C OMPOSITIO M ATHEMATICA
H ISAYOSI M ATUMOTO
On the representations of U (m, n) unitarily induced from derived functor modules
Compositio Mathematica, tome 100, n
o1 (1996), p. 1-39
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
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On the representations of U(m, n) unitarily induced
from derived functor modules
HISAYOSI MATUMOTO*
Department of Mathematics, SUNY at Stony Brook, Stony Brook, New York, 11794-3651, USA e-mail: [email protected]
Received 14 June 1994; accepted in final form 26 September 1994
Abstract. We prove a decomposition formula of a representation of
U(m, n)
unitarily induced froma derived functor module, which enables us to reduce the problem of irreducible decompositions
to the study of derived functor modules. In particular, we show such an induced representation is decomposed into a direct sum of irreducible unitarily induced modules from derived functor modules.
© 1996 Kluwer Academic Publishers. Printed in the Netherlands.
0. Introduction
The easiest nontrivial
decomposition
of aunitarily
inducedrepresentation
of areal reductive Lie group from a
parabolic subgroup
is thedecomposition
of non-spherical principal
series ofSL(2,R)
at thesingular parameter
into two limits of discreteseries,
which are realized asHardy
spaces on the upper and lowerhalf-planes respectively.
Thisdecomposition
iscertainly
’easiest’.However,
it isnot very easy and it is
extremely important.
Forexample,
thanks to the recentprogress of the Beilinson-Bemstein
theory,
we can reduce Schmid’s characteridentity
at the wall([27, 28])
to the easiestdecomposition
forSL(2,R),
whichis
nothing
but the easiest Schmididentity, using
certainchange
ofpolarization (cf. [37],. [23], [7], [29,30], [22]).
In view of theKnapp-Zuckerman theory
onthe irreducible
tempered representations ([18]),
this means that the reducibilities ofunitarily
induced modules from discrete series arise from the above easiestdecomposition.
We can consider the
degenerate setting. Namely,
we considerunitary degen-
erate series instead of
unitary principal
series and derived functor modules(cf.
[36,38,39,41], [43], [17], [44, 45], etc.)
instead of discrete series. Ourobject
ofstudy
is thedecomposition
ofunitarily
induced modulesof U(m, n)
from derived functor modules(We
call such induced modulesgeneralized unitary degenerate series.).
Kashiwara and
Vergne
found a remarkabledecomposition
into n + 1 distinctirreducible factors of the
degenerate
seriesof SU(n, n)
withrespect
to theSiegel parabolic subgroup
at the mostsingular parameter ([15]).
Two of the irreducible factors arerepresentations
realized as theHardy
spaces on theSiegel
upper and lowerhalf-planes.
Theirembeddings
intodegenerate
series arenothing
but the* Supported by NSF-grant DMS-9100367.
boundary
value map to the Shilovboundary. Perhaps,
theembeddings
of otherirreducible factors can be
regarded
as certainboundary
value maps of ’cohomo-logical Hardy spaces’.
The case ofSU( 2, 2)
is considered in[21]. Although
acomplex analytical interpretation
of thedecomposition
is not clear at thistime,
the
corresponding algebraic interpretation
isavailable,
thanks to[2],
Theorem 4.2.Each irreducible factor is a derived functor module.
In this
article,
we show theKashiwara-Vergne decompositions play
a role onour
degenerate setting
forU(m, n)
similar to the role of the easiestdecomposition
for
SL(2, R)
on theKnapp-Zuckerman theory.
Since we shall consider the
Vogan-Zuckerman cohomological
inductions of Harish-Chandra modules(cf. [36])
withrespect
to variousparabolic subalgebras
ofthe
complexified
Liealgebra
ofU( m, n),
we introduce thefollowing terminology.
We call
cohomological
induction withrespect
to aparabolic subalgebra
stableunder a Cartan involution
(resp.
thecomplex conjugation
withrespect
to the realform) elliptic
induction(resp. hyperbolic induction). Namely, elliptic
induction iscohomological parabolic
induction in the sense of[39] Chapter 6,
andhyperbolic
induction is usual
parabolic
induction withrespect
to aparabolic subgroup.
Aderived functor module is
nothing
but theelliptic
induction from a one-dimensionalunitary representation satisfying
a certainpositivity
condition(’weakly
fair’ in thesense of
[41]). So, generalized unitary degenerate
series arehyperbolic
inductionof
elliptic
induction from certain one-dimensionalrepresentations.
In Section
2,
we considerexchange
of the order ofapplications
of these twoinductions.
Actually,
it ispossible
under a certainregularity
condition(’good enough’
see 2.1below.),
and the result is thatgeneralized unitary degenerate
seriesin the
good enough
range can be written as theelliptic
induction of the external ten- sorproduct
ofunitary degenerate
series withrespect
toSiegel parabolic subgroups
and one-dimensional
unitary representations (Theorem 2.2.3, Corollary 2.2.5).
