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Ark. Mat., 36 (1998), 191-200

@ 1998 by Institut Mittag-Leffler. All rights reserved

Invariant fundamental solutions and solvability for symmetric spaces of type GC/GR with

only one conjugacy class of Cartan subspaces

Nils Byrial Andersen

I n t r o d u c t i o n

Let G / H be a reductive s y m m e t r i c space and let D: C ~ ( G / H ) - ~ C ~ ( G / H ) be a non-trivial G-invariant differential operator. An invariant fundamental solution for D is a left-H-invariant distribution T on G / H solving the differential equation

(*) D T = 5,

where 5 is the Dirac measure at the origin of G / H .

Assume t h a t G / H is of t y p e G c / G R (G complex and H a real form of G) and t h a t H , up to conjugacy, has only one C a r t a n subalgebra. Let A denote the associated C a r t a n subset of G / H , identified with a real abelian subgroup of G.

Using results from the theory of orbital integrals defined on G / H obtained by Bouaziz, Harinck and Sano, we can t h e n reduce (*) to a differential equation on A,

F ( D ) T a = 5A

for some distribution TA on A, where F ( D ) is a uniquely defined differential ope- rator with constant coefficients on A and 5A is the Dirae measure at the origin of A, i.e. TA is by definition a fundamental solution for F ( D ) . Our main result is the following theorem.

T h e o r e m 5. Let D be as above. Then D has an invariant fundamental solu- tion on G / H if F ( D ) has a fundamental solution on A.

Our result is similar to results obtained by Helgason for R i e m a n n i a n s y m m e t r i c spaces, see [11, T h e o r e m 4.2], and by Rouvi~re for semisimple Lie groups with only

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one conjugacy class of C a r t a n subalgebras, see [15, T h e o r e m 4.2], and our approach is very much inspired by their works.

Assume now t h a t D has an invariant fundamental solution on

G/H.

T h e n D is solvable, in the sense t h a t

DC~(G/H)=C~(G/H),

if

G/H

is D-convex, see [1, pp. 301ff.]. Van den B a n and Schlichtkrull give in [1, T h e o r e m 2] a necessary con- dition on D for D-convexity of

G/H,

and we show t h a t this condition implies t h a t F ( D ) has a fundamental solution on A, and hence, as an application of T h e o r e m 5, t h a t D is solvable, see T h e o r e m 7.

N o t a t i o n

Let G be a reductive complex connected Lie group with Lie algebra g, and let H be a real form of G with Lie algebra ~. Let cr denote the conjugation of 1~ relative to b and let also cr denote the involution of G whose differential is a, t h e n H is the open connected subgroup of G ~, the fixpoint set of cr in G. T h e space

G/H

is said to be a reductive s y m m e t r i c space of t y p e

Gc/Ga.

Let 9=%Oq be the decomposition of g into the d-l-eigenspaces of a, where q = i b . Let 0 be a C a r t a n involution of

~t c o m m u t i n g with or, and let g=t~Gp be the usual C a r t a n decomposition into the i l - e i g e n s p a c e s of 0. Let

K=G ~

be the m a x i m a l c o m p a c t subgroup of G consisting of fixpoints of 0, with Lie algebra t~.

Let p be the canonical projection of G onto

G/H

and let ~ be the m a p of

G/H

into G defined by

G/HDp(g)~gcr(g ) t CG, gcG.

T h e image of p in G, denoted by X, is a closed submanifold of G, see [14, p. 402], and p is seen to be a G-isomorphism from

G/H

onto X, equipped with the G-action

g.x-gxa(g) -1, xEX, 9cG.

We will in the following use this realization of the s y m m e t r i c space

G/H.

Denote the space of distributions on X by 7?t(X). T h e group G acts naturally on ~D'(X) via the contragradient representation (on

G/H),

and we denote the H - invariant distributions under this action by ~D~(X) H.

Let exp denote the exponential m a p of 9 into G.

