Zonal spherical function

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In mathematics, a zonal spherical function or often just spherical function is a function on a locally compact group G with compact subgroup K (often a maximal compact subgroup) that arises as the matrix coefficient of a K-invariant vector in an irreducible representation of G. The key examples are the matrix coefficients of the spherical principal series, the irreducible representations appearing in the decomposition of the unitary representation of G on L²(G/K). In this case the commutant of G is generated by the algebra of biinvariant functions on G with respect to K acting by right convolution. It is commutative if in addition G/K is a symmetric space, for example when G is a connected semisimple Lie group with finite centre and K is a maximal compact subgroup. The matrix coefficients of the spherical principal series describe precisely the spectrum of the corresponding C* algebra generated by the biinvariant functions of compact support, often called a Hecke algebra. The spectrum of the commutative Banach *-algebra of biinvariant L¹ functions is larger; when G is a semisimple Lie group with maximal compact subgroup K, additional characters come from matrix coefficients of the complementary series, obtained by analytic continuation of the spherical principal series.

Zonal spherical functions have been explicitly determined for real semisimple groups by Harish-Chandra. For special linear groups, they were independently discovered by Israel Gelfand and Mark Naimark. For complex groups, the theory simplifies significantly, because G is the complexification of K, and the formulas are related to analytic continuations of the Weyl character formula on K. The abstract functional analytic theory of zonal spherical functions was first developed by Roger Godement. Apart from their group theoretic interpretation, the zonal spherical functions for a semisimple Lie group G also provide a set of simultaneous eigenfunctions for the natural action of the centre of the universal enveloping algebra of G on L²(G/K), as differential operators on the symmetric space G/K. For semisimple p-adic Lie groups, the theory of zonal spherical functions and Hecke algebras was first developed by Satake and Ian G. Macdonald. The analogues of the Plancherel theorem and Fourier inversion formula in this setting generalise the eigenfunction expansions of Mehler, Weyl and Fock for singular ordinary differential equations: they were obtained in full generality in the 1960s in terms of Harish-Chandra's c-function.

The name "zonal spherical function" comes from the case when G is SO(3,R) acting on a 2-sphere and K is the subgroup fixing a point: in this case the zonal spherical functions can be regarded as certain functions on the sphere invariant under rotation about a fixed axis.

Definitions

Properties

A zonal spherical function h has the following properties:^[3]

h is uniformly continuous on G
$h(x)h(y)=\int _{K}h(xky)\,dk\,\,(x,y\in G).$
h(1) =1 (normalisation)
h is a positive definite function on G
f * h is proportional to h for all f in C_c(K\G/K).

These are easy consequences of the fact that the bounded linear functional χ defined by h is a homomorphism. Properties 2, 3 and 4 or properties 3, 4 and 5 characterize zonal spherical functions. A more general class of zonal spherical functions can be obtained by dropping positive definiteness from the conditions, but for these functions there is no longer any connection with unitary representations. For semisimple Lie groups, there is a further characterization as eigenfunctions of invariant differential operators on G/K (see below).

In fact, as a special case of the Gelfand–Naimark–Segal construction, there is one-one correspondence between irreducible representations σ of G having a unit vector v fixed by K and zonal spherical functions h given by

$h(g)=(\sigma (g)v,v).$

Such irreducible representations are often described as having class one. They are precisely the irreducible representations required to decompose the induced representation π on H₁. Each representation σ extends uniquely by continuity to A(K\G/K), so that each zonal spherical function satisfies

$\left|\int _{G}f(g)h(g)\,dg\right|\leq \|\pi (f)\|$

for f in A(K\G/K). Moreover, since the commutant π(G)' is commutative, there is a unique probability measure μ on the space of * homomorphisms X such that

$\int _{G}|f(g)|^{2}\,dg=\int _{X}|\chi (\pi (f))|^{2}\,d\mu (\chi ).$

μ is called the Plancherel measure. Since π(G)' is the centre of the von Neumann algebra generated by G, it also gives the measure associated with the direct integral decomposition of H₁ in terms of the irreducible representations σ_χ.

