Multiple Dirichlet Series Gautam Chinta 2013-02-18 Mon Previous - - PowerPoint PPT Presentation

multiple dirichlet series
SMART_READER_LITE
LIVE PREVIEW

Multiple Dirichlet Series Gautam Chinta 2013-02-18 Mon Previous - - PowerPoint PPT Presentation

Multiple Dirichlet Series Gautam Chinta 2013-02-18 Mon Previous talks of Sol Friedberg 1. Fourier expansion of (metaplectic) GL 2 Eisenstein series Previous talks of Sol Friedberg 1. Fourier expansion of (metaplectic) GL 2 Eisenstein series 2.


slide-1
SLIDE 1

Multiple Dirichlet Series

Gautam Chinta 2013-02-18 Mon

slide-2
SLIDE 2

Previous talks of Sol Friedberg

  • 1. Fourier expansion of (metaplectic) GL2 Eisenstein series
slide-3
SLIDE 3

Previous talks of Sol Friedberg

  • 1. Fourier expansion of (metaplectic) GL2 Eisenstein series
  • 2. The dth Fourier coefficient is a Dirichlet series with

◮ functional equations ◮ analytic continuation

slide-4
SLIDE 4

Previous talks of Sol Friedberg

  • 1. Fourier expansion of (metaplectic) GL2 Eisenstein series
  • 2. The dth Fourier coefficient is a Dirichlet series with

◮ functional equations ◮ analytic continuation

  • 3. These properties came from the analytic properties of the

Eisenstein series

slide-5
SLIDE 5

This talk

◮ Focus on n = 2: Fourier coeffs now involve quadratic

Dirichlet L-functions: E(z, s) = ∗ +

  • d=0

L(s′, χd)e2πixdWs(dy)

slide-6
SLIDE 6

This talk

◮ Focus on n = 2: Fourier coeffs now involve quadratic

Dirichlet L-functions: E(z, s) = ∗ +

  • d=0

L(s′, χd)e2πixdWs(dy)

◮ Mellin transform produces a “double Dirichlet series”

  • d=0

L(s, χd) |d|w

slide-7
SLIDE 7

This talk

◮ Focus on n = 2: Fourier coeffs now involve quadratic

Dirichlet L-functions: E(z, s) = ∗ +

  • d=0

L(s′, χd)e2πixdWs(dy)

◮ Mellin transform produces a “double Dirichlet series”

  • d=0

L(s, χd) |d|w

◮ Properties can be established independent of theory of

Eisenstein series (mostly)

slide-8
SLIDE 8

This talk

◮ Focus on n = 2: Fourier coeffs now involve quadratic

Dirichlet L-functions: E(z, s) = ∗ +

  • d=0

L(s′, χd)e2πixdWs(dy)

◮ Mellin transform produces a “double Dirichlet series”

  • d=0

L(s, χd) |d|w

◮ Properties can be established independent of theory of

Eisenstein series (mostly)

◮ “Axiomatic development” of the theory of WMDS

slide-9
SLIDE 9

Transition to local parts

◮ Emphasis on construction of local parts. Two methods:

◮ Functional Equations (Chinta/Gunnells) ◮ Crystal basis description (Brubaker, Bump, Friedberg)

slide-10
SLIDE 10

Transition to local parts

◮ Emphasis on construction of local parts. Two methods:

◮ Functional Equations (Chinta/Gunnells) ◮ Crystal basis description (Brubaker, Bump, Friedberg)