C a r t a n s u b s p a c e s , C a r t a n s u b s e t s a n d r o o t s y s t e m s

A C a r t a n subspace a for X is defined (cf. [14, w as a m a x i m a l abelian subspace of q consisting of semisimple elements. We see, since ~ is a real form of g, t h a t a is a C a r t a n subspace for X if and only if

ia

is a C a r t a n subalgebra of ~1. T h e C a r t a n subset A of X associated to a C a r t a n subspaee a for X, is defined (cf. [14,

gll)

as the set of d e m e n t s x ~ X centralizing a in G (under the adjoint action).

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Invariant fundamental solutions and solvability for symmetric spaces 193 So let a be a C a r t a n subspace of q. We denote by A = A ( B , a c ) the root system of the pair (0, a e ) , where

ac=a+ia.

We choose a set of positive roots denoted by A +. Let W denote the Weyl group corresponding to the root system A. Let Ha, respectively 1~, denote the coroot, respectively the root space, of the root a C A .

We say t h a t a root s E A is real, respectively imaginary or complex, if it is real- valued, respectively imaginary-valued, or neither real- nor imaginary-valued, on the Cartan subalgebra

ia

of 0. The set of real roots, positive real roots, imaginary roots, positive imaginary roots, complex roots and positive complex roots are denoted by A m A ~ , AI, A~, A c and A ~ respectively.

Let a E A I . The root a is called compact if and only if ( g ~ + f t _ ~ + C H ~ ) N 0 is isomorphic to su(2), respectively noncompact if and only if ( I ~ + I ~ - ~ + C H ~ ) N O is isomorphic to N(2, R). T h e set of imaginary noncompact roots is denoted by AInc.

We will in the following assume that there is only one H-conjugacy class of Cartan subalgebras of b. This is obviously equivalent to H having only one conju- gacy class of C a f t a n subalgebras (or C a f t a n subgroups). So fix a 0-invariant C a f t a n subalgebra

ia

of 0. T h e n A R = A I n ~ = 0 , see [13, Proposition 11.16]. Let A denote the Cartan subset of X associated to the C a f t a n subspace a for X. T h e n A is given by

A = exp a = ~(p(exp a)),

see [9, Corollaire 1.7], i.e. A is a connected real abelian Lie subgroup of G with Lie algebra a. Let S(a) denote the symmetric algebra of the complexification of a. This algebra can be identified with the algebra of differential operators D(A) on A with constant coefficients, by means of the action generated by

X f(a)

= ~ f ( e x p d

tX.a)It=0

for

XEa,

where

fcC~176

and

aEA.

Regular elements

P u t n = r a n k o and let x C X . The characteristic polynomial of the C-linear endomorphism

A d ( x ) - I

on l ~ = q c = O c can be written as

detc((l+z)I-Ad(x)) =znDx(x)

mod z '~+1

for all z E C . The function D x so defined is an H-invariant analytic function on X.

An element x in X is called regular (cf. [14, w if D x ( x ) # 0 , and the set of regular elements in any subset U C X will be denoted by U'.

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Define for every root a a function ~a on A by

~ ( e x p X ) = e ~(x)

for X c a . We see, using the root space decomposition of t~, t h a t D x ( a ) = n ( 1 - ~ _ ~ ( a ) )

c~cA

for a c A . We furthermore, for all subsets S c A , define the function b ~ - -

n

( 1 - ~ _ ~ )

on the set A r. We note, since all of the functions ~ , a E A ; , are real, t h a t the function bA+ is • on the connected components of A t.

We easily see t h a t ZH(a)=ZH(a) if a c A ' (since a = e x p i X , where X is a reg- ular element of ~) and t h a t ZH(a)-~-ZH(A) (since A is connected), i.e. the quotient

N.(A)/Z.(A)

is nite and equal to The subgroup

is a C a r t a n subgroup of H . The m a p from H / Z H ( A ) • into X defined by (hZH(A), a)~--§ is an everywhere regular ]NH(A)/ZH(A)I-to-one m a p onto X ' , see [14, T h e o r e m 2(ii)], and we thus have the decomposition X'=Uh~H h.A'. Let U C X be a c o m p a c t subset. Since D x is an H-invariant continuous function on X, we conclude from regularity of the m a p (hZH(A),a)~-~h.a, t h a t the subset H[U] = U h ~ h. U is closed in X. We see in particular t h a t the H - o r b i t H[a] t h r o u g h any regular element a c A ~ is closed in X.

