Harish-Chandra's c-function

From HandWiki
Revision as of 18:47, 6 February 2024 by TextAI (talk | contribs) (update)
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)

In mathematics, Harish-Chandra's c-function is a function related to the intertwining operator between two principal series representations, that appears in the Plancherel measure for semisimple Lie groups. Harish-Chandra (1958a, 1958b) introduced a special case of it defined in terms of the asymptotic behavior of a zonal spherical function of a Lie group, and Harish-Chandra (1970) introduced a more general c-function called Harish-Chandra's (generalized) C-function. Gindikin and Karpelevich (1962, 1969) introduced the Gindikin–Karpelevich formula, a product formula for Harish-Chandra's c-function.

Gindikin–Karpelevich formula

The c-function has a generalization cw(λ) depending on an element w of the Weyl group. The unique element of greatest length s0, is the unique element that carries the Weyl chamber [math]\displaystyle{ \mathfrak{a}_+^* }[/math] onto [math]\displaystyle{ -\mathfrak{a}_+^* }[/math]. By Harish-Chandra's integral formula, cs0 is Harish-Chandra's c-function:

[math]\displaystyle{ c(\lambda)=c_{s_0}(\lambda). }[/math]

The c-functions are in general defined by the equation

[math]\displaystyle{ \displaystyle A(s,\lambda)\xi_0 =c_s(\lambda)\xi_0, }[/math]

where ξ0 is the constant function 1 in L2(K/M). The cocycle property of the intertwining operators implies a similar multiplicative property for the c-functions:

[math]\displaystyle{ c_{s_1s_2}(\lambda) =c_{s_1}(s_2 \lambda)c_{s_2}(\lambda) }[/math]

provided

[math]\displaystyle{ \ell(s_1s_2)=\ell(s_1)+\ell(s_2). }[/math]

This reduces the computation of cs to the case when s = sα, the reflection in a (simple) root α, the so-called "rank-one reduction" of (Gindikin Karpelevich). In fact the integral involves only the closed connected subgroup Gα corresponding to the Lie subalgebra generated by [math]\displaystyle{ \mathfrak{g}_{\pm \alpha} }[/math] where α lies in Σ0+. Then Gα is a real semisimple Lie group with real rank one, i.e. dim Aα = 1, and cs is just the Harish-Chandra c-function of Gα. In this case the c-function can be computed directly and is given by

[math]\displaystyle{ c_{s_\alpha}(\lambda)=c_0{2^{-i(\lambda,\alpha_0)}\Gamma(i(\lambda,\alpha_0))\over\Gamma({1\over 2} ({1\over 2}m_\alpha + 1+ i(\lambda,\alpha_0)) \Gamma({1\over 2} ({1\over 2}m_\alpha + m_{2\alpha} + i(\lambda,\alpha_0))}, }[/math]

where

[math]\displaystyle{ c_0=2^{m_\alpha/2 + m_{2\alpha}}\Gamma\left({1\over 2} (m_\alpha+m_{2\alpha} +1)\right) }[/math]

and α0=α/〈α,α〉.

The general Gindikin–Karpelevich formula for c(λ) is an immediate consequence of this formula and the multiplicative properties of cs(λ), as follows:

[math]\displaystyle{ c(\lambda)=c_0\prod_{\alpha\in\Sigma_0^+}{2^{-i(\lambda,\alpha_0)}\Gamma(i(\lambda,\alpha_0))\over\Gamma({1\over 2} ({1\over 2}m_\alpha + 1+ i(\lambda,\alpha_0)) \Gamma({1\over 2} ({1\over 2}m_\alpha + m_{2\alpha} + i(\lambda,\alpha_0))}, }[/math]

where the constant c0 is chosen so that c(–iρ)=1 (Helgason 2000).

Plancherel measure

The c-function appears in the Plancherel theorem for spherical functions, and the Plancherel measure is 1/c2 times Lebesgue measure.

p-adic Lie groups

There is a similar c-function for p-adic Lie groups. Macdonald (1968, 1971) and (Langlands 1971) found an analogous product formula for the c-function of a p-adic Lie group.

References