C OMPOSITIO M ATHEMATICA
A LLEN M OY
Representations of GSp(4) over a p-adic field : part 2
Compositio Mathematica, tome 66, n
o3 (1988), p. 285-328
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285
Representations of GSp(4)
over ap-adic field: part 2
ALLEN MOY Compositio
© Kluwer Academic Publishers, Dordrecht - Printed in the Netherlands
Department of Mathematics GN-50, University of Washington, Seattle, WA 98195, USA;
current address: Mathematical Sciences Research Institute, 1000 Centennial Drive,
Berkeley, CA 94720, USA
Received 15 March 1987; accepted 9 October 1987
In Part 1 of this paper, we defined a
nondegenerate representation
ofG ==
GSp (4)
as apair (L, Q) consisting
of acompact
opensubgroup
L anda
representation
Q of Lsatisfying
a certaincuspidality
orsemisimplicity
condition
(see
Section1).
Theorem 2.1 showed that every irreduciblerepresentation
of G must obtain anondegenerate representation (see
also[HM2], [M]).
In Section3,
weanalyzed
those irreduciblerepresentations
ofG which contained a
nondegenerate representation (L, Q)
with L aparahoric subgroup.
In Part
2,
wegive
ananalysis
of thoserepresentations
of G which contain theremaining nondegenerate representations.
These are the unramified and ramifiedrepresentations.
Thekey point again
is to reduce the classification ofrepresentations
of G to the samequestion
for a smaller group. This is doneby establishing
Heckealgebra isomorphisms (see
Section3).
4. Unramified
representations
Recall from Section 1 that a
nondegenerate
unramifiedrepresentation (L, Q)
is described
by
two parameters. Oneparameter
is apositive integer
whichis a measure of the level of the
nondegenerate representation.
The otherparameter
is a nonscalarsemisimple
element s Eg(Fq),
theFq-rational points
of the
algebraic
Liealgebra
g =GJp(4).
We make a few remarks about thesemisimple parameter
s.A
semisimple
element is of course contained in a Cartansubalgebra.
Therefore,
it is natural togive
arough
classification ofsemisimple
elementsbased on Cartan
subalgebras.
The Cartansubalgebras
ofg(F.)
are par-ametrized,
up toconjugacy, by
theconjugacy
classes of elements in theWeyl
group
(e.g.
see[C]).
In the caseof GSp(4),
theWeyl
group is the dihedral group of ordereight.
Inparticular,
there are five classes of Cartansubalgebras.
Inorder to
give representatives
for the fiveclasses,
we recall some notation from Section 1. The 4 x 4 matrix whose(r, s) entry
is03B4r,l03B4s,j
is denoteEi,j.
Consider the five Cartan
subalgebras
inà/(4 ) (Fq) given by
In the above sets, a and b run over
Fq.
In(4.1e), A
+BJt;
is anonsquare
inFq[03B5].
The fiveconjugacy
classes of Cartansubalgebras of g(Fq)
are thesubalgebras
in(4.1)
direct sum with the scalar matrices.The element s ~ 0 can be taken to be in the form
(4.1).
If s is type(4.1 b,
c,d, e),
we can further assume that b ~ 0. If s istype (4.1 d),
weassume a ~ {0, ± b} .
As stated
above,
the other parameter needed tospecify
an unramifiednondegenerate representation
is a level parameter i ~ N. To describe how to construct(L, QJ
from i and s, we recall some notation established in Section 1. The groupG (resp. K )
is the groupGL4(F) (resp. GL4(R)).
Foru E
N,
the groupKu
is the u-thprincipal
congruencesubgroup
ofK.
IfL
isa
subgroup
ofG,
then L is the intersection ofL
with G. To establish some morenotation,
letEach set in
(4.2)
is a R-order inM4(F), i.e.,
an R-submodule which is alsoa
ring. If
is an R-order in(4.2),
let denote the unitsin .
The group287
Ci
is an opencompact subgroup
ofG
=GL4(F). As A
varies over the fourorders in
(4.2),
we use the obviousnotation k (resp. È, Q
andM )
for.
The
groups K, B, Q
and M are theparahoric subgroups
of G encountered in Section 1. In the notation of Section1,
we haveEach
parahoric subgroup
possesses a natural filtration(see
Section1).
Thefiltration
subgroups
can beeasily interpreted
in terms of the R-orders in(4.2).
To do this letY()
to be thetopological
Jacobson radicalof .
Thedescription
ofY()
for each of the four orders in(4.2)
isgiven by
the
diagonal
entries of x lie inp}
entry
(2, 3)
of x lies inp}
entries
(1, 2)
and(3, 4)
of x lie inp}.