O r b i t a l i n t e g r a l s

Definition 1. Let f E C ~ ( X ) . T h e orbital integral K S of f , relative to the C a r t a n subset A, is the function defined on the regular elements a E A t by

Ks(a) = IDx(a)l 1/2

fmz.(A)

f(h.a) di~, where dh is an H - i n v a r i a n t measure on H/ZH(A).

Remarks. Let a 6 A t and let f ~ C c ~ ( X ) , then supp fnH[a] c X is compact, and the above integral converges. We also easily see t h a t K S C C ~ (At).

Consider the space I(A) of functions F ~ C ~ (A t) satisfying the properties:

I I ( A ) : SUPaevn A, }XF(a)l<oo for all c o m p a c t subsets V c A and for all X C s(a).

/2 (A): T h e function bA+ F extends to a C~ on A.

I4(A): There exists a c o m p a c t subset V c A such t h a t F(a)=-O for a c A ' \ V .

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Invariant fundamental solutions and solvability for symmetric spaces 195 We note that the space I(A) is isomorphic to the space I ( X ) , see [10, pp. 9ft.], of H-invariant differentiable functions on X ' satisfying the (similar) properties I~(X), iE{1, 2, 3, 4}, since condition Ia(X) is empty when there is only one conjugacy class of Cartan subspaces.

Let U c X and V c A be compact subsets, and consider the F%chet spaces C ~ ( X ) = { f 9 C ~ ( X ) I supp f C U},

C ~ ( A ) = {F E C ~ ( A ) I supp F C V}, C ~ ( A ' ) = {F 9 I(A) IF(a) = 0 for a E A ' \ V } .

T h e o r e m 2. Let U c X be compact. There exists a compact subset V c A, only depending on U, such that Kf(a)--O for a c A ' \ V for all f c C ~ ( X ) ; and the map f ~ K I is a continuous map from C ~ ( X ) into c ~ ( m ' ) .

Proof. By mimicking [4, w for the space X, see also [4, w we see that H[U]NA is a bounded and closed subset of A, hence compact. The orbital inte- gral Ky is obviously identically zero outside H[U]f~A t, so we can choose the subset V c A as H[U] NA. There exists around every a E A t a completely G-invariant neigh- bourhood V in G, see [4, w for the construction and definition of completely G- invariant neighbourhoods. We conclude from Harish-Chandra's method of descent, [4, Lemme 8.2.1], and properties Ii(m), /2(m) and I4(m) of the orbital integral Ym defined on the Lie algebra m, see [3, w and [4, w that K / s a t i s f i e s the properties II(A), I2(A) and h ( A ) listed above, since they are all of local nature. Let a c A ' , then the map f ~ K / ( a ) is a continuous functional on C ~ ( X ) (a Radon measure on C ~ ( X ) ) , and continuity of the map f ~ K / thus follows from the closed graph theorem. []

C o r o l l a r y 3. Let U C X be compact and let V c A be a compact subset as in Theorem 2. The map f~-~bA+K f is a continuous map from C ~ ( X ) into C ~ ( A ) .

Proof. The map f ~ b A + i K f is a continuous map from C ~ ( X ) into C ~ ( A ' ) since b~x+ - • oil the connected components of A t. T h e map extends to a continuous map from C ~ (X) into C ~ (A) by T h e o r e m 2, since A' is dense in A. []

Let D ( X ) denote the algebra of G-invariant differential operators on X. This algebra is isomorphic to the center Z(b) of the universal enveloping algebra of the complexification of b, see [2, ThSor~me 2.1] for details (valid in the general case as well), and we identify the two algebras. Let F denote the Harish-Chandra isomorphism of D ( X ) = Z ( O ) onto S(~) W, the Weyl group invariant elements of s ( a ) , see e.g. [13, p. 220].

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Let D E D ( X ) , then we have

( K D f ) (a) = F ( D ) K $ (a)

for all aCA', see [16, L e m m a 12.1]. Since b z x + - + l on tile connected components of A', we also get

(ba+ I KD$) (a) = F (D) bA+ I K f (a) for all a E A ~, and hence by density and continuity for all a EA.

Let ~2 [ I ~ z x + H o E S ( a ) and let 5ET?'(X) H denote the Dirac measure at the origin of X.

