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Bernstein components via the Bernstein center

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A Correction to this article was published on 13 March 2019

Abstract

Let G be a reductive p-adic group. Let \(\Phi \) be an invariant distribution on G lying in the Bernstein center \({\mathcal {Z}}(G)\). We prove that \(\Phi \) is supported on compact elements in G if and only if it defines a constant function on every component of the set \({\text {Irr}}(G)\); in particular, we show that the space of all elements of \({\mathcal {Z}}(G)\) supported on compact elements is a subalgebra of \({\mathcal {Z}}(G)\). Our proof is a slight modification of the argument from Section 2 of Dat (J Reine Angew Math 554:69–103, 2003), where our result is proved in one direction.

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References

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Authors and Affiliations

Authors

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Correspondence to Alexander Braverman.

Additional information

Dedicated to J. Bernstein on the occasion of his 70th birthday

R.B. was partially supported by the National Science Foundation Grant DMS-1102434. D.K. was partially supported by the European Research Council. A.B, D.K., R.B all supported by the US-Israel Binational Science Foundation. Appendix section contributed by R. Bezrukavnikov.

Appendix: Proof of Theorem 1.8 (by R. Bezrukavnikov)

R. Bezrukavnikov, Department of Mathematics, MIT, Cambridge, MA 02139, USA. Email: bezrukav@math.mit.edu

Appendix: Proof of Theorem 1.8 (by R. Bezrukavnikov)

1.1 Decomposition of \(\overline{{\mathcal {H}}}(G)\)

We have an obvious perfect pairing between \({\mathcal {D}}^{\mathrm{inv}}(G)\) and \(\overline{{\mathcal {H}}}(G)\). We claim that there is a decomposition

$$\begin{aligned} \overline{{\mathcal {H}}}(G)=\bigoplus \limits _{(P,\lambda )\in {\mathcal {P}}(G)} \overline{{\mathcal {H}}}(G)_{P,\lambda }, \end{aligned}$$
(4.1)

which is compatible with (1.2) by means of the above pairing. Namely, we let \(\overline{{\mathcal {H}}}(G)_{P,\lambda }\) be the image of \({\mathcal {H}}(G)_{P,\lambda }\) where the latter consists of functions supported on \(G_{P,\lambda }\). The fact that (4.1) holds is clear.

1.2 Spectral description of \(\overline{{\mathcal {H}}}(G)\)

The space \(\overline{{\mathcal {H}}}(G)\) admits the following well-known description. Let \(\pi \in {\mathcal {M}}(G)\) be a finitely generated representation and let E be an endomorphism of \(\pi \). It is well-known (cf. e.g., [8]) that we can associate to the pair \((\pi ,E)\) and element \([\pi ,E]\) of \({\mathcal {H}}(G)\). Moreover, \({\mathcal {H}}(G)\) is isomorphic to the \(\mathbb {C}\)-span of symbols \([\pi ,E]\) subject to the relations:

  1. (a)

    Let \(\pi _1,\pi _2\in {\mathcal {M}}(G)\) and let \(u\in {\text {Hom}}(\pi _1,\pi _2), v\in {\text {Hom}}(\pi _2,\pi _1)\). Then \([\pi _1,vu]=[\pi _2,uv]\).

  2. (b)

    \([\pi _1,E_1]+[\pi _3,E_3]=[\pi _2,E_2]\) for a short exact sequence \(0\rightarrow \pi _1\rightarrow \pi _2\rightarrow \pi _3\rightarrow 0\) which is compatible with the endomorphisms \(E_i\in {\text {End\,}}(\pi _i)\).

  3. (c)

    \([\pi , c_1E_1+c_2E_2]=c_1[\pi ,E_1]+c_2[\pi ,E_2]\), where \(c_i\in \mathbb {C}\) and \(E_i\in {\text {End\,}}(\pi )\).

The action of \({\mathcal {Z}}(G)\) on \(\overline{{\mathcal {H}}}(G)\) can also be described in these terms. Namely, let \(\Phi \in {\mathcal {Z}}(G)\). Then \(\Phi \cdot [\pi ,E]=[\pi ,E\circ \pi (\Phi )]\).

In addition, let \(\rho \) be an admissible representation of G. Then we have

$$\begin{aligned} \langle [\pi ,E],{\text {ch}}_\rho \rangle =\sum \limits _i (-1)^i {\text {Tr}}(E,{\text {Ext}}^i(\pi ,\rho )). \end{aligned}$$
(4.2)

In view of the Trace Paley–Wiener theorem (cf. [2]), (4.2) defines \([\pi ,E]\) uniquely.

1.3 Spectral description of \(\overline{{\mathcal {H}}}_{P,\lambda }\)

Now let us fix \((P,\lambda )\in {\mathcal {P}}(G)\). Also let \(\sigma \) be a finitely generated representation of M. Set

$$\begin{aligned} \pi =i_{GP}(\sigma ). \end{aligned}$$
(4.3)

Let us now choose a uniformizer t of our local field. Then any \(\lambda \in Z(M)/Z(M^0)\) lifts naturally to an element \(t^{\lambda }\in Z(M)\). Hence it defines an endomorphism of \(\sigma \) and thus also of \(\pi \). We shall denote this endomorphism by \(E_{\lambda }\).