Themain
ingredient
of ourproof
is thetheory
ofchange
ofpolarization
for standard moduleoriginated by Vogan ([37])
andcompleted by Hecht, Milicic, Schmid,
andWolf
([22], [29-31]). Actually, they
worked onD-modules,
but as is mentioned in[29],
we can translate their result to thecohomological
inductionsetting using
theHecht-Milii-Schmid-Wolf
duality
theorem([11]).
In Section
3, combining
the above result on thechange
of thepolarization
andthe
decomposition
formula ofunitary degenerate
series withrespect
to theSiegel parabolic subgroups [ 15], [2], [14],
we derive adecomposition
formula ofgeneral-
ized
unitary degenerate
series in thegood enough
range into non-zero irreduciblegeneralized degenerate
series(Theorem 3.2.2).
Thedecomposition
formula(The-
orem
3.3.1)
in thegeneral
case is deduced from the formula for thegood enough
range
using
aprecise
version of the translationprinciple developed
in[41].
Thedirect summand
appeared
in the formula in thegeneral
case is either irreducibleor zero. In order to obtain the ’true’
decomposition formula,
we must determinethe
ghost
direct summands. Weeasily
see thisproblem
is reduced to theproblem
of determination of the
parameters
in the fair range such that thecorrresponding
derived functor module is zero.
Although
somepartial
results are known(cf. [20]
Theorem
1.1, [41 ] Theorem 6.5, [19]
Sect.5),
that remains to be solved in future.Our result
suggests that,
for any real linear reductive group,generalized unitary degenerate
series aredecomposed
into a direct sum of irreduciblegeneralized unitary degenerate
series.Unfortunately,
this is a mere wishfulthinking.
The easiestcounterexample
is knownby
K. Gross[10]. Namely,
forSpin(5, C)
we considerthe
unitary degenerate
series for aparabolic subgroup
whose Levipart corresponds
to the
long simple
root. Thedegenerate
seriesdecomposed
into two irreduciblecomponents
at the mostsingular parameter. (Cf. [1])
Thisdecomposition gives
acounterexample.
Thisreducibility
of thedegenerate
series arises from the failure of thebirationality
of the moment map(to
itsimage)
of thecotangent
bundle ofthe
corresponding generalized flag variety. (For
moreprecise theory,
see[3].) Probably,
moremysterious decomposition
is theKashiwara-Vergne decomposi-
tion
([15]) for Sp(2n+1, R),
which seems verylikely
to be anothercounterexample.
At
least,
some irreducible factors are not the naturalcandidates, namely
’cohomo-logical Hardy spaces’,
which are derived functor modulesarising
from certainCayley
transforms.(For example,
it follows from[25,26].)
If all the irreducible factors should be derived functormodules,
we would have acounterexample
for theBarbasch-Vogan conjecture
on thequantized Kostant-Sekiguchi correspondence.
This
decomposition
is verynicely explained
in terms of the dual reductivepair.
However,
I do not know any reasonabledescription
of some irreducible factors in terms ofSp( 2n
+1, R)
itself.I was
inspired through
the effort to understand whathappens
on theunitary
axisin a result in
[12]. (There
is atiny overlap
between their results andours.)
List of
Symbols
1.1
A - B, G~,
[V],
1.2
C03C1(u),
Riq((I, L ~ K) ~ (g, K); V), Riq(I ~ g; V), Ind(P ~ G; Y), IndGP(V),
A(q fi
g;A), 49(A),
1.3
M~(C),
B(X, Y),
C~[p,q],
e1,...,e~,
Jl,
U(m, n), u(m, n), g(m, n), P~(m, n), P(m, n),
(m, n),
U(m, n), g(m, n), K(m, n), ~(m, n), (m,n)03C3,
03A6m,n, ~m,n, Pd(r), P(r),
r *
(p, q), U(r, r)
*U(p, q),
1.4
Ci, Cr(X), G1L( m, C), S(m),s(m),
h(m,
n;s), 0(m,
n;s), W(m,
n;s), lm,
n;. s] i,
(1),
P(m,
n;s), Pu(m,
n;s), h(m,
n;s)*
0394+(m,
n; s;03BB),
p+(m,
n;s), 03C1-(m.n; s), p(m,
n;s), z(m, n), [[m, n]],
bx(m, n; s),
Di(m,
n;s), 0394r(m,
n;s), 0394c(m,
n;s), S (m, n),
h(m,
n;s), H(m,
n;s), 0(m,
n;s), 0(m,
n;s), W(m,
n;s), W(m,
n,s), 0394i(m, n; s), OT (m,
n;s), 0394c(m,
n;s),
CÀ (m, n; s),
[m,
