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Bessel functions outside GL p 2 q . Jack Buttcane University of - - PowerPoint PPT Presentation

Bessel functions outside GL p 2 q . Jack Buttcane University of Maine Orono, ME 26 September 2020 Jack Buttcane Bessel functions outside GL p 2 q . 1/14 What are Bessel functions outside of GL p 2 q ? Let G PGL p n , R q GL p n , R q{


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Bessel functions outside GLp2q.

Jack Buttcane

University of Maine Orono, ME

26 September 2020

Jack Buttcane Bessel functions outside GLp2q. 1/14

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What are Bessel functions outside of GLp2q?

Let G “ PGLpn, Rq “ GLpn, Rq{Rˆ, UpRq the upper triangular unipotent matrices, Y the diagonal matrices, Y ` the positive diagonal matrices, K “ POpn, Rq.

Jack Buttcane Bessel functions outside GLp2q. 2/14

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What are Bessel functions outside of GLp2q?

Define characters

  • f Y :

pµ ˆ a1 ...

an

˙ “

n

ź

i“1

|ai|µi, χδ ˆ a1 ...

an

˙ “

n

ź

i“1

sgnpaiqδi,

Jack Buttcane Bessel functions outside GLp2q. 3/14

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SLIDE 4

What are Bessel functions outside of GLp2q?

Define characters

  • f Y :

pµ ˆ a1 ...

an

˙ “

n

ź

i“1

|ai|µi, χδ ˆ a1 ...

an

˙ “

n

ź

i“1

sgnpaiqδi,

  • f UpRq: ψypxq “ ψIpyxy´1q “ e py1x1 ` . . . ` yn´1xn´1q,

y “ ¨ ˚ ˝

y1¨¨¨yn´1 y1¨¨¨yn´2

...

y1 1

˛ ‹ ‚ , x “ ¨ ˝

1 xn ˚

... ...

1 x1 1

˛ ‚ ,

Jack Buttcane Bessel functions outside GLp2q. 3/14

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SLIDE 5

What are Bessel functions outside of GLp2q?

Define characters

  • f Y :

pµ ˆ a1 ...

an

˙ “

n

ź

i“1

|ai|µi, χδ ˆ a1 ...

an

˙ “

n

ź

i“1

sgnpaiqδi,

  • f UpRq: ψypxq “ ψIpyxy´1q “ e py1x1 ` . . . ` yn´1xn´1q,

y “ ¨ ˚ ˝

y1¨¨¨yn´1 y1¨¨¨yn´2

...

y1 1

˛ ‹ ‚ , x “ ¨ ˝

1 xn ˚

... ...

1 x1 1

˛ ‚ , normalizations: ρ “ pn´1

2 , n´3 2 , . . . , ´n´1 2 q, use pρ`µ, assume n

ÿ

i“1

µi “ 0, extend to G by pρ`µpxykq “ pρ`µpyq.

Jack Buttcane Bessel functions outside GLp2q. 3/14

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What are Bessel functions outside of GLp2q?

Spherical Jacquet-Whittaker function: W pg, µ, ψq “ ż

UpRq

pρ`µpwlxgqψpxqdx, wl “ ˆ

1

...

1

˙ .

Jack Buttcane Bessel functions outside GLp2q. 4/14

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What are Bessel functions outside of GLp2q?

Spherical Jacquet-Whittaker function: W pg, µ, ψq “ ż

UpRq

pρ`µpwlxgqψpxqdx, wl “ ˆ

1

...

1

˙ . Since pρ`µ is an eigenfunction of the Casimir operators, so is the Whittaker function, with the same eigenvalues. Call µ the (Harish-Chandra/Langlands) spectral parameters.

Jack Buttcane Bessel functions outside GLp2q. 4/14

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What are Bessel functions outside of GLp2q?

Conjecture (Interchange of Integrals) If f pµq is homorphic with rapid decay on an open tube domain containing Repµq “ 0, and y P Y , t P G, then ż

UpRq

ż

Repµq“0

f pµqW pywlxt, µ, ψIqdµ ψIpxqdx “ ż

Repµq“0

f pµq r Kwlpy, t, µqdµ, where r Kwlpy, t, µq :“ lim

RÑ8

ż

UpRq

h ´

}x} R

¯ W pywlxt, µ, ψIqψIpxqdx is smooth in t and y, entire in µ and polynomially bounded in the coordinates of y, t, y´1, t´1, µ for Repµq in some fixed, compact set and h smooth and compactly supported with hp0q “ 1. Convergence!

Jack Buttcane Bessel functions outside GLp2q. 5/14

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What are Bessel functions outside of GLp2q?

It follows from work of Shalika that r Kwlpy, t, µq “ Kwlpy, µqW pt, µ, ψIq for some function Kwlpy, µq, and this is called the long-element, spherical Bessel function for GLpnq.

Jack Buttcane Bessel functions outside GLp2q. 6/14

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What are Bessel functions outside of GLp2q?