For u E
N,
consider the idealy()u.
A trivial calculation showsThis
periodicity
relationpermits
us to definey()u
for allintegers
u. ForU E N, let
288 and
The
G,u’s
are the filtrationsubgroups of G
defined in Section 1(cf. (1.15)).
As
varies over the fourorders
in(4.2),
we denote the groupsG,i,u by Ku, Bu, Qu
andMu respectively.
TheCayley
transformc(x) - (1 - x) ( 1
+x)-’
maps
f (j)u
to,u
and takesto
G,u . If
u v, the induced maps fromare
isomorphisms.
An unramified
nondegenerate representation (L DJ
has Lequal
to somefiltration
subgroup G 1i,u’ Indeed,
if i is the level of thenondegenerate representation (cf. (1.24)),
thenLet n be the index of the filtration group L in
(4.9), i.e.,
L =G,n .
Therepresentation 03A9s
is a character ofG lI,1l IGÎI,N 11 .
To describeQs,
we first recallmore notation from Section 1.
The
rings 9 == M4(F) and (R) = M4(R)
are the F and R-rationalpoints
of the Lie
algebra gl(4 ).
The Lierings,
g(resp. g(R))
are theanalogous
setsfor the Lie
algebra W-jll(4).
Given a latticeÎ
cg,
the dual latticewas defined in
(1.17). Recall, ,>
is the formx, y> =
tr(xy). For É-7e
anorder in
(4.2)
let r be theperiod given
in(4.5), i.e.,
The dual lattice of
cI(ift) 1 , j
e Z isLet 03A8 be the additive character of F with conductor R used in
(1.21).
Forintegers j > k
>0, identify
the character group withby
the map(oc
+03A903B1
This is
just (1.21).
With the obviousidentifications,
this realization of characters identifies the charactergroup
withWe now
explain
how the characterS2S
ofG,n/G,n+1,
is realized as a coset(4.12)
in terms of theparameter
s. For each of thesubalgebras b(Fq)
in(4.1 ), let b
c g be the obvioussubalgebra
so thatThe character
03A9s
is realizedby choosing
an-(i+1)03B1
E{b
ny()(-r-n)}
satisfying
s = a modp.
Theinteger i,
is theinteger
in(4.9).
With this
description
of L andns, we proceed
to formulate thekey
resulton Hecke
algebras.
Letg’(Fq)
be the centralizerCg(Fq)(s)
of s Eg(Fq).
We canpick
a so that ifg’ = Cg(03B1),
thenLet G’ -
CG(03B1)
be the centralizer of a in G. Set J’ = G’ n J. Ourgoal
isto
classify
the irreduciblerepresentations
of G which contain(L, 03A9ts)
via theHecke
algebra Yf(GIIIJ’, 1).
To prepare for theprecise
statement, we needsome constructions based on the Cartan
subalgebra b
and itsorthogonal complement
in g.If b is a subalgebra of g,
let1)-L (resp. b#)
be theorthogonal complement
of b
in g(resp. g).
Wehave b# = b~
~g*.
LetWith the obvious identifications via the
Cayley transform,
we haveWe are now
ready
to state the main result on Heckealgebras. Let j (resp. j ’)
be thegreatest integer
in(n
+1)/2 (resp. (n
+1)/2).
Define latticesand let J
(resp. J+)
be the group J =c(I) (resp. J+ = c(+)). Clearly
L c
J+
c J.If n + 1 =
2j,
thenJ+ -
Jand Ç4
can be extended to a character S2 of Jby setting a equal
to 1 onc(gJj)’
If n =
2j,
thenJ+ ~
J. The character03A9s
extendstrivally
onc(g’~j+1)
togive
a character onJ+ .
In both cases, let S2 denote the extended character. There is a
unique representation a
of J whose restriction toJ+
is amultiple
of Q. In the caseJ =1=
J+, 03C3
is theHeisenberg representation.
We state our main results asTHEOREM 4.1.
Any
irreduciblerepresentation of
G which contains(L, 03A9s)
mustcontain
(J, a).
THEOREM 4.2. There is a
*-isomorphism of algebras
so that
supp(~(f)
=J{supp(f)} J for f ~ Yf(G’IIJ’, 1).
The
isomorphism ~
shall be describedexplicitly
in theproof
of Theorem4.2.
