves,
good
reduction. -IfC/K
is any curve, then for v of K where e hasnondegenerate
reduction withrespect
to thegiven embedding
in thereis an
analogue
of the formulaabove,
withI(z~ , .z~))~ given by
the v-adicsphe-
rical metric on This is defined as
follows ?
fix asysteu
of affine coordi-on
Then,
forz2
E if there is somepatch
in which both
z
andz
haveintegral coordinates,
(using
thecoordinates
in thatpatch).
Otherwise~z1, z2~v
= 1 . It is easy to check that!lz1, Z2~v
is invariant under achange
of coordinates inwhere 0
is thering
ofintegers
inK .
Genus 1 :
Elliptic
curves.- Archimedean case. We use the fact that an
elliptic
curve overC,
is iso-morphic
to acomplex
torus03C92]. NÉRON
hasgiven
anexplicit
formulafor the local
height pairing
in terns of the Weierstrass03C3-function,
andby
mo-difying things slightly
weget
the canonical distance. Letbe the 03C3-function for the lattice L ==
[03C91, 03C92].
WriteT;
for theperiod
of(,(u)
=d/du(log o(u))
under03C91,
andTt
for theperiod
ofunder 03C92,
gothat
by
theLegendre relation, 11
03C91 -Tj
a) == M . Given u we canuniquely
u1 + 03C92 u
withu , u2
e R . Define1l(u) = T. u + Tj u ,
and let
i ~/ B
Then
k(u+
=-k.(u) ,
andk(u + UJ2)
=-k(u) ,
so thatI
isperiodic L»iG [L]).
Letu and u correspond
toz
andz
underthe
isomorphism C/[03C91 , 03C92] ~ c(c) . Defining ((z1, z2))v
=|k(u1 - u2) I,
we have- Nonarchimedean case, bad reduction. The canonical distance is invariant under base
extension,
so we can assuwe in this case that C is a Tate curve. Then there is soneq E K wi th
1 such isisomorphic
toK*v/(q).
Ashas
pointed out,
one can express Néron’s localheight pairing
in terns ofp-adic theta-functions ; similarly,
weget
the canonical distance. The basic theta- function isPut
vq(u)
= and define the "nollifier"Then
k(u) = b(u~ . ~
is a real-valued function such that all u ,k(qu)
=k(u-1) = k(u),
as follows from the functionalequations
of the theta-func- tion. It is well known thatalgebraic
functions on a Tate curve canbe expressed
interns of
e(u) ,
and a short calculation shows that if weput «z.1 >
=then we have the fauiliar formula
Genus
g ~
2 .- Archimedean
case. Although
the foruulas are not asexplicit
as in theprevious
cases, their theoreticalsignificance
is clearer. It turns out that(z1, z ))
is a
multiple
of the Arakelov-Green’s functionz2) .
ARAKELOV introduced his functions in order to extend Neron’spairing
frou divisors ofdegree
0 to di- visors ofarbitrary degree
in the archinedean case, in a way uodeled on intersec- tiontheory (see
ARAKELOV[Ar]) .
Such an extension is notunique ;
an Arakelov-Green’s function is determinedby giving
a voluueforu,
or uoregenerally
a ueasuredu ,
norualized so
that c(c)
has total uass 1 .Then,
there is aunique nonnegative
real-valued function
G(z , w)
on such that(a) G( z , w)
is snooth andpositive
off thediagonal,
with asimple
zeroalong
the .
(0) log G(z , w)
dz =w
for every w ;
(c) ~ ’ a ~(c.) log G( z , w)
0 for each w .Condition
(c)
issimply
a convenientnormalization ;
the crucialproperties
are(a)
and(b),
which ensure thatw2))
is harmonic forz ~
with
logarithmic singularities
ofopposite signs
at thosepoints.
Green’s idcnti-ties show that
G( z , w)
issymmetric.
