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IGA Lecture V: Applications to Verlinde Formulas Eckhard Meinrenken Adelaide, September 9, 2011 Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas Review We assume G compact, simple, simply connected. We consider q-Hamiltonian


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IGA Lecture V: Applications to Verlinde Formulas

Eckhard Meinrenken Adelaide, September 9, 2011

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Review

We assume G compact, simple, simply connected. We consider q-Hamiltonian G-spaces, Φ: M → G:

1 ι(ξM)ω = − 1

2Φ∗(θL + θR) · ξ,

2 dω = −Φ∗η, 3 ker(ω) ∩ ker(dΦ) = 0. Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Review

We constructed a canonical twisted Spinc-structure, (Φ, Sop): C l(TM) A(h∨).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Review

We constructed a canonical twisted Spinc-structure, (Φ, Sop): C l(TM) A(h∨). We defined a level k pre-quantization of dω = −Φ∗η (Φ, E): M × C A(k).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Review

We constructed a canonical twisted Spinc-structure, (Φ, Sop): C l(TM) A(h∨). We defined a level k pre-quantization of dω = −Φ∗η (Φ, E): M × C A(k). Then (Φ, E ⊗ Sop): C l(TM) A(k+h∨) defines a push-forward in twisted K-homology Φ∗ : K G

0 (M, C l(TM)) → K G 0 (G, A(k+h∨)).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Review

We constructed a canonical twisted Spinc-structure, (Φ, Sop): C l(TM) A(h∨). We defined a level k pre-quantization of dω = −Φ∗η (Φ, E): M × C A(k). Then (Φ, E ⊗ Sop): C l(TM) A(k+h∨) defines a push-forward in twisted K-homology Φ∗ : K G

0 (M, C l(TM)) → K G 0 (G, A(k+h∨)).

The l.h.s. contains the fundamental class [M]. The r.h.s. is the level k fusion ring Rk(G), by the FHT theorem. We define Q(M) := Φ∗([M]) ∈ Rk(G).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring

Notation T ⊂ G maximal torus, P+ = P ∩ t∗

+ dominant weights,

θ ∈ P+ weight of adjoint representation (highest root), · basic inner product on g ∼ = g∗: θ · θ = 2, ρ ∈ P+ shortest weight in P ∩ int(t∗

+),

h∨ = 1 + ρ · θ dual Coxeter number

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

A = {ξ ∈ t+| θ · ξ ≤ 1} is the fundamental alcove. Definition The level k weights are elements of Pk = P ∩ kA. ρ = θ ρ θ G = SU(3) k = 3 G = Spin(5) k = 4

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

For λ ∈ Pk define the special element tλ = exp( λ+ρ

k+h∨ ) ∈ T.

Definition The level k fusion ring (Verlinde ring) is the quotient Rk(G) = R(G)/Ik(G) where Ik(G) = {χ ∈ R(G)| χ(tλ) = 0 ∀ λ ∈ Pk}.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Remark Rk(G) is the fusion ring of level k projective representations of the loop group LG. (But we don’t need that here.) Remark For G = SU(r + 1), the level k fusion ideal has generators χ(k+1)̟1, . . . χ(k+r)̟1 where ̟1 ∈ P+ labels the defining representation. Similar descriptions exist for the compact symplectic groups. (Bouwknegt-Ridout, 2006)

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Some properties of Rk(G) = R(G)/Ik(G): Rk(G) is unital ring with involution. Rk(G) has finite Z-basis the images τµ of χµ, µ ∈ Pk. Thus Rk(G) = Z[Pk]. Rk(G) has a trace, Rk(G) → Z, τ → τ G where τ G

µ = δµ,0.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Notation Tensor coefficents Nµ1µ2µ3 = (χµ1χµ2χµ3)G, µi ∈ P+ Level k fusion coefficents N(k)

µ1µ2µ3 = (τµ1τµ2τµ3)G,

µi ∈ Pk.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Notation Tensor coefficents Nµ1µ2µ3 = (χµ1χµ2χµ3)G, µi ∈ P+ Level k fusion coefficents N(k)

µ1µ2µ3 = (τµ1τµ2τµ3)G,

µi ∈ Pk. Then N(k)

µ1µ2µ3 = Nµ1µ2µ3,

k >> 0.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: SU(2)

For G = SU(2), identify P+ = {0, 1, . . .}, Pk = {0, 1, . . . , k}.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: SU(2)

