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Matrix-coefficient formulas and decay for the discrete and principal series

Statement

Assume the Axiom of Choice (The Axiom of Choice).

(a) Discrete series. Let n≥2, let un=fn,0/∥fn,0∥n∈Dn− be the normalized extremal vector of Holomorphic and antiholomorphic discrete-series models, and let cn(g)=⟨πn(g)un,un⟩ be its matrix coefficient (Matrix coefficient of a unitary representation). Then for all τ∈R, cn(aτ)=cosh⁡(τ/2)−n. Moreover, for every X,Y∈U(gC) there is C=C(n,X,Y)>0 such that ∣⟨πn(g)Xun,Yun⟩∣≤C e−n∣τ∣/2(g=k1aτk2).

(b) Limits and unitary principal series. In the compact picture of I1,0 (The compact picture of the SL2(R) principal series, Unitarity of the unitary principal series, The two limits of discrete series), let Π0 be the unitary action on L12(K) and f1(kθ)=eiθ the normalized weight-one vector. Then ⟨Π0(aτ)f1,f1⟩=sech⁡(τ/2)=2eτ/2+e−τ/2. Consequently ∫0∞∣⟨Π0(aτ)f1,f1⟩∣2sinh⁡τ dτ=+∞, and this matrix coefficient is not in L2(G) by the KAK formula (KAK integration formula for K-bi-invariant functions on SL2(R)).

More generally, for every odd integer m and every real spectral parameter s, let cm,s(τ)=⟨Πis(aτ)fm,fm⟩ in the unitary compact picture of I1,is. Then for an absolute constant C>0, ∣cm,s(τ)∣≤C(1+∣τ∣)e−∣τ∣/2(τ∈R).

Facts & Assumptions

Given: AC; the holomorphic and antiholomorphic models and their K-finite vectors; the weighted disk norm; the odd compact-picture basis; and the unitary principal-series action.

[F1]

The model action is unitary for the weighted inner product, and the vectors fn,j are nonzero, mutually orthogonal K-eigenvectors with characters e−i(n+2j)θ (Holomorphic and antiholomorphic discrete-series models, The weighted area form is SL2(R)-invariant, The weighted discrete-series space is a Hilbert space with K-type basis).

[F2]

The model vectors are smooth K-eigenvectors with the displayed raising/lowering actions; every element of U(gC) sends un to a finite sum of these K-types (Smooth and K-finite vectors for SL2(R), and the (g,K)-module, Holomorphic and antiholomorphic discrete-series models).

[F3]

The discrete-series model is unitary and strongly continuous, and its matrix coefficient is defined by the first-variable-linear Hilbert pairing (The weighted area form is SL2(R)-invariant, Matrix coefficient of a unitary representation).

[F4]

In the compact picture, for kg=atnxkψ, the action is (Πν(g)f)(k)=e(1+ν)t/2f(kψ); the odd Fourier vectors fm(kθ)=eimθ form an orthonormal basis (The compact picture of the SL2(R) principal series, K-type decomposition of the SL2(R) principal series).

[F5]

For ν∈iR, the compact-picture action is a strongly continuous unitary representation; its matrix coefficients use the same L2 pairing (Unitarity of the unitary principal series, Matrix coefficient of a unitary representation).

[F6]

For continuous nonnegative K-bi-invariant functions, ∫Gψ(g)dg=2π∫0∞ψ(aτ)sinh⁡τ dτ (KAK integration formula for K-bi-invariant functions on SL2(R)).

[F7]

The positive-weight limit vector f1 is a unit vector in the D1+ summand of I1,0 (The two limits of discrete series).

[A1]

AC is inherited through the weighted and compact-picture constructions (The Axiom of Choice).

Proof

technique · direct

Given: The notation and assumptions of the Statement.

1.1F1F2algebraA1

Let w=(z−i)/(z+i), Ff(w)=(z+i)nf(z), and r=tanh⁡(τ/2). Solving gives z=i(1+w)/(1−w), so direct substitution gives Ffn,j(w)=(z−i)j(z+i)−j=wj. Substituting this inverse coordinate in the inverse-action formula for aτ=diag⁡(eτ/2,e−τ/2) gives Fπn(aτ)f(w)=cosh⁡(τ/2)−n(1−rw)−nFf ⁣(w−r1−rw). For Ffn,j(w)=wj, this is cosh⁡(τ/2)−n(w−r)j(1−rw)−n−j. Its Taylor coefficient at wk equals cosh⁡(τ/2)−nQjk(r), where Qjk(r)=∑p=0min⁡(j,k)(−1)j−p(jp)(n+j+k−p−1k−p)rj+k−2p.

1.2F4F5algebraA1

Write t=eτ and D(θ,τ)=cos⁡2θ+e2τsin⁡2θ. Multiplying kθaτ and comparing its bottom row with the ANK form gives eσ/2=eτ/2/D and eiψ=(cos⁡θ+ieτsin⁡θ)/D. Hence in I1,is, cm,s(τ)=12π∫02π(eτ/2D)1+iseim(ψ−θ)dθ. The character factors and the is-power have modulus one, so ∣cm,s(τ)∣≤eτ/22π∫02πD−1/2dθ. For τ≥1, D=1+(e2τ−1)sin⁡2θ≥1+ce2τθ2 on 0≤θ≤π/2 for a fixed c>0, using sin⁡θ≥2θ/π. Substitution u=eτθ gives ∫0π/2D−1/2dθ≤C(1+τ)e−τ, since ∫0R(1+cu2)−1/2du≤C(1+log⁡(1+R)). The other three quadrants have the same bound; for 0≤τ≤1 it follows after increasing C. Thus ∣cm,s(τ)∣≤C(1+τ)e−τ/2 for τ≥0, uniformly in odd m and real s. For negative τ, unitarity gives ∣cm,s(−τ)∣=∣cm,s(τ)∣, proving the stated bound.

2.1F1step 1.1algebra

By [F1] the vectors fn,j,fn,k with j≠k are orthogonal, so the expansion of step 1.1 gives ⟨πn(aτ)fn,j,fn,k⟩=cosh⁡(τ/2)−nQjk(r)∥fn,k∥n2. In particular Q00=1, so normalizing fn,0 gives cn(aτ)=cosh⁡(τ/2)−n. Each fixed polynomial Qjk is bounded for ∣r∣≤1.

3.1F2F3step 2.1algebra

For fixed X,Y∈U(gC), [F2] writes Xun and Yun as finite sums of fn,j. In g=k1aτk2, the left and right K factors multiply each K-type vector by a scalar of modulus one. Thus the matrix coefficient is a fixed finite sum of the radial coefficients in step 2.1, with bounded factors Qjk(tanh⁡(τ/2)). Since cosh⁡(τ/2)−n≤2ne−n∣τ∣/2, this proves the derivative-vector bound with a constant depending only on n,X,Y and with polynomial exponent m=0.

4.1F4F5F6F7step 1.2algebra∎

At m=1,s=0, the integrand in step 1.2 has real part (cos⁡2θ+tsin⁡2θ)/D and odd imaginary part, so c1,0(τ)=t2π(Ic+tIs), where Ic=∫02πcos⁡2θ/D dθ and Is=∫02πsin⁡2θ/D dθ. Substitution x=tan⁡θ on each quadrant gives I0:=Ic+Is=2π/t and Is=4∫0∞x2(1+x2)(1+t2x2)dx=2π/(t(t+1)); for t≠1 the last integral follows from partial fractions, and at t=1 it is ∫02πsin⁡2θ dθ=π. Therefore Ic=2π/(t+1) and c1,0(τ)=2t/(t+1)=sech⁡(τ/2). Consequently ∣c1,0(τ)∣2sinh⁡τ→2, so the radial integral diverges. Since ∣c1,0(k1gk2)∣=∣c1,0(g)∣ by unitarity and the K-character property of f1, [F6] implies this matrix coefficient is not in L2(G).

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