Fourier transform for nilpotent Lie groups Index sets and - - PowerPoint PPT Presentation

fourier transform for nilpotent lie groups
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Fourier transform for nilpotent Lie groups Index sets and - - PowerPoint PPT Presentation

The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Fourier transform for nilpotent Lie groups Index sets and representations Granada Index sets and representations June 22 2013 Index


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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Fourier transform for nilpotent Lie groups

Granada June 22 2013

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Nilpotent Lie algebras and nilpotent Lie groups

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Nilpotent Lie algebras and nilpotent Lie groups

Let g be a nilpotent Lie algebra over R, i.e; the sequence

  • f ideals

g0 = g, gj = [g, gj−1] stops with gd = {0} for some d > 0.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Nilpotent Lie algebras and nilpotent Lie groups

Let g be a nilpotent Lie algebra over R, i.e; the sequence

  • f ideals

g0 = g, gj = [g, gj−1] stops with gd = {0} for some d > 0. Let G = exp(g) be the corresponding simply connected connected (nilpotent) Lie group.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Nilpotent Lie algebras and nilpotent Lie groups

Let g be a nilpotent Lie algebra over R, i.e; the sequence

  • f ideals

g0 = g, gj = [g, gj−1] stops with gd = {0} for some d > 0. Let G = exp(g) be the corresponding simply connected connected (nilpotent) Lie group. Jordan-H¨

  • lder basis of g:

Z = {Z1, · · · , Zn} i.e. gj := span{Zj, · · · , Zn} ideal of g, j = 1, · · · , n.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Let h be a subalgebra of g, let H = exp(h).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Let h be a subalgebra of g, let H = exp(h). A Malcevbasis Y = {Y1, · · · , Ys} of g modulo h is a basis of g modulo h such that

s

  • i=j

RYi + h is a subalgebra for j = 1, · · · , s.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Let h be a subalgebra of g, let H = exp(h). A Malcevbasis Y = {Y1, · · · , Ys} of g modulo h is a basis of g modulo h such that

s

  • i=j

RYi + h is a subalgebra for j = 1, · · · , s. The mapping EY : Rs × h → G; (t1, · · · , ts, U) → exp(t1Y1) · · · · · exp(tsYs) · h is a diffeomorphism.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

g∗

ℓ ∈ g∗,

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

g∗

ℓ ∈ g∗, g(ℓ) := {U ∈ g, ℓ, [U, g] = {0}},

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

g∗

ℓ ∈ g∗, g(ℓ) := {U ∈ g, ℓ, [U, g] = {0}}, a(ℓ) =

  • g∈G

g( Ad ∗(g)ℓ) = largest ideal of g contained in g(ℓ).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

g∗

ℓ ∈ g∗, g(ℓ) := {U ∈ g, ℓ, [U, g] = {0}}, a(ℓ) =

  • g∈G

g( Ad ∗(g)ℓ) = largest ideal of g contained in g(ℓ). Ad ∗(g)ℓ, V := ℓ, Ad (g−1)V , V ∈ g.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

g∗

ℓ ∈ g∗, g(ℓ) := {U ∈ g, ℓ, [U, g] = {0}}, a(ℓ) =

  • g∈G

g( Ad ∗(g)ℓ) = largest ideal of g contained in g(ℓ). Ad ∗(g)ℓ, V := ℓ, Ad (g−1)V , V ∈ g. A polarization at ℓ is a subalgebra p of g of dimension

1 2(dim(g) + dim(g(ℓ))) such that

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

g∗

ℓ ∈ g∗, g(ℓ) := {U ∈ g, ℓ, [U, g] = {0}}, a(ℓ) =

  • g∈G

g( Ad ∗(g)ℓ) = largest ideal of g contained in g(ℓ). Ad ∗(g)ℓ, V := ℓ, Ad (g−1)V , V ∈ g. A polarization at ℓ is a subalgebra p of g of dimension

1 2(dim(g) + dim(g(ℓ))) such that

ℓ, [p, p] = {0}.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Vergne polarisation

Let ℓ ∈ g∗. Let Z = {Z1, · · · , Zn} be a Jordan-H¨

  • lder

basis of g: Vergne polarization at ℓ: pZ(ℓ) :=

n

  • j=1

gj(ℓ|gj)

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Monomial representation:

Let H = exp(h) ⊂ G be a closed connected subgroup.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Monomial representation:

Let H = exp(h) ⊂ G be a closed connected subgroup. G/H admits a G-invariant Borel measure dx.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Monomial representation:

Let H = exp(h) ⊂ G be a closed connected subgroup. G/H admits a G-invariant Borel measure dx. Let ℓ ∈ g∗ with ℓ, [h, h] = {0}.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Monomial representation:

Let H = exp(h) ⊂ G be a closed connected subgroup. G/H admits a G-invariant Borel measure dx. Let ℓ ∈ g∗ with ℓ, [h, h] = {0}. χℓ(h) := e−2iπℓ,log(h), h ∈ H.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Monomial representation:

Let H = exp(h) ⊂ G be a closed connected subgroup. G/H admits a G-invariant Borel measure dx. Let ℓ ∈ g∗ with ℓ, [h, h] = {0}. χℓ(h) := e−2iπℓ,log(h), h ∈ H.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Definition

Hℓ,h = L2(G/H, χℓ) = {ξ : G → C, measurable ,

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Definition

Hℓ,h = L2(G/H, χℓ) = {ξ : G → C, measurable , ξ(gh) = χℓ(h−1)ξ(g), g ∈ G, h ∈ H}

  • G/H

|ξ(g)|2dg < ∞.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Definition

Hℓ,h = L2(G/H, χℓ) = {ξ : G → C, measurable , ξ(gh) = χℓ(h−1)ξ(g), g ∈ G, h ∈ H}

  • G/H

|ξ(g)|2dg < ∞. Let σℓ,h(g)ξ(s) := ξ(g−1s), g, s ∈ G, ξ ∈ L2(G/H, χℓ).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Definition

Hℓ,h = L2(G/H, χℓ) = {ξ : G → C, measurable , ξ(gh) = χℓ(h−1)ξ(g), g ∈ G, h ∈ H}

  • G/H

|ξ(g)|2dg < ∞. Let σℓ,h(g)ξ(s) := ξ(g−1s), g, s ∈ G, ξ ∈ L2(G/H, χℓ).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Proposition

For F ∈ L1(G): σℓ,h(F)ξ(s) =

  • G/H

Fℓ,h(s, t)ξ(t)dt, where Fℓ,h(s, t) =

  • H

F(sht−1)χℓ(h)dh.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Orbit picture

Theorem

◮ Let ℓ ∈ g∗ and let p be a polarization at ℓ. Then σℓ,p

is irreducible.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Orbit picture

Theorem

◮ Let ℓ ∈ g∗ and let p be a polarization at ℓ. Then σℓ,p

is irreducible.

◮ Let ℓi ∈ g∗ and let pi, i = 1, 2 be a polarization at

ℓi, i = 1, 2. Then σℓ1,p1 ≃ σℓ2,p2 ⇔ Ad ∗(G)ℓ2 = Ad ∗(G)ℓ1. Write: [πℓ] := [σπ,p]

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Orbit picture

Theorem

◮ Let ℓ ∈ g∗ and let p be a polarization at ℓ. Then σℓ,p

is irreducible.

◮ Let ℓi ∈ g∗ and let pi, i = 1, 2 be a polarization at

ℓi, i = 1, 2. Then σℓ1,p1 ≃ σℓ2,p2 ⇔ Ad ∗(G)ℓ2 = Ad ∗(G)ℓ1. Write: [πℓ] := [σπ,p]

◮ Let (π, Hπ) ∈

G ⇒ ∃ℓ ∈ g∗ such that [π] = [πℓ]

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A homeomorphism

Theorem

The mapping K : g∗/G → G defined by K( Ad ∗(G)ℓ) := [πℓ] is a homeomorphism

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A partition of the orbit space

Index sets:

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A partition of the orbit space

Index sets: Let Z = {Z1, · · · , Zn} be a Jordan-H¨

  • lder

basis of g and let ℓ ∈ g∗.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A partition of the orbit space

Index sets: Let Z = {Z1, · · · , Zn} be a Jordan-H¨

  • lder

basis of g and let ℓ ∈ g∗. The index set I(ℓ) = I Z(ℓ) of ℓ ∈ g∗ is defined by:

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A partition of the orbit space