For G = SU(2), identify P+ = {0, 1, . . .}, Pk = {0, 1, . . . , k}. Ring structure of R(SU(2)) χlχm = χl+m + χl+m−2 + . . . + χ|l−m|.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: SU(2)

For G = SU(2), identify P+ = {0, 1, . . .}, Pk = {0, 1, . . . , k}. Ring structure of R(SU(2)) χlχm = χl+m + χl+m−2 + . . . + χ|l−m|. One finds Ik(SU(2)) = χk+1.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: SU(2)

For G = SU(2), identify P+ = {0, 1, . . .}, Pk = {0, 1, . . . , k}. Ring structure of R(SU(2)) χlχm = χl+m + χl+m−2 + . . . + χ|l−m|. One finds Ik(SU(2)) = χk+1. Quotient map R(G) → Rk(G) is ‘signed reflection’ across indices k + 1, 2k + 3, 3k + 5, . . ..

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: SU(2)

For G = SU(2), identify P+ = {0, 1, . . .}, Pk = {0, 1, . . . , k}. Ring structure of R(SU(2)) χlχm = χl+m + χl+m−2 + . . . + χ|l−m|. One finds Ik(SU(2)) = χk+1. Quotient map R(G) → Rk(G) is ‘signed reflection’ across indices k + 1, 2k + 3, 3k + 5, . . .. Example Calculation of τ3τ4 in R5(SU(2)): χ3χ4 = χ7 + χ5 + χ3 + χ1 ⇒ τ3τ4 = τ3 + τ1 since χ7 → −τ5, χ5 → τ5.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

For general G the quotient map R(G) = Z[P+] → Rk(G) = Z[Pk] is ‘signed reflection’ for a shifted Stiefel diagram. 3A Shifted affine Weyl action at level k = 3, G = SU(3)

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

For general G the quotient map R(G) = Z[P+] → Rk(G) = Z[Pk] is ‘signed reflection’ for a shifted Stiefel diagram. 3A Shifted affine Weyl action at level k = 3, G = SU(3)

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

For general G the quotient map R(G) = Z[P+] → Rk(G) = Z[Pk] is ‘signed reflection’ for a shifted Stiefel diagram. Shifted affine Weyl action at level k = 3, G = SU(3)

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

For general G the quotient map R(G) = Z[P+] → Rk(G) = Z[Pk] is ‘signed reflection’ for a shifted Stiefel diagram. Shifted affine Weyl action at level k = 3, G = SU(3)

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

For general G the quotient map R(G) = Z[P+] → Rk(G) = Z[Pk] is ‘signed reflection’ for a shifted Stiefel diagram. Shifted affine Weyl action at level k = 3, G = SU(3)

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Evaluation of characters at tλ = exp( λ+ρ

k+h∨ ) descends to the fusion

ring: Rk(G) → C, τ → τ(tλ).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Evaluation of characters at tλ = exp( λ+ρ

k+h∨ ) descends to the fusion

ring: Rk(G) → C, τ → τ(tλ). Rk(G) ⊗ C has another basis ˜ τµ s.t. ˜ τµ(tλ) = δλ,µ. In the new basis, ˜ τµ˜ τν = δµ,ν˜ τν.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Evaluation of characters at tλ = exp( λ+ρ

k+h∨ ) descends to the fusion

ring: Rk(G) → C, τ → τ(tλ). Rk(G) ⊗ C has another basis ˜ τµ s.t. ˜ τµ(tλ) = δλ,µ. In the new basis, ˜ τµ˜ τν = δµ,ν˜ τν. The bases are related by the S-matrix: τµ =

  • ν∈Pk

S−1

0,ν S∗ µ,ν˜

τν; here S is a symmetric, unitary matrix with S0,ν > 0.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

⇒ Verlinde formula for level k fusion coefficients: N(k)

µ1µ2µ3 =

  • ν∈Pk

Sµ1,νSµ2,νSµ3,ν S0,ν .