n; s;i]j, [[m,
n; s;i]]+, [[m,
n; s;i]]-, [[m,
n; s;i]], W(r),
9(LR(r, C), bLR(r, C), S(r), s(r),
2.1
I(r; p, q), L(r; p, q),
c(r; pl q),
[[r; p, q; i]],
0394+(r;p,q;t), p, q), q(r; p, q), Sr;p,q,
p(r; p, q),
P(r;
p,q), P*(r; p, q), P*u(r; p, q),
C03BB(r; p, q),
m(r;
P,q), M(r;
P,q), 0394(r;
p,,q;t),
p(r;
p,q), q(r; p, q), P+ p, q), P+u p, q),
(03BB), 03BB(k),03BB(k),
9 (r; I!, q),
q(m, m), b(m, m), p(m, m), P+(m, m), G(m, m),
2.2
0394+2(r;p,q;t;03BB),
to(r;p,q;03BB),f(r;p,q;03BB), P2(r; p, q; 03BB),
q1(r;p,q;03BB), fr;
P,q; A,a(p ),
2.3
W (1:; p, q; t), 0394(r; p, q; t), 0394+(r; p, q; t; ri), n(r;
p, q;t- ’11) b(r;
p, q;t- ’11) 1!(r;
p, q;t; ~), 03A0(r;
p, q;t; ~),
03C1(r;
p, q;t; i), e(r;
p, q;t), p(r; p, q; t), W(;t),03C1(;t),0394+(;t)x,03A0(;t)x,b(;t)xn(;t)x,
St,x,
b(;t)x,0394+(;t)x,03A0(;t)x,
b1(;t;03BB)x,0394+1(;t;03BB)x,03A01(;t;03BB)x,
2.4
{i}j,ht(0394+),
3.1
c( r), 03BB(z,03BC),
3.2
À (z, 03BC),
X(r;
p,q), Y(r;
p,q), e(03C3;i),(i),r|k,
3.3
c(a).
1. Notations
1.1. GENERAL NOTATIONS
In this
article,
we use thefollowing
notations.As usual we denote the
complex
numberfield,
the real numberfield,
the ratio-nal number
field,
thering
ofintegers,
and the set ofnon-negative integers by C, R, Q, Z,
and Nrespectively.
For a
complex
vector spaceV,
we denoteby
V* the dual vector space. For a real vector spaceVo,
we denoteby V¿
the real dual vector space ofVo.
We denoteby 0
theempty
set and denoteby
A - B the set theoretical difference of A from B.For each set
A,
we denoteby
card A thecardinality
of A. For acomplex
number a(resp.
a matrix X overC),
we denoteby a (resp. X)
thecomplex conjugation.
Ifp > g, we put 03A3qi=p = 0.
Let R be a
ring
and let M be a left R-module. We denoteby AnnR(M)
theannihilator of M in R.
In this
article,
a character of a Lie group G means a(not necessarily unitary)
continuous
homomorphism
of G toC .
For a matrix X =
(aij),
we denoteby tX, tr X,
and det X thetranspose (aji)
of
X,
the trace ofX,
and the determinant of Xrespectively.
We denote
by 61
the Ahsymmetric
group.For a
complex
Liealgebra
g, we denoteby U ( g )
its universalenveloping algebra.
For a Harish-Chandra module
V,
we denoteby [V]
thecorresponding
distri-bution character. In this
article,
an irreducible Harish-Chandra module should benon-zero.
Ad means the
adjoint
action of a Lie group on itscomplexified
Liealgebra.
1.2. COHOMOLOGICAL INDUCTION
Next,
we fix the notations on theVogan-Zuckerman cohomological
induction of aHarish-Chandra module
(cf. [36,38,39,41], [44,45], [16], [43], etc.).
Let G be a connected real reductive linear Lie group and let g be its
complexified
Lie
algebra. (Assuming
connectednesssimplifies
definitions below a littlebit.)
Wefix a maximal
compact subgroup
K of G and denoteby 0
thecorresponding complexified
Cartan involution of g. We denoteby t
thecomplexified
Liealgebra
of K. Let q be a
parabolic subalgebra
of g with a Levidecomposition
q = l + usuch that l is stable under 0 and the
complex conjugations
withrespect
to G. Wefix a Cartan
subalgebra h
of and aWeyl
group invariantnon-degenerate
bilinearform
(, ).
Let L be thecorresponding
Levisubgroup
in G to L LetC03C1(u)
be a1-dimensional
representation
of themetaplectic
double cover L~ of L which is asquare root of z -
det(Ad(x)|u) (cf. [41]).
Let(K
nL )"
be the maximalcompact subgroup
of L~corresponding
to L n Il.Let V be a Harish-Chandra
(i, (li
nL)-)-module
such thatV 0 C03C1(u)
is aHarish-Chandra
([,
AT flL)-module. Introducing
the trivial action of u, we alsoregard V 0 Cp(u)
as aq-module.
Let À be the infinitesimal character of V withrespect
toh. (It
is well-defined up to theWeyl
group action ofL)
Following [41],
we introduce thefollowing
notions. We call Vgood (or
À is inthe
good range),
ifRe(À, a)
> 0 holds for each root aof h
in u. We assume[1, 1]
acts on V
trivially.