◮ Two methods are (more or less) equivalent when they

both apply, but it’s not so easy to see

slide-11
SLIDE 11

A2 quadratic double Dirichlet series

Goal: construct a two variable Dirichlet series which is roughly

  • f the form

Z(s, w) =

  • d

L(s, χd) dw

slide-12
SLIDE 12

A2 quadratic double Dirichlet series

Goal: construct a two variable Dirichlet series which is roughly

  • f the form

Z(s, w) =

  • d

L(s, χd) dw We will require that this series satisfy two functional equations as

◮ (s, w) → (1 − s, s + w − 1/2) ◮ (s, w) → (s + w − 1/2, 1 − w)

slide-13
SLIDE 13

A2 quadratic double Dirichlet series

Goal: construct a two variable Dirichlet series which is roughly

  • f the form

Z(s, w) =

  • d

L(s, χd) dw We will require that this series satisfy two functional equations as

◮ (s, w) → (1 − s, s + w − 1/2) ◮ (s, w) → (s + w − 1/2, 1 − w)

Where do these functional equations come from?

slide-14
SLIDE 14

Background on quadratic Dirichlet L-functions

Define L(s, χd0) =

  • n=1

χd0(n) ns =

  • p
  • 1 − χd0(p)

ps −1

slide-15
SLIDE 15

Background on quadratic Dirichlet L-functions

Define L(s, χd0) =

  • n=1

χd0(n) ns =

  • p
  • 1 − χd0(p)

ps −1

◮ Euler product ◮ Analytic continuation

◮ For d0 a fundamental discriminant, L(s, χd0) is entire

unless d0 = 1

◮ Functional equation

◮ For d0 a fundamental discriminant,

L(s, χd0) = ∗|d|1/2−sL(1 − s, χd0)

slide-16
SLIDE 16

Background on quadratic Dirichlet L-functions

Define L(s, χd0) =

  • n=1

χd0(n) ns =

  • p
  • 1 − χd0(p)

ps −1

◮ Euler product ◮ Analytic continuation

◮ For d0 a fundamental discriminant, L(s, χd0) is entire

unless d0 = 1

◮ Functional equation

◮ For d0 a fundamental discriminant,

L(s, χd0) = ∗|d|1/2−sL(1 − s, χd0)

But we need to define for all d. How to do this without messing up the earlier properties?

slide-17
SLIDE 17

Weighting polynomials

Define L(s, d) = L(s, χd0) · P(s, d) for P a weighting polynomial.

slide-18
SLIDE 18

Weighting polynomials

Define L(s, d) = L(s, χd0) · P(s, d) for P a weighting polynomial. What properties do we want this weighting polynomial to have?

◮ Euler product: P(s, d) = pα||d Pp(p−s, d) ◮ functional equation: P(s, d) = (d/d0)1/2−sP(1 − s, d).

We want this so that L(s, d) = ∗d1/2−sL(1 − s, d)

slide-19
SLIDE 19

Weighting polynomials

Define L(s, d) = L(s, χd0) · P(s, d) for P a weighting polynomial. What properties do we want this weighting polynomial to have?

◮ Euler product: P(s, d) = pα||d Pp(p−s, d) ◮ functional equation: P(s, d) = (d/d0)1/2−sP(1 − s, d).

We want this so that L(s, d) = ∗d1/2−sL(1 − s, d) If this last condition is satisfied, then the double Dirichlet series will have a functional equation (s, w) → (1 − s, s + w − 1/2)

slide-20
SLIDE 20

Passage to p-parts

Two types of p-parts for L(s, d) = L(s, χd0) · P(s, d):

◮ if (p, d0) = 1:

(1 − χd0(p)p−s)−1 times Pp(p−s, d)

◮ if p|d0,

Pp(p−s, d)

slide-21
SLIDE 21

Passage to p-parts

Two types of p-parts for L(s, d) = L(s, χd0) · P(s, d):

◮ if (p, d0) = 1:

(1 − χd0(p)p−s)−1 times Pp(p−s, d)

