C AHIERS DE
TOPOLOGIE ET GÉOMÉTRIE DIFFÉRENTIELLE CATÉGORIQUES
J EAN -L UC B RYLINSKI
Central extensions and reciprocity laws
Cahiers de topologie et géométrie différentielle catégoriques, tome 38, no3 (1997), p. 193-215
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© Andrée C. Ehresmann et les auteurs, 1997, tous droits réservés.
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
CENTRAL EXTENSIONS AND RECIPROCITY LAWS by
Jean-Luc BRYLINSKICAHIERS DE TOPOLOGIE ET
GEOMETRIE DIFFERENTIELLE CATEGORIQUES
Volume XXXVIII-3 (1997)
R6sum6. Cet article
d6veloppe
la th6orie d’un groupeagissant
sur ungroup6ide
connexe. Une telle action donne lieu a une extensioncanonique
du groupe. On d6montre que toute extension de groupe est obtenue par ceproc6d6. Lorsque
le groupe a un
objet
fixe dans legroupoide, on
prouve que 1’extension de groupe est scind6e. On donne diversesapplica-
tions de ce th6or6me de
point
fixes. Laprernibre
est une preuvecat6gorique
de la loi dereciprocity quadratique
sur un corpsglobal quelconque;
c’est en fait une distillation de 1’essencecat6gorique
de la preuve due a A. Weil. La secondeapplica-
tion est la d6monstration de la nature
purement symplectique
du théorème des
point
fixes deAtiyah-Bott
pour un fibr6 endroites
holomorphe
sur une variete kaehl6rienne.Introduction
In this paper we
develop
ageometric description
of group exten- sions based on theconcept
of a groupacting
on agroupoid.
We provea new
type
of fixedpoint
theorem: if the group fixes someobject
of thecategory,
then the extensionsplits.
Thesplitting
then has numerical consequences. As anapplication,
we derive thequadratic reciprocity
law over any
global
field E of characteristic notequal
to 2. The rel-evant
groupoid
has asobjects
thelagrangian subgroups
of the groupA2,
where A denotes the additive group of adeles of E. Themorphisms
are
given by intertwining operators
between two models of the Stone-von Neumann
representation
of theHeisenberg-Weil
group associated toA2.
The groupSL(2, E)
acts on thegroupoid
in a natural way, and the fixedobject
is thelagrangian subgroup E2 of A2.
When a group G acts on some
manifold,
one can make G act on194-
various
categories
of bundles over themanifold,
where the bun- dles areequipped
with extra structures such as a connection. Thenwe show that the extension of G
splits
if andonly
if there exists anequivariant
bundle in ourcategory.
In the case of a group G of sym-plectomorphisms
of aquantizable symplectic manifold,
thecategory
consists of the
quantum
line bundles and the central extension of G is the well-known Kostant central extension. Ingeneral,
one can ofteninterpret
a fixddobject
ascorresponding
to someequivariant bundle,
or to some
equivariant
fiber functor. If G has a fixedpoint,
then thecentral extension
splits.
Given two fixedpoints,
thecorresponding splittings
differby
anexplicit
character of G. This can be used to show that in the case of a, torusacting by automorphisms
of a Kaehlermanifold,
theright
hand side of theAtiyah-Bott
fixedpoint
formulacan be
given
apurely symplectic interpretation,
up to a character of G. This recovers a result ofJeffrey [4].
I first started
thinking
about the results of this paper in theSpring
of
1992,
and I talked about someaspects
of them atcolloquiums
atCornell and Princeton Universities at that time. I am
grateful
to Cor-rado De
Concini,
PierreDeligne,
LisaJeffrey,
Victor Kac and DennisMcLaughlin
for useful discussions. This research wassupported
inpart by
NSFgrant
DMS-9203517.1. ACTION OF A GROUP ON A CATEGORY
It
hardly
needs to bepointed
out that the notion of a groupacting
on a set is one of the most
prevalent
notions ingeometry.
Infact,
if onetakes F. Kl%in to his
word,
this is the same asgeometry.
The notionof a group
acting
on acategory
C is morecomplicated, although
it isimplicitly
encountered every time a group acts on a space.Definition 1.1. An action
of
a group G on acategory
C consistsof
afunctor Tg :
C -> Cfor
any g EG, together
with invertible naturaltransformations 1Jg,h : Tgh -> Tg o Th, defined for
anyg, h
EG,
satisfying
thefollowing
conditions:(A)
For any 91, 92,93 EG,
tlaefollowing diagram
is commutative:(B)
We haveT1 ==
Id ando1,9
=Id, og,1 =
Id.I
recently
learned from Sasha Beilinson that this definition ap- pearsalready
in Verdier’s thesis. it was alsorecently proposed by Kapranov [5]
in connection with hisconjectural
framework forhigher
dimensional
Langlands philosophy.
The basic
example
is thefollowing.
Let G actby homeomorphisms
on a space
X,
’and let C be thecategory
such that anobject
of C isa vector bundle E -> X over
X,
and amorphism
E -> F is a bundleisomorphism.
Then for any g EG,
define the functorTg
as thepull-
back
by g-1
so thatFor any vector bundle
E,
andfor g, h
EG,
we have a natural iso-morphism
between(gh)* (E)
and9*(h*(E)).
Thisgives
the natural transformationog, h .
Thecoherency
condition(A)
is obvious(so
obvi-ous that it takes some time to convince oneself that there is
something
to
prove).
To obtain a group extension of G from an action of G on a
category C,
one needs someassumptions
on thecategory,
which we nowgive:
(C)
C is agroupoid,
i.e. every arrow in C is invertible.(D)
C isconnected,
i.e. for twoobjects P¡
andP2
ofC,
thereexists an arrow from
P¡
toP2.
Then for any
object
P ofC,
we have the fundamental group7r¡(C, P)
ofC,
which is the groupAut(P)
of arrows from P to itself.Given an arrow
f : P1 -> P2,
we have an inducedisomorphism f. :
7r1
(C, P1 ) ->
7r1(C, P2 ).
Theisomorphism depends
on the choice of thearrow
f ,
butonly
modulo innerconjugations.
Hence if we introducethe
category
OutGr,
whoseobjects
are groups, and whose arrows areclasses of group
isomorphisms
modulo innerautomorphisms,
we havea well-defined
object 7r,(C)
of Out Gr. Note that theautomorphism
196
group of 7r E
Ob(Out Gr)
is the groupOut(7r)
:=Aut(7r)/Inn(7r)
ofouter
automorphisms
of 7r.The action of G on C induces an action of G on the
object TTi(C’)
of Out
Gr,
i.e. a grouphomomorphism f :
G -Out( 7rl ( C)).
Proposition
1.2.(1)
For anobject
Pof C,
there is an associatedgroup extension
for
which the induced grouphomomorphism
G ->Out( 11"1 (C))
coin-cides with
f .
We have:GP
={(g, a) :
g EG, a
EHomc(Tg(P), P)}.
(II) Any
arrozuP, --+ P2
in C induces anisorrLOrphism of
exten-sions
from ë PI
toG P2.
Thisisomorphism depends
on the arrowonly
up to inner
conjugation by
a,n elementof
thesubgroup 7r1(C).
Proof. We define
Gp
={(g, a) :
g EG, a
EHomc(Tg(P), P)}
as in
(1),
withproduct
lawThe
associativity
follows from the commutativediagram (A).
The in-verse of
(g,a)
is(g-1,T9-1(a)-1
0o9-1,g),
where we useTi (P)
= P.So
Gp
is a group, we have a grouphomomorphism
p :Gp
--jG, p(g, a)
= g; p issurjective
because of condition(D).
The kernel ofp identifies with
Aut (P) =
7r1(C, P),
and the grouphomomorphism
G ->
Out(7rl (C, P))
withf..
Let h :
Pi - P2
be an arrow in C. Then we have ahomomorphism
of
extensions h* : GPl
->GP2
such thath* (g, a) = (g, haT9(h)-1).
The
composition
of arrows induces thecomposite
of thecorresponding homomorphisms
of group extensions. ForPI
=P2,
anautomorphism
h of
PI
induces thecorresponding
innerautomorphism
ofGPl.
Thisproves
(2). 1
We will now
explain
thesignificance
of this group extension ina
geometric
context. Consider somecategory
C ofgeometric objects
over a space X.
