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Geometric Methods in Representation Theory Columbia, Missouri, - - PowerPoint PPT Presentation

Geometric Methods in Representation Theory Columbia, Missouri, November 23-25, 2014 Varieties of Invariant Subspaces of Linear Operators Markus Schmidmeier (Florida Atlantic University) . . . . . . . . . . . . . . . . . . .


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Geometric Methods in Representation Theory Columbia, Missouri, November 23-25, 2014 Varieties of Invariant Subspaces

  • f Linear Operators

Markus Schmidmeier (Florida Atlantic University)

  • .

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ϕ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .................... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

mg sin(ϕ) mg

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . u

A report on a joint project with Justyna Kosakowska (Nicolaus Copernicus University)

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Short exact sequences of nilpotent linear operators

Definition: For α a partition and k a field, we denote the nilpotent linear operator of type α by Nα =

  • i

k[T]/(T αi). For fixed partitions α, β, γ, we are interested in short exact sequences of nilpotent linear operators 0 − → Nα

f

− → Nβ − → Nγ − → 0 Definition: Vβ

α,γ = {f : Nα → Nβ | Cok(f ) ∼

= Nγ} Vβ

α,γ is a constructible subset of the affine variety Homk(Nα, Nβ).

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SLIDE 3

Aim

◮ Motivation I: Varieties of type Vβ α,γ occur in a applications. ◮ Motivation II: They are interesting geometrically. ◮ The components: Study the partition

α,γ =

  • Γ LR-tableau of shape (α, β, γ)

  • f Vβ

α,γ into irreducible components VΓ. ◮ The relation: Introduce the closure relation V˜ Γ ∩ VΓ = ∅ to

see how the components are linked.

◮ Example: Review the case α1 ≤ 2 (all parts of α are at most

2).

◮ Main result: Compare this relation on the set of LR-tableaux

  • f shape (α, β, γ) with combinatorial relations ≤box, ≤part and

algebraic relations ≤ext, ≤hom.

◮ Part of the proof: Show that ≤closure implies ≤part.

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Motivation I: Control Systems

A linear time invariant dynamical system Σ is given by the differential equations Σ : dx

dt

= Bx + Au y = Cx where u(t) ∈ Cm is the input or control x(t) ∈ Cn the state and y(t) ∈ Cp the output at time t.

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Motivation I: Control Systems

A linear time invariant dynamical system Σ is given by the differential equations Σ : dx

dt

= Bx + Au y = Cx where u(t) ∈ Cm is the input or control x(t) ∈ Cn the state and y(t) ∈ Cp the output at time t. Time invariance means that A ∈ Cn×m, B ∈ Cn×n, and C ∈ Cp×n, so we are dealing with a linear representation: Σ : Cm

·A

− → ·B Cn

·C

− → Cp

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Motivation I: Inverted Pendulum

In every text book on control theory, you will find this example.

  • .

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ϕ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .................... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

mg sin(ϕ) mg

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . u

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Motivation I: Inverted Pendulum

In every text book on control theory, you will find this example.

  • .

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ϕ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .................... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

mg sin(ϕ) mg

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . u

After linearization, the differential equation m ¨ ϕ = mg sin(ϕ) + u becomes m ¨ ϕ = mgϕ + u. So the assignments x = ϕ ˙ ϕ

  • ,

y = ϕ, u = u lead to the dynamical system Σ :

  • dx

dt

= 0 1

g 0

  • · x +

1/m

  • · u

y = (1 0) · x Challenge: Apply torque u to bring and keep the pendulum in the vertical position.

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Motivation I: The Kalman Decomposition

A linear time-invariant dynamical system Σ : Vin

a

− → T V

c

− → Vout gives rise to two T-invariant subspaces of V : VC =

  • k≥0 imT ka

the controlable subspace V ¯

O

=

  • k≥0 ker cT k

the non-observable subspace

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Motivation I: The Kalman Decomposition

A linear time-invariant dynamical system Σ : Vin

a

− → T V

c

− → Vout gives rise to two T-invariant subspaces of V : VC =

  • k≥0 imT ka

the controlable subspace V ¯

O

=

  • k≥0 ker cT k

the non-observable subspace The Kalman embedding VC ∩ V ¯

O ⊂ VC ⊂

  • V is a system of two

invariant subspaces. Putting VK = VC/VC ∩ V ¯

O, we obtain a completely controlable

and completely observable system, the minimal realisation: Σmin : Vin

¯ a

− → ¯

T

VK

¯ c

− → Vout

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Motivation II: Arbitrary Operators

Suppose v, u are natural numbers with 0 ≤ u ≤ v and V is a (complex) vector space of dimension v. Observations:

  • 1. Generically, a linear operator T : V → V decomposes as the

direct sum of v linear operators, each acting with a different eigen value on a one-dimensional eigen space.

  • 2. Each T -invariant subspace U of V of dimension u is

determined by a subset of u elements of the set of eigen values. · · · · · ·

  • E(λ1)

E(λu) E(λu+1) E(λv)

  • 3. In this sense, “Semisimple is dense”.
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Motivation II: Nilpotent Operators

Suppose that v, u are natural numbers with 0 ≤ u ≤ v, that V is a vector space of dimension v, and that T : V → V acts nilpotently. Observations:

  • 1. Generically, a nilpotent linear operator T : V → V has only
  • ne Jordan block of size v corresponding to the eigen value 0.
  • 2. In this case, there is a unique T -invariant subspace U of V of

dimension u. Pv

u :

. . . . . .