For any choice of an func-tion,
we canput j~z 9 z2))v
=G(
andget
a of distance functionsby
the usual formula. For curves of genus 0 and 1above,
we have chosen((zl ’
tocorrespond
to the constantpositive
curvature and flatietrics,
res-pec tively.
It should be noted that GROSS has
given
a foruula for the Arakelov-Green’s function of a curve ofgenus %
2 with the constantnegative
curvature metric. Hisformula uses the uniformization of the curve
by
the upperhalf-plane,
and expressesG( z , w)
as the residue at s = 1 of a Poincaré series fOrDed fromLegendre
func-tions of the second kind.
- Nonarchimedean case. Here the construction of functions
((
whichdecompose
the canonical distancedepends
on intersectiontheory.
If is afinite
extension, put CW
= espec (1 ) .
LetC
be theregular
modelof C, and R(C )
the dualgraph
to thespecial
fibre of a finitew w w
extension of the
base,
e has semi-stablereduction,
and hence thegraphs R(C )
wall have the sane
topology
forlarge
L . One can forn a "reductiongraph" R( e) ,
w
which is
essentially
the direct limit of theR(C ) together
with a metric on thew
edges,
in such a way that thecomponents
of thespecial
fibres of theC "’1
corres-pond
to a dense set ofpoints
onR (e) .
The final result is as follows. There is a
decomposition
in which take rational values.
Furthermore,
and
Here i
(x , y)
is apurely
"local" term: it is 0 unless both x and yv
reduce to the same
nonsingular point
0:1. thespecial
f ibr. e of someCW ,
and thenit is i
(x , y)
-- -g
v for anappropriate
local uniformizer g(x)
aty . on the other
v
(x ,y)
is notunique,
but isspecifiea by giving
ameasure of total mass 1 on
R(C) .
As a function of x and y , itdepends only
on the
special
fibre to which x and.
y reduce.
Thus,
itand j v (x , y~
can beregarded
as functions onR( e) .
For any twopoints 00FF, ç
ofR(e;;, y~-
is a
piecewise
linear functionof x
ER( e) taking
its naxinun aty
and its m-ninun
at 03B6.
Itobeys
a mean-valueproperty
like that of harmonic functions.A remark on the
triangle inequality. -
The constant M in the weaktriangle
ine-quality (property
7° of the canonicaldistance)
isdefinitely
sometimesgreater
than 1. For a Tate curve
isonorphic
to 111= q
v .Thus,
M can bearbitrarily large.
In the Archimedean case, numericalcomputations
forelliptic
curves
1J yield
lower bounds for anM
such that -Some values are in the
following
table.Construction of local Green’s functions. - Given the canonical
distance,
for eachplace
v and set F cc(:R: ) ,
one can define thecapacity
and construct Green’sv v
functions
following
the classicalpattern.
’
For a
conpact
setE , and
v apoint’
E v not inE ,
v letIf
V03B6(EV) ~ ~,
there is aunique
the"equilibrium distribution",
v
for which the inf is achieved. Define the Green’ s ~~~unc tion
by
We understand this to mean ~ if
V03B6(EV)
= (X),and z, ,
are not inE .
Define
G( z § . E ) =
’ ’v
0 if either zor 03B6 belongs
to E . v(Note
thatV (E .) c
vand y
"(Ev) depend
on the nomalization chosen for the canonical distance[ z , w]"
but
G j z , I.: ; Ev)
and03B6
donot.)
It can be shown that ifEVl
CEv2 ’
then forall
z, ,
theinequality G(z, , ; EV1) ~ G(z , , ;
holds. For anarbitrar,y
set
F ,put
v
At this
point
there is acomplication,
siuilar to the one indefining
a measurable set inLebesgue’
t stheory.
Above we have defined thecapaci ty
f°r acompact
set. Another. class of sets for which the
capacity
can be definednaturally
aresets U =
~z
E~(K ~ ; ~ ( .~ R ~
where is analgebraic
1 v v v v
function on C whose
only poles
areat 03B6,
andRv belongs
to the value group.V
of K . If
f( z)
hasdegree
n, and is normalized solim| f(z) ( /[Z, w]n
n =1,
then
it
is natural thatR1/n.
wants
G( z , S
’ yU )
=(1/n) log ( Rw).