In the case n + 1 =
2j, ~
iseasily
described.Fix g
E G’. There is anunique element /g
EYf(GIIJ, a)
withsupp(fg)
=JgJ and fg(g)
= 1(cf. Proposition 4.9). Let eg
EYe(G’IIJ’, 1)
be the characteristic function ofJ’gJ’. Then,
the map q isgiven by
We defer the
description of 1
when n + 1 is odd.We
begin
theproof of Theorems
4.1 and 4.2 with a fewpreliminary
resultson the support of Hecke
algebras.
Let a realizeS2S
as in(4.11).
Thedecomposition
yields
adecomposition
of g,u and asFor x E g, let
ad(x)
be theadjoint
mapLet d = - r - n,
so that a + g,d+1 is coset ofg representing Qs.
An element x E a + g9i,d+l, determines a mapad(x):
g,u ~Furthermore,
the mapad(x)
induces aquotient
mapwhich is
independent
of x. The mapad(x)
mapsg
to zero andLEMMA 4.3. For all u,
is an
isomorphism.
Proof.
For each of the Cartansubalgebras
in(4.1), let 1) c
g be the Cartansubalgebra
in(4.13).
In all cases,except
g’ - 1).
In theseregular
cases,g~
is the direct sum of those root spaces of g with respectto I)
on which ad actsnontrivially.
These root spacedecompositions respect
the groupsg.
Sincead(x)
is nonzero oneach root space, we have
is an
isomorphism.
Consider the four
"singular"
cases of s in(4.21). Type (4.1 a)
witha =
+ b.
We can assume a = b.Then,
in the notationof ( 1.2)
and(1.7), g’
is the
subalgebra
and
It is obvious from
(4.24)
thatgl - g~+
(Bg 1 ,
whereare
ad(x)
invariant. Ong~+ (resp. g~-), ad(x)
ismultiplication by
m-12a(resp. --i2a).
It is obvious from this that(4.22)
is anisomorphism.
DThe other three
singular
cases are similar.Type (4. la)
with b = 0. Theng’
is thesubalgebra
and
For the
type (4.1 b)
and a =0,
we haveand
For
type (4.1 c)
and a =0,
we haveand
In all cases,
(4.22)
iseasily
verified to be anisomorphism.
The next lemma is
analogous
to Lemma 3.2 in[HM3].
LEMMA 4.4.
Suppose
a + g,d+1 realizesQs
and x E a + g,d+I lies ing’
mod g,d+ufor
someinteger
u 1. Then x isconjugate by G,u
to anelement in
g".
Proof.
Theproof is essentially
that of Lemma 3.2 in[HM3].
We show xis
G,u-conjugate
to an elementof g’
mod g,d+u+1. Write x aswith and
By
Lemma4.3,
there is z~ Eg~,u
so thatThen
By induction,
there is a convergentsequence xv ~ x’
of elements ing’
anda
convergent
sequence gv - g of elements inG,u
so thatHence,
Ad(g) (x) -
x’.As an immediate
corollary
we haveIn
particular,
Theorem 4.1 followsdirectly
fromCorollary
4.5.Let
I*
be the dual lattice of1+
soInspection
of theproof
of Lemma 4.4.gives
COROLLARY 4.6. Ad
The next two lemmas on Hecke
algebra support
areanalogues
of Lemmas3.4 and 3.5 in
[HM3].
LEMMA 4.7. An element g E G lies in supp
Yf(GIIJ+, S2S) if
andonly if
theintersection
is nonempty.
Proof:
This isexactly
as in Lemma 3.4 in[HM3].
D LEMMA 4.8. suppX(G//J+, 03A9s)
c JG’JProof : By
Lemma4.7,
ifg ~ X(G//J+ , 03A9s),
then there are x1, x2 E C( +I*+,
so thatAd(g)(x1 )
= X2’By Corollary 4.6,
we can findx’1, x2 E
a +g,d+1
andkl, k2
E J sothat xs
=Ad(ks)(x’s)
for s = 1 or 2.This means the element
g’ = k-12gk1 conjugates xl
tox;. Inspection
of the various cases for
g’, i.e.,
sregular
orsingular,
showsg’ ~ G’,
sog ~ JG’J.
DAs a consequence of Lemmas 4.7 and
4.8,
we have PROPOSITION 4.9. supp£(GIIJ, (J) ==
JG’J.Proof: By
Lemma4.7,
G’ c supp£(GIIJ, 6). Also, by
Lemma 4.8supp
£(GIIJ, 03C3)
c JG’J.Whence,
suppX(G//J, 6) -
JG’J.Our next
goal
is to showPROPOSITION 4.10.
Let g’
E G’. ThenProposition
4.10 is trivial in cases(4.1d, e)
since G’ iscompact
and J is normalizedby
G’. To showProposition
4.10 in cases(4.la, b, c)
we use theBruhat
decomposition [BT].