Index sets: Let Z = {Z1, · · · , Zn} be a Jordan-H¨

  • lder

basis of g and let ℓ ∈ g∗. The index set I(ℓ) = I Z(ℓ) of ℓ ∈ g∗ is defined by: I(ℓ) = ∅ if ℓ is a character.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A partition of the orbit space

Index sets: Let Z = {Z1, · · · , Zn} be a Jordan-H¨

  • lder

basis of g and let ℓ ∈ g∗. The index set I(ℓ) = I Z(ℓ) of ℓ ∈ g∗ is defined by: I(ℓ) = ∅ if ℓ is a character. Otherwise, let j1 = j1(ℓ) = max{j ∈ {1, . . . , n} | Zj ∈ a(ℓ)} k1 = k1(ℓ) = max{k ∈ {1, . . . , n} | < l, [Zj1(ℓ), Zk] >= 0}.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

We let ν1(ℓ) : = ℓ, [Zk1, Zj1] S1 = S1(ℓ) : = 1 ν1(ℓ)[Zk1, Zj1], Y1 = Y1(ℓ) : = Zj1 − ℓ, Y1 ν1(ℓ) S1 X1 = X1(ℓ) : = Zk1 − ℓ, Zk1 ν1(ℓ) S1.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

We let ν1(ℓ) : = ℓ, [Zk1, Zj1] S1 = S1(ℓ) : = 1 ν1(ℓ)[Zk1, Zj1], Y1 = Y1(ℓ) : = Zj1 − ℓ, Y1 ν1(ℓ) S1 X1 = X1(ℓ) : = Zk1 − ℓ, Zk1 ν1(ℓ) S1. Then we have that: ℓ, X1 = ℓ, Y1 = 0, (0.1) ℓ, [X1, Y1] = 1. We consider g1(ℓ) := {U ∈ g | < l, [U, Y1(ℓ)] >= 0} (0.2) which is an ideal of codimension one in g.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A Jordan-H¨

  • lder basis of (g1(ℓ), [·, ·]) is given by

{Z 1

i (ℓ) | i = k1(ℓ)} defined by

Z 1

i (ℓ) = Zi − < l, [Zi, Y1(ℓ)] >

ν1(ℓ) X1(ℓ), i = k1(ℓ). (0.3)

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A Jordan-H¨

  • lder basis of (g1(ℓ), [·, ·]) is given by

{Z 1

i (ℓ) | i = k1(ℓ)} defined by

Z 1

i (ℓ) = Zi − < l, [Zi, Y1(ℓ)] >

ν1(ℓ) X1(ℓ), i = k1(ℓ). (0.3) As previously we may now compute the indices j2(ℓ), k2(ℓ) of l1 := l|g1(ℓ) with respect to this new basis and construct the corresponding subalgebra g2(ℓ) with its associated basis {Z 2

i (ℓ) | i = k1(ℓ), k2(ℓ)}.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

A Jordan-H¨

  • lder basis of (g1(ℓ), [·, ·]) is given by

{Z 1

i (ℓ) | i = k1(ℓ)} defined by

Z 1

i (ℓ) = Zi − < l, [Zi, Y1(ℓ)] >

ν1(ℓ) X1(ℓ), i = k1(ℓ). (0.3) As previously we may now compute the indices j2(ℓ), k2(ℓ) of l1 := l|g1(ℓ) with respect to this new basis and construct the corresponding subalgebra g2(ℓ) with its associated basis {Z 2

i (ℓ) | i = k1(ℓ), k2(ℓ)}.

This procedure stops after a finite number rℓ = r of

  • steps. Let

IZ(ℓ) = I(ℓ) =

  • (j1(ℓ), k1(ℓ)), . . . , (jr(ℓ), kr(ℓ))
  • is called the index of ℓ in g with respect to the basis

Z = {Z1, . . . .Zn}.

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It is known that the last subalgebra gr(ℓ) obtained by this construction coincides with the Vergne polarization of ℓ in g with respect to the basis Z.

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It is known that the last subalgebra gr(ℓ) obtained by this construction coincides with the Vergne polarization of ℓ in g with respect to the basis Z. The length |I| = 2r of the index set I(ℓ) gives us the dimension of the coadjoint orbit Ad ∗(G)ℓ.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Partition of g∗/G

For an index set I ∈ N2j, j = 0, · · · , dim(g/2): g∗

I := {ℓ ∈ g∗, I(ℓ) = I, l, Xi(ℓ) = 0, l, Yi(ℓ) = 0, i = 1, · · · , r}.