The sets for which the formulas for’ v v Y v
coupact
sets and PL03B6-donains arecompatible
will be calledcapacitable.
For an ar-bitrary
setF v ,let
the "inner" and "outer"capacities
ofF
beF is
capaci table
if for all 03B6 in the o fF , Ý r.(F ) = Y...(F ) . (In
amanuscript
of this paper, I called such setsadnissible. )
An RL-domain(Ra-
tional Lemniscate
douain)
is a set of the form(z
Ee(íè );
vI f( z) I
vR J
v forsome
f(z)
E Finite unions ofcompact
sets and RL-domains arecapacitable.
An
example
of anon-capacitable
set is a setcontaining
onepoint
ininfinitely
ma-ny residue classes
(nod v)
ofe(K) .
v If F v iscapacitable,
However,
the collection ofcapacitable
sets is not closed under intersection.The Green’s function of
Fv
has thefollowing properties :
i°
(Positivity) z~ ; F )~0 ;
and ifz
orz~
then3° (Transitivity)
IfF v
iscapacitable,
and ifG(zl’ z 2 ; F)
and4° (Galois statility)
For all 03C3 E5°
(Approximability)
For any RL-domain U contained in thecomplement
ofF y
any e >
0 ~
and there is analgebraic
function~(~)
whoseonly
poles
are at~y
such that for allz~ ~~
6°
tContinuity) G~ z~ ,
;F ;
is continuous as a function of two variables forz # z2
in theconpleuent
of F . If v isarchimedean,
it is harmonic in each variableseparately.
The ideas behind the
proofs. -
In the archimedean case, thedevelopment
of capa-ci ty theory
on Rienann surfaces is doneby following
theproofs
in TSUJI’ s book[Ts]
which are all coordinate-free. Once one has the canonical
distance,
there is no-thing
new. The main fact used is the maximum nodulusprinciple
for haruonic func- tions.In the nonarchiuedean case, the
goals
of thetheory
are the sane, but the nethodsare somewhat different. The
primary difficulty
isrelating
local behavior of func- tions toglobal behavior,
and this is doneby using
therigidity
ofalgebraic
func- tions. There are four naintools,
two localand
twoglobal.
1° Local
parauetrizability
ofC(v) by
power series. - is embedded inP,
y and let be the v-adic distance on induced fronPn() .
There is a 6 > 0 such that for anypoint C(v) ,
the ballcan be
parametrized by convergent
power series. This is wellknown,
and isproved by using
Hensel’s lemma to refineapproximate parametrizations.
Theuniformity
comes
by using
a lemma of Weil from thetheory
ofheights
to show that the v-adicsingularness
ofe,(K)
is bounded.v
2° The "Jacobian construction
principle"
for functions. - Leta =} ç
be two ar-bitrary points
ofe(K) ,
v and let U v be aneighborhood
of a.Then,
there is afunction
E K
v(e) ,
all of whose zeros lie in U v and whoseonly poles
are at03B6 .
This circumvents thedifficulty
that for genusg 1 ,
not every divisor isprincipal.
It isproved by using
the fact that the Abel napis open for the v-adic
topology except
on a set of codimension 1 .(This
is wellknown for the Zariski
topology,
and it follows for thev-topology by
theinplicit
function theorem for power
series.)
One takes theimage
of the divisor(a) - (ç)
in the Jacobian.
By choosing
nappropriately,
one can arrange thatn[(a) - ((,)’]
be
arbitrarily
near theorigin
ofJ(v) .