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

⇒ Verlinde formula for level k fusion coefficients: N(k)

µ1µ2µ3 =

  • ν∈Pk

Sµ1,νSµ2,νSµ3,ν S0,ν . This is one of several formulas called ‘Verlinde formulas’ – this is not the difficult one.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Using the S-matrix, any τ ∈ Rk(G) may be recovered from the values τ(tλ), λ ∈ Pk: τ =

  • λ∈Pk

τ(tλ)˜ τλ =

  • λ∈Pk

τ(tλ)S0,λ

  • µ∈Pk

Sλµτµ.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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The level k fusion ring (Verlinde ring)

Using the S-matrix, any τ ∈ Rk(G) may be recovered from the values τ(tλ), λ ∈ Pk: τ =

  • λ∈Pk

τ(tλ)˜ τλ =

  • λ∈Pk

τ(tλ)S0,λ

  • µ∈Pk

Sλµτµ. Goal: For level k pre-quantized q-Hamiltonian G-space (M, ω, Φ), find Q(M)(tλ) ∈ C via localization to the fixed point set.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Recall tλ = exp( λ+ρ

k+h∨ ). Let F ⊆ Mtλ a component of the fixed

point set. Since tλ regular, Φ(F) ⊆ G tλ = T.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Recall tλ = exp( λ+ρ

k+h∨ ). Let F ⊆ Mtλ a component of the fixed

point set. Since tλ regular, Φ(F) ⊆ G tλ = T. The Morita morphism C l(TM) A(k+h∨) restricts to C l(TM|F) A(k+h∨)|T.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Recall tλ = exp( λ+ρ

k+h∨ ). Let F ⊆ Mtλ a component of the fixed

point set. Since tλ regular, Φ(F) ⊆ G tλ = T. The Morita morphism C l(TM) A(k+h∨) restricts to C l(TM|F) A(k+h∨)|T. Now a nice thing happens:

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Recall tλ = exp( λ+ρ

k+h∨ ). Let F ⊆ Mtλ a component of the fixed

point set. Since tλ regular, Φ(F) ⊆ G tλ = T. The Morita morphism C l(TM) A(k+h∨) restricts to C l(TM|F) A(k+h∨)|T. Now a nice thing happens: Lemma A(k+h∨)|T is Morita trivial; equivariantly for action of tλ ⊂ T.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Remark Non-equivariantly, the Morita triviality of A(k+h∨)|T follows since the pull-back of η ∈ Ω3(G) to T is zero. Hence H3(G, Z) → H3(T, Z) is the zero map.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Remark Non-equivariantly, the Morita triviality of A(k+h∨)|T follows since the pull-back of η ∈ Ω3(G) to T is zero. Hence H3(G, Z) → H3(T, Z) is the zero map.Equivariantly, one shows that H3

G(G, Z) → H3 T(T, Z) = H3(T, Z) ⊕ H2 T(pt, Z) ⊗ H1(T, Z)

takes the generator to the basic inner product ·, viewed as an element of P ⊗ P.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Remark Non-equivariantly, the Morita triviality of A(k+h∨)|T follows since the pull-back of η ∈ Ω3(G) to T is zero. Hence H3(G, Z) → H3(T, Z) is the zero map.Equivariantly, one shows that H3

G(G, Z) → H3 T(T, Z) = H3(T, Z) ⊕ H2 T(pt, Z) ⊗ H1(T, Z)

takes the generator to the basic inner product ·, viewed as an element of P ⊗ P. Remark The choice of Morita trivialization of A(k+h∨)|T is not canonical in general.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Fix a tλ-equivariant Morita trivialization of A(k+h∨)|T.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Fix a tλ-equivariant Morita trivialization of A(k+h∨)|T. By composition C l(TM|F) A(k+h∨)|T C the bundle TM|F acquires a tλ-equivariant Spinc-structure.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Fix a tλ-equivariant Morita trivialization of A(k+h∨)|T. By composition C l(TM|F) A(k+h∨)|T C the bundle TM|F acquires a tλ-equivariant Spinc-structure. Thus, although we didn’t construct a global Spinc-Dirac operator

  • n M, there are such operators along fixed point manifolds.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Fix a tλ-equivariant Morita trivialization of A(k+h∨)|T. By composition C l(TM|F) A(k+h∨)|T C the bundle TM|F acquires a tλ-equivariant Spinc-structure. Thus, although we didn’t construct a global Spinc-Dirac operator

  • n M, there are such operators along fixed point manifolds.

⇒ Atiyah-Segal-Singer fixed point contributions are defined.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Fix a tλ-equivariant Morita trivialization of A(k+h∨)|T. By composition C l(TM|F) A(k+h∨)|T C the bundle TM|F acquires a tλ-equivariant Spinc-structure. Thus, although we didn’t construct a global Spinc-Dirac operator

  • n M, there are such operators along fixed point manifolds.