Letmonomial matrices in G
Iwahori
subgroup
of G’The Bruhat
decomposition
for G’ isIn the notation of
(1.24),
setThe
group J
is normalizedby
N’. For c a root of the root systemC2,
and v EN,let
Uc,v
be the v-th filtration root group in(1.4).
Let C be the set of roots c sothat Uc ~ J = {1}.
For w E N’,wUc,vw-1 (resp. w-1Uc,vw)
isequal
to someU(resp. U).
For c E C,let Jc = Uc
n J. DefineFix some
ordering
on the sets in(4.36)
and define setsLet J’+
(resp.
J’ - ,J’0)
be the intersection of J+(resp.
J - ,J0)
with G’. Then LEMMA 4.11.Suppose
s isregular
orof
type(4.1 a). If
w E N’, then the doublecosets JwJ and J"wJ" have the
unique decompositions
There is an
analogue
of Lemma 4.11 in theremaining
cases:(4.1 b, c)
with a = 0.Let H denote the Cartan
subgroup
of Gcorresponding to b
in(4.13).
In thenotation of
(1.2),
definesubspaces
of g for case(4.1 b) by
and case
(4.1 c) by
span of span of span of span of
These
subspaces
can beexponentiated
into the group G. Denote these setsby
and
The individual sets are
Ad(H)-invariant.
In either case b or c, the collection of sets isAd(N’)-invariant.
Let C be the set of indices in(4.39b, c).
For c E C,let Jc
=U,
n J. Define sets as in(4.36)
and(4.37).
With thesedefinitions,
one
readily
verifiesLEMMA 4.12.
Suppose
s isof
type(4.1 b, c)
and a = 0.If
wENI,
then the double cosets JwJ and J"wJ" have theunique decompositions
Proposition
4.10 for cases(4.1 a, b, c)
follows from Lemmas 4.11 and 4.12.Proof of’
Theorem 4.2 in cases(4. l d, e)
Here,
JG’J - G’J is a group. Inparticular,
when a isone-dimensional,
themap q in
(4.17)
reduces to1(e,)
=h
and isclearly
anisomorphism.
Theother case we need to consider is when n is even. Consider the restriction of Q to J’. Fix an extension 9 of Q on J’ to G’. There is an extension of 6 to G’J
provided by
9 and the oscillatorrepresentation [H]. For g
EG’,
leth
EX(G//J, a)
be the element with supportJgJ and fg(g) = a(g). Then,
themap q:
X(G’//J’) ~ X(G//J, 6)
definedby
is an
isomorphism.
r-1Modulo the group T in
(3.8),
G’J iscompact. Hence,
arepresentation
of Gwhich contains 03C3t must be
supercuspidal.
Theserepresentations
are obtainedby taking
the différent extensions of a toG’JJ T
andinducing
up to G. Thereare # {G’/J’T}
suchrepresentations.
Proof of
Theorem 4.2 in theregular
casesof (4. la, b, c)
The
proof in
all three cases is very similar to theproofs
ofProposition 3.7,
3.15 and 3.20. As
such,
wemerely
outline theproofs
and omit the rather tedious details.Case
(4. la). Here,
G’ - A is thesubgroup
ofdiagonal
elements. Let i be asin
(4.9), and q
be the order of the residue fieldIFq == RI ft.
Therepresentation
6 is one dimensional when i is even
and q
dimensional when i is odd. In the latter case, it is convenient to set k =(i
-1 )/2
anddefine, using
the rootgroup notation
of ( 1.4),
The group
J*
is normalizedby B’,
the character Q onJ+
extends to acharacter o
onJ*
trivial onJ#,
and a = Ind o. This meansX(G//J, 6) - X(G//J*, Q). Furthermore, Propositions
4.9 and 4.10 hold with(J, a) replaced by (J*, o).
For notationalconvenience,
we shall use the notation(J, 6)
to refer to(J, 6)
when i is even and(J*, Q)
when i is odd.Regardless
of the
parity of i,
we can therefore assume a is one dimensional. For each g EA,
let egand fg
be as in(4.17).
Taked+ , h,
as in(3.23).
Theproof
ofProposition
3.5 iseasily
modified to showJg’JdJ
n JG’J =Jg’dJ,
wheng’ E G’
andd ~ {I, d+ , h+}. So, fg’* fd
is amultiple
offg’d.
Since{I, d+, h+} ~
B’ generateG’,
we concludethat fg * fg’,
ismultiple offgg,
for
arbitrary g,g’
E G’. Theproof
ofProposition
3.7 is noweasily adapted
to the
present
situation to show1.e., q
is anisomorphism.