By geometric object
we mean sometype
of bundleover
X, maybe equipped
with some structure like aconnection, possi- bly satisfying
some condition on the curvature. We assume that thiscategory
satisfies conditions(C)
and(D).
Assume that a discrete group G acts on Xby_homeomorphisms.
Assume that for P in thecategory,
thepull-back object g* P
alsobelongs
to it. Then we have an action ofG on the
category,
so thatTg
is thepull-back
underg-1.
We have thenotion of a
G-equivariant object
of C. This is anobject
to which- theaction of G lifts. The
following
resultexplains
thegeometric meaning
of the extension of G obtained in
Proposition
1.2.Proposition
1.3. Assume that the group G actsby
homeomor-phisms
on a spaceX ,
and let C somecategory. of geometric objects
onX,
whichsatisfies (C)
and(D).
Assume thatfor
g E G and P Eob(C),
the
pull-back g* P belongs
to C. Then thefollowing
conditions areequivalent:
(I)
The group extension 1 -> 7r1(C, P) -> GP
-> G -> 1of Propo-
sition 1.2
splits.
(II)
There exists aG-equivariant object of
C.Proof. A
splitting s :
G -G
of the extension is a map g E G ->Og : g* P+
such thato9h = h* (og)
0oh
for all g, h E G. This amountsexactly
to an action of G on the bundle P which lifts the action on X.This shows that
(I) implies (II).
The samereasoning, joined
with thefact that all
objects
of P areisomorphic,
show that(II) implies (I). 8
We are
mostly
interested in the case where7r1 (C)
isabelian,
inwhich case
Out(7r,(C)) = Aut(7r1 (C) ) .
if the action of Gon 7r1(C)
istrivial,
thenProposition
1.2gives
a central extension of Gby 7r1(C),
which is defined
uniquely,
np to aunique isomorphism.
We illustra.te
Proposition
1.3 with thefollowing example.
LetM be an oriented Riemannian manifold such that
H1(M,Z/2) =
0.Assume that G acts on M
by orientation-preserving
isometries. Let P -> M be the oriented orthonormalbundle,
which is aprincipal SO(n)-bundle.
Assume that the structue group of this bundle can be lifted toSpin(n),
in other words M is aSpin
manifold. We constructa
category
as follows. Theobjects
of C areSpin(n)-bundles Q ->
M, together
with anisomorphism o : Q/Z/2->P
ofSO(n)-bundles
198
over M. A
morphism
is a,nisomorphism
ofSpin (n)-bundles, which
is induces the
identity
on P. The group C acts on Cby pull-backs.
The
assumptions (A)-(D)
aresatisfied,
therefore we have a centralextension
G
of Gby 1rl (C) = Z/2Z.
The central extensionsplits
ifand
only
there exists aG-equivariant Spin (n) -structure
on M.If we work with differentiable
categories
and differentiable groupactions,
weget
extensions of Lie groups.Proposition
1.4.Any
group extension 1 -> K ->G-> P G - >
1arises
from
an actionof
G on somegroupoid
Csatisfying
conditions(A)- (D) .
Proof. We define a
groupoid
C as follows. The setOb(C)
ofobjects
of C isequal
to G.To g
E G associate the setp-1 (g)
CG
equipped
with the action of Kby right
translations. Given gl, g2 EG2,
an arrow from gi to g2 is a
bij ection 0 : p-1 (g1) = p- 1 (g2 )
which is K-equivariant. Thus 0
isgiven by right multiplication by
some elementh of
G
such thatp(h)
=g1-1g2. Given g
EG,
letTg :
C - Cbe the
following
functor.Tg (g1 )
= ggl onobjects,
andTg (h)= h
on arrows. More
precisely,
if we viewright multiplication by h
EG
as an arrow from gi to g2, then
Tg (h)
is the arrow h from gg1 to gg2. It is clear that axioms(A)-(D)
are verified. We then describe the extension 1 ->Aut(1 )
-> E -> G -> 1. The group ofautomorphisms
of1 E G =
Ob(C)
identifies with K. The group E consists ofpairs (g, h), where g
EG, h
EG
andp(h) =
g, withproduct (gi, h1) (g2, h2 )
=(g1g2, h1h2)-
But this identifies withG. 8
So wc have a. sort of universal construction of group extensions in terms of groups
acting
ongroupoids.