Thenwiggling
a few of thecopies
of(a)
within
Uv gives
aprincipal
divisor.3°
The naxinun modulusprinciple. - Actually
two naxinun uodulusprinciples
areused : a local one for power
series,
which is wellknown ;
and aglobal
one for al-gebraic
functions over RL-donains. It is as follows. ifg(z) E
is non-constant, put
Then,
iff(z)
EK
v(e)
has nopoles
inD,
v achieves its maximum value for ze D at a
point
ofThis is
proved by considering
theequation relating f(z)
andg(z) (which
exists because C has dimension
1 ),
its Newtonpolygon
for a fixed z, andreducing
to the case ofP1 .
OnP1
it is due toCANTOR,
who used the facto- rizationof
in terns of its zeros andpoles,
and adecomposition
theoremshowing
that an RL-domain is a finite union of"punctured
discs".4° The intersection
theory
formula forNeron’s pairing (see
GROSS[Gr~)). -
Thisgives
anexpression
for the canonical distance which lets onegeneralize
Cantor’sdecomposition
theorem for RL-domains toarbitrary
curves. One of its consequences is that finite intersections and unions ofRL-domains
areagain
RL-domains. The intersection formula ismainly
used instudying
the canonical distance on curveswith bad reduction. A weak version of the
theory
can be established withoutit,
res-tricting
tocompact
sets atplaces
where C has bad reduction. We will not discuss it further here.In
developing
thetheory,
thegeneral technique
is to reducequestions
about furc-tions on C to
questions
on balls around their zeros,by
the maximum uodulusprin- ciple.
On theballs, algebraic
functions can beexpanded
in powerseries,
and socontrolled.
Compact
setsplay a key role,
becausethey
can be covered with a finiteunion of
parametrizable balls,
and such sets are RL-domains.In his
original theory
forP~ ,
CANTOR used a differentapproach.
He took the ca-pacities
and Gre en’ s functions of RL-donains asbasic,
rather than those of con-pact
sets. He could do so because hisdecomposition
theorem for RL-domains(proved
using
theglobal
coordinatesysten
onP1 )
allowed him to construct RL-domains inprofusion.
Onarbitrary
curves, at least at thestart,
one does not knowenough
about RL-domains to
get anywhere.
Thekey
idea is toreplace
theglobal
existenceproblem
with a local one, which can be solvedusing
the Jacobian constructionprin- ciple. Using capacity theory
forcompact sets,
onegradually gains
more and moreglobal information,
untilfinally
it can be seen that Cantor’sapproach
would havesucceeded after all.
However,
thecapacities
of bothcompact
sets and RL-d0153mainsare
important,
for it turns out that innercapacity
is the correct notion for pro-ving
one half of theFekete-Szego theorem,
and outercapacity
for the other.Definition of the
global
adeliccapacity. -
Once one has the local Green’s func-tions,
Cantor’s formalism for the extendedglobal capacity
goesthrough unchanged.
In the
previous sections,
we have stated localcapacity theory
f:)r sets in0(K ),
but we could
equally
well have done so for sets inC(v) .
There are no differences.For the
global theory
it is convenient to restrict to that case.It is
useful
to introduce a crude adelization ofK
relative to K . For eachplace
v ofK ,
fix anembedding of K
into and let0
be thering
of -integers
ofK . v
DefineK
to be the restricted directproduct
of theK
rela-tive to the
,.., ë , v
where theproduct
is taken over theplaces
of K .K
embeds na-turally
inK
"on thediagonal".
We will bedealing
with sets of the formnEe C(K.)
in which each E is stable underGal(v /K ) ,
so the choices ofv v A v v v
the
embeddings
will not matter.Suppose
X = ... ,xrJ
ce(:K)
is a finite set ofglobal algebraic points
an
e,
stable under.Gal(K/K) .
For eachplace
v ofK ,
let a setE
cbe
given.
We assume :(a)
Each E iscapacitable, disjoint
fronX ,
and stable under(b)
All butfinitely
many Ev
are "trivial with
respect
to X tf in the follow-.
ing
sense: v is aplace
such that e hasnondegenerate reduction, x1,...,xr
reduce to distinct
points v) ,
andEv
is tho set ofpoints
on whichdo not reduce to the same
point
as one of thex.. Equivalently,
if, w||v
isthe v-adic
spherical
uetric onP. (K ) y
thenGiven such a
collection, write!