T h e o r e m 4. Let f ~ C ~ ( X ) . There exists a constant c7~0 such that (5, f l = f ( e ) = cf~bzx + K$(e),

where e denotes the identity element of G (A).

Proof. It follows from [10, Lemme 7.1(ii)], since ia is a fundamental Cartan subalgebra of [?. [~

Y~lndamental s o l u t i o n s a n d s o l v a b i l i t y

Let D c D ( X ) . An invariant fundamental solution for D is a solution T E

~ ) ' ( X ) H to the differential equation D T = 6 . Consider F ( D ) E S ( a ) as a differen- tial operator on A, then a fundamental solution for

P(D)

is a solution TAE:D'(A), the space of distributions on A, to the differential equation F(D)TA=bA, where 5A denotes the Dirac measure on A at the origin.

Both the symmetric space X and the Lie group A carry invariant measures, which in a natural way induce bilinear pairings of C ~ (X) and C ~ (A) with them- selves. We denote these linear pairings by ( . , - } and (-,-}A respectively. Let D E D ( X ) ( D A C D ( A ) ) and let D* (D~) denote the adjoint of D (DA) with respect to the pairing ( - , - } ( ( . , ")A)-

Define the isomorphism 7 , from D ( X ) onto S(a) W as on [2, p. 59]. This isomorphism is identical to the isomorphism ~ from D ( X ) onto S(a) W defined on [1, p. 304] (with a = a a and W~-W1), see [8, pp. 15ff.] for further details. We have the following identities: 2 ~ for D E D ( X ) homogeneous, see [2, p. 59]. It follows from [1, L e m m a 3] that F ( D ) * = F ( D * ) .

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Invariant fundamental solutions and solvability for symmetric spaces 197 T h e o r e m 5. Let D E D ( X ) . Then D has an invariant fundamental solution on X if F ( D ) has a fundamental solution on A.

Proof. Let TAED'(A) be a f l m d a m e n t a l solution for F ( D ) . Define a distribu- tion T E D ' ( X ) H by

(W, f} = {TA, ~bA+ KS}A

for f E C ~ ( X ) . Continuity follows from Corollary 3, and H-invariance from H - invariance of K f . We easily see that:

(DT, f) ( T , D * f } = ( T A , c ~ b ~ T K D . f ) A

= (TA, c ~ r ( D * ) b < KS)A = (TA, r ( D * ) o ~ b < KS)A

= (r(D*)~TA, cf~bA+Kf)A = c~bA+ K f (e) = f(e) = (8, f}, since r(D*)*=r(D). []

We decompose a according to the C a r t a n decomposition as a=ae|174 a•p. Let A K = A N K = e x p a e and A p - - e x p a p be the compact, respectively the euclidean, part of A = A K A p . We similarly decompose the complex dual of a as a~ a~,c • % , c , the p r o d u c t of the complex duals of ae and ap. T h e lattice of char- acters of the c o m p a c t abelian group AK is canonically identified with the lattice A of analytically integral elements AEa~, o. Consider now the elements of S(a) in the natural setup as polynomials on a~. Let X E S ( a ) and let Aca~' c , t h e n we define the polynomial X~ on a;, c as X ~ ( v ) = X ( A , v) for z~Ea;, c . Let {X1, . . . , X m } be a basis for ap, and define a norm on S(ap), the s y m m e t r i c algebra of the complexification of a,, as ]]Xll'2=~(a!)2]a~l u for X = ~ a~X~ ~ ... X ~ "~ written in the multi-index notation. Let ]. I* denote any norm on a~.

P r o p o s i t i o n 6. Let X E S ( a ) . The differential operator X on A has a fun- damental solution on A if and only if there exists a constant C > 0 and an integer N c N U { 0 } such that

(**) IIX~,ll > c ( 1 + IAI.) -N

for all )~cA.

Proof.