Theorem 4.4

The subspace \(\overline{{\mathcal {H}}}_{P,\lambda }\) is spanned by elements \([\pi ,E_{\lambda }]\) as above.

Remark

The element \([\pi ,E_{\lambda }]\) actually depends on the choice of t; however, it is easy to see that the span of all the \([\pi ,E_{\lambda }]\) does not.

Proof

For \((P,\lambda )=(G,0)\) this is the “abstract Selberg principle” (cf. [5]). The case \(P=G\) and arbitrary \(\lambda \) is completely analogous.

Let us now take arbitrary P and \(\lambda \). Let \(\sigma \) be a finitely generated representation of the Levi group M as above and \(\lambda \) – a strictly dominant cocharacter of \(\pi \). Then we have a natural identification \(t^{\lambda }M^0_c/ \hbox {Ad}(M)=G_{P,\lambda }/\hbox {Ad} (G)\). Hence we get a natural isomorphism between \(\overline{{\mathcal {H}}}(M)_{M,0}\) and \(\overline{{\mathcal {H}}}(G)_{P,\lambda }\). Indeed, if an element of \(\overline{{\mathcal {H}}}(M)\) is represented by some \(h\in {\mathcal {H}}(M)\) supported on \(M^0_c=M_{M,0}\), then let us denote by \(h_{\lambda }\) the corresponding element of \({\mathcal {H}}(M)\) supported on \(M_{M,\lambda }=t^{\lambda } \cdot M_c^0\). For an open compact subgroup K of G, let us denote by \(h_{\lambda ,K}\) the result of averaging \(h_{\lambda }\) with respect to the adjoint action of K. Its image in \(\overline{{\mathcal {H}}}(G)\) is independent of K and the assignment \(h\text { mod} [{\mathcal {H}}(M),{\mathcal {H}}(M)]\mapsto h_{\lambda ,K}\text { mod} [{\mathcal {H}}(G),{\mathcal {H}}(G)]\) is the desired isomorphism. Let us denote it by \(\eta _{P,\lambda }\).

Now in order to finish the proof, it is enough to show that for \(\pi \) as in (4.3) we have

$$\begin{aligned}{}[\pi ,E_{\lambda }]=\eta _{P,\lambda }([\sigma ,{\text {Id}}]). \end{aligned}$$
(4.4)

Let \(h=[\sigma ,{\text {Id}}]\). Then it is easy to see that

$$\begin{aligned}{}[\sigma ,t^{\lambda }]=h_{\lambda }. \end{aligned}$$
(4.5)

Now to prove (4.4) it is enough (by the Trace Paley–Wiener theorem) to check that both the LHS and the RHS of (4.4) have the same inner product with \({\text {ch}}_{\rho }\) where \(\rho \) stands for an irreducible representation of G. But we have

$$\begin{aligned} {\text {Ext}}^i_G(i_{GP}(\sigma ),\rho )={\text {Ext}}^i_M(\sigma , r_{G{\overline{P}}}(\rho )). \end{aligned}$$

Hence \(\langle [\pi ,E_{\lambda }],{\text {ch}}_{\rho }\rangle =\langle [\sigma ,\lambda ],r_{G{{\overline{P}}}}(\rho )\rangle \) and (4.4) follows from (4.5) and from the Casselman formula for the character of \(r_{G{\overline{P}}}(\rho )\) (cf. [5]) which says for any \(g\in G\) such that \(P_g={{\overline{P}}}\), we have \({\text {ch}}_{\rho }(g)={\text {ch}}_{r_{G{{\overline{P}}}}(\rho )}(g)\). \(\square \)

Corollary 4.5

Theorem 1.8 holds.

Proof

It is enough to show that the action of any \(\Phi \in {\mathcal {Z}}_{lc}(G)\) preserves every \(\overline{{\mathcal {H}}}_{P,\lambda }\). Let us consider an element \([\pi ,E]\) as above; without loss of generality we may assume that all irreducible subquotients of \(\sigma \) lie in one component of \({\mathcal {C}}(M)\). But then all irreducible subquotients of \(\pi \) as also lie in one component \(\Omega \in {\mathcal {C}}(G)\) and it follows that \(\Phi \star [\pi ,E_{\lambda }]=[\pi ,f(\Phi )|_{\Omega }\cdot E_{\lambda }]=f(\Phi )|_{\Omega }\cdot [\pi ,E_{\lambda }]\) (note that \(f(\Phi )|_{\Omega }\in \mathbb {C}\) as \(\Phi \in {\mathcal {Z}}_{lc}(G)\)). Hence the span of all the \([\pi ,E_{\lambda }]\) is preserved by the convolution with \(\Phi \).

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Braverman, A., Kazhdan, D. Bernstein components via the Bernstein center. Sel. Math. New Ser. 22, 2313–2323 (2016). https://doi.org/10.1007/s00029-016-0277-3

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