Arthur–Selberg trace formula

• F is a global field, such as the field of rational numbers.
• A is the ring of adeles of F.
• G is a reductive algebraic group defined over F.

In the (rare) case when G(F)∖G(A) is compact the representation splits as a direct sum of irreducible representations, and the trace formula is similar to the Frobenius formula for the character of the representation induced from the trivial representation of a subgroup of finite index.

In the compact case, which is essentially due to Selberg, the groups G(F) and G(A) can be replaced by any discrete subgroup Γof a locally compact group G with Γ\G compact. The group G acts on the space of functions on Γ∖G by the right regular representation R, and this extends to an action of the group ring of G, considered as the ring of functions f on G. The character of this representation is given by a generalization of the Frobenius formula as follows. The action of a function f on a function φ on Γ∖G is given by

${\displaystyle \displaystyle R(f)(\phi )(x)=\int _{G}f(y)\phi (xy)\,dy=\int _{\Gamma \backslash G}\sum _{\gamma \in \Gamma }f(x^{-1}\gamma y)\phi (y)\,dy.}$

In other words, R(f) is an integral operator on L²(Γ∖G) (the space of functions on Γ∖G) with kernel

${\displaystyle \displaystyle K_{f}(x,y)=\sum _{\gamma \in \Gamma }f(x^{-1}\gamma y).}$

Therefore, the trace of R(f) is given by

${\displaystyle \displaystyle \operatorname {Tr} (R(f))=\int _{\Gamma \backslash G}K_{f}(x,x)\,dx.}$

The kernel K can be written as

${\displaystyle K_{f}(x,y)=\sum _{o\in O}K_{o}(x,y)}$

where O is the set of conjugacy classes in Γ, and

${\displaystyle K_{o}(x,y)=\sum _{\gamma \in o}f(x^{-1}\gamma y)=\sum _{\delta \in \Gamma _{\gamma }\backslash \Gamma }f(x^{-1}\delta ^{-1}\gamma \delta y)}$

where γ is an element of the conjugacy class o, and Γ_γ is its centralizer in Γ.

On the other hand, the trace is also given by

${\displaystyle \displaystyle \operatorname {Tr} (R(f))=\sum _{\pi }m(\pi )\operatorname {Tr} (R(f)|\pi )}$

where m(π) is the multiplicity of the irreducible unitary representation π of G in L²(Γ∖G).

One version of the trace formula (Arthur 1983) asserts the equality of two distributions on G(A):

${\displaystyle \sum _{o\in O}J_{o}^{T}=\sum _{\chi \in X}J_{\chi }^{T}.}$

The left hand side is the geometric side of the trace formula, and is a sum over equivalence classes in the group of rational points G(F) of G, while the right hand side is the spectral side of the trace formula and is a sum over certain representations of subgroups of G(A).

The version of the trace formula above is not particularly easy to use in practice, one of the problems being that the terms in it are not invariant under conjugation. Arthur (1981) found a modification in which the terms are invariant.

The invariant trace formula states

${\displaystyle \sum _{M}{\frac {|W_{0}^{M}|}{|W_{0}^{G}|}}\sum _{\gamma \in (M(Q))}a^{M}(\gamma )I_{M}(\gamma ,f)=\sum _{M}{\frac {|W_{0}^{M}|}{|W_{0}^{G}|}}\int _{\Pi (M)}a^{M}(\pi )I_{M}(\pi ,f)\,d\pi }$

where

• f is a test function on G(A)
• M ranges over a finite set of rational Levi subgroups of G
• (M(Q)) is the set of conjugacy classes of M(Q)
• Π(M) is the set of irreducible unitary representations of M(A)
• a^M(γ) is related to the volume of M(Q,γ)\M(A,γ)
• a^M(π) is related to the multiplicity of the irreducible representation π in L²(M(Q)\M(A))
• ${\displaystyle \displaystyle I_{M}(\gamma ,f)}$ is related to ${\displaystyle \displaystyle \int _{M(A,\gamma )\backslash M(A)}f(x^{-1}\gamma x)\,dx}$
• ${\displaystyle \displaystyle I_{M}(\pi ,f)}$ is related to trace ${\displaystyle \displaystyle \int _{M(A)}f(x)\pi (x)\,dx}$
• W₀(M) is the Weyl group of M.

Langlands (1983) suggested the possibility a stable refinement of the trace formula that can be used to compare the trace formula for two different groups. Such a stable trace formula was found and proved by Arthur (2002).

Two elements of a group G(F) are called stably conjugate if they are conjugate over the algebraic closure of the field F. The point is that when one compares elements in two different groups, related for example by inner twisting, one does not usually get a good correspondence between conjugacy classes, but only between stable conjugacy classes. So to compare the geometric terms in the trace formulas for two different groups, one would like the terms to be not just invariant under conjugacy, but also to be well behaved on stable conjugacy classes; these are called stable distributions.

The stable trace formula writes the terms in the trace formula of a group G in terms of stable distributions. However these stable distributions are not distributions on the group G, but are distributions on a family of quasisplit groups called the endoscopic groups of G. Unstable orbital integrals on the group G correspond to stable orbital integrals on its endoscopic groups H.

There are several simple forms of the trace formula, which restrict the compactly supported test functions f in some way (Flicker & Kazhdan 1988). The advantage of this is that the trace formula and its proof become much easier, and the disadvantage is that the resulting formula is less powerful.

For example, if the functions f are cuspidal, which means that

${\displaystyle \int _{n\in N(A)}f(xny)\,dn=0}$

for any unipotent radical N of a proper parabolic subgroup (defined over F) and any x, y in G(A), then the operator R(f) has image in the space of cusp forms so is compact.

Jacquet & Langlands (1970) used the Selberg trace formula to prove the Jacquet–Langlands correspondence between automorphic forms on GL₂ and its twisted forms. The Arthur–Selberg trace formula can be used to study similar correspondences on higher rank groups. It can also be used to prove several other special cases of Langlands functoriality, such as base change, for some groups.

Kottwitz (1988) used the Arthur–Selberg trace formula to prove the Weil conjecture on Tamagawa numbers.

Lafforgue (2002) described how the trace formula is used in his proof of the Langlands conjecture for general linear groups over function fields.

• Maass wave form
• Harmonic Maass form

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• Works of James Arthur at the Clay institute
• Archive of Collected Works of James Arthur at the University of Toronto Department of Mathematics