We denoteby 3
the center of I. We call Vweakly
fair(or À
is inthe
weakly
fairrange), ifRe(ÀI3’ 03B1~
0 for each root aof h
in u.For a
non-negative integer i,
we denoteby Riq((l,
L flK) ~ (g, K); V)
the resultof
applying
the ith Zuckerman functor(namely,
the ithright
derived functor oftaking
’the K-finitepart’)
toHomu(q)(U(g), V 0 Cp(u),
where Hom is definedusing
the left action of q onU(g)
and made into a leftg-module using
theright
action.
(For details,
see[36], etc.) Riq((l,
L flK) ~ (g, K); V)
is zero or a Harish-Chandra
(g, K)-module
with ageneralized
infinitesimal character À.(For example,
we can prove this as follows.
Using
inductionon ~ ~lambda (cf. [38] Corollary 3.25)
and
long
exact sequences, we can reduce theproblem
to the case of standardmodules, namely
the case that q is a Borelsubalgebra. Then,
we canapply
theHecht-Milicic-Schmid-Wolf
duality
theorem and can reduce theproblem
to thecase of standard
D-modules.)
If L ~ K isconnected,
wesimply
writeRI([ ~ g; V)
for
Riq((l,
L nK) ~ (g, K); V).
Infact,
forU(m, n)
this connectedness conditionalways
holds.The
following
threeparticular
cases areimportant (in
thisarticle).
(1) (Hyperbolic induction).
If q is stable under thecomplex conjugation
of g withrespect
toG,
there is aparabolic subgroup Q
= L U whosecomplexified
Liealgebra
is q and whose nilradical is U. In this case, we have
Riq((l,
L nK) ~ (g, K); V)
= 0for all i > 0 and
RO«[,
L flK) 1 (g, K); V)
coincides with the usualparabolic
induction
Ind(Q ~ G; V) (We
also writeIndGQ(V).).
HereInd(Q fi G; V)
is the K-finite
part
ofHere, (03C0, H)
is any Hilbertglobalization
ofV ~ C03C1(u) .
If V isunitarizable,
sois
Ind(Q ~ G; V) (unitary induction).
If L is connected and ifCA
is the one-dimensional
L-representation
with infinitesimal characterÀ,
wesimply
writeIndGQ(03BB)
orInd(Q ~ G; 03BB)
forIndGQ(C03BB).
We have the
following
additiveproperty.
Let
Vo, Vi, ... , Vk
be Harish-Chandra(r, (L
flK)~)-modules
such thatV0 ~
Cp(u) i
...,Vk 0 C03C1(u)
are reduced to Harish-Chandra(1,
L nK)-modules.
Letnl, ... , nk be
integers.
If we have a characteridentity [V]
=03A3ki=1ni[Vi],
we have[Ind(Q 1 G; V)] = 03A3ki=1 nk[Ind(Q 1 G; Vi)].
(2) (Elliptic induction).
Assume q is 0-stable andput
S =dim(u nt).
IfV is
good,
thenRiq((l,
L flK) 1 (g, K); V)
= 0 for i~
S. If V is irreducible(resp. unitarizable)
andgood, RSq((l,
L nK) ~ (g, li ); V)
is also irreducible(resp.
unitarizable) ([38]).
Moreover,
we assume[1, 1]
acts on Vtrivially
and V is irreducible andunitary.
In this case, V is 1-dimensional and we denote it
by CA.
Assume that À is in theweakly
fair range.Then, Riq((l,
L nK) 1 (g, K); CA)
= 0 for all i~
S. We alsohave
Riq((l,
L flK) 1 (g, K); Cx )
is either zero or non-zero unitarizable Harish- Chandra module([38]).
In this case, weput
We call it a derived functor module.
(Our parameterization
is different from thatof
[43].)
Ingeneral, A(q 1 g; À)
may be reducible for someweakly
fair À.(An example
occurs inSO(5,C) (K.
Gross[10], Borho).
Anotherexample by
D. A.Vogan
is described in[4].) However,
if G =U( m, n ) (or
othertype
Agroups),
thesituation is much
simpler.
The moment map ofcotangent
bundle of anygeneralized flag variety
ofGL( n, C)
is birational to itsimage
and the closure of anynilpotent
orbit of
gl(n, C)
is normal. Hence the canonicalhomomorphism
of the universalenveloping algebra to
thering
ofglobal
sections of the sheaf of twisted differentialoperators
on ageneralized flag variety
ofGL(n, C)
isalways surjective (cf. [4]
6.2Proposition (a)). Hence,
if G =U(m, n), 4(q 1
g;a)
is zero or irreducible for anyweakly
fair À(cf. [41], [4]).
The
additivity property
ofRSq
in this case is described as follows. We fix aninfinitesimal character À in the
good
range withrespect
to q. LetVo, Yl, ... , Vk
be Harish-Chandra
(1, ( L
nK)-)-modules
with infinitesimal character À and let nl,..., nk beintegers.
We alsoassume Y2
~Cp(u)
is reduced to a Harish-Chandra(1,
L nK)-module
for each0
i k. Moreover we assume a character iden-tity [V] = 03A3ki=1ni[Vi]
holds.Then,
we have[RSq((l, L
nK) ~ (g, K); V)] =
03A3ki=1nk[RSq((l, L ~ K) ~ (g, K); Vi)].