As anillustration,
westudy
a
type
of inductionoperation
for group extensions. Let 1 -> K ->p G --+
1 be a groupextension,
and letf :
G -Out(K)
theassociated outer action of G on K. Let H be a group which contains G as a
subgroup.
Then we construct a group extension 1 -> A ->H
->H -
1;
when K isabelian,
the group A is the groupMapG(H, K)
ofG-equivariant maps H -> K, equipped
withpointwise product,
andH acts on this group in the natural way. If K is not
abelian,
thedescription
of A is lesssirnple.
To construct the new groupextension,
we introduce a
groupoid
C. The setOb(C)
isequal
to the set of mapsm : H -> G such that
m(gh)
= g.m(h)
for any g EG, h
E H. Notethat such a map m is
completely by m-1(1)
CH,
which is a set ofrepresentatives
for the left G-cosets in H. Given mi M2 : H -> G asabove,
an arrow mi -> m2 is afamily cPh
ofK-equivariant bijections oh p-1 (m1 (h)) -> p-1 (m2 (h))
such thatfor g
EG, h
EH, Øh
andogh
are
given by
the same element ofG.
The group H actsnaturally
onC. For h’ E
H,
the functorTh,
transforms theobject (mh)
into thefamily (mh(h’)-1),
and the arrow(oh)
into the arrow(oh(h’)-1).
Given a set S c H of
representatives
for the leftG-cosets,
thereis an an associated
object
of C. itsautomorphism
group A issimply
the cartesian power
Ks.
There results ahomomorphism
A : H -Out(Ks),
which may be described as follows. First for any g EG,
one needs to choose an
automorphism i(g)
of Krepresenting 1(9)
EOut(K).
Let h EH;
then for any sE S,
one can writesh-1
=gss’
for a
unique pair (gs, s’)
E G x S. ThenA(h)
is the class of theautomorphism
which maps(hs)sES
to the element ofKs
whoses’
component
isf (gs) . hs.
We summarize this construction in
Proposition
1.5. Let G cHand let 1 -> K ->G
-> G - > 1 bea group extensions. Then there exists an induced extension 1 -> A -
if
-> H ->1,
where A isisomorphic to
the cartesian powerKGBH
We have:
(I)
For Kabelian,
A isisomorphic to MapG(H,K)
as an H-module,
and the above constructionrepresents
theShapiro
isomor-phism
H2(G, K)-> H2(H, MapG(H, K)) in group cohomology.
(II)
Assume that thehomomorphism f :
G ->Out(K) lifts to a homomorphism 1:
G ->Aut(K).
Then the extensionof G splits
as asemi-direct
product if
andonly if
the induced extensionof H splits.
2. CONSTRUCTIONS OF CENTRAL EXTENSIONS
We will
give
severalexamples
of our construction of central ex-tensions,
which are related toequivariant
bundles and toreciprocity
laws.
- 200
First let
(M, w)
be asymplectic manifold,
and assume that thecohoinotogy class
ot w isintegral
so that there exists some line bundle with curvature K =21rv"--l -
w. Let G be some group ofsymplecto- morphisms
of(M, w).
Let C be thefollowing category.
Theobjects
ofC are
pairs (L, V),
where L is a line bundle onM,
and V a connectionon L with curvature w. A
morphism h : (L1, V1) -> (L2, V2)
is an iso-morphism h : L1-> L,
of line bundles which iscompatible
with the con-nections. Then G acts on C
by Tg (L, V) - (g-1) * (L,V) - g* (L, V).
The natural transformation
og1,g2 is
the obvious one. Axioms(A), (B)
and(C)
areeasily
verified. Axiom(D)
will hold true if allpairs (L, V)
areisomorphic,
and thishappens
when any flat line bundle onM is
trivial,
i.e.HI (M, C*).
The group 1rl(C)
isequal
toC*,
and theaction of G on C* is trivial. So in this case we
get
a central extension of the group G ofsymplectomorphisms by C*.
This isisomorphic
toKostant’s central extension
([6],
see also[3]).
There are several variants of this construction. If one works in- stead with a
category
of circle bundles withconnection,
onegets
acentral extension
by
the circle group T instead of C*. If w is notintegral,
but hasperiod
group A CR,
one can work with a cate-gory of
C/A-torsors,
and one recovers Weinstein’sgeneralization
ofthe Kostant central extension
[15].