Let I := {I ∈ dim(g/2)

  • j=0

Nj, g∗

I = ∅}.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Partition of g∗/G

For an index set I ∈ N2j, j = 0, · · · , dim(g/2): g∗

I := {ℓ ∈ g∗, I(ℓ) = I, l, Xi(ℓ) = 0, l, Yi(ℓ) = 0, i = 1, · · · , r}.

Let I := {I ∈ dim(g/2)

  • j=0

Nj, g∗

I = ∅}.

Then: g∗/G ≃ g∗

I := ˙

  • I∈Ig∗

I

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Properties of the g∗

I :

There exists an index I gen ∈ I such that g∗

gen := {ℓ ∈ g∗, I(ℓ) = I gen}

is G-invariant and Zariski open in g∗.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Properties of the g∗

I :

There exists an index I gen ∈ I such that g∗

gen := {ℓ ∈ g∗, I(ℓ) = I gen}

is G-invariant and Zariski open in g∗. There exists an order on I such that

◮ I gen is maximal for this order, ◮ such that

g∗

≤I :=

  • I ′≤I

g∗

I ′

is Zariski closed in g∗.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Realization on L2(Rr)

Proposition

◮ For every I ∈ I the mappings

g∗

I ∋ ℓ → Xj(ℓ), ℓ → Yj(ℓ), ℓ → pZ(ℓ)

are smooth.

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Realization on L2(Rr)

Proposition

◮ For every I ∈ I the mappings

g∗

I ∋ ℓ → Xj(ℓ), ℓ → Yj(ℓ), ℓ → pZ(ℓ)

are smooth.

◮ The family of vectors X(ℓ) = {Xj(ℓ), j = 1, · · · , r}

form a Malcev-basis of g modulo pZ(ℓ), the vectors {Yj(ℓ), j = 1, · · · , r} form a Malcev basis

  • f pZ(ℓ) modulo g(ℓ).
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Realization on L2(Rr)

Proposition

◮ For every I ∈ I the mappings

g∗

I ∋ ℓ → Xj(ℓ), ℓ → Yj(ℓ), ℓ → pZ(ℓ)

are smooth.

◮ The family of vectors X(ℓ) = {Xj(ℓ), j = 1, · · · , r}

form a Malcev-basis of g modulo pZ(ℓ), the vectors {Yj(ℓ), j = 1, · · · , r} form a Malcev basis

  • f pZ(ℓ) modulo g(ℓ).

◮ We identify the Hilbert space L2(G/PZ(ℓ), χℓ) with

L2(Rrℓ) using the unitary operator: Uℓ(η) = η ◦ E Z

ℓ ∈ L2(Rrℓ), η ∈ L2(G/PZ(ℓ), χℓ).

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An example

Let g = span {A, B, C, D, U, V }. [A, B] = U, [C, D] = V , [A, C] = V , [B, D] = sU (s ∈ R∗).

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Let ℓ ∈ g∗ µ = ℓ, U, ℓ, V = ν.

◮ ν = 0 ⇒

g1(ℓ) = span{A, B − sµ ν C, D, U, V }, j1(ℓ) = 4, k1(ℓ) = 3

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Let ℓ ∈ g∗ µ = ℓ, U, ℓ, V = ν.

◮ ν = 0 ⇒

g1(ℓ) = span{A, B − sµ ν C, D, U, V }, j1(ℓ) = 4, k1(ℓ) = 3 Z 1

1 = A, Z 1 2 = B − sµ

ν C, Z 1

4 = D, Z 1 5 = U, Z 1 6 = V .

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[Z 1

1 , Z 1 2 ]s,µ,ν = Z 1 5 − sµ

ν Z 1

6 ,

[Z 1

2 , Z 1 4 ]s,µ,ν = sZ 1 5 − sµ

ν Z 1

6 .

j2(ℓ) = 2, k2(ℓ) = 1, if s = 1.

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If ν = 0, µ = 0 ⇒ g1(ℓ) = span{A, C, D, U, V }

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If ν = 0, µ = 0 ⇒ g1(ℓ) = span{A, C, D, U, V } and j1(ℓ) = 4, k1(ℓ) = 2.

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Variable groups.