Gelfand pairs

Cartan–Helgason theorem

Let G be a compact semisimple connected and simply connected Lie group and τ a period two automorphism of a G with fixed point subgroup K = G^τ. In this case K is a connected compact Lie group.^[6] In addition let T be a maximal torus of G invariant under τ, such that T $\cap$ P is a maximal torus in P, and set^[13]

$S=K\cap T=T^{\tau }.$

S is the direct product of a torus and an elementary abelian 2-group.

In 1929 Élie Cartan found a rule to determine the decomposition of L²(G/K) into the direct sum of finite-dimensional irreducible representations of G, which was proved rigorously only in 1970 by Sigurdur Helgason. Because the commutant of G on L²(G/K) is commutative, each irreducible representation appears with multiplicity one. By Frobenius reciprocity for compact groups, the irreducible representations V that occur are precisely those admitting a non-zero vector fixed by K.

From the representation theory of compact semisimple groups, irreducible representations of G are classified by their highest weight. This is specified by a homomorphism of the maximal torus T into T.

The Cartan–Helgason theorem^[14]^[15] states that

the irreducible representations of G admitting a non-zero vector fixed by K are precisely those with highest weights corresponding to homomorphisms trivial on S.

The corresponding irreducible representations are called spherical representations.

The theorem can be proved^[6] using the Iwasawa decomposition:

${\mathfrak {g}}={\mathfrak {k}}\oplus {\mathfrak {a}}\oplus {\mathfrak {n}},$

where ${\mathfrak {g}}$ , ${\mathfrak {k}}$ , ${\mathfrak {a}}$ are the complexifications of the Lie algebras of G, K, A = T $\cap$ P and

${\mathfrak {n}}=\bigoplus {\mathfrak {g}}_{\alpha },$

summed over all eigenspaces for T in ${\mathfrak {g}}$ corresponding to positive roots α not fixed by τ.

Let V be a spherical representation with highest weight vector v₀ and K-fixed vector v_K. Since v₀ is an eigenvector of the solvable Lie algebra ${\mathfrak {a}}\oplus {\mathfrak {p}}$ , the Poincaré–Birkhoff–Witt theorem implies that the K-module generated by v₀ is the whole of V. If Q is the orthogonal projection onto the fixed points of K in V obtained by averaging over G with respect to Haar measure, it follows that

$\displaystyle {v_{K}=cQv_{0}}$

for some non-zero constant c. Because v_K is fixed by S and v₀ is an eigenvector for S, the subgroup S must actually fix v₀, an equivalent form of the triviality condition on S.

Conversely if v₀ is fixed by S, then it can be shown^[16] that the matrix coefficient

$\displaystyle {f(g)=(gv_{0},v_{0})}$

is non-negative on K. Since f(1) > 0, it follows that (Qv₀, v₀) > 0 and hence that Qv₀ is a non-zero vector fixed by K.

Harish-Chandra's formula

If G is a non-compact semisimple Lie group, its maximal compact subgroup K acts by conjugation on the component P in the Cartan decomposition. If A is a maximal Abelian subgroup of G contained in P, then A is isomorphic to its Lie algebra under the exponential map and, as a further generalisation of the polar decomposition of matrices, every element of P is conjugate under K to an element of A, so that^[17]

G =KAK.

There is also an associated Iwasawa decomposition

G =KAN,

where N is a closed nilpotent subgroup, diffeomorphic to its Lie algebra under the exponential map and normalised by A. Thus S=AN is a closed solvable subgroup of G, the semidirect product of N by A, and G = KS.

If α in Hom(A,T) is a character of A, then α extends to a character of S, by defining it to be trivial on N. There is a corresponding unitary induced representation σ of G on L²(G/S) = L²(K),^[18] a so-called (spherical) principal series representation.