Case
(4.1b). Regardless
of the dimension of a, letv6
denote the space of 03C3.Set
G’(R) =
G’ nG.
A character 9 ofG"(R)
which extends n on J’again
determines an extension of a to
G’(R).
Let T be the group(3.8),
anddefine
h+,
h- as in(3.23).
For x an element of the groupgenerated by
T ~{h+, h_},
define6(x)
to be theidentity operator,
and definefx
EX(G//J, a),
x EG/(R) u
T ~{h+, h_},
to be the element with support JxJand fx(x) = 6(x).
Eachelement g
E G’ has aunique decomposition
g -
thmk,
where t ET,
h E{h+, h_},
m0,
and k EG"(R).
Definef
EX(G//J, 03C3) by
Observe that
The terms on the
right
hand side can be taken in any order. This means the terms on theright
hand side of(4.42)
can be taken in anyorder, i.e., they
commute. To show the map il defined
by
is an
isomorphism,
we needonly
showThe
proof
ofProposition
3.5again easily adapts
to showJh+ Jh_ J n
JG’J =
J; whence, fh+ * fh_
is amultiple of fI.
Since(4.45)
followsimmediately.
Case
(4. l c).
Therepresentation
6 has dimension q. An extension Qof 03A9s
toG’(R) -
G’ nG ;, again
determines an extension of 6 toG’(R)J.
Anelement
g E G’
has aunique decomposition g = tdm k,
with t ET,
h ~ {d+, d_}, m 0,
and k EG"(R).
Definefg
EX(G//J, 03C3) by
theanalogue
of(4.43).
The map q definedby (4.44)
is anisomorphism.
DREMARK. In all three cases,
Gl T
has a noncompact center and so no squareintegrable representations. By implication,
there are no squareintegrable representations
ofG/T containing (J, a’).
Proof of
Theorem 4.2 in thesingular
casesof (4. la, b, c)
Here,
as in Section3,
we shallgive
apresentation
ofX(G’//J’, 1)
interms of
generators
and relations and show thatX(G//J, 6)
possessesparallel generators
and relations. We then define a*-isomorphism
via thesegenerators.
Case
(4. la), a
= b ~ 0. Recall some notation from Section1,
e.g.,Let
uu (x)
andu-a(x)
be the root elements(1.3).
LetIn the notation of
(1.7),
and
(cf. (3.80)).
Inparticular,
G’ isisomorphic
toThe
group B’
is an Iwahorisubgroup
of G’ and a Bruhatdecomposition
ofG’ is
given by
The affine
Weyl
groupW,,all = N’ {B’
nN’}
isgenerated by
theimages
ofPROPOSITION 4.13. The Hecke
algebra X(G’//J’, 1)
isgenerated by
theelements eg, g E
{r0,
rl,d+, d_, t’, t’-1}
U B’. These elementssatisfy
therelations
The above relations are a
defining
setof relations for
thealgebra.
Proof.
This isproved exactly
as Theorem 2.1 inChapter
3[HM1].
~To exhibit
parallel
relationsin X(G’//J, 03C3),
we need to make apreliminary
reduction. The
representation
6 is one-dimensional when i is even and q dimensional when i is odd. In the odd case define(J*, Q) by (4.40),
then
X(G//J, a) = X(G//J*, Q); whence,
if wereplace (J, 03C3) by (J*, Q)
when i is
odd,
we can assume a is one-dimensional in all cases. We havesupp(e(G//J, u» =
JG’J.If g E G’,
there is aunique element fg
EX(G//J, 03C3)
with
supp(fg)
=JgJ and fg (g) =
1.Define 17: X(G’//J’, 1)
-X(G//J, 03C3) by
The map 11 is
clearly
a linearisomorphism.
That ~ is aisomorphism
ofalgebras,
isequivalent
toPROPOSITION 4.14. The Hecke
algebra X(G//J, 03C3)
isgenerated by
theelements fg,
g E{r0,
ri,d+ , d_, t-l
u B’. Theelements fg satisfy
the relations303
Proof.
If g,g’
E G’ andJgJg’J = Jgg’J, i.e., vol(JgJ)vol(Jg’J) = vol(Jgg’J ), then fg * hl
is amultiple of hgl.
If eitherof JgJ, Jg’J has
volumeone, we in fact have
equality.
Since J is normalizedby B’,
thisimmediately implies
relations(a), (b)
and(e(ii))
when g E B’. LetN’0 (resp. N’1)
be thesubgroup of N’ generated by r0, r1, and A’(R) =
N’ nB’ (resp. N’0, t’).