Definition

A variable locally compact group is a pair (B, G) where B and G are locally compact topological spaces, such that for every β ∈ B there exists a group multiplication ·β on G, which turns (G, ·β) into a topological group, such that

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Variable groups.

Definition

A variable locally compact group is a pair (B, G) where B and G are locally compact topological spaces, such that for every β ∈ B there exists a group multiplication ·β on G, which turns (G, ·β) into a topological group, such that B × (G × G) → G, (β, (s, t)) → s ·β t is continuous.

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Definition

A variable nilpotent Lie algebra is a triple (g, Z, B)

  • f a real finite dimensional vector space g, of a basis

Z = {Z1, · · · , Zn} of g and a smooth manifold B, such that

◮ for every β ∈ B there is a Lie algebra product [, ]β

  • n g,

◮ [Zi, Zj]β = n k=j+1 ci,j k (β)Zk, 1 ≤ i < j ≤ n ◮ and such that the functions β → ci,j k (β) are all

smooth.

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Fourier transform

Definition

l∞( G) := {(ϕ(ℓ) ∈ K(Hℓ)ℓ∈g∗

I, ϕ∞ := sup

ℓ∈g∗

I

ϕ(ℓ)op < ∞}.

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Fourier transform

Definition

l∞( G) := {(ϕ(ℓ) ∈ K(Hℓ)ℓ∈g∗

I, ϕ∞ := sup

ℓ∈g∗

I

ϕ(ℓ)op < ∞}. Write for ℓ ∈ g∗

I, (πℓ, Hℓ) = (σℓ,pZ(ℓ), L2(Rrℓ).

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Fourier transform

Definition

l∞( G) := {(ϕ(ℓ) ∈ K(Hℓ)ℓ∈g∗

I, ϕ∞ := sup

ℓ∈g∗

I

ϕ(ℓ)op < ∞}. Write for ℓ ∈ g∗

I, (πℓ, Hℓ) = (σℓ,pZ(ℓ), L2(Rrℓ).

For F ∈ L1(G), let F(F)(ℓ) = F(ℓ) := πℓ(F), ℓ ∈ g∗

I.

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Fourier transform

Definition

l∞( G) := {(ϕ(ℓ) ∈ K(Hℓ)ℓ∈g∗

I, ϕ∞ := sup

ℓ∈g∗

I

ϕ(ℓ)op < ∞}. Write for ℓ ∈ g∗

I, (πℓ, Hℓ) = (σℓ,pZ(ℓ), L2(Rrℓ).

For F ∈ L1(G), let F(F)(ℓ) = F(ℓ) := πℓ(F), ℓ ∈ g∗

I.

For u ∈ U(g) let

  • u(ℓ) = dπℓ(u) ∈ PD(RrI ), ℓ ∈ g∗

I

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Properties of u

◮ For every u ∈ U(g), for ℓ ∈ gI,

dσℓ,pZ(ℓ)(u) = u(ℓ) =

  • α∈RrI

pu

α(ℓ)∂α

with polynomial coefficients pu

α(ℓ) which depend

smoothly on ℓ ∈ g∗

I .

Let dµ(u) := (dσℓ,pZ(ℓ)(u))ℓ∈I gen

◮ For every D = α∈NrI pα∂α there exists a smooth

mapping ρD,I : g∗

I → U(g), such that

dσℓ,pZ(ℓ)(ρD,I(ℓ)) = D, ℓ ∈ g∗

I .

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Properties of F, F ∈ S(G)

◮ With respect to the basis X(ℓ) = {X1(ℓ), · · · , Xr(ℓ)}

the kernel functions of the operators σℓ,pZ(ℓ)(F) : FZ(ℓ, x, x′) :=

  • PZ(ℓ)

F(EX(ℓ)(x)hEX(ℓ)(x′)−1)χℓ(h)dh defined on g∗

I × Rr × Rr are smooth and Schwartz in

x, x′.

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Properties of F, F ∈ S(G)

◮ With respect to the basis X(ℓ) = {X1(ℓ), · · · , Xr(ℓ)}

the kernel functions of the operators σℓ,pZ(ℓ)(F) : FZ(ℓ, x, x′) :=

  • PZ(ℓ)

F(EX(ℓ)(x)hEX(ℓ)(x′)−1)χℓ(h)dh defined on g∗

I × Rr × Rr are smooth and Schwartz in

x, x′.