◮ if p|d0,

Pp(p−s, d) We will next describe the construction of the p-part as in Chinta-Gunnells

slide-22
SLIDE 22

A generating series

Two variable generating function F(x, y) =

  • k≥0

(1 − x)−1Pp(x, p2k)y 2k +

  • k≥0

Pp(x, p2k+1)y 2k+1

slide-23
SLIDE 23

A generating series

Two variable generating function F(x, y) =

  • k≥0

(1 − x)−1Pp(x, p2k)y 2k +

  • k≥0

Pp(x, p2k+1)y 2k+1 We need F to satisfy

  • 1. (1 − x) [F(x, y) + F(x, −y)] and 1

y [F(x, y) − F(x, −y)]

are invariant under (x, y) →

  • 1

px , xy√p

  • .
  • 2. Also need 2nd functional equation
  • 3. Limiting behavior F(x, 0) =

1 1−x

slide-24
SLIDE 24

A generating series

Two variable generating function F(x, y) =

  • k≥0

(1 − x)−1Pp(x, p2k)y 2k +

  • k≥0

Pp(x, p2k+1)y 2k+1 We need F to satisfy

  • 1. (1 − x) [F(x, y) + F(x, −y)] and 1

y [F(x, y) − F(x, −y)]

are invariant under (x, y) →

  • 1

px , xy√p

  • .
  • 2. Also need 2nd functional equation
  • 3. Limiting behavior F(x, 0) =

1 1−x

= ⇒ F(x, y) = 1 − xy (1 − x)(1 − y)(1 − px2y 2)

slide-25
SLIDE 25

Definition of a group action

Let f be the monomial xay bzc. Define (σ1f )(x, y, z) = f (y, x, z) if a − b even f (y, x, z) x2−tx1

x1−tx2

if a − b odd and define σ2f similarly.

slide-26
SLIDE 26

Definition of a group action

Let f be the monomial xay bzc. Define (σ1f )(x, y, z) = f (y, x, z) if a − b even f (y, x, z) x2−tx1

x1−tx2

if a − b odd and define σ2f similarly. Extend to polynomials by linearity and then to rational

  • functions. This will define an action of S3 on rational

functions.

slide-27
SLIDE 27

Construction of p-parts

For a ≥ b ≥ c define the polynomials Na,b,c(x, y, z) =

  • w∈W (−1)length(w)w(xa+2y b+1zc)

∆(x) · D(x) where D(x) =

  • i<j

(x2

i − t2x2 j ) and ∆(x) =

  • i<j

(x2

i − x2 j ).

slide-28
SLIDE 28

Construction of p-parts

For a ≥ b ≥ c define the polynomials Na,b,c(x, y, z) =

  • w∈W (−1)length(w)w(xa+2y b+1zc)

∆(x) · D(x) where D(x) =

  • i<j

(x2

i − t2x2 j ) and ∆(x) =

  • i<j

(x2

i − x2 j ).

These polynomials arise in the construction of the A2 multiple Dirichlet series. They also arise as Whittaker functions on the double cover of GL3.

slide-29
SLIDE 29

Comparison with the Gelfand-Tsetlin formula

Will describe the “right-leaning” Gelfand-Tsetlin formula of BBFH (I think).

slide-30
SLIDE 30

Comparison with the Gelfand-Tsetlin formula

Will describe the “right-leaning” Gelfand-Tsetlin formula of BBFH (I think). Let I be the GT pattern    a00 a01 a02 a11 a12 a22    .

slide-31
SLIDE 31

Comparison with the Gelfand-Tsetlin formula

Will describe the “right-leaning” Gelfand-Tsetlin formula of BBFH (I think). Let I be the GT pattern    a00 a01 a02 a11 a12 a22    . Define the weight of I to be (a00 + a01 + a02 − a11 − a12, a11 + a12 − a22, a22) and “(right sum) — (up-and-right sum)” coordinates r11 = (a11 − a01) + (a12 − a02), r12 = a12 − a02, r22 = a22 − a12.

slide-32
SLIDE 32

GT-formula (cont.)

We say

◮ I is nonstrict if the rows of I are not strictly decreasing ◮ I is right-leaning at (i, j) if ai,j = ai−1,j ◮ I is left-leaning at (i, j) if ai,j = ai−1,j−1

slide-33
SLIDE 33

GT-formula (cont.)

We say

◮ I is nonstrict if the rows of I are not strictly decreasing ◮ I is right-leaning at (i, j) if ai,j = ai−1,j ◮ I is left-leaning at (i, j) if ai,j = ai−1,j−1

Define G(I) =

  • if I is nonstrict

G(I; 1, 1)G(I; 1, 2)G(I; 2, 2)

  • therwise
slide-34
SLIDE 34

GT-formula (cont.)

We say

◮ I is nonstrict if the rows of I are not strictly decreasing ◮ I is right-leaning at (i, j) if ai,j = ai−1,j ◮ I is left-leaning at (i, j) if ai,j = ai−1,j−1

Define G(I) =

  • if I is nonstrict

G(I; 1, 1)G(I; 1, 2)G(I; 2, 2)

  • therwise

where left-leaning right-leaning non-leaning rij even −t2 1 1 − t2 rij odd t 1

slide-35
SLIDE 35

GT-formula (cont.)

Finally we define Ma,b,c(x, y, z) =

  • I

G(I)xwt(I) where the sum is over all GT-patterns with top row a + 2, b + 1, c.

slide-36
SLIDE 36

GT-formula (cont.)

Finally we define Ma,b,c(x, y, z) =

  • I

G(I)xwt(I) where the sum is over all GT-patterns with top row a + 2, b + 1, c. “Conjecture” For all a ≥ b ≥ c we have Na,b,c = Ma,b,c.

slide-37
SLIDE 37

GT-formula (cont.)

Finally we define Ma,b,c(x, y, z) =

  • I

G(I)xwt(I) where the sum is over all GT-patterns with top row a + 2, b + 1, c. “Conjecture” For all a ≥ b ≥ c we have Na,b,c = Ma,b,c. (Follows from work of McNamara, Chinta-Offen, Chinta-Gunnells. But more direct proof??)

slide-38
SLIDE 38

Other problems

  • 1. Construct/study G2 quadratic Dirichlet series

◮ Weighted sum of quadratic Dirichlet L-functions ◮ What is it counting?

slide-39
SLIDE 39

Other problems

  • 1. Construct/study G2 quadratic Dirichlet series

◮ Weighted sum of quadratic Dirichlet L-functions ◮ What is it counting?

  • 2. SU(3) Gauss sums (as in McNamara)

◮ Can be used to construct multiple Dirichlet series ◮ What are they?

slide-40
SLIDE 40

Other problems

  • 1. Construct/study G2 quadratic Dirichlet series

◮ Weighted sum of quadratic Dirichlet L-functions ◮ What is it counting?

  • 2. SU(3) Gauss sums (as in McNamara)

◮ Can be used to construct multiple Dirichlet series ◮ What are they?

  • 3. Function fields

◮ Multiple Dirichlet series are rational functions

slide-41
SLIDE 41

Multiple Dirichlet series arising in other settings

Multiple Dirichlet series arise in many different settings, many

  • f which are not (obviously) related to WMDS, but..
slide-42
SLIDE 42

Multiple Dirichlet series arising in other settings

Multiple Dirichlet series arise in many different settings, many

  • f which are not (obviously) related to WMDS, but..

◮ Are they related? ◮ Can techniques introduced/refined in the study of WMDS

be used in different settings

slide-43
SLIDE 43

Some other sources of multiple Dirichlet series

  • 1. Point evaluations of higher rank Eisenstein series

◮ Representation numbers of quadratic forms ◮ Count integral points on flag varieties ◮ Predict or give evidence for automorphic liftings

slide-44
SLIDE 44

Some other sources of multiple Dirichlet series

  • 1. Point evaluations of higher rank Eisenstein series

◮ Representation numbers of quadratic forms ◮ Count integral points on flag varieties ◮ Predict or give evidence for automorphic liftings

  • 2. Zeta functions of prehomogeneous vector spaces

◮ Well-developed theory for reductive groups ◮ Rich arithmetic theory evident in spaces coming from

parabolic subgroups of reductive spaces