=% = "v Ev .
aregoing
to define the capa-city ’y(!, X)
of E withrespect
If
L/K
is a finiteextension,
there is a natural way to associate an adelic set1B c
toEK . Namely,
for eachplace
11{ of Klying
over v ofK,
f17-an
isomorphism
ofL
withK , and put
E =E .
Thecapacity
will be definedso as to be invariant under base extension.
Hence,
withoutloss,
can suppose that each of the x, E ’l’ is rational over K.i
For each
point
x. , chaose a functiong. ( z)
rational over K and1 1
having
asimple
zero at x..(It
isreally only
the choice of aglobal tangent
vec-tor that
matters, not
theuniformizing parameter.)
for each v, define a "local Green’s
I ,
w.hich will be an rby
r matrix with
nonnegative
entries off thediagonal, given by
1f/IIIfà. . ,
All but
finitely
many of the are the zero natrix. Let =[Kv : Q.( ) ]
andN =
[K : ~J
be the local andglobal degrees, respectively,
wherep(v)
is the ra-tional below v .
The
"global
Green’s uatrix" F= F(E , 3l)
will bewhere if v = 00 we understand
p(v) =
e .By
theproduct fornula,
1" isindepen-
dent of the choice of
gi (z) ’s .
It isagain
asymmetric
r x r real r:atrix withnonnegative off-diagonal
entries. letV(E , 3C)
be the value of r as a matrixgane, defined
by
Here (P is the set of r-element real
probability
vectors o vectors with iionnega- tivc entriesadding
up to 1 .Finally,
theglobal capacity
isThe Lost unusual
thing
in the definition is the value of F as a matrix gane.First,
it should be noted that the formula is forced ifpullbacks
are to w ork pro-perly. However,
it would be hard toanticipate
thegeneralization
from thecapacity
with
respect
to onepoint,
anddoing
so is one of Cantor’s main achieveLents.Second,
nost definitions in the
subject depend
upon theequivalence
of two extreal proper-ties,
forexample
theprinciple "minimizing
is the sane asequalizing"
for the ma-gnitude
of oscillations ofTchebychey polynomials. V(E ,X )
is aquantity
ofthat
type.
IfV(E , X) 0 ,
there is aunique probability
vector w such that allthe entries of
fw
areequal ;
and their value in that case isexactly V(lS , 3E) .
Nonetheless,
the truemeaning
of theglobal capacity
remainsuysterious.
Functoriality properties
of theglobal capacity. - ~Y(E , X)
has nice functoria-lity properties.
From theweights
which go into the definition of the Green’s ma-trix,
it is invariant under basechange.
Thatis,
ifL/K
is a finiteextension,
then
Y(~. ~ ~~ _ ~~ . Furthermore,
it behavessmoothly
underpullbacks.
Suppose
F :C
-->C
is a nonconstant rational nap between two curves definedover K . Let
E and X
begiven
and let F havedegree m .
ThenLastly,
if E= , I
vEv
and F = " vFv are
tii* adelic Sets inK/» )
Whose capa- cities withrespect
to 3l aredefined,
and iffor
each v , E CF ,then
v v
y(E , 3l) % Y(F , lC) . Monotonicity
in thevariable X
is an openquestion;
somecare is needed even to formulate what it should mean, since
Y(E , % )
hasonly
been defined if almost all of the E v are "trivial with
respect
to X It .In the case of
P1 ,
CANTORproved
a"separation inequality". Suppase E
and 3lare such that 3l can be
partitioned
into two setsX1
andX2
such that forany
~2 ’ ~
haveG(x1’ x2 ; E) = 0 .
This Deansthat
for
every v ,X1
andX2
are contained in different"components"
of thecoupleuent
of E . CANTOR showed that(under
aslight
extension ?f the definitionv
of
capacity above)
It renains open whether this is true for curves of
higher
genus.The r~ain theorem. - The