⇒ Atiyah-Segal-Singer fixed point contributions are defined. One proves:

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Let (M, ω, Φ) be a compact q-Hamiltonian G-space with a level k pre-quantization, and let Q(M) ∈ Rk(G) be its quantization. Theorem For all λ ∈ Pk, Q(M)(tλ) =

  • F⊂Mtλ
  • F
  • A(F) Ch(LF, tλ)1/2

DR(νF, tλ) . Here LF → F is the ‘Spinc-line bundle’ for C l(TM|F) C, and νF is the normal bundle to F.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Let (M, ω, Φ) be a compact q-Hamiltonian G-space with a level k pre-quantization, and let Q(M) ∈ Rk(G) be its quantization. Theorem For all λ ∈ Pk, Q(M)(tλ) =

  • F⊂Mtλ
  • F
  • A(F) Ch(LF, tλ)1/2

DR(νF, tλ) . Here LF → F is the ‘Spinc-line bundle’ for C l(TM|F) C, and νF is the normal bundle to F. One can use this formula to compute examples.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Localization to the fixed point set

Here the various characteristic forms are, in terms of curvature forms:

  • A(F) = det−1/2

R

(j( 1

2πRTF)), j(z) = sinh(z/2) z/2

Ch(LF, t) = trC

  • µ(t) exp( 1

2πRL)

  • DR(νF, t) = i

1 2 rk(νF )det1/2 R

  • 1 − AF(t)−1 exp( 1

2πRF)

  • .

Here µ(t) ∈ U(1) is the action of t on LF, and AF(t) ∈ Γ(F, O(νF)) is the action of t on νF.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: conjugacy classes

Example Let C ⊂ G be a level k pre-quantized conjugacy class. Thus C = G. exp(µ/k) where µ ∈ Pk. Then Q(C) = τµ, the basis element of Rk(G) corresponding to µ. This is similar to the quantization of coadjoint orbits O = G.µ ⊂ g∗, µ ∈ P+. Q(O) = χµ.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: conjugacy classes

Example Let C ⊂ G be a level k pre-quantized conjugacy class. Thus C = G. exp(µ/k) where µ ∈ Pk. Then Q(C) = τµ, the basis element of Rk(G) corresponding to µ. This is similar to the quantization of coadjoint orbits O = G.µ ⊂ g∗, µ ∈ P+. Q(O) = χµ. Both formulas are verified using the fixed point formula.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Example Let D(G) = G × G be the q-Hamiltonian G-space, with diagonal action of G and moment map Φ(a, b) = aba−1b−1. One finds: Q(D(G)) =

  • λ∈Pk

τλτ ∗

λ.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Example Let D(G) = G × G be the q-Hamiltonian G-space, with diagonal action of G and moment map Φ(a, b) = aba−1b−1. One finds: Q(D(G)) =

  • λ∈Pk

τλτ ∗

λ.

The Hamiltonian analogue is the non-compact Hamiltonian G-space T ∗G. Any reasonable quantization scheme for non-compact spaces gives Q(T ∗G) =

  • µ∈P+

χµχ∗

µ

(character for conjugation action on L2(G), defined in a completion of R(G)).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch) The fixed point set of tλ on D(G) = G × G is F = D(T) = T × T, with normal bundle νF = g/t × g/t.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch) The fixed point set of tλ on D(G) = G × G is F = D(T) = T × T, with normal bundle νF = g/t × g/t. Since F is a torus, A(F) = 1.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch) The fixed point set of tλ on D(G) = G × G is F = D(T) = T × T, with normal bundle νF = g/t × g/t. Since F is a torus, A(F) = 1. Let J(t) be the Weyl denominator, J(t) =

  • w∈W

(−1)l(w)twρ = tρ

α>0

(1 − t−α). Then DR(g/t, t) = J(t). Hence D(νF, tλ) = |J(tλ)|2.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch, ctd’) The pull-back of ω to the fixed point manifold F is symplectic. One argues that c1(L|F) is a pre-quantum line bundle for the symplectic structure on F at level 2(k + h∨). Hence

  • F

Ch(L, tλ)1/2 =

  • F

e(k+h∨)ωF = |Tk+h∨| where Tk+h∨ =

  • 1

k + h∨ P

  • Q∨ ⊂ t/Q∨ = T.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch, ctd’) The pull-back of ω to the fixed point manifold F is symplectic. One argues that c1(L|F) is a pre-quantum line bundle for the symplectic structure on F at level 2(k + h∨). Hence

  • F

Ch(L, tλ)1/2 =

  • F

e(k+h∨)ωF = |Tk+h∨| where Tk+h∨ =

  • 1

k + h∨ P

  • Q∨ ⊂ t/Q∨ = T.