(3) (Standard modules).
The case of q = Borel. In this case, the induced modules are called standardrepresentations.
Suchrepresentations
areprecisely
studied in
[34], [36], [11], [31], [29,30], [22],
etc.Finally,
we recall the notion ofinduction-by-stage ([36] Corollary 6.3.10).
Letqi
( i
=1, 2)
beparabolic subalgebras
of g with Levidecompositions
qi== (i
+ ui suchthat [j
is stable under 0 and thecomplex conjugation
withrespect
to G. Wedenote
by Li
thesubgroup
of Gcorresponding
toCi. Moreover,
we assume q2 C q1.Then q3 =
q2 n r,
is aparabolic subalgebra of l1
with a Levidecomposition
q3 =12
+(u2 ~ (1).
Put u3 =u2 ~ (1. Let p
bea non-negative integer and
let V be a Harish-Chandra
(12, (L2 ~ K)~)-module
such thatV ~ C03C1(u2)
is reduced to a Harish-Chandra(12, L2 ~ K)-module. Assume that Riq3((l2, L2 ~ K) ~ (l1,L1~K); V~ Cp(u1)
= 0for all
i ~
p.Then,
forall q 0,
we haveIf
cp( u 1)
is reduced to a character ofL 1,
we can rewrite the above formula asfollows.
1.3. NOTATIONS FOR
U(m, n)
Let 1 be a
positive integer.
We denoteby Mi ( C)
the space ofcomplex
1 x £-matrices.We
regard d
as a space of vertical vectors.M~(C)
and thegeneral linear
groupGL(2, C)
act onC~ by
the leftmultiplication.
We denoteby gl(~, C)
the Liealgebra
of
GL(~, C)
andidentify
it withM~(C).
We denoteby Il
theidentity
matrix inM~(C).
ForX,
Y Egl(~, C),
weput
Then,
B is anon-degenerate symmetric
bilinear form ong[(~, C)
which is invariantunder the
adjoint
action. We denoteby Ep,q
the matrix such that its(p, q)-entry
is 1 and the other entries are 0. For
1 z k z ~,
we denoteby
ek CC~
the vertical vector such that its i-thentry
is 1 and the other entries are zero. We call 61,..., el the standard basisof d .
For1 p q ~,
we defineIf q
p, weput C~[p, q] = {0}.
We define a matrixJi
inM~(C)
as follows.We fix
non-negative integers
m and n such that m + n > 0. We fix thefollowing non-degenerate
indefinite Hermitian forms oncm+n
as follows.We consider the
following
realization of the indefinite groupU(m, n) = tg
EGL(m + n, C) 1 (gx, gy) = (x, y) (x, y E V ) 1 .
We denote
by u(m, n)
the Liealgebra
ofU(m, n). Namely,
weput u(m, n) = tX
Eg(( m
+ n,C) | (Xx, y)
+(x, Xy) = 0 (x, y
eV)},
Then
gt(m
+ n,C)
can beregarded
as thecomplexification of u(m, n).
In order tomake our notation
systematic,
we also denotegl(m
+ n,C) by g(m, n).
We alsomean
by U(0, 0)
the trivial group{1}
andby u(0, 0)
the trivial Liealgebra {0}.
For a,
b, c, d ~ N
such that0 z a z b
m and0
cd
n, weput
U(m,
n; a,b;
c,d) = tg
eU(m, n) 1 g
satisfies thefollowing (1), (2).}.
Using
this t, we canidentify U( m,
n; a,b;
c,d)
andU(b -
a, d -c).
We call suchan identification the standard identification.
Let 1 be a
positive integer.
PutWe also
put
If
(m, n) E P(m, n )
satisfies(m, n)
EP~(m, n),
we call ~ thelength
of(m, n).
For
(m,n)
=((m1,...,m~),(n1,...,n~))~P~(m,n),
we denoteby U( m, n)
thesubgroup
ofU( m, n ) generated by U( m, n; 03A3k-1i=1 mi, 03A3ki=1 mi;
m +n - 03A3ki=1 ni,
m +n - 03A3k-1i=1 ni)
for all1 k
~.Through
the standard identifica-tion,
we have the standard identificationsof U(m, n)
as follows.If m = n =
0,
weput U((0), (0)) = {1}.
We denote the Lie
subalgebra
ofg(m, n) corresponding
toU(m, n) by g(m, n).
Then,
we have thefollowing
standard identifications:We
put K(m, n)
=U((m,0),(0,n)) ~ U(m)
xU(n)
andt(m,n) = g((m, 0), (0, n)). K(m, n)
is a maximalcompact subgroup of U(m, n).
We denoteby 0
thecomplexified
Cartan involution ofg(m, n)
withrespect
tot((m, n).