We now introduce a
category inspired by
the Stone-von Neumann theorem. This will be crucial in ourproof
of thequadratic reciprocity
law. Let, B be a
locally compact
abeliantopological
group which is second countable. Leti3
be thePontryagin
dual of B. The there is anassociated
Heisenberg group
H =H(B)
introducedby
A. Weil[14].
We will
give
adescription
of itslightly
different fromWeil’s;
we willalways
assume that themap x H x2
from H to itself isinvertible;
the inverse map will be denoted x ->
x1/2 .
TheHeisenberg
group H =H(B)
is the group H = 1r x B xi3
with theproduct
The commutator factors
through
thenon-degenerate skew-symmetric pairing
S((b1, x1), (b2, x2)) = x2(bi) . X1 (b2).
Note thatH(B)
is a centralextension of B x
B by 7,
with centerequal
to 7. Ourdescription
of HhlBR the
advantage
that tlmsymplectic
groupSp(B
xB),
which consistsof all
automorphisms
of H xB preserving
theskew-symmetric pairing,
acts
naturally
onH,
the action on the factor T of H = T x B x Bbeing
trivial.Recall now the
generalized
Stone-von Neumann theorem.Theorem 2.1.
(see !14]
Thereis exactly
oneisomorphism
classof
irreducibleunitary representation
p :H(B) - Aut(H)
such thatp(z)
= z . I df or z
E T.A
representation satisfying
theassumption
of Theorem 2.1 will be called a Stone-von Neumannrepresentation
of H. A construction of such arepresentation
is obtained from anylagrangian subgroup
Aof B x
B.
This means that A is maximalisotropic
withrespect
to S. Then T x A C H is a commutativesubgroup,
and we have thecharacter
n(z, x)
= z of T x A. Pick a Haar measure it on B xB.
Lemma 2.2. Let
H-(A)
be the inducedrepresentation
Let
p(g) . f (h)
=f (g-lh).
Then(H-(A), p) is a
Stone-von Neumannrepresentation of H.
Note that any g E
Sp(B
xB)
induces anintertwining isomorphism
g. :
H(A)->H(g . A),
such that(g* f )(h)
=f (g-1h).
We then come to the
category
C. Anobject
of C is alagrangian subgroup
A of B xB.
An arrowf : A1 -> A2
is aunitary intertwining operator f : H(A1)-> H(A2).
The group G will be somesubgroup
of thegroup
Sp(B
xB)
ofsymplectic automorphisms
of B xB.
The action isgiven by
the functorTg
which sends A tog(A)
andf : H(A1)->H(A2)
to the
intertwining
operatorTg (f)
defined so as togive
a commutativediagram
202-
The natural transformation
og1,g2
is the obvious one.The group
ofautomorphisms
of anobject
A isequal
toT,
andSp(B
xB)
actstrivially
on T. So fromProposition
1.2 one derives acentral extension
where
Mp(B
xB)
is the so-calledmetaplectic
gloup(Weil actually gives
this name to asubgroup
ofMp(B
xf3),
which is a central ex-tension of
Sp(B
xB) by Z/2).
Of
particular
interest is the case B =Kn,
for K some localfield,
i.e. K = R or
C,
or a finite extension ofQp,
or a power series fieldFq((x))
over a finite field of characteristic notequal
to 2. Then onecan
identify k
with K in thefollowing
way. One chooses a non-trivial
character V) :
K -T;
then the continuoushomomorphism
z -
(y -> Y(x. y))
from K toK
is anisomorphism.
Thus for B = Knwe have
B->Kn,
andSp(B
xÊ)
is thesymplectic
groupS’p(2n, K).
The last
example
is taken from work ofArbarello,
De Concini and Kac[1],
and is ananalog
forhnilrlings
of the Kostant central exten- sion. Let k be afield,
and let E be a vector space over k(not
of finitedimension).
Twosubspaces F,
andF2
of E are called commensurable ifFl
nF2
is of finite codimension in bothFl
andF2.