The result is Q(D(G))(tλ) = |Tk+h∨| |J(tλ)|2 = S−2

0,λ.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch, ctd’) The pull-back of ω to the fixed point manifold F is symplectic. One argues that c1(L|F) is a pre-quantum line bundle for the symplectic structure on F at level 2(k + h∨). Hence

  • F

Ch(L, tλ)1/2 =

  • F

e(k+h∨)ωF = |Tk+h∨| where Tk+h∨ =

  • 1

k + h∨ P

  • Q∨ ⊂ t/Q∨ = T.

The result is Q(D(G))(tλ) = |Tk+h∨| |J(tλ)|2 = S−2

0,λ.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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Example: The double

Computation of Q(D(G)) (Sketch, ctd’) Hence Q(D(G)) =

  • λ∈Pk

S−2

0,λ˜

τλ =

  • λ∈Pk

τλτ ∗

λ.

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Example: The sphere S2n

Example Recall that S2n is a q-Hamiltonian SU(n)-space, pre-quantized at all levels k ≥ 0. Fixed point set of tλ consists of ‘poles’. One computes Q(S2n) = τ0 + τ̟1 + · · · + τk̟1 where ̟1 is the weight of the defining representation.

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Example: The sphere S2n

Example Recall that S2n is a q-Hamiltonian SU(n)-space, pre-quantized at all levels k ≥ 0. Fixed point set of tλ consists of ‘poles’. One computes Q(S2n) = τ0 + τ̟1 + · · · + τk̟1 where ̟1 is the weight of the defining representation. This is consistent with ‘quantization commutes with reduction’, since S2n is multiplicity free, with moment polytope is ∆(S2n) = {s̟1| 0 ≤ s ≤ 1}.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 59

Example: symplectic Verlinde formulas

Write the results for conjugacy classes and for the double in terms

  • f the basis ˜

τµ, where ˜ τµ(tλ) = δλ,µ: Q

  • G. exp(1

k µ)

  • =
  • ν∈Pk

S∗

µ,ν

S0,ν ˜ τν. Q(D(G)) =

  • ν∈Pk

1 S2

0,ν

˜ τν.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 60

Example: symplectic Verlinde formulas

Write the results for conjugacy classes and for the double in terms

  • f the basis ˜

τµ, where ˜ τµ(tλ) = δλ,µ: Q

  • G. exp(1

k µ)

  • =
  • ν∈Pk

S∗

µ,ν

S0,ν ˜ τν. Q(D(G)) =

  • ν∈Pk

1 S2

0,ν

˜ τν. Using Q(M1 × M2) = Q(M1)Q(M2) this gives ...

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 61

Example: symplectic Verlinde formulas

Let µ1, . . . , µr ∈ Pk, and Cj = G. exp( 1

k µj). Then

Q

  • D(G)h × C1 × · · · × Cr
  • =
  • ν∈Pk

S∗

µ1,ν · · · S∗ µr,ν

S2h+r

0,ν

˜ τν

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 62

Example: symplectic Verlinde formulas

Let µ1, . . . , µr ∈ Pk, and Cj = G. exp( 1

k µj). Then

Q

  • D(G)h × C1 × · · · × Cr
  • =
  • ν∈Pk

S∗

µ1,ν · · · S∗ µr,ν

S2h+r

0,ν

˜ τν Using Q(M/ /G) = Q(M)G and ˜ τ G

ν = S2 0,ν this gives...

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 63

Example: symplectic Verlinde formulas

Theorem (Symplectic Verlinde formulas) Let µ1, . . . , µr ∈ Pk, and Cj = G. exp( 1

k µj). The level k

quantization of the moduli space M(Σr

h, C1, . . . , Cr) = (D(G)h × C1 × · · · × Cr)/

/G is given by Q

  • M(Σr

h, C1, . . . , Cr)

  • =
  • ν∈Pk

Sµ1,ν · · · Sµr,ν S2h+r−2

0,ν

C1 C2 C3

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 64

Verlinde formulas for non-simply connected groups

Let Z = Z(G), G ′ = G/Z(G). Then D(G ′)h/ /G ′ is the moduli space of flat G ′-bundles over Σ0

h.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 65

Verlinde formulas for non-simply connected groups

Let Z = Z(G), G ′ = G/Z(G). Then D(G ′)h/ /G ′ is the moduli space of flat G ′-bundles over Σ0

h.