◮ Let Q ∈ C[g]. For every I = I gen, there exists a

partial differential operator DQ(I) on g∗

I × RrI with

polynomial coefficients in the variable (x, x′) ∈ RrI × RrI and smooth coefficients in ℓ ∈ g∗

I ,

such that for every F ∈ S(G): (QF)Z(ℓ, x, x′) = DQ(ℓ)(FZ)(ℓ, x, x′).

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Properties of F, F ∈ S(G)

◮ With respect to the basis X(ℓ) = {X1(ℓ), · · · , Xr(ℓ)}

the kernel functions of the operators σℓ,pZ(ℓ)(F) : FZ(ℓ, x, x′) :=

  • PZ(ℓ)

F(EX(ℓ)(x)hEX(ℓ)(x′)−1)χℓ(h)dh defined on g∗

I × Rr × Rr are smooth and Schwartz in

x, x′.

◮ Let Q ∈ C[g]. For every I = I gen, there exists a

partial differential operator DQ(I) on g∗

I × RrI with

polynomial coefficients in the variable (x, x′) ∈ RrI × RrI and smooth coefficients in ℓ ∈ g∗

I ,

such that for every F ∈ S(G): (QF)Z(ℓ, x, x′) = DQ(ℓ)(FZ)(ℓ, x, x′). Let δ(Q) := (DQ(ℓ))ℓ∈I gen

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Properties of F, F ∈ L1(G):

  • 1. the operator field

F is contained in l∞( G).

  • 2. on the subsets g∗

I , I ∈ I, the mappings

ℓ → F(ℓ) ∈ K(L2(RrI )) are operator -norm continuous.

  • 3. For every sequence ( Ad ∗(G)ℓk)k∈N which goes to

infinity in g∗/G, we have that lim

k→∞

F(ℓk)op = 0.

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Questions:

◮ Characterize the image of C ∗(G) in l∞(

G) under the Fourier transform,i.e. understand how πℓ(F) varies if ℓ ∈ g∗

I approaches

the boundary of g∗

I .

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Questions:

◮ Characterize the image of C ∗(G) in l∞(

G) under the Fourier transform,i.e. understand how πℓ(F) varies if ℓ ∈ g∗

I approaches

the boundary of g∗

I . ◮ Characterize the image of S(G) in l∞(

G) under the Fourier transform.

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Properly converging sequences in G

Let I ∈ I and let O = (πOk) be a properly converging sequence in GI with limit set L(O) contained in G<I, then the elements ρ ∈ L(O) are “entangled ” by O:

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Properly converging sequences in G

Let I ∈ I and let O = (πOk) be a properly converging sequence in GI with limit set L(O) contained in G<I, then the elements ρ ∈ L(O) are “entangled ” by O: For instance if for some F ∈ C ∗(G) we have that πOk(F) = 0 for an infinity of k’s then ρ(F) = 0, ∀ρ ∈ L(O).

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Properly converging sequences in G

Let I ∈ I and let O = (πOk) be a properly converging sequence in GI with limit set L(O) contained in G<I, then the elements ρ ∈ L(O) are “entangled ” by O: For instance if for some F ∈ C ∗(G) we have that πOk(F) = 0 for an infinity of k’s then ρ(F) = 0, ∀ρ ∈ L(O). Question: What is the relation between the sequence of

  • perators

(πOk(F) ∈ B(L2(RrI )))k and the operator field (ρ(F))ρ∈L(O)?

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S( G)

Definition

Let L2( G) = {(ϕ(ℓ))ℓ∈g∗

Igen, ℓ → ϕ(ℓ) measurable,

  • G

ϕ(ℓ)2

H−Sdµ(ℓ) < ∞}

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S( G)

Definition

Let L2( G) = {(ϕ(ℓ))ℓ∈g∗

Igen, ℓ → ϕ(ℓ) measurable,

  • G

ϕ(ℓ)2

H−Sdµ(ℓ) < ∞}

Let S( G) = {ϕ ∈ L2( G),

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S( G)

Definition

Let L2( G) = {(ϕ(ℓ))ℓ∈g∗

Igen, ℓ → ϕ(ℓ) measurable,

  • G

ϕ(ℓ)2

H−Sdµ(ℓ) < ∞}

Let S( G) = {ϕ ∈ L2( G), dµ(u)(ϕ) ∈ L2( G), u ∈ U(g),

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S( G)

Definition

Let L2( G) = {(ϕ(ℓ))ℓ∈g∗

Igen, ℓ → ϕ(ℓ) measurable,

  • G

ϕ(ℓ)2

H−Sdµ(ℓ) < ∞}

Let S( G) = {ϕ ∈ L2( G), dµ(u)(ϕ) ∈ L2( G), u ∈ U(g), δ(Q)ϕ ∈ L2( G), Q ∈ C[g]}.