  • u

           v

x

B = (V , T) = x k[T]/(T v) A = (U, T) = (x T v−u)

  • 3. In this case, the embedding (A ⊂ B) is a “picket” since the

ambient space B is a uniserial module. “Pickets are dense”.

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Motivation II: Operators with fixed Jordan type

Let α, β, γ be partitions. Observations:

  • 1. The operators Nα, Nβ, Nγ are determined uniquely, up to

isomorphism, by the partitions.

  • 2. The number of irreducible components in Vβ

α,γ is given by the

Littlewood-Richardson coefficient cβ

α,γ.

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Motivation II: Operators with fixed Jordan type

Let α, β, γ be partitions. Observations:

  • 1. The operators Nα, Nβ, Nγ are determined uniquely, up to

isomorphism, by the partitions.

  • 2. The number of irreducible components in Vβ

α,γ is given by the

Littlewood-Richardson coefficient cβ

α,γ.

Recall: The LR-coefficient features prominently in many exciting algebraic problems:

◮ Multiplication of Schur polynomials ◮ Eigenvalues of sums of Hermitian matrices ◮ Number of points in intersection of Schubert varieties ◮ Leading coefficient of the Hall polynomial

Combinatorially, cβ

α,γ counts the LR-tableaux of shape (α, β, γ).

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The components: LR-tableaux

Definition: An LR-tableau of shape (α, β, γ) is a Young diagram of shape β in which the region β \ γ contains α′

1 entries 1 , ..., α′ s entries s ,

where s = α1 is the largest entry, such that

◮ in each row, the entries are weakly increasing, ◮ in each column, the entries are strictly increasing, ◮ for each ℓ > 1 and each column c: on the right hand side of c,

the number of entries ℓ − 1 is at least the number of entries ℓ. Example: Let α = (211), β = (4321), γ = (321); then α′ = (31). Γ :

1 2 1 1

Γ = [321, 4221, 4321] Notation: Write Γ = [γ(0), . . . , γ(s)] where γ(i) denotes the region in the Young diagram β which contains the entries , 1 , ... , i .

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The components: The LR-tableau of an embedding

Theorem (Green and Klein, 1968): There exists a short exact sequence 0 − → Nα − → Nβ − → Nγ − → 0 if and only if there exists an LR-tableau of shape (α, β, γ). Definition: The LR-tableau Γ of an embedding A ⊂ B is given by Γ = [γ(i)]i=0,...,s, where s = α1 and γ(i) = type B/T iA. Property: Vβ

α,γ =

  • Γ LR-tableau of shape (α, β, γ)

VΓ where the VΓ = {f : Nα → Nβ | f has LR-tableau Γ} are Glα × Glβ-invariant irreducible varieties of the same dimension.

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The relation: The closure relation for LR-tableaux

Definition: For partitions α, β, γ, we denote by T β

α,γ the set of all

LR-tableaux of shape (α, β, γ). We are interested how the varieties VΓ, Γ ∈ T β

α,γ, are linked.

Definition: For LR-tableaux Γ, ˜ Γ ∈ T β

α,γ we write Γ≤closure˜

Γ if V˜

Γ ∩ VΓ = ∅.

Remark: The closure relation is a pre-order (i.e. reflexive and antisymmetric) as we will see. In general, ≤closure is not transitive. Definition: We denote by ≤∗

closure the transitive closure.

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Example: The variety V4321

211,321

∆6 :

1 1 1 21

❅ ❅ ❅ ❅ ■

∆4 :

1 1 1 22

∆5 :

1 1 21 1

✻ ✻

∆1 :

1 1 1 23

∆3 :

1 21 1 1

❅ ❅ ❅ ❅ ■

∆2 :

1 1 22 1

         dim = 12          dim = 11          dim = 13

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Example: The variety V4321

211,321

∆6 :

  • • • •

3 2 1

✤ ✜

❅ ❅ ❅ ❅ ■

∆4 :

  • • • •

3 2 1

✓ ✏

∆5 :

  • • • •

3 2 1

✓ ✏ ✻ ✻

∆1 :

  • • • •

3 2 1

✞ ☎

∆3 :

  • • • •

3 2 1

✞ ☎

❅ ❅ ❅ ❅ ■

∆2 :

  • • • •

3 2 1

✞ ☎

         dim = 12          dim = 11          dim = 13

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Example: The variety V4321

211,321

∆6 :

❅ ❅ ❅ ❅ ■

∆4 :

  • ∆5 :

∆1 :

  • ∆3 :

❅ ❅ ❅ ❅ ■

∆2 :

        dim = 12          dim = 11          dim = 13

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Main result: The combinatorial orders

Definition: Let T β

α,γ be the set of all LR-tableaux of shape (α, β, γ).

Recall that there is a natural partial ordering for partitions given by α≤partβ if for all j, j

i=0 αi ≥ j i=0 βi.

Definition: For LR-tableaux Γ = [γ(0), . . . , γ(s)], ˜ Γ = [˜ γ(0), . . . , ˜ γ(s)], we say Γ ≤part ˜ Γ if for each i, γ(i)≤part˜ γ(i). Example:

1 1 1 2

>part

1 1 2 1

>part

1 2 1 1 [321,3321,4321] [321,4221,4321] [321,4311,4321]

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Main result: The combinatorial orders

Definition: Let T β

α,γ be the set of all LR-tableaux of shape (α, β, γ).

Recall that there is a natural partial ordering for partitions given by α≤partβ if for all j, j

i=0 αