Bourbaki

Lemma 5

Tag 03EY, permanent. Cite it as [Bourbaki, Tag 03EY].

Théories spectrales, chapter V, § 4. Représentations des groupes compacts

Let π\pi be a unitary representation of G in a Hilbert space E of finite dimension. Let (ϱi)i∈I(\varrho_i)_{i\in I} be a family of non-zero unitary representations of G and (ni)i∈I(n_i)_{i\in I} a family of integers ⩾1\geqslant 1 such that the representation π‾⊗π\overline{\pi}\otimes \pi of G (resp. the representation π⊗π\pi \otimes \pi ) is isomorphic to the direct sum ⨁i∈Iϱini\bigoplus_{i\in I}\varrho^{n_i}_i. Then one has

M4(π)⩾∑i∈Ini2 M_4(\pi )\geqslant \sum_{i\in I}n^2_i

with equality if and only if the representations ϱi\varrho_i are irreducible and pairwise non-isomorphic.

Let us denote by χi\chi_i the character of ϱi\varrho_i for i∈Ii\in I. One has

∣χπ∣2=χπ‾⊗π=∑i∈Iniχi|\chi_{\pi}|^2=\chi_{\overline{\pi}\otimes\pi}=\sum_{i\in I}n_i\chi_i, (resp. χπ2=χπ⊗π=∑i∈Iniχi\chi^2_{\pi}=\chi_{\pi\otimes\pi}=\sum_{i\in I}n_i\chi_i).

From the definition and Cor. 3 of V, p. 466, there follows

M4(π)=∫G∣χπ∣4dμ M_4(\pi ) =\int_G|\chi_{\pi}|^4d\mu

whence, in both cases, the formula

M4(π)=∑i,jninj∫Gχiχ‾jdμ=∑i,jninjM_4(\pi ) =\sum_{i,j}n_in_j\int_G\chi_i\overline{\chi}_jd\mu=\sum_{i,j}n_in_j dim HomG(ϱi,ϱj)_G(\varrho_i, \varrho_j)

(Cor. 4, b) of V, p. 459). Let i∈Ii\in I. Since the representation ϱi\varrho_i is not zero, the space HomG(ϱi,ϱi)_G(\varrho_i, \varrho_i) is non-zero, and one deduces the lower bound

M4(π)⩾∑i∈Ini2 M_4(\pi )\geqslant \sum_{i\in I}n^2_i

Moreover, since ni⩾n_i\geqslant 1, there is equality if and only if one has dim HomG(ϱi,ϱj)=0_G(\varrho_i, \varrho_j) = 0 if i≠ji\not =j and dim HomG(ϱi,ϱi)=1_G(\varrho_i, \varrho_i) = 1 for all ii. The second condition holds if and only if the representations ϱi\varrho_i are irreducible (loc. cit.). The first is then satisfied if and only if the representations ϱi\varrho_i are pairwise non-isomorphic, by Schur’s Lemma (V, p. 387, Cor. 2).

If E is a module over a commutative ring A, the a-module S2(E)\mathsf{S}^2(E) (resp. ∧2E\wedge^2E) will be called the symmetric square (resp. exterior square) of E.

Bourbaki sets the proof directly after the statement, and the corpus does not separate them, so what is above is the statement and its proof together.

Cited by

Nothing.

Cites

Nothing.

Machine translation of the English, by gpt-5.4, against glossary version 34. Not checked by a person.