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Parameter identifications in the SL2(R) unitary dual

Statement

Assume the Axiom of Choice (The Axiom of Choice) and use the normalized parameter Iε,ν and exceptional lattice Wε of The normalized principal series I(epsilon, nu). The following records the parameter identifications and reducible endpoints in this normalization.

For ν∉Wε, the irreducible principal-series representations satisfy Iε,ν≅Iε,−ν. For nonzero ν∈Wε, the two reducible full induced modules are not isomorphic. At ε=1,ν=0, one has I1,0=D1−⊕D1+.

The K-types of Iε,ν are exactly the characters of parity m≡ε(mod2), each with multiplicity one. If n∈Wε and n≥1, then at ν=n the composition factors are Ln−1 and the two extremal modules Mn+1−,M−(n+1)+, with Ln−1 the quotient; at ν=−n the finite-dimensional factor is the submodule and the two tails form the quotient. For n≥2, the algebraic K-finite modules of the discrete series Dn− and Dn+ are isomorphic to M−n+ and Mn−, respectively, at ν=n−1; the Hilbert representations are the weighted completions in Holomorphic and antiholomorphic discrete-series models. At ε=0,ν=±1, the trivial module L0 is a subquotient.

The unitary principal-series parameters are I0,is for s≥0 and I1,is for s>0; the even point I0,0 is irreducible, while I1,0 is the limit split above. The spherical complementary family has parameters I0,r for 0<r<1, with the sign labels r and −r identified; ν=±1 are degenerate endpoints, not additional irreducible complementary-series points. Within each principal or complementary family, no two different absolute parameter values give isomorphic representations.

Facts & Assumptions

Given: AC; the normalized principal-series conventions; the compact-picture K-type decomposition; the generic irreducibility and exceptional-parameter results; and the discrete and limit-series models.

[F1]

W0 is the odd integer lattice and W1 is the even integer lattice; the normalized parameter is used throughout (Iwasawa and minimal-parabolic data for SL2(R), The normalized principal series I(epsilon, nu)).

[F2]

In Iε,ν the one-dimensional K-types are precisely Cfm, m≡ε(mod2), and each occurs once (K-type decomposition of the SL2(R) principal series).

[F3]

Off Wε, Iε,νK is irreducible and Iε,ν≅Iε,−ν. At nonzero exceptional parameters, the finite-dimensional constituent is a quotient at +n and a submodule at −n (Parameter-sign equivalence and its exceptional failures for SL2(R), Generic irreducibility and the exceptional parameter lattice).

[F4]

At ν=n∈Wε, n≥1, the factors are Ln−1 and Mn+1−,M−(n+1)+; at −n the finite-dimensional submodule and two-tail quotient are reversed. The central element acts by (ν2−1)/8 (Generic irreducibility and the exceptional parameter lattice, Highest- and lowest-weight submodules at the exceptional parameters).

[F5]

I1,0 splits into D1− and D1+, and for n≥2, their algebraic K-finite spans Vn− and Vn+ identify with M−n+ and Mn−, respectively at ν=n−1 (The two limits of discrete series, Unitarity and irreducibility of the limits of discrete series, Holomorphic and antiholomorphic discrete-series models).

[F6]

The compact-picture action is strongly continuous and unitary for ν∈iR (The compact picture of the SL2(R) principal series).

[A1]

AC is assumed and inherited from the normalized Iwasawa and compact-picture constructions (The Axiom of Choice).

[F7]

For 0<∣ν∣<1, the spherical invariant form has positive even Fourier weights an(ν), its weighted Hilbert completion is irreducible and strongly continuous unitary, and no real nonzero odd parameter admits a positive-definite full-module invariant form (Unitarity of the complementary series). The weights satisfy an(−ν)=an(ν)−1.

Proof

technique · compile the exact parameter equivalences, K-type data, exceptional subquotients, and unitary ranges; distinguish the parameter values by K-types and the central character

Given: The conventions and claims recorded in the Statement.

1.1F1F3A1

By [F1], W0=2Z+1 and W1=2Z. The generic parameter set is their complement, so the sign-equivalence claim in the Statement is restricted to irreducible induced modules; nonzero lattice points are reducible.

1.2F3F5F6F7

The compact-picture theorem [F6] supplies the principal unitary axis; [F3] supplies irreducibility at its even zero and [F5] supplies the odd zero split. The positive weighted Hilbert completion and odd-parity invariant-form obstruction in [F7] give precisely the spherical complementary interval and absence of an odd complementary family.

2.1F3F5F7step 1.1algebra

For ν∉Wε, [F3] gives Iε,ν≅Iε,−ν. For nonzero ν∈Wε, [F3] gives the opposite positions of L∣ν∣−1 in the two modules, so they are not isomorphic. For spherical real 0<∣ν∣<1, the normalized smooth intertwiner Rν of [F3] has multipliers an(ν). By [F7], B−ν(Rνf,Rνf)=∑nan(−ν)∣an(ν)f^(n)∣2=Bν(f,f) on finite Fourier sums. Its inverse is R−ν, so density extends it to an onto unitary intertwiner of the completed complementary representations. At ε=1,ν=0, [F5] gives the direct sum of the two limits.

3.1F2F4F5step 2.1

The K-type parity and multiplicity statement is [F2]. At a positive exceptional integer n, [F4] gives the finite quotient and two extremal submodules; at −n it gives the reversed submodule/quotient orientation. When n=1 and ε=0, L0 is the trivial representation, so the two endpoints ν=±1 have the stated trivial subquotient. For n≥2, [F5] identifies the extremal modules at ν=n−1 with the algebraic K-finite spans of Dn− and Dn+, whose weighted Hilbert completions give the group representations. Thus an exceptional full induced module is not a second irreducible class to be counted alongside its irreducible constituents.

4.1F2F3F4step 3.1∎

For two generic parameters of the same parity, [F4] gives the central scalar c(ν)=(ν2−1)/8; equivalent representations must have equal central scalars, hence their parameters differ only by sign. Different parities have disjoint K-type supports by [F2]. On the principal unitary axis ν=is, the scalar is −(s2+1)/8, so it determines ∣s∣; on the spherical complementary interval 0<r<1, it is (r2−1)/8, so it determines r. These ranges are disjoint, and the sign equivalence [F3] therefore leaves no further identification between distinct absolute parameter values in either family.

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