“…Recall that there exists a g f -invariant Pukanszky polarization p 0 ⊂ h at f 0 ∈ h * because g is exponential, see §4, Chapter I of [19] and Chapter 5 of [1]. We shall verify that p = g f + p 0 ⊂ g defines a Pukanszky polarization at f ∈ g * : Clearly…”
Section: Proof By Lemma 44(i) There Exists a Unit Vectormentioning
confidence: 97%
“…In order to prepare the proof of Theorem 2.6 we recall the well-known restrictioninduction-lemma of Fell, see Theorem 3.1 and Lemma 4.2 of [11]. A proof can also be found on p. 32 of [19]. We presume the definition of induced representations.…”
Section: Inducing Primitive Ideals From a Stabilizermentioning
confidence: 99%
“…connected, simply connected, solvable Lie groups G such that the exponential map exp : g −→ G is a global diffeomorphism). We will use the construction of irreducible representations π = K(f ) = ind G P χ f via Pukanszky / Vergne polarizations p at f and the bijectivity of the Kirillov map K : g * / Ad * (G) −→ G, see Chapters 4 and 6 of [1], and Chapter 1 of [19]. Mostly we regard K as a map from g * onto G which is constant on coadjoint orbits.…”
Section: Lemma 211 Let H Be a Closed Normal Subgroup Of A Locally Cmentioning
confidence: 99%
“…First we recall how to compute the C * -kernel of π | N in the Kirillov picture, compare Theorem 9 in Section 5 of Chapter 1 in [19]. Note that the linear projection r : g * → −→ n * given by restriction is Ad * (G)-equivariant so that r(Ad * (G)f ) = Ad * (G)l.…”
Section: Closed Orbits In the Unitary Dual Of The Nilradicalmentioning
“…Recall that there exists a g f -invariant Pukanszky polarization p 0 ⊂ h at f 0 ∈ h * because g is exponential, see §4, Chapter I of [19] and Chapter 5 of [1]. We shall verify that p = g f + p 0 ⊂ g defines a Pukanszky polarization at f ∈ g * : Clearly…”
Section: Proof By Lemma 44(i) There Exists a Unit Vectormentioning
confidence: 97%
“…In order to prepare the proof of Theorem 2.6 we recall the well-known restrictioninduction-lemma of Fell, see Theorem 3.1 and Lemma 4.2 of [11]. A proof can also be found on p. 32 of [19]. We presume the definition of induced representations.…”
Section: Inducing Primitive Ideals From a Stabilizermentioning
confidence: 99%
“…connected, simply connected, solvable Lie groups G such that the exponential map exp : g −→ G is a global diffeomorphism). We will use the construction of irreducible representations π = K(f ) = ind G P χ f via Pukanszky / Vergne polarizations p at f and the bijectivity of the Kirillov map K : g * / Ad * (G) −→ G, see Chapters 4 and 6 of [1], and Chapter 1 of [19]. Mostly we regard K as a map from g * onto G which is constant on coadjoint orbits.…”
Section: Lemma 211 Let H Be a Closed Normal Subgroup Of A Locally Cmentioning
confidence: 99%
“…First we recall how to compute the C * -kernel of π | N in the Kirillov picture, compare Theorem 9 in Section 5 of Chapter 1 in [19]. Note that the linear projection r : g * → −→ n * given by restriction is Ad * (G)-equivariant so that r(Ad * (G)f ) = Ad * (G)l.…”
Section: Closed Orbits In the Unitary Dual Of The Nilradicalmentioning
“…This may be handled most easily by the concept of variable Lie structures. Such structures were already considered in [5], [11], [10] and [9], among others.…”
Section: Variable Lie Algebras and Groupsmentioning
We establish a Fourier inversion theorem for general connected, simply connected nilpotent Lie groups G = exp(g) by showing that operator fields defined on suitable sub-manifolds of g * are images of Schwartz functions under the Fourier transform. As an application of this result, we provide a complete characterisation of a large class of invariant prime closed two-sided ideals of L 1 (G) as kernels of sets of irreducible representations of G.
We generalize the classical Paley-Wiener theorem to special types of connected, simply connected, nilpotent Lie groups: First we consider nilpotent Lie groups whose Lie algebra admits an ideal which is a polarization for a dense subset of generic linear forms on the Lie algebra. Then we consider nilpotent Lie groups such that the co-adjoint orbits of all the elements of a dense subset of the dual of the Lie algebra g * are flat.
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