See e.g. [5, w or [~5, Proposition 3.2]. []

Remark. The inequality [IX-Y][ >CNHXH [[YH holds for all X, Y E S ( a p ) of de- gree < N , with N E N , where CN>O is a constant only depending on N . It follows, t h a t if X and Y satisfy (**) for some AEA, then so does the product X . Y . Let D~, D 2 E D ( X ) and assume t h a t

F(D~)

a n d

F(D2)

b o t h have fundamental solutions on A, t h e n it follows, t h a t the product D1-D2 has an invariant fundamental solution on X. In particular, if D ~ D ( X ) and F ( D ) has a fundamental solution on A, then a]l powers D m, m E N , have invariant flmdamental solutions on X.

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T h e o r e m 7.

Let

0 r

Then D is solvable, i.e. D C ~ ( X ) = C ~ ( X ) , if

d e g r ( D ) = d e g r ( D ) x

for some Aea~, c.

Proof.

We first notice that if d e g F ( D ) = d e g F ( D ) x for some ,kea[,c, then d e g F ( D ) = d e g F ( D ) x for all

Aea~, c.

Let {Y1, ... ,Y1} be a basis for as, and write r(D) as ~ , Z a ~ , z Y l z l ' Y~Z~X7 ~ ' X : m There exists a coefficient

aa,or

with Ic~l = d e g F(D), and we have the estimate [tr(D)x II-> Ila~,0X~ ~ .--X~ = II =a!la~,0 I>0 for all AChe, c . We conclude from Theorem 5 and Proposition 6 that D has an invariant fundamental solution on X.

The algebra

ap--aNp

is a maximal abelian subalgebra of pNq, the so-called split part of a. Let Ap and A c denote the root systems of ap and a in g c (the complexification of g) respectively, and denote by Wp and W c the corresponding Weyl groups. We note that the pair ( A c , W c ) is isomorphic to the pair (A, W), the roots having multiplicity 2 respectively 1 in the two root systems. Define as on [1, pp. 305 306] homomorphisms 7 and r], of D ( X ) onto

S(a) W~

respectively into

S(ap) W~ .

We note again that F(D)(2A)=-y(D)(A), AChe. The correspondence between ~/(D) and "~(D) can be expressed as

~l(D)(u):'y(O)(u-~,~)=?(D) e,~(u)

for

~,ea~,cCa~,

where ~m is a fixed e]ement of

a~,cCa~,

see [1, L e m m a 1]. We conclude that deg~/(D) deg'y(D), and hence, by [1, Theorem 2], that X is D- convex. It now follows, by [1, p. 301], that D is solvable. []

E x a m p l e s a n d f u r t h e r r e s u l t s

(1) Let A c D ( X ) denote the Casimir operator on X, then it is easily seen that F(A)(~,

u)=/k./k+u.u-s

for ),Ea~,c,

uea~,c,

where 0 is half the sum of the pos- itive roots of A c . Assume that ap•{0}, then we see that d e g F ( A ) = d e g F ( A ) ~ for all AChe, c , and we conclude from the above that A has a fundamental solution and that it is solvable. Solvability of the Casimir operator was proved, for general semisimple symmetric spaces, by Chang in [7]. Let D E D ( X ) be a differential oper- ator of the form A "~ +D1, with m E N, where deg D1 < deg D = 2 m . Again assuming that ap ~ {0}, we see that F(D) satisfies the conditions in T h e o r e m 5 and Theorem 7, i.e. D has a fundamental solution and it is solvable.

(2) Let K be a compact Lie group and let K c denote the complexification of K , then

K c / K

is a Riemannian symmetric space (of type

Gc/Ga)

with only one conjugacy class of Cartan subspaces. Since a ap, we easily see from the above, t h a t every non-zero invariant differential operator D E D ( K c / K ) has a K-invariant fun- damental solution and that it is solvable. Helgason obtained these results for general Riemannian symmetric spaces in [11] and [12], as mentioned in the introduction.

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Invariant fundamental solutions and solvability for symmetric spaces 199

(3) Let H be a complex connected semisimple Lie group. By choosing a suitable complexification H e of H, we can view H ~ - - H c / H as a symmetric space of type G C / G R with only one conjugacy class of C a r t a n subspaces. Then Theorem 5 is a well-known result by C~r~zo and Rouvi~re, see [6, Proposition 1]. In this case however, it follows that D is solvable if F(D) has a fundamental solution on A, see [6, Proposition 2]. These results are also valid on general connected semisimple Lie groups with only one conjugacy class of Cartan subalgebras, see [15, Theorem 4.2].

(4) There are up to coverings two families and one exceptional example of non-complex, non-compact connected semisimple Lie groups with one conjugacy class of Cartan subalgebras, namely S 0 o ( 2 n + 1 , 1), n_>0, (dim a = n + l , dim ap 1);

SU*(2n), n>_3, ( d i m a = 2 n - 1 , d i m a p = n - 1 ) and e6(26) ( d i m a = 6 , d i m a p = 2 ) . Remerciernents. Je remercie Jean-Philippe Anker de m'avoir suggSr5 ce prob- l~me et de l'avoir suivi pendant sa r6solution, Abderrazak Bouaziz et Pascale Ha- rinck de m'avoir expliqu6 leurs travaux et Henrik Schlichtkrull de m'avoir patiem- meat 6cout6 et fait b6nSficier de ses critiques 5clair~es pendant l'6laboration de ce travail.

R e f e r e n c e s

1. VAN DEN BAN, E. P. and SGHLICHTKRULL, H., Convexity for invariant differential operators on semisimple symmetric spaces, Compositio Math. 89 (1993), 301 313.

2. BoPP, N. and HARINCK, P., Formule de Plancherel pour GL(n, C)/U(p, q), J. Reine Angew. Math. 428 (1992), 45 95.

3. BOUAZIZ, A., Int~grales orbitales sur les alg~bres de Lie r6ductives, Invent. Math.

115 (1994), 163 207.

4. BOUAZIZ, A., Int~grales orbitales sur les groupes de Lie r~ductifs, Ann. Sci. l~cole Norm. Sup. 27 (1994), 573 609.

5. C~R~zo, A. and ROUVIERE, F., Solution 61~mentaire d'un opSrateur invariant gauche sur un groupe de Lie compact, Ann. Sci. l~,cole Norm. Sup. 2 (1969), 561-581.

6. C~rt~zo, A. and ROUVI~;RE, F., Op6rateurs diff6rentiels invariants sur un groupe de Lie, Sdm. Goulaouic~chwartz 1972 1973: Equations aux ddrivdes partieUes et analyse fonctionelle, Exp. 10, Centre de Math., t~cole Polytechnique, Paris, 1973.

7. CHANG, W., Global solvability of the Laplacians on pseudo-Riemannian symmetric spaces, J. Funct. Anal. 34 (1979), 481492.

8. FLENSTED-JENSEN, M., Analysis on Non-Riemannian Symmetric Spaces, CBMS Re- gional Conf. Ser. in Math. 61, Amer. Math. Soc., Providence, R. I., 1986.

9. HARINCK, P., Correspondance de distributions sphSriques entre deux espaces sym~tri- ques du type Gc /GR , J. Funct. Anal. 124 (1994), 42~474.

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10. HARINCK, P., Fonctions orbitales sur G c / G a . Formule d'inversion des int~grales orbitales et formule de Plancherel, J. Funet. Anal. 153 (1998), 52 107.

11. HELGASON, S., F u n d a m e n t a l solutions of invariant differential operators on symmetric spaces, Amer. J. Math. 86 (1964), 565 601.

12. HELGASON, S., The surjectivity of invariant differential operators on symmetric spaces, Ann. of Math. 98 (1973), 4,51 480.

13. KNAPP, A., Representation Theory of Semisimple Lie Groups, Princeton Univ. Press, Princeton, N. J., 1986.

14. OSHIMA, T. and MATSUKI, T., Orbits on affine symmetric spaces under the action of the isotropy subgroups, J. Math. Soc. Japan 32 (1980), 399 414.

15. ROUVIi~RE, F., Invariant differential equations on certain semisimple Lie groups, Trans. Amer. Math. Soc. 243 (1978), 97 114.

16. SANO, S., Distributions sphdriques invariantes sur les espaces sym~triques semi- simples G c / G , J. Math. Kyoto Univ. 31 (1991), 377 417.

Received June 2, 1997 Nils Byrial Andersen

D e p a r t m e n t of M a t h e m a t i c s Louisiana State University Baton Rouge, LA 70803 U.S.A.

email: byrial@math.lsu.edu

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