Thegroup
fl’ = N’0/A’(R)
is an infinite dihedral group, while the groupW’1 = N,"IA(R)
is the affineWeyl
group of theGL2(F) component
of G’. Lete denote the
length
function onN¡.
We haveIt follows that JwJw’J = Jww"J whenever w, w’ E
N§,
and£(ww’) = e(w)
+~(w’); whence,
under thesehypotheses
When i is odd the element t’ normalizes J and so
(4.55)
is also valid for w, w’ EN’1.
This inparticular implies
relations(c(ii))
and(c(iii)).
When i is event’ does not normalize J. We have
Thus, ft’ * fw
=h’w and j;/,o * fw = ft’r0w provided
w is of the form(r1r0)u
or(r1r0)ur1,
u 0. Weshow ft’ *fr0
=qft’r0. Regardless
of theparity of i,
letk be the
greatest integer
ini/2.
For h EG,
denoteby bh,
the Diracpoint
massmeasure at h. When i is even,
write ft’
aswhere z runs over
the q2
elements of J mod{J
nt’Jt’-1}.
In the notation of(1.4),
we can takerepresentatives
for z in the form z = u1u2 where u,(resp. u2)
runs overUb,kIUh,k+I (resp. U-2a-b,k+1/U-2a-b,k+2). Similarly,
wehave
But, Jt’zxro J
n G" =~
unless u1v1 EUh,k+1
1 and u2v2 EU-2a-bk+2.
Underthese
conditions,
the nonzero summands have the formTherefore,
An
analogous
calculation showsWe conclude relations
(c(li»
and(c(iii))
from(4.60)
and(4.61).
We canfurther conclude from the above that
regardless
of theparity of i,
provided w,
w’EN;,
andt(ww’) == £(w)
+~(w’). Consequently,
theéléments
g EGL2 (F)
lie in thesubalgebra
ofX(G//J, 03C3) generated by fg,
g
~ {r0,
rl,tl
u B’. Once we show relations(e(i ))
and(e(ii))
it will followthat fg, g ~ {r0,
r, ,d+ , d_, t’} ~ B’
generate/(GJJJ, 6).
To show the first relation in(e(i)),
writeand
where x = x0x1x2 and xx E
U03B1a+b,k/U03B1a+b,k+1,
a -l, 2;
XI EUh,kIUh,k+1 (resp. Uh,A+II Ub,k+2)
when i is even(resp. odd). Then,
But Jd+xd- J ~
G’ -QS
unless x =1,
so the summands are all zero except when x is theidentity representative.
This is the desired result.Similarly .f,i - *.f ,,
=q3fI.
Consider the relation(e(ii)).
We havealready
shown(e(ii))
when g E B’.
By
the Bruhatdecomposition therefore,
it isenough
toconsider g - w
EN’1.
LetS( - )
be the set of roots defined in(4.36).
Writefl,
aswhere z = The intersection
Jd+ xzwJ n
G’is empty
precisely
when one canpick x
sothat xx
lies in someJc
andx03B1zc ~ U03B1a+b,k+1. Set f3
= #{{b, a
+b,
2a +b}
nS(-)}. Then,
The calculation
for fu *fd_
isanalogous
and omitted. The above methods areeasily adapted
to prove relations(c(i))
and(d).
Wegive
the details for(d)
when i is
odd,
and omit those for the easier case of i even as well as relation(c(i))
for all i. For notationalconvenience,
abbreviateUa (x)
tou(x).
Writefr1 *Ju(x)
=fr1u(x) and fr1
as306
with z e
Rift,
and v - v1v2, VI EU2a+b,k/U2a+b,k+1,
v2 ~U-b,k+1/U-b,k+2.
Let y = x
+ m’z E R . ThenSince , the intersection
is
nonempty precisely when vz
is theidentity representative.
The summation in(4.65) collapses
toRewrite the summand as
Combining (4.66)
and(4.67)
we obtain relation(d)
when i is odd. Thiscompletes
theproof
ofProposition
4.14.For the
remaining
three cases, thetechniques
of the above caseadapt readily.
We formulate the results andgive
detailsonly
whenthey
differsignificantly
from the abovearguments.
Case
(4. la), b
= 0.Here,
As in the above case, we can assume
(J, 03C3)
is one dimensionalby replacing (J, a) by (J*, Q)
in(4.40),
when i is odd. Then the map definedby (4.53)
isa
*-isomorphism
ofalgebras.
The
representation a
is one-dimensional when i is oddand q
dimensional when i is even. When a isone-dimensional,
the map ~:X(G’//J’, 1)
~,»’(GIIJ, a)
definedby (4.53)
is a*-isomorphism.