This representation can be described explicitly as follows. Unlike G and K, the solvable Lie group S is not unimodular. Let dx denote left invariant Haar measure on S and Δ_S the modular function of S. Then^[6]

$\int _{G}f(g)\,dg=\int _{S}\int _{K}f(x\cdot k)\,dx\,dk=\int _{S}\int _{K}f(k\cdot x)\Delta _{S}(x)\,dx\,dk.$

The principal series representation σ is realised on L²(K) as^[19]

$(\sigma (g)\xi )(k)=\alpha ^{\prime }(g^{{-1}}k)^{{-1}}\,\xi (U(g^{{-1}}k)),$

where

$g=U(g)\cdot X(g)$

is the Iwasawa decomposition of g with U(g) in K and X(g) in S and

$\alpha ^{\prime }(kx)=\Delta _{S}(x)^{{1/2}}\alpha (x)$

for k in K and x in S.

The representation σ is irreducible, so that if v denotes the constant function 1 on K, fixed by K,

$\varphi _{\alpha }(g)=(\sigma (g)v,v)$

defines a zonal spherical function of G.

Computing the inner product above leads to Harish-Chandra's formula for the zonal spherical function

$\varphi _{\alpha }(g)=\int _{K}\alpha ^{\prime }(gk)^{{-1}}\,dk$

as an integral over K.

Harish-Chandra proved that these zonal spherical functions exhaust the characters of the C* algebra generated by the C_c(K \ G / K) acting by right convolution on L²(G / K). He also showed that two different characters α and β give the same zonal spherical function if and only if α = β·s, where s is in the Weyl group of A

$W(A)=N_{K}(A)/C_{K}(A),$

the quotient of the normaliser of A in K by its centraliser, a finite reflection group.

It can also be verified directly^[3] that this formula defines a zonal spherical function, without using representation theory. The proof for general semisimple Lie groups that every zonal spherical formula arises in this way requires the detailed study of G-invariant differential operators on G/K and their simultaneous eigenfunctions (see below).^[5]^[6] In the case of complex semisimple groups, Harish-Chandra and Felix Berezin realised independently that the formula simplified considerably and could be proved more directly.^[6]^[20]^[21]^[22]^[23]

The remaining positive-definite zonal spherical functions are given by Harish-Chandra's formula with α in Hom(A,C*) instead of Hom(A,T). Only certain α are permitted and the corresponding irreducible representations arise as analytic continuations of the spherical principal series. This so-called "complementary series" was first studied by Bargmann (1947) for G = SL(2,R) and by Harish-Chandra (1947) and Gelfand & Naimark (1947) for G = SL(2,C). Subsequently in the 1960s, the construction of a complementary series by analytic continuation of the spherical principal series was systematically developed for general semisimple Lie groups by Ray Kunze, Elias Stein and Bertram Kostant.^[24]^[25]^[26] Since these irreducible representations are not tempered, they are not usually required for harmonic analysis on G (or G / K).

Eigenfunctions

Harish-Chandra proved^[5]^[6] that zonal spherical functions can be characterised as those normalised positive definite K-invariant functions on G/K that are eigenfunctions of D(G/K), the algebra of invariant differential operators on G. This algebra acts on G/K and commutes with the natural action of G by left translation. It can be identified with the subalgebra of the universal enveloping algebra of G fixed under the adjoint action of K. As for the commutant of G on L²(G/K) and the corresponding Hecke algebra, this algebra of operators is commutative; indeed it is a subalgebra of the algebra of mesurable operators affiliated with the commutant π(G)', an Abelian von Neumann algebra. As Harish-Chandra proved, it is isomorphic to the algebra of W(A)-invariant polynomials on the Lie algebra of A, which itself is a polynomial ring by the Chevalley–Shephard–Todd theorem on polynomial invariants of finite reflection groups. The simplest invariant differential operator on G/K is the Laplacian operator; up to a sign this operator is just the image under π of the Casimir operator in the centre of the universal enveloping algebra of G.

Thus a normalised positive definite K-biinvariant function f on G is a zonal spherical function if and only if for each D in D(G/K) there is a constant λ_D such that

$\displaystyle \pi (D)f=\lambda _{D}f,$

i.e. f is a simultaneous eigenfunction of the operators π(D).

If ψ is a zonal spherical function, then, regarded as a function on G/K, it is an eigenfunction of the Laplacian there, an elliptic differential operator with real analytic coefficients. By analytic elliptic regularity, ψ is a real analytic function on G/K, and hence G.

Harish-Chandra used these facts about the structure of the invariant operators to prove that his formula gave all zonal spherical functions for real semisimple Lie groups.^[27]^[28]^[29] Indeed the commutativity of the commutant implies that the simultaneous eigenspaces of the algebra of invariant differential operators all have dimension one; and the polynomial structure of this algebra forces the simultaneous eigenvalues to be precisely those already associated with Harish-Chandra's formula.

Example: SL(2,C)

See also: SL(2,C), Representations of the Lorentz group, and Spectral theory of ordinary differential equations

The group G = SL(2,C) is the complexification of the compact Lie group K = SU(2) and the double cover of the Lorentz group. The infinite-dimensional representations of the Lorentz group were first studied by Dirac in 1945, who considered the discrete series representations, which he termed expansors. A systematic study was taken up shortly afterwards by Harish-Chandra, Gelfand–Naimark and Bargmann. The irreducible representations of class one, corresponding to the zonal spherical functions, can be determined easily using the radial component of the Laplacian operator.^[6]

Indeed any unimodular complex 2×2 matrix g admits a unique polar decomposition g = pv with v unitary and p positive. In turn p = uau*, with u unitary and a a diagonal matrix with positive entries. Thus g = uaw with w = u* v, so that any K-biinvariant function on G corresponds to a function of the diagonal matrix

$a={\begin{pmatrix}e^{{r/2}}&0\\0&e^{{-r/2}}\end{pmatrix}},$

invariant under the Weyl group. Identifying G/K with hyperbolic 3-space, the zonal hyperbolic functions ψ correspond to radial functions that are eigenfunctions of the Laplacian. But in terms of the radial coordinate r, the Laplacian is given by^[30]

$L=-\partial _{r}^{2}-2\coth r\partial _{r}.$

Setting f(r) = sinh (r)·ψ(r), it follows that f is an odd function of r and an eigenfunction of $\partial _{r}^{2}$ .

Hence

$\varphi (r)={\sin(\ell r) \over \ell \sinh r}$

where $\ell$ is real.

There is a similar elementary treatment for the generalized Lorentz groups SO(N,1) in Takahashi (1963) and Faraut & Korányi (1994) (recall that SO⁰(3,1) = SL(2,C) / ±I).

Complex case

If G is a complex semisimple Lie group, it is the complexification of its maximal compact subgroup K. If ${{\mathfrak g}}$ and ${\mathfrak {k}}$ are their Lie algebras, then

${\mathfrak {g}}={\mathfrak {k}}\oplus i{\mathfrak {k}}.$

Let T be a maximal torus in K with Lie algebra ${\mathfrak {t}}$ . Then

$A=\exp i{\mathfrak {t}},\,\,P=\exp i{\mathfrak {k}}.$

Let

$W=N_{K}(T)/T$

be the Weyl group of T in K. Recall characters in Hom(T,T) are called weights and can be identified with elements of the weight lattice Λ in Hom( ${\mathfrak {t}}$ , R) = ${\mathfrak {t}}^{*}$ . There is a natural ordering on weights and very finite-dimensional irreducible representation (π, V) of K has a unique highest weight λ. The weights of the adjoint representation of K on ${\mathfrak {k}}\ominus {\mathfrak {t}}$ are called roots and ρ is used to denote half the sum of the positive roots α, Weyl's character formula asserts that for z = exp X in T

$\displaystyle \chi _{\lambda }(e^{X})\equiv {{\rm {Tr}}}\,\pi (z)=A_{{\lambda +\rho }}(e^{X})/A_{{\rho }}(e^{X}),$

where, for μ in ${\mathfrak {t}}^{*}$ , A_μ denotes the antisymmetrisation

$\displaystyle A_{\mu }(e^{X})=\sum _{{s\in W}}\varepsilon (s)e^{{i\mu (sX)}},$

and ε denotes the sign character of the finite reflection group W.

Weyl's denominator formula expresses the denominator A_ρ as a product:

$\displaystyle A_{\rho }(e^{X})=e^{{i\rho (X)}}\prod _{{\alpha >0}}(1-e^{{-i\alpha (X)}}),$

where the product is over the positive roots.

Weyl's dimension formula asserts that

$\displaystyle \chi _{\lambda }(1)\equiv {{\rm {dim}}}\,V={\prod _{{\alpha >0}}(\lambda +\rho ,\alpha ) \over \prod _{{\alpha >0}}(\rho ,\alpha )}.$

where the inner product on ${\mathfrak {t}}^{*}$ is that associated with the Killing form on ${\mathfrak {k}}$ .

Now

every irreducible representation of K extends holomorphically to the complexification G

every irreducible character χ_λ(k) of K extends holomorphically to the complexification of K and ${\mathfrak {t}}^{*}$ .

for every λ in Hom(A,T) = $i{\mathfrak {t}}^{*}$ , there is a zonal spherical function φ_λ.

The Berezin–Harish–Chandra formula^[6] asserts that for X in $i{\mathfrak {t}}$

$\varphi _{\lambda }(e^{X})={\chi _{\lambda }(e^{X}) \over \chi _{\lambda }(1)}.$

In other words:

the zonal spherical functions on a complex semisimple Lie group are given by analytic continuation of the formula for the normalised characters.

One of the simplest proofs^[31] of this formula involves the radial component on A of the Laplacian on G, a proof formally parallel to Helgason's reworking of Freudenthal's classical proof of the Weyl character formula, using the radial component on T of the Laplacian on K.^[32]

In the latter case the class functions on K can be identified with W-invariant functions on T. The radial component of Δ_K on T is just the expression for the restriction of Δ_K to W-invariant functions on T, where it is given by the formula

$\displaystyle \Delta _{K}=h^{{-1}}\circ \Delta _{T}\circ h+\|\rho \|^{2},$

where

$\displaystyle h(e^{X})=A_{\rho }(e^{X})$

for X in ${\mathfrak {t}}$ . If χ is a character with highest weight λ, it follows that φ = h·χ satisfies

$\Delta _{T}\varphi =(\|\lambda +\rho \|^{2}-\|\rho \|^{2})\varphi .$

Thus for every weight μ with non-zero Fourier coefficient in φ,

$\displaystyle \|\lambda +\rho \|^{2}=\|\mu +\rho \|^{2}.$

The classical argument of Freudenthal shows that μ + ρ must have the form s(λ + ρ) for some s in W, so the character formula follows from the antisymmetry of φ.

Similarly K-biinvariant functions on G can be identified with W(A)-invariant functions on A. The radial component of Δ_G on A is just the expression for the restriction of Δ_G to W(A)-invariant functions on A. It is given by the formula

$\displaystyle \Delta _{G}=H^{{-1}}\circ \Delta _{A}\circ H-\|\rho \|^{2},$

where

$\displaystyle H(e^{X})=A_{\rho }(e^{X})$

for X in $i{\mathfrak {t}}$ .

The Berezin–Harish–Chandra formula for a zonal spherical function φ can be established by introducing the antisymmetric function

$\displaystyle f=H\cdot \varphi ,$

which is an eigenfunction of the Laplacian Δ_A. Since K is generated by copies of subgroups that are homomorphic images of SU(2) corresponding to simple roots, its complexification G is generated by the corresponding homomorphic images of SL(2,C). The formula for zonal spherical functions of SL(2,C) implies that f is a periodic function on $i{\mathfrak {t}}$ with respect to some sublattice. Antisymmetry under the Weyl group and the argument of Freudenthal again imply that ψ must have the stated form up to a multiplicative constant, which can be determined using the Weyl dimension formula.

Example: SL(2,R)

The theory of zonal spherical functions for SL(2,R) originated in the work of Mehler in 1881 on hyperbolic geometry. He discovered the analogue of the Plancherel theorem, which was rediscovered by Fock in 1943. The corresponding eigenfunction expansion is termed the Mehler–Fock transform. It was already put on a firm footing in 1910 by Hermann Weyl's important work on the spectral theory of ordinary differential equations. The radial part of the Laplacian in this case leads to a hypergeometric differential equation, the theory of which was treated in detail by Weyl. Weyl's approach was subsequently generalised by Harish-Chandra to study zonal spherical functions and the corresponding Plancherel theorem for more general semimisimple Lie groups. Following the work of Dirac on the discrete series representations of SL(2,R), the general theory of unitary irreducible representations of SL(2,R) was developed independently by Bargmann, Harish-Chandra and Gelfand–Naimark. The irreducible representations of class one, or equivalently the theory of zonal spherical functions, form an important special case of this theory.

The group G = SL(2,R) is a double cover of the 3-dimensional Lorentz group SO(2,1), the symmetry group of the hyperbolic plane with its Poincaré metric. It acts by Moebius transformations. The upper half-plane can be identified with the unit disc by the Cayley transform. Under this identification G becomes identified with the group SU(1,1), also acting by Moebius transformations. Because the action is transitive, both spaces can be identified with G/K, where K = SO(2). The metric is invariant under G and the associated Laplacian is G-invariant, coinciding with the image of the Casimir operator. In the upper half-plane model the Laplacian is given by the formula^[6]^[7]

$\displaystyle \Delta =-4y^{{2}}(\partial _{x}^{2}+\partial _{y}^{2}).$

If s is a complex number and z = x + i y with y > 0, the function

$\displaystyle f_{s}(z)=y^{{s}}=\exp({s}\cdot \log y),$

is an eigenfunction of Δ:

$\displaystyle \Delta f_{s}=4s(1-s)f_{s}.$

Since Δ commutes with G, any left translate of f_s is also an eigenfunction with the same eigenvalue. In particular, averaging over K, the function

$\varphi _{s}(z)=\int _{K}f_{s}(k\cdot z)\,dk$

is a K-invariant eigenfunction of Δ on G/K. When

$\displaystyle s={1 \over 2}+i\tau ,$

with τ real, these functions give all the zonal spherical functions on G. As with Harish-Chandra's more general formula for semisimple Lie groups, φ_s is a zonal spherical function because it is the matrix coefficient corresponding to a vector fixed by K in the principal series. Various arguments are available to prove that there are no others. One of the simplest classical Lie algebraic arguments^[6]^[7]^[33]^[34]^[35] is to note that, since Δ is an elliptic operator with analytic coefficients, by analytic elliptic regularity any eigenfunction is necessarily real analytic. Hence, if the zonal spherical function corresponds is the matrix coefficient for a vector v and representation σ, the vector v is an analytic vector for G and

$\displaystyle (\sigma (e^{{X}})v,v)=\sum _{{n=0}}^{\infty }(\sigma (X)^{n}v,v)/n!$

for X in $i{\mathfrak {t}}$ . The infinitesimal form of the irreducible unitary representations with a vector fixed by K were worked out classically by Bargmann.^[33]^[34] They correspond precisely to the principal series of SL(2,R). It follows that the zonal spherical function corresponds to a principal series representation.

Another classical argument^[36] proceeds by showing that on radial functions the Laplacian has the form

$\displaystyle \Delta =-\partial _{r}^{2}-\coth(r)\cdot \partial _{r},$

so that, as a function of r, the zonal spherical function φ(r) must satisfy the ordinary differential equation

$\displaystyle \varphi ^{{\prime \prime }}+\coth r\,\varphi ^{\prime }=\alpha \,\varphi$

for some constant α. The change of variables t = sinh r transforms this equation into the hypergeometric differential equation. The general solution in terms of Legendre functions of complex index is given by^[3]^[37]

$\varphi (r)=P_{\rho }(\cosh r)={1 \over 2\pi }\int _{0}^{{2\pi }}(\cosh r+\sinh r\,\cos \theta )^{\rho }\,d\theta ,$

where α = ρ(ρ+1). Further restrictions on ρ are imposed by boundedness and positive-definiteness of the zonal spherical function on G.

There is yet another approach, due to Mogens Flensted-Jensen, which derives the properties of the zonal spherical functions on SL(2,R), including the Plancherel formula, from the corresponding results for SL(2,C), which are simple consequences of the Plancherel formula and Fourier inversion formula for R. This "method of descent" works more generally, allowing results for a real semisimple Lie group to be derived by descent from the corresponding results for its complexification.^[38]^[39]

Further directions

The theory of zonal functions that are not necessarily positive-definite. These are given by the same formulas as above, but without restrictions on the complex parameter s or ρ. They correspond to non-unitary representations.^[6]
Harish-Chandra's eigenfunction expansion and inversion formula for spherical functions.^[40] This is an important special case of his Plancherel theorem for real semisimple Lie groups.
The structure of the Hecke algebra. Harish-Chandra and Godement proved that, as convolution algebras, there are natural isomorphisms between C_c^∞(K \ G / K ) and C_c^∞(A)^W, the subalgebra invariant under the Weyl group.^[4] This is straightforward to establish for SL(2,R).^[7]
Spherical functions for Euclidean motion groups and compact Lie groups.^[6]
Spherical functions for p-adic Lie groups. These were studied in depth by Satake and Macdonald.^[41]^[42] Their study, and that of the associated Hecke algebras, was one of the first steps in the extensive representation theory of semisimple p-adic Lie groups, a key element in the Langlands program.

Notes

↑ Dixmier 1996, Algèbres hilbertiennes.
↑ If σ is a unitary representation of G, then $\sigma (f)=\int _{G}f(g)\sigma (g)\,dg$ .
↑ 3.0 3.1 3.2 3.3 3.4 Dieudonné 1978
↑ 4.0 4.1 Godement 1952
↑ 5.0 5.1 5.2 Helgason 2001
↑ 6.0 6.1 6.2 6.3 6.4 6.5 6.6 6.7 6.8 6.9 6.10 6.11 6.12 6.13 Helgason 1984
↑ 7.0 7.1 7.2 7.3 Lang 1985
↑ Cartier 1954-1955
↑ Hochschild 1965
↑ Dieudonné 1978, pp. 55–57
↑ Dieudonné 1977
↑ Helgason 1978, p. 249
↑ Helgason 1978, pp. 257–264
↑ Helgason 1984, pp. 534–538
↑ Goodman & Wallach 1998, pp. 549–550
↑ Goodman & Wallach 1998, p. 550
↑ Helgason 1978, Chapter IX.
↑ Harish-Chandra 1954a, p. 251
↑ Wallach 1973
↑ Berezin 1956a
↑ Berezin 1956b
↑ Harish-Chandra 1954b
↑ Harish-Chandra 1954c
↑ Kunze & Stein 1961
↑ Stein 1970
↑ Kostant 1969
↑ Harish-Chandra 1958
↑ Helgason 2001, pages 418–422, 427-434
↑ Helgason 1984, p. 418
↑ Davies 1990
↑ Helgason 1984, pp. 432–433
↑ Helgason 1984, pp. 501–502
↑ 33.0 33.1 Bargmann 1947
↑ 34.0 34.1 Howe & Tan 1992
↑ Wallach 1988
↑ Helgason 2001, p. 405
↑ Bateman & Erdelyi 1953, p. 156
↑ Flensted-Jensen 1978
↑ Helgason 1984, pp. 489–491
↑ Helgason 1984, pp. 434–458
↑ Satake 1963
↑ Macdonald 1971

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External links

Casselman, William, Notes on spherical functions

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