It has several connected components, indexed by topological types

  • f G ′-bundles.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 66

Verlinde formulas for non-simply connected groups

Let Z = Z(G), G ′ = G/Z(G). Then D(G ′)h/ /G ′ is the moduli space of flat G ′-bundles over Σ0

h.

It has several connected components, indexed by topological types

  • f G ′-bundles.

Consider D(G ′) as a q-Hamiltonian G-space. Then D(G ′)h/ /G is the moduli space of flat connections on Σ0

h × G ′.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 67

Verlinde formulas for non-simply connected groups

By D. Krepski’s result, D(G ′) is pre-quantized at level k if and

  • nly if

P∨ · P∨ ⊆ 1 k Z, where P∨ = Q∗ is the co-weight lattice. The in-equivalent pre-quantizations are indexed by Hom(Z × Z, U(1)).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 68

Verlinde formulas for non-simply connected groups

By D. Krepski’s result, D(G ′) is pre-quantized at level k if and

  • nly if

P∨ · P∨ ⊆ 1 k Z, where P∨ = Q∗ is the co-weight lattice. The in-equivalent pre-quantizations are indexed by Hom(Z × Z, U(1)). So, what is Q(D(G ′))?

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 69

Verlinde formulas for non-simply connected groups

Let Z → W = N(T)/T, c → wc be the group homomorphism defined by w−1

c

exp(A) = c exp(A).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 70

Verlinde formulas for non-simply connected groups

Let Z → W = N(T)/T, c → wc be the group homomorphism defined by w−1

c

exp(A) = c exp(A). The action of Z on G commutes with conjugation. Hence it induces a Z-action on A = G/ Ad(G). In turn, this induces an action on Pk.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 71

Verlinde formulas for non-simply connected groups

Let Z → W = N(T)/T, c → wc be the group homomorphism defined by w−1

c

exp(A) = c exp(A). The action of Z on G commutes with conjugation. Hence it induces a Z-action on A = G/ Ad(G). In turn, this induces an action on Pk. Lemma The fixed point set of tλ on G ′ = G/Z is (G ′)tλ =

  • c∈Zλ

N(T ′)c where N(T ′)c ⊂ N(T ′) is the pre-image of wc ∈ W = N(T ′)/T ′.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 72

Verlinde formulas for non-simply connected groups

Hence, the components of D(G ′)tλ are all (left translates of) tori. Calculating the fixed point contributions requires more work. Eventually one gets:

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 73

Verlinde formulas for non-simply connected groups

Hence, the components of D(G ′)tλ are all (left translates of) tori. Calculating the fixed point contributions requires more work. Eventually one gets: Q(D(G ′)) = 1 |Z|2

  • c∈Z×Z

φ(c1, c2)

  • λ∈Pc

k

S−2

0,λ˜

τλ where φ(c1, c2) are phase factors depending on the pre-quantization, and Pc

k ⊂ Pk are weights fixed by c1, c2.

The phase factor is explicitly φ(c1, c2) = ψ(c1, c2)e−2πik

  • (1−w∗)−1ζ1
  • ·ζ2

where ψ ∈ Hom(Z × Z, U(1)) labels the pre-quantization, ζi ∈ A exponentiate to ci, and w∗ is the Coxeter transformation.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 74

Verlinde formulas for non-simply connected groups

Following the argument for G, one finds: Theorem (Fuchs-Schweigert formula) Q(D(G ′)h/ /G) = 1 |Z|2h

  • c∈Z 2h

φ(c1, . . . , c2h)

  • λ∈Pc

k

S2−2h

0,λ

.

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 75

Verlinde formulas for non-simply connected groups

Following the argument for G, one finds: Theorem (Fuchs-Schweigert formula) Q(D(G ′)h/ /G) = 1 |Z|2h

  • c∈Z 2h

φ(c1, . . . , c2h)

  • λ∈Pc

k

S2−2h

0,λ

. The case with markings is more complicated, and is presently only worked out for SO(3).

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas

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SLIDE 76

Verlinde formulas for non-simply connected groups

Following the argument for G, one finds: Theorem (Fuchs-Schweigert formula) Q(D(G ′)h/ /G) = 1 |Z|2h

  • c∈Z 2h

φ(c1, . . . , c2h)

  • λ∈Pc

k

S2−2h

0,λ

. The case with markings is more complicated, and is presently only worked out for SO(3).

Thanks!

Eckhard Meinrenken IGA Lecture V: Applications to Verlinde Formulas