It follows from work of Shalika that r Kwlpy, t, µq “ Kwlpy, µqW pt, µ, ψIq for some function Kwlpy, µq, and this is called the long-element, spherical Bessel function for GLpnq. Kwlpy, µq has the bi-UpRq-invariance property Kwlpxy, µq “ Kwlpypwlxwlq, µq “ ψIpxqKwlpy, µq, and is an eigenfunction of the Casimir operators with eigenvalues matching pρ`µ.

Jack Buttcane Bessel functions outside GLp2q. 6/14

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What are Bessel functions outside of GLp2q?

It follows from work of Shalika that r Kwlpy, t, µq “ Kwlpy, µqW pt, µ, ψIq for some function Kwlpy, µq, and this is called the long-element, spherical Bessel function for GLpnq. Kwlpy, µq has the bi-UpRq-invariance property Kwlpxy, µq “ Kwlpypwlxwlq, µq “ ψIpxqKwlpy, µq, and is an eigenfunction of the Casimir operators with eigenvalues matching pρ`µ. There are Bessel functions Kwpy, µ, δq attached to the other elements of the Weyl group and to non-spherical χδ ‰ 1, as well.

Jack Buttcane Bessel functions outside GLp2q. 6/14

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What do we know about these Bessel functions?

Conjecture (Asymptotics) Dropping the µ integral and ignoring issues of convergence, replacing the Whittaker function in the definition of Kwpy, µ, δq with its first-term asymptotics as Y Q y Ñ 0 yields the first-term asymptotics of Kwpy, µ, δq.

Jack Buttcane Bessel functions outside GLp2q. 7/14

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What do we know about these Bessel functions?

Conjecture (Asymptotics) Dropping the µ integral and ignoring issues of convergence, replacing the Whittaker function in the definition of Kwpy, µ, δq with its first-term asymptotics as Y Q y Ñ 0 yields the first-term asymptotics of Kwpy, µ, δq. Conjecture (Uniqueness) The function Kwpy, µ, δq is uniquely determined by its first-term asymptotics, bi-UpRq-invariance and eigenvalues under the Casimir

  • perators.

Jack Buttcane Bessel functions outside GLp2q. 7/14

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What do we know about these Bessel functions?

The uniqueness conjecture is true in the long element case: p´ρpgqKwlpggT, µ, δq is the spherical Whittaker function W pg, 2µ, ψ2

I q, up to a function Cpµ, δq

Jack Buttcane Bessel functions outside GLp2q. 8/14

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What do we know about these Bessel functions?

The uniqueness conjecture is true in the long element case: p´ρpgqKwlpggT, µ, δq is the spherical Whittaker function W pg, 2µ, ψ2

I q, up to a function Cpµ, δq

so for y P Y `, Kwlpy, µ, δq “ Cpµ, δqpρ{2pyqW p?y, 2µ, ψ2

I q

Jack Buttcane Bessel functions outside GLp2q. 8/14

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What do we know about these Bessel functions?

The uniqueness conjecture is true in the long element case: p´ρpgqKwlpggT, µ, δq is the spherical Whittaker function W pg, 2µ, ψ2

I q, up to a function Cpµ, δq

so for y P Y `, Kwlpy, µ, δq “ Cpµ, δqpρ{2pyqW p?y, 2µ, ψ2

I q

from Hashizume’s solution of the Whittaker differential equations: Kwlpy, µ, δq “ ÿ

wPW

Cwpµ, δ, sgnpyqqJwlpy, µwq, Jwlpy, µq “ pρ`µpyq ÿ

mPNn´1

ampµqp4π2yqm ˜n´1 ÿ

j“0

pmj ´ mj`1q2 ´

n´1

ÿ

j“1

mn´jpµj`1 ´ µjq ¸ ampµq “

n´1

ÿ

j“1

am´ejpµq a0pµq “ 1, m0 “ mn “ 0.

Jack Buttcane Bessel functions outside GLp2q. 8/14

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What do we know about these Bessel functions?

The uniqueness conjecture is true in the long element case: p´ρpgqKwlpggT, µ, δq is the spherical Whittaker function W pg, 2µ, ψ2

I q, up to a function Cpµ, δq

so for y P Y `, Kwlpy, µ, δq “ Cpµ, δqpρ{2pyqW p?y, 2µ, ψ2

I q

from Hashizume’s solution of the Whittaker differential equations: Kwlpy, µ, δq “ ÿ

wPW

Cwpµ, δ, sgnpyqqJwlpy, µwq, Jwlpy, µq “ pρ`µpyq ÿ

mPNn´1

ampµqp4π2yqm ˜n´1 ÿ

j“0

pmj ´ mj`1q2 ´

n´1

ÿ

j“1

mn´jpµj`1 ´ µjq ¸ ampµq “

n´1

ÿ

j“1

am´ejpµq a0pµq “ 1, m0 “ mn “ 0. The asymptotics determine Cwpµ, δ, sgnpyqq.

Jack Buttcane Bessel functions outside GLp2q. 8/14

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What do we know about these Bessel functions?

What about the other Weyl elements?

Jack Buttcane Bessel functions outside GLp2q. 9/14

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What do we know about these Bessel functions?