We fix a com-mensurability
class S ofsubspaces
of E. We introduce acategory C,
whose
objects
aresubspaces
F C E in thegiven commensurability
class. To define the arrows, we need the
following
construction.Proposition
2.3. There exists aunique way to assign
a 1-dimensional vector space
(Fl F2)
to apair of subspaces
in the classC, together
withisomorphisms
such that:
(I)
ForFI
CF2,
we have:For
Fl g F2 g F3,
theisomorphism W(Fl, F2, F3)
is the canonicalone.
(II)
GivenF1,F2,F.1, F4
ES’,
11Je have a commutativediagram
Then we define
H omc(Fl, F2)
to be(F1lF2) B {0},
the set of non-zero elements in the line
(F1l F2). Composition
of arrows is inducedby
the
isomorphism
w(F1, F2, F3),
and(2) guarantees
thatcomposition
of arrows is as-sociative. The
category
C is a connectedgroupoid,
andAut(F)
= k*for any
object F,
so that7r1(C)
= k*.Let G =
GL(E, S)
be thesubgroup
ofGL(E)
which preservesthe
commensurability
class S. Then Goperates
on thecategory
C.For g
EG,
define the functorTg :
C - Cby Tg (F) = g . F,
andTg : (F1lF2) -> (g . F1|g . F2 )
is the canonicalisomorphism,
which existsby
theuniqueness part
ofProposition
2.3. Then weactually
haveTgh
=TgTh
forg, h, E G,
so we takeØg,h
= I d. Thus we have anaction of the group G on the
category
C.Consequently
we have acentral extension
In
particular
let E =k((x))n,
and let S be the commensurabil-ity
class of the "lattice"k[[x]]n
Ck((x))n.
Then the linear groupGL(n, k((x))) preserves this commensurability class,
hence we have acentral extension
GL(n, k((x)))
ofGL(n, k((x))).
For n = 1 we havethe
following computation
Proposition
2.4. Letf,g
Ek((x))*.
Letf, 9
be elementsof k((x))*
which map tof,
resp. g. Then the commutator[f,g]
isequal
to 1 I-
where v denotes the valuation
of
aforinal
power series(order of
zeroat the
origin).
204-
Proof. As both the commutator
[f
and theexpression (7)
arebilinear in
f and g
andskew-symmetric,
we may reduce theproof
totwo cases:
(a) v(f) = 0,g =
x;(b) v(f)
=v(g)
= 0.In the first case, we
pick
theobject
O =k[[x]]
ofC,
and we take/ = (f,1),
where 1 is the canonical element of(1.010) = (O|O).
Andwe
pick x
=(x, [1]),
where[1]
E(x. O|O)
=k . 1
is the element 1. Theproduct It
isequal
to(fx, w(1 0 f([1])).
Nowf([1])
E(x . 010)
is thetransform of
[1]
underf ,
so it is the class[f (0)] of f in O/x .
O. Onthe other
hand,
wehave: xl
=(fx, w([1] @ x .1),
and x . 1 isagain
thecanonical element of
(xO|x(O).
So we find[f,x] = f (0)
as claimed.In the second case, it is easy that the two lifts
f
andg commute. 1
3. THE FIXED POINT THEOREM
Given a central extension
1 -> A -> G -> G -> 1 of G, we
have a natural
homomorphism f : H2 (G, Z) -
A. Recall its concrete definition. First wecompute the multiplier
groupH2 (G,Z)
ofSchur using
a freepresentation
1 -> R ->F-> P G - >
1. ThenH2 (G, Z)
=Fl H
R/[F, R],
where F’ denotes the commutatorsubgroup
of F. Let[x1, y1] ... [xg, yg]
be an element of F’ fl R. Thensetting
ai =p(xs),
bi
=p(yi),
we have the relation[a,, bi] ... [ag, bg]
= 1 in G. Thenchose lifts
ai
of aiand 6i of bi
inG.
Theexpression [5i, b1] ... [iig bg]
belongs
toA,
and isindependent
of the choice ofa1,..., bg.
We thenhave:
This may be
interpreted
in a way which does not involve thegiven
freepresentation
of G: anyfamily
of elements(a1,...,
ag,b1),..., b9)
suchthat
[a1, bi
...[ag , bg]
= 1gives
rise to an element ofH2 (G, Z) .
A
splitting
of the central extension 1 -> A -G->q G ->
1 is agroup
homomorphism s :
G ->G
such that qs =I dG .