Theorem

The Fourier transform maps S(G) onto S( G).

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Inverse Fourier transform

Theorem

There exists a G-invariant polynomial function Pgen on g∗ such that for every F ∈ S(G): F(g) =

  • g∗

Igen

tr (πℓ(g−1) ◦ F(ℓ))|Pgen(ℓ)|dℓ, =

  • G

tr (π(g−1) ◦ π(F))dµ(π), g ∈ G.

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Smooth compactly supported operator fields

Definition

Let C ∞

c (

G) = {(ϕ(ℓ) ∈ K(RrIgen)), ℓ ∈ g∗

I gen;

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Smooth compactly supported operator fields

Definition

Let C ∞

c (

G) = {(ϕ(ℓ) ∈ K(RrIgen)), ℓ ∈ g∗

I gen;

support (ϕ) compact in g∗

I gen,

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Smooth compactly supported operator fields

Definition

Let C ∞

c (

G) = {(ϕ(ℓ) ∈ K(RrIgen)), ℓ ∈ g∗

I gen;

support (ϕ) compact in g∗

I gen,

the function (ℓ, x, x′) → ϕ(ℓ)(x, x′) is smooth in ℓ and Schwartz in (x, x′) ∈ Rrgen × Rrgen.}

Theorem

For every ϕ ∈ C ∞

c (

G) there exists a unique F ∈ S(G), such that

  • F = ϕ.
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Un-sufficient data

What can we do, if we have only a smooth field (ϕ(ℓ) ∈ K(L2(Rr)))ℓ∈M defined on a smooth submanifold

  • f

G?

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Un-sufficient data

What can we do, if we have only a smooth field (ϕ(ℓ) ∈ K(L2(Rr)))ℓ∈M defined on a smooth submanifold

  • f

G? Example: M is the one point set {πℓ}

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Un-sufficient data

What can we do, if we have only a smooth field (ϕ(ℓ) ∈ K(L2(Rr)))ℓ∈M defined on a smooth submanifold

  • f

G? Example: M is the one point set {πℓ} Let p be a polarization at ℓ, X = {X1, · · · , Xr} Malcev basis with respect to p.

Theorem

(R. Howe) For every ϕ ∈ S(Rr × Rr) there exists F ∈ S(G) such that Fℓ,p(EX(x), EX(x′)) = ϕ(x, x′), x, x′ ∈ Rr.

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Un-sufficient data

What can we do, if we have only a smooth field (ϕ(ℓ) ∈ K(L2(Rr)))ℓ∈M defined on a smooth submanifold

  • f

G? Example: M is the one point set {πℓ} Let p be a polarization at ℓ, X = {X1, · · · , Xr} Malcev basis with respect to p.

Theorem

(R. Howe) For every ϕ ∈ S(Rr × Rr) there exists F ∈ S(G) such that Fℓ,p(EX(x), EX(x′)) = ϕ(x, x′), x, x′ ∈ Rr. This means that σℓ,p(S(G)) = B(Hℓ,p)∞.

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Fourier inversion for sub-manifolds

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Fourier inversion for sub-manifolds

Theorem

(Currey-L-Molitor-Braun) Let g∗

I be a fixed layer of g∗.

Let M be a smooth sub-manifold of g∗

I .

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Fourier inversion for sub-manifolds

Theorem

(Currey-L-Molitor-Braun) Let g∗

I be a fixed layer of g∗.

Let M be a smooth sub-manifold of g∗

I .

There exists an open subset M0 of M such that for any smooth kernel function Φ with compact support C ⊂ M0, there is a function F in the Schwartz space S(G) such that πℓ(F) has Φ(ℓ) as an operator kernel for all ℓ ∈ M0.