What about the other Weyl elements? The long element case of the interchange of integrals is the most difficult (highest dimension), the others are only difficult because there are many things to keep track of.

Jack Buttcane Bessel functions outside GLp2q. 9/14

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What do we know about these Bessel functions?

What about the other Weyl elements? The long element case of the interchange of integrals is the most difficult (highest dimension), the others are only difficult because there are many things to keep track of. The positive sign case is no longer the spherical Whittaker function, so we lose Hashizume’s (and Harish-Chandra’s) and Stade’s work, so we have to work out the differential equations and power series solutions ourselves.

Jack Buttcane Bessel functions outside GLp2q. 9/14

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What do we know about these Bessel functions?

What about the other Weyl elements? The long element case of the interchange of integrals is the most difficult (highest dimension), the others are only difficult because there are many things to keep track of. The positive sign case is no longer the spherical Whittaker function, so we lose Hashizume’s (and Harish-Chandra’s) and Stade’s work, so we have to work out the differential equations and power series solutions ourselves. The trivial Bessel function is 1; the Voronoi Bessel function (probably) also shows up.

Jack Buttcane Bessel functions outside GLp2q. 9/14

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Work in progress.

Theorem (B, in progress) The interchange of integrals conjecture is true in the spherical and non-spherical cases for all Weyl elements on GLp2q, GLp3q, GLp4q and Spp4q.

Jack Buttcane Bessel functions outside GLp2q. 10/14

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Work in progress.

Theorem (B, in progress) The interchange of integrals conjecture is true in the spherical and non-spherical cases for all Weyl elements on GLp2q, GLp3q, GLp4q and Spp4q. Theorem (B) Assuming the interchange of integrals, the asymptotics conjecture is true for all Weyl elements in the spherical and non-spherical cases on GLpnq.

Jack Buttcane Bessel functions outside GLp2q. 10/14

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Applications - Spectral Kuznetsov trace formula.

Take the Fourier coefficient of a Poincar´ e series using Wallach’s Whittaker inversion formula and Langland’s spectral expansion: ż

Bpσq

ρξpnqρξpmqf pµξqW pt, µξ, χ, σ, ψIqdξ “ ÿ

wPW

ÿ

cPApZq

pρpcqSwpψm, ψn, cqHwpf ; mcwn´1w´1q,

Jack Buttcane Bessel functions outside GLp2q. 11/14

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Applications - Spectral Kuznetsov trace formula.

Take the Fourier coefficient of a Poincar´ e series using Wallach’s Whittaker inversion formula and Langland’s spectral expansion: ż

Bpσq

ρξpnqρξpmqf pµξqW pt, µξ, χ, σ, ψIqdξ “ ÿ

wPW

ÿ

cPApZq

pρpcqSwpψm, ψn, cqHwpf ; mcwn´1w´1q, Hwpf ; yq “ p´ρpyq ż

apσq

Kwpy, µ, χqf pµqW pt, µ, χ, σ, ψIqd˚µ

Jack Buttcane Bessel functions outside GLp2q. 11/14

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Applications - Spectral Kuznetsov trace formula.

Take the Fourier coefficient of a Poincar´ e series using Wallach’s Whittaker inversion formula and Langland’s spectral expansion: ż

Bpσq

ρξpnqρξpmqf pµξqW pt, µξ, χ, σ, ψIqdξ “ ÿ

wPW

ÿ

cPApZq

pρpcqSwpψm, ψn, cqHwpf ; mcwn´1w´1q, Hwpf ; yq “ p´ρpyq ż

apσq

Kwpy, µ, χqf pµqW pt, µ, χ, σ, ψIqd˚µ General Stone-Weierstrass-type argument to get rid of the spare Whittaker function? Still needs Stade’s formula to convert to Hecke eigenvalues.

Jack Buttcane Bessel functions outside GLp2q. 11/14

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Applications - Arithmetically-weighted Weyl laws.

From the Spectral Kuznetsov formula, the Mellin-Barnes integrals of the Bessel functions and good bounds for the Kloosterman sums, we get ż

Bpσq µξPΩ

1 Lp1, Ad2 ξqdξ “ ż

dspecµ ` O ˜ż

BΩ`Bp0,1q

dspecµ ¸ Theorem (Blomer/B) Arithmetically-weighted Weyl laws with error term for SLp3, Zq. On a set TΩ, we can probably improve the radius in the error term from 1 to plog Tq´δ for some δ P p0, 1

2q.

Jack Buttcane Bessel functions outside GLp2q. 12/14

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Applications - Subconvexity.

With much work, we get Theorem (Blomer,B) For φ a cusp form for SLp3, Zq such that µφ is in “generic position”,

  • 1. If φ is spherical, then Lp1

2, φq ! }µφ}

3 4 ´ 1 120000 .

  • 2. If φ has weight d ě 3, then Lp1

2, φq ! }µφ}

3 4 ´ 1 140000 .

Generic position: µi, µi ´ µj — }µ}.

Jack Buttcane Bessel functions outside GLp2q. 13/14

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Thank you!

Jack Buttcane Bessel functions outside GLp2q. 14/14