The existence of asplitting implies
that the central extension isisomorphic
to thetrivial one
1 -> A -> A x G -> G -> 1,
hence that thecorresponding
homomorphism f : H2 (G, Z) ->
A is trivial.Theorem 3.1. Let C be n.
category satisfying
theassumptions (C)
and
(D) of § 1,
and let the group G act on C. Assume that A =1rl(C)
is
abelian,
and that the actionof
G is trivial. Assume that there existsan
object
Pof C
such thatTg (P)
= Pfor
all g E G. Then the centralextension
1 -> A -> G -> G -> 1 of § 1
has a naturalsplitting.
Proof. Use the notations of the
proof
ofProposition
1.2. We usethe
object
P to describe the central extension. We sets(g) = (g, Idp).
This
gives
asplitting
of the centralextension. 1
4. THE
QUADR.ATIC
RECiPROCITY LAWWe will use the Fixed Point Theorem 3.1 to obtain a
proof
of theordinary reciprocity
law.First of all we consider the
metaplectic
central extension 1 -a T ->Mp(2,K) -> SL(2, K)
=Sp(2, K) ->
1 of§2,
for F a localfield. There is an induced
homomorphism f : H2(SL(2, K),Z) ->
T.We recall that for
elements a,
b E K* we have acorresponding
ele-ment of
H2 (SL(2, K), Z),
denotedby {a, b};
this construction of Stein-berg [12]
works over any field. In thelanguage
of§4,
this element{a, b}
can be constructed as follows. One introduces the free group F ongenerators X(u), Y(u) (for
u EK).
There is asurjective
ho-momorphism
p : F ->,SL(2, K)
such thatp(X(u))
=1 u
andp(Y(u)) =1 0 u 1 ( ). Choose an element k of K* such that c = k2 -I
1.
Then introduce for u E K* the element
w(u)
=X (u)Y(-u-1)X (u)
of
F,
which maps to(0u -u-1 0)
ofSL(2, K).
Thenh(u)
=w(u).
w (1)
maps to InSL(2, K)
we have theexpression
, and a similar
expression
forNow write a
product
of commutators in F as follows. Write-206
down
h,(a)h(b)h(ab)-1
as aproduct
of elements of thetype X(u)
orY(v),
andreplace
each of theseby
a commutator in F which has the sameimage
inSL(2, K).
Then onegets
aproduct
of commu-tators which maps to 1 E
SL(2, K);
thisgives
the element{a, b}
ofH2(8L(2, K), Z).
Lemma 4.1.
[8]
For K a localfield
andfor
themetaplectic
central extension
of SL(2, K),
we have:where
(a" b)
is the Hilbert norm residuesymbol
has a solution otherwise
Proof. This well-known fact follows
easily by comparing
Mat-surrloto’s formula
[9]
for acocycle representing
the central extensionof
SL(2, K) by K2(K)
with Kubota’s formula[7]
for acocycle
repre-senting
themetaplectic
centralextension
Now assume that K is a non-archimedean local field with
ring
ofintegers
0. The additivecharacter Y :
K -> T is calledunramified
ifits kernel is
equal
to O.Lemma 4.2. Assume the
character
K - 1r isunramified
andthat the residue
field of
0 has characteristicdifferent from
2. Thenthe central extension 1 -> 1 -
Mp(2n, K) -> Sp(2n, K) ->
1splits canonically
over thesubgroup Sp(2n, O) .
Proof. It is easy to see that
02n
is alagrangian subgroup
ofK2n,
which is fixed underSp(2n, 0).
Thisgives
anobject 02n
of thecategory C,
such thatTg . O2n
=02n
for any g ESp(2n,O). By
thefixed
point theorem,
the central extension ofSp(2n, 0) splits.
Using
thissplitting,
we may viewSp(2n, O)
as asubgroup
ofMp(2n, K).
Now let E be a
global
field of characteristic notequal
to 2. LetS be the set of non-trivial
places (not-trivial
absolutevalues)
of E.For each
place
P denoteby EP
thecompletion
of E atP,
which isa local field. There exists a choice a choice of non-trivial characters
0-p : Ep - T
such that(1)
for almost all non-archimedeanplaces P,
the character1/J’P
isunramified.
(2)
for all a EE,
we have theproduct
formula:Note that Lemma
1 ’ and
condition(1) imply
that all butfinitely
many
1/Jp ( a)
are non-trivial.For a number
field,
the construction of such afamily (YP)
isgiven
in Tate’s thesis
[13].
For the field ofmeromorphic
functions on a curveover
Fq,
it involvcs the choice of ameromorphic
differential on thecurve.
In order to obtain the
quadratic reciprocity
law in the formgiven
to it
by Hilbert,
we introduce thering
of adelesA,
which is the re-stricted
product
A =n;ES Ep.
Thering A
consists of families(xp
6Ep),
such that for almost allP,
Xpbelongs
toOp.
We havethe
diagonal embedding
E -A,
which identifies E with a discretesubring
ofA,
withcompact quotient.
We have thecharacter 1/J
of Asuch
that Y((xp))
=TTPES Yp(xp).
This character has trivial re-striction to E. We use this character to
identify
A with its dual[13].
We consider the central extension
of the
symplectic subgroup
with coefficients in A. We are concernedmostly
with the case n = 1.The group
Sp(2n, A)
is the restrictedproduct
of the groupsSp(2n, EP)
with
respect
to thesubgroups Sp(2n, OP).
One can take the restrictedproduct
-208-
TTrpES Mp(2n, EP)
of the groupsMp(2n, EP),
withrespect
to the sub-groups
Sp(2n, Op).
This is a central extension ofTTrpEs Sp(2n, Ep)
by
EÐPES T. We have a commutativediagram
Consider the case n = 1. Let a =
(aP)PES, b
=(bP)PES
beinvertible adeles
(i.e. ideles).
For eachP E S,
we have the elementfap,bp} of H2(SL(2,Ep),Z).
Letf : H2 (SL(2, A), Z) ->
T be thehomomorphism
associated to the central extension(1-11)
ofSL(2, A),
and let
fP : H2(SL(2, EP), Z) -> T be
thehomomorphism
associatedto the local central extension. Then we have:
For utmost, every
pla ce
’P ES,
we have:ap,bp
E0*,
hencefp ({ap, bp})
= 1. So theproduct
in(13)
is indeed finite.Now we note:
Lemma 4.3. The
subgroup E2 of  2 is lagrangian.
Proof. The
character 0 :
A --4 T which we use toidentify A
withthe dual group has the
property
that E is its ownorthogonal
withrespect
to thepairing A
x A -> Tgiven by Y (x . y) .
HenceE2
is itsown
orthogonal
withrespect
to thepairing
We see that the
subgroup SL(2, E)
ofSL(2, A)
fixes thelagrangean subgroup E2
ofA2.
We viewE2
as anobject
of thecategory C,
suchthat
Tg(E2)
=E2
for all g ESL(2, E).
So we have:Theorem 4.4. The restriction to
SL(2, E) of
the central exten- sion(11)
has a canonicalsplt*tting.
This is a
group-theoretic
version of thequadratic reciprocity
law.Indeed,
theexpression (13)
must beequal
to 1 when a and bbelong
to E* . Therefore we obtain:
Corollary
4.5.(Hilbert’s form of
thequadratic reciprocity law)
For a, b E
E*,
we have:We refer to
[11]
for (B discussion of theequivalence
between thisproduct,
formula of HUbort and the usualreciprocity
law in the caseE =
Q;
thisequivalence
is of course anelementary
fact.Tlle
proof given
here is somewhat similarspirit
to Weil’sproof [14],
whicl itself is akin t,o one of Gauss’sproofs, namely
the onel)Hsed on theta-functions. The role of theta-functions in Weil’s
proof
is to
give
concrete vectors in t,lie model?nC(E2)
of the(adelic)
Stone-von Neumann
representation.
Thepoint
of thepresent categorical approach
is toget
rid of allcomputations,
save those over local fieldswhich were recalled in
§2.
5. THE ATIYAH-BOTT FIXED POINT THEOREM
Theorem 3.1 is not the
only
case when the existence of a fixedpoint implies
a"reciprocity
law". For a group ofsymplectomorphisms
we have an
analogous
theorem.Theorem 5.1.
(sere [3,
Theorem2.4.12])
Let(M,w)
be a con-nected