When 6is q dimensional,
we cannot
replace (J, 03C3) by
some(J*, )
since there are no propersubgroups
between J and
J+
normalizedby
B’.Here,
we workdirectly
with 6. Thesituation is
analogous
to Case II inChapter
3 of[HM1].
The oscillatorrepresentation yields
arepresentation
w of B’ trivial on G’ nQ,
with theproperty
Let Y
(resp. Y+)
denote the intersection of J(resp. J+)
with the group(4.68).
The group Y has twopertinent properties:
(i)
restriction of therepresentation
6 to Y remains irreducible.(ii)
the group N’ - G’ n N normalizes Y.We deduce an action ev of N’ on the
space V6
of Q so that(4.70)
holds withg E N’ and x E Y. The ev action is in fact the trivial
representation.
TheBruhat
decomposition
of G’yields
amapping
satisfying
For g E
G’, define eg (resp. fg)
in Yf ==X(G’//J’, 1) (resp.
X’ =X(G’//J, 03C3)) by
supp
supp
Up
to scalarmultiples eg (resp. fg)
are theonly
elements of(resp. X’)
with support
J’gJ’ (resp. JgJ).
Define~: X ~ à by
308
PROPOSITION 4.15. The map ~: X’ ~ X is a
*-isomorphism of algebras.
Proposition
4.15 isproved by establishing analogues
ofPropositions
4.13and 4.14. Let
Abbreviate
U2a+b(X) (resp. U-2a-b(x))
tou(x) (resp. u(x)).
PROPOSITION 4.16. The Hecke
algebra ,î(G-’IIJ", 1)
isgenerated by
theelements eg, g
~ {r0,
rI,mI, m -’11
u B’. The elements egsatisfy
the relationsPROPOSITION 4.17. The Hecke
algebra X(G//J, a)
isgenerated by
theelements fg,
g E{r0,
rI,mIl
u B’. Theelements fg satisfy
the relationsProof :
Relations(a), (b)
and(c(ii))
are obvious since ûJ satisfies(4.71).
Theproof
of the four relations in(c(i))
and(d)
are similar. Wegive
the details for the first relation in(d)
and omit those for the other three easier cases.Let
v(z, z’)
=ua(z)ua+b(z’).
Thenwhere I is the
identity operator
andx’,
z, z’ run over R modp. Let y
= x +m’x’ and v =
v(m’z, m’z’).
Theconvolution fr0 *fu(x) * Iro
is thereforeThe relation
r0u(y)r0 = u(-y-1)r0 d(-y, 1, 1 ) u( - y-’ )
allows us tobring
the factor
03B4r0vr0
to the leftwhere,
afterappropriate transformations,
it can beabsorded
into fI.
Whenb,ov,o
is commuted pass03B4u(-l-1),
the term03B403B3
isintroduced,
where y is the commutatorThe
factor l5"
can absorbedinto fj
on theright
with the introduction of the factora(y) = 03A8(-1(z2 - Ez’2)).
It follows thatThe Gauss sum
{03A3z,z’03A8(-1(z2 - 03B5z’2))}
istrivially
calculated to be q. We concludeTo see
that fg,
g~ {r0,
r, ,I}
u B’ do indeed generate thealgebra,
observethat
{r0,
r, ,I}
generate N’ mod N’ n B. Sincevol(JroJ) = q3, vol(Jrj J ) =
q and
vol(J(r0r1)uJ)
=q4lul;
wehave f» * fw’
=fww’ whenever,
w, w’ E N’and
£(ww’) = £(w)
+~(w’). Here, £(w)
is of course the number of r E{r0, r1}
in a reduced
expression
for w. Thealgebra
isthus, by
the Bruhatdecompo- sition, generated by
the indicated elements. Thiscompletes
theproof
ofTheorem 4.17. D
Define eg, g E G’ as before.
PROPOSITION 4.18. The Hecke
algebra X(G’//J’, 1)
isgenerated by
theelements e,, g E
{r0,
r, ,t’, ,t1
U B’. The elements egsatisfy
the relationsThe above relations are a
defining
setof relations fôr
thealgebra.
The dimensional of a is
q2
when i is oddand q
when is even. In the odd case,we can reduce to a one dimensional
representation o
as before. To dothis,
let k =
(i
-1)/2.
Defineand set
Extend the character Q on
J-,
across J #trivially
to get acharacter o of J* . Clearly,
6 = Ind Q, soX(G//J, Q) - ,3i’(GIIJ*, Q).
The obvious map q(cf. (4.44))
is a*-isomorphism
ofalgebras.