For
(m, n)
eP(m, n), U(m, n), u(m, n),
andg(m, n)
are 0-stable. PutK(m, n) = K(m, n)
nU(m, n)
and denoteby e(m, n)
the+1-eigenspace
withrespect
to 0 ing(m, n). K(m, n)
is a maximalcompact subgroup
ofU(m, n)
andë(m, n)
is thecomplexified
Liealgebra
ofK(m, n).
We define a group
homomorphism ~m,n: G~ ~ Gm+n
as follows.For any
subgroup H
ofU(m,n),
we denoteby
H03C3 thesubgroup 03A6m,n(03C3)
H03A6m,n(03C3)-1 of U(m03C3,n03C3).
Let r be a
non-negative integer
such thatr min{m, b}
and let d be apositive integer.
Weput
We also
put
Comparing
the standard identifications ofU(p, q), U(r, r),
andU(r, r) * U(p, q),
we obtain the standard identification
U(r, r) *U(p, q) - U(r, r)
xU(p, q).
For anysubgroup Hl
ofU(r, r)
and anysubgroup H2 of U(p, q),
wedenote by Hl * H2
the
subgroup
ofU(p, q) * U(r, r) corresponding
toHl x H2
under the standard identification.We have
K(r, r) * K(m, n)
=K(r * m, r * n)).
We use similar notations for the Liealgebras.
1.4. CAYLEY TRANSFORMS AND CARTAN SUBALGEBRAS
Let m, n be
non-negative integers
such that m + n > 0 as above. For1
imin{m, n},
weput
Clearly, Ci’s
are commutative with each other and we havetCi
=C-1i.
For
1 x
r xmin{m, nl
and X EMm+n(C),
weput
We also
put co(X)
= X. We canregard
c, as an innerautomorphism
of bothGL(m
+ n,C)
andg(m, n).
For a
while,
we areconsidering
aspecial
case m = n. In this case,Cm cm -
...Ci
eGL(2m, C)
is written as follows.We denote
by U(m, m)
thesubgroup
inGL(2m, C)
such thatcm (U (m, m)) = U(m, m).
We callU(m, m)
the twisted realizationof U(m, m).
U(m, m)
contains thefollowing subgroup.
Hence
GL(m, C)
is asubgroup
ofU(m, m).
We define the standard identificationGL ( m, C) ~ GL(m, C) by
For m =
(ml, ... , ml)
eIID( m),
we denoteby GL(m, C)
thesubgroup of U(m, m)
corresponding
toGL(mi, C)
x ... xG1L( ml, C)
via the standard identification ofU(m, m).
PutGIL((0), C)
={1}.
We also consider thefollowing
Liesubalgebras
in
g(m, m).
Then
glL(m, C)
xg(R( m, C)
is thecomplexified
Liealgebra
ofGL(m, C).
We denote
by 6(m, C)
the Borelsubalgebra
ofg(( m, C) consisting
of the uppertriangular
matrices. PutWe call
S(m) (resp. z(m»
theSiegel parabolic subgroup (resp. subalgebra)
ofU(m, m) (resp. g(m, m)).
Next,
we fix thecomplexification
of acompact
Cartansubalgebra of u(m, n)
asfollows.
For
1
smin{m, n},
we consider thefollowing
Cartansubalgebras:
{h(m,n;0),h(m,n;1),...,h(m,n;mm{m,n})}
forms acomplete system
ofrepresentatives
ofK(m, n ) conjugacy
class of Cartansubalgebras
ofg(m, n)
stable under 0 and
complex conjugation
withrespect
tou( m, n ) .
We introducea
symmetric
bilinearform (, )
induced fromB ( , ) on h(m,
n;s)*.
Of course,the
Cayley
transform c, induces anisometry of h ( m, n; 0)* to h (m, n; s)*.
Wedenote
by 0394(m,
n;s ) (resp. W(m,
n;s ) )
the rootsystem (resp.
theWeyl group)
of(g(m, n), h(m,
n;s)).
We denoteby [m,
n;s]1,..., [m,
n;s]m+n
the dual basis ofh(m,
n;s)*
tocs(E1,1),..., cs(Em+n,m+n).
We call[m,
n;s]1,..., [m,
n;s]m+n
the standard basis
of h(m,
n;s)*.
Then we have:W(m,
n;s )
isnothing
but the groupconsisting
of all thepermutations
of[m,
n;s]1
,...,
[m,
n;8]m+n-
We shallidentify
an element of theWeyl
groupW(m,
n;s)
andthe
corresponding permutation
of1,...,
m + n so thatw[m,
n;S]i
=[m,
n;s]w(i)
for all w e
W(m,
n;s)
and1
i m + n. Then(, )
is aWeyl
group invariantnon-degenerate symmetric
bilinear form onb (m,
n;s)*
such that[m,
n;s]1,..., [m,
n;s]m+n
form an orthonormal basisof f)(m,
n;s )*.
PutLet
H( m,
n;s )
be the Cartansubgroup of U( m, n ) corresponding to h(m,
n;s ) . They
are all connected. Weeasily
see À~ h(m, n)*
can beexponentiated
to acharacter
(resp.
aunitary character)
ofH( m,
n;s )
if andonly
if À~ P(m, n ) (resp.