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Fourier inversion for sub-manifolds

Theorem

(Currey-L-Molitor-Braun) Let g∗

I be a fixed layer of g∗.

Let M be a smooth sub-manifold of g∗

I .

There exists an open subset M0 of M such that for any smooth kernel function Φ with compact support C ⊂ M0, there is a function F in the Schwartz space S(G) such that πℓ(F) has Φ(ℓ) as an operator kernel for all ℓ ∈ M0. Moreover, the Schwartz function F may be chosen such that πℓ(F) = 0 for all ℓ ∈ M \ M0 and for any ℓ in g∗

<I

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Fourier inversion for sub-manifolds

Theorem

(Currey-L-Molitor-Braun) Let g∗

I be a fixed layer of g∗.

Let M be a smooth sub-manifold of g∗

I .

There exists an open subset M0 of M such that for any smooth kernel function Φ with compact support C ⊂ M0, there is a function F in the Schwartz space S(G) such that πℓ(F) has Φ(ℓ) as an operator kernel for all ℓ ∈ M0. Moreover, the Schwartz function F may be chosen such that πℓ(F) = 0 for all ℓ ∈ M \ M0 and for any ℓ in g∗

<I

and such that the map Φ → F is continuous with respect to the corresponding function space topologies.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

An application

Let A ⊂ Aut(G) be a Lie group of auto-morphisms of G acting smoothly on G.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

An application

Let A ⊂ Aut(G) be a Lie group of auto-morphisms of G acting smoothly on G. For instance if G is connected Lie group containing G as nil-radical and A = Ad (G).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

An application

Let A ⊂ Aut(G) be a Lie group of auto-morphisms of G acting smoothly on G. For instance if G is connected Lie group containing G as nil-radical and A = Ad (G). Let J ⊂ L1(G) be a closed A-prime ideal.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

An application

Let A ⊂ Aut(G) be a Lie group of auto-morphisms of G acting smoothly on G. For instance if G is connected Lie group containing G as nil-radical and A = Ad (G). Let J ⊂ L1(G) be a closed A-prime ideal. For instance : (ρ, E) an irreducible bounded representation ρ of G on a Banach space E and J = ker(ρ|G)L1(G).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

  • G is Baire space, L1(G) has the Wiener property and J is

A-prime

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

  • G is Baire space, L1(G) has the Wiener property and J is

A-prime ⇒ the hull h(J) of J in G is the closure of an A-orbit in G: h(J) = A · πℓ for some ℓ ∈ g∗.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Let JS := J ∩ S(G).

Theorem

The ideal JS is a closed A-prime ideal in S(G).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Let JS := J ∩ S(G).

Theorem

The ideal JS is a closed A-prime ideal in S(G). ker(h(J))S/j(h(J))S is nilpotent ⇒ JS = ker(h(J))S.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Problem: Is JS dense in J?

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Problem: Is JS dense in J? Let ϕ ∈ L∞(G), such that ϕ, JS = {0}.

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Problem: Is JS dense in J? Let ϕ ∈ L∞(G), such that ϕ, JS = {0}. Is ϕ = 0 on J?

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

If A · πℓ is closed (or locally closed) in G, then A · πℓ is a smooth manifold

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

If A · πℓ is closed (or locally closed) in G, then A · πℓ is a smooth manifold and the theorem above tells us that S(G)/JS ≃ S(A · πℓ)

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

If A · πℓ is closed (or locally closed) in G, then A · πℓ is a smooth manifold and the theorem above tells us that S(G)/JS ≃ S(A · πℓ) and ϕ defines a tempered distribution dϕ on S(A · πℓ)

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

If A · πℓ is closed (or locally closed) in G, then A · πℓ is a smooth manifold and the theorem above tells us that S(G)/JS ≃ S(A · πℓ) and ϕ defines a tempered distribution dϕ on S(A · πℓ) From this one can show that |ϕ, F| ≤ sup

π∈A·πℓ

π(F)op, F ∈ L1(G).

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The dual space of a nilpotent Lie group Index sets and representations Index sets and representations Index sets and representations Index sets and representations Index sets and representations An example Variable groups Fourier Transform Un-sufficient data Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds Fourier inversion for sub-manifolds

Theorem

Suppose that J ⊂ L1(G) is A-prime and h(J) = A · π is a closed A-orbit in G, then J = ker(A · π).