When i = 2k is even, let Y be the intersection of J with the group
(4.49).
The group Y is normalized
by
N’ - G’n N,
and 6 remains irreducible onrestriction to Y. As in case
(4.1 b),
the oscillatorrepresentation
and Bruhatdecomposition
determine amapping
satisfying (4.71).
We may assume and(see
the discussion of Case II inChapter [HM1]).
The map ~: X’ ~X,
definedby (4.72)
and(4.73)
is a*-isomorphism of algebras.
A novel feature in theproof
of thisisomorphism
isshowing
We use
The convolution
fr0 * fu(x) */ro
isequal
toThe relation
allows us to
bring
to the left to be absordedinto fI.
Letso that
When r-10v(kz, mkz’)ro
is commutedby u(-1/(03B5y)),
the commutatoris introduced on the
right
side. When the measurebï,
is absorbedinto f;
onthe
right, 03C3(03B3)
appears. We obtain onsimplification
Hence,
But
since it intertwines
u(x)
and03C3(r0xr-10 ),
x E J nrû 1 Jra. Taking
the trace ofboth
sides,
we find themultiple
to be q. This proves(4.77).
REMARK. In both cases of
(4. la)
and also case(4.1b),
the center ofG’/T
is noncompact; and hence
G’/T
has no squareintegrable representations.
We conclude
GIT
has no squareintegrable representations containing (J, 6’ )
in these cases. In case(4.1 c), G’/T has
acompact
center and therefore discrete series.Here, q yields
abijection
between the discrete series ofG’/T
which have a contain a J’ fixed vector and those of
G/T
which contain(J, 6’ ).
5. Ramified
representations
We
complete
our classification of the irreduciblerepresentations
of Gby
describing
those which contain a ramifiedrepresentation (L, 03A9s).
The resultsin this section are very
analogous
to those of the level one and unramifiedrepresentations
in Sections 3 and 4.Consequently,
mostproofs
willjust
besketched.
The ramified
representations
were defined in Section 1. We recall the situation in(1.25).
For i EN,
considered the setsHere,
a,b,
c,d, e,f c- R,
and u, v, e ER ,
E a nonsquare. Write a set s in(5.1)
as
(cf. (1.26)).
Let 1 = n g. A ramifiedrepresentation (L, 03A9s) is
obtainedfrom s
by setting
1* (resp. 1*) equal
to the dual latticeof Î (resp. 1) in g (resp. g)
The group L is a
parahoric
filtrationsubgroup
in cases(5.1 a, b, d, e).
Incases
(5. la)
and(5.1 d),
L is a filtrationsubgroup
of the Iwahorisubgroup
B.
Indeed,
we have L =B4t-1 (resp.
L =B41-3)
for case(5. 1 a) (resp. (5.1 d)).
In case
(5.1 b),
L =M2t-1 (see (4.9)).
For the case(5.1 e),
letIt is trivial to check that
é
is an R-order inM4(F)
with radicalY().
Define the
parahoric subgroup
Nby (4.6)
and the filtrationsubgroups N,,
ofN by (4.7).
In thissetup,
L =N2t-2(i 2).
For case(5.1 c),
the group L is not a filtration group of aparahoric.
We say more about this case later.Cases
(5.1 a, d, e).
Webegin
with some normalizations. The set(5.1d)
isconjugate
under the Iwahorisubgroup B
to a set(5.1 d)
with u = 1.Similarly,
the set
(5.1 e)
isconjugate
via theparahoric subgroup
N to a set(5.1e)
with u = 1. Assume these normalizations.
Furthermore,
in case(5.1e)
ifv2 -
u2
modp,
take v2 = U2 . Define ocby (5.2). Let,
as in the unramified case,g’ (resp. G’)
denote the centralizer of a in g(resp. G).
Letg’~
be theorthogonal complement
tog’.
For aof type (5.1 a),
matrices ing’, g/-L
havethe form
and
respectively. Similarly,
if s is type(5.1 d),
matrices ing’
andg’~
have the formand
To describe the centralizer in case
(5.1 e),
we need todistinguish
whether v2and u2
areequal. If v2 ~ u2,
then317 If v2 =
U2,
thenIn all cases G’ is
anisotropic.
In cases(5.1 a), (5.1d)
and(5.5e.1),
G’ is ananisotropic
torus. In case(5.5e.2),
G’ isisogenous
to ananisotropic unitary
group in two variables over the unramified
quadratic
extension of F.Define g,u,
gi,u
andg by
the obviousanalogues
of(4.15).
The abovedescriptions
ofg’
andg~ yield decompositions
Let
In
analogy
with(4.20)
is