03BB ~ Pu(m, n; s)).
For À
= 03A3m+ni=103BBi[m, n; s]i ~ h(m, n)*c, we define a positive system of 0394(m, n; s)
as follows.
For À
~ h (m, n)*c,
we denoteby n(m,
n; s;03BB)
the sum of all the root spacein
g(m, n) corresponding to 0394+(m, n;,s; 03BB).
Putb(m, n; s; 03BB) = h(m, n; s)
+n( m,
n; s;03BB). Then b(m,
n;s; 03BB)
is a Borelsubalgebra of g ( m, n )
with the nilradi- caln(m,
n; s;03BB).
This Borelsubalgebra
ismaximally
real in the sense of[29,30].
We also
put
as follows.For x E
W(m,
n;s ),
weput bx( m,
n;s ) = b(m,
n; s;x03C1(m,
n;s ) )
andn( m,
n;s) = n(m,
n; s;xp(m,
n;s)).
We denote
by z(m, n)
the center ofg(m, n). Namely z(m, n)
is the one-dimensional
subalgebra consisting
of scalar matrices.Using ~ , ~,
we canregard z(m, n)*
as asubspace of h(m,
n;s)*.
If weput
then
[ [m, n]] does
notdepend
on s and we have[[m, n]] E 3(m, n)*.
The Cartan involution 0 acts
on h(m,
n;s)
as follows.Put
An element of
0394i(m, n; s), 0394r(m, n; s),
and0394c(m, n; r)
are calledimaginary, real,
andcomplex, respectively.
Next,
we fix(m, n) = ((m1,..., m~), ( n 1, ... , n~))
EP~(m, n).
Weput
We also put S)((0), (0)) = (0).Fors= (s1,...,s~) ~ S(m,n) and 03C3 ~ G~, we
put
s03C3 =(s03C3(1),..., s03C3(~) ~ S(m03C3, n03C3). For s = (s1,..., si)
ES(m, n),
we denoteby h(m, n; s)
the Cartansubalgebra
ofg(m, n) corresponding to h(m1, n1; s1)
x...
h(m~,
n£;si)
via the standard identification ofg(m, n).
We also introduce anon-degenerate Weyl
group invariant bilinear form( , ) on h(m,
n;s)*.
Let
H(m,
n;s)
be thecorresponding
Cartansubgroup
ofU(m, n).
We denoteby 3(m, n)
the center ofg(m, n). Using (, ),
weregard 3(m, n)* as
asubspace
ofh(m, n; s)*.
Let
0(m, n; s) (resp. A(m,
n;s))
be the rootsystem
ofg(m, n) (resp. g(m, n))
with
respect to h(m, n; s).
LetW(m, n; s) (resp. W(m, n; s))
be theWeyl
groupof
g(m, n) (resp. g(m, n))
withrespect to h(m,
n;s).
We also defineP(m,
n;s), Pu(m,n;s), Ai (m!,
n;s), A, (m,
n;s),
and0394c(m,
n;s)
as above. We have the fol-lowing
standard identifications.À
~ h(m, n; s)*
can beexponentiated
to a character ofH(m, n; s)
if andonly
if À
~ P(m, n; s).
We denoteby C03BB(m, n; s)
the one-dimensionalrepresentation
of the
metaplectic
double cover ofH(m, n; s) corresponding
to À~ 1 2 P(m, n; s).
C03BB (m, n; s)
is unitarizable if andonly
if À E1 2 Pu(m, n; s).
For À
~ h(mi,
ni ;si)* (1
i~),
we denoteby 03BB(i)
thecorresponding
elementin h(m, n; s)*
withrespect
to the standard identification. For1
i~
and1
j
mi + ni, weput [m,
n; s;i]j
=[mi,
ni;si] (i)j.
Hence all the[m,
n; s;i]j
form a basis
of h(m,
n;s)*.
If m, n, and s are
given
and if there is noconfusion,
wesimply
write[i]j
for[m, n; s; i]j.
We dénote
by f)(m,
n;s)*c
the subsetof h(m,
n;s)* coressponding to h(m1,
n1;s1)*c
···h(m~,
ni;s~)*c
via the standard identification.For
1
i~,
weput
We
easily
see[[m, n; i]]
=[[m,
n; s;i]]+
+n; 5; i]]-
for all i. We also see[[m, n. 1]],..,. [[m, n; ~]] form
a basisof 3 (m, n)*. For A c- z(m, n)* ~ 1 2 P (m,
n;0~),
we denote
by C03BB (m, n)
thecorresponding
one-dimensionalrepresentation
of themetaplectic
double cover ofU(m, n).
For the case m = n, for r =
(r1, ... , rd) E P(m),
we denoteby G1L(r, C) (resp.
6’(r))
thesub-group of U(m, m)
whichcorresponds
toGL(ri, C)
x ... xGLL(rd, C)
(resp. S(rl)
... xS(rd))
via the standard identification. We denoteby
glLR(r, C) (resp. bLR(r, C))
the Liesubalgebra
ofg(m, m) corresponding
to(g(L( rI, c)
XglR(r1, C))
X ... x(glL(rd, C)
XglL(rd, C)) (resp. (bL(r1, C)
XbR(rl, C))
X ... X(bL(rd, C)
XbR(rd, C)))
via the standard identification. We also defines(r) similarly. g(LR(r, C)
is thecomplexified
Liealgebra
ofGL(r, C).
We dénote
by W(ri)
theWeyl
group for(glL(ri, C)
Xg(R(ri, C), h(ri,
ri ;ri))
for
1
i d. We also denoteby W(r)
theWeyl
group for(g(LR(r, C), h(r, r; r)).
Then we have the
following
standard identification.2.
Change
ofpolarizations
2.1. GENERALIZED UNITARY DEGENERATE SERIES
We fix
non-negative integers
m, n, and r such that m + n > 0 and0
rmin{m, n}.
Put p = m - rand q
= n - r. We also fix r =(rl, ... , rd)
EPd(r) and(p,q) = ((P1,...,ph),(q1,...,qh)) ~ Ph(p,q). Put ~ = d + h and (m, n) = ((m1,..., 5 MI), (y,
... ,ni)) = (r *
p, r *q)
EP~(m, n).
For
simplicity,
we writel(r; p, q)
andL(r;
p,q)
forg(LR(r, c)
*g(p, q)
andGL(r, C)* U(p, q) respectively.
Fort
= (tl,...,th) ~ S(p, q)
we have r*t =(r1,...,rd,t1,...,th)
eS(m,n).
And h(m,
n ;r * t) (resp. H(m,
n;r * t))
is a Cartansubalgebra (resp. subgroup)
of1(r;
p,q) (resp. L(r;
p,q)).
We denoteby c(r;
p,q)
the center of((r;
p,q). Using (, ),
weregard c(r; p, q)*
as asubspace of h(m,
n ; r *t)*.
For
1
i 2d +h,
weput
We
immediately
see[[r;
p, q;1]],..., [[r;
p, q; 2d +h]
form a basis ofc(r;
p,q)*
and
they
areindependent of t
eS(p, q).
We define the
following
subset of0(m,
n; r *t)
for t ~ S(p, q).
We denote
by u(r;
p,q)
the sum of the root spacescorresponding to 0+(r;
p, q;t).
We
easily
seeb(r;
p,q)
does notdepend
on the choice of t. Putq(r; p, q) =
((r;
p,q)
+n(r;
p,q).
Thenq(r;
p,q)
is aparabolic subalgebra
ofg(m, n)
with aLevi part (resp. the nilradical) ((i;
p,q) (resp. b(r; p, q)).
We also
put
We see that À E
c(r; p, q)
can beexponentiated
to a character ofL(r; p, q)
if andonly
if À eP(r;
p,q).
We denoteby C03BB (r;
p,q)
thecorresponding
one-dimensionalrepresentation
of themetaplectic
double cover ofL(r; p, q) to À e P (r; p, q).
For03BB ~ 15* (r;
p,q), C03BB (r;
p,q)
is unitarizable if andonly
if À eP*u(r;
p,q).
Next,
we considera parabolic subgroup of U(m, n).
We denoteby m(r;
p,q)
theLie
subalgebra of g((r1, ... ,
rd,p), (r1, ... ,
rd,q)) corresponding
toglLR(r1, C)
x... x
OILR(rd, (C)
xg(p, q)
via the standard identification. If p = q =0,
weput m(r; 0, 0)
=g(LR(r, C).
We denoteby M(r;
p,q)
thesubgroup
ofU(m, n) corresponding
toGL(r, C)
xU(p, q)
via the standard identification. We denoteby 0(r; p, q; t)
the rootsystem
for(m(r; p, q), h(m, n; r * t)).
Putp(r; p, q) = q(r; p, q)
+m(r; p, q). Then, p(r; p, q)
is stable under thecomplex conjugation
of
g(m, n)
withrespect
tou(m, n).
We denoteby P(r;
p,q)
thecorresponding parabolic subgroup
ofU(m, n)
top(r;p, q)
with a Levipart M(r; p, q).
We alsodenote
by N(r;
p,q)
the nilradicalof P(r;
p,q).
Anarbitrary parabolic subgroup
ofU(m, n)
isconjugate
to someP(r,p, q).
Next,
weput q(r; p, q)
=q(r;
p,q)
nm(r;
p,q). Then, q(r;
p,q)
is a 0-stableparabolic subalgebra of m(r; p, q)
with a Levipart f(r;
p,q).
We denoteby b(r;
p,q)
the nilradical
ofq(r;
p,q).
Weeasily
seedim(!!(r;
p,q) fl (m(r;
p,q)
nt( m, h))) = Sr;p,q.
We put
We
immediately
see:LEMMA 2.1.1. For A E
P (r;
p,q),
A EP+ (!:;
p,q) ifand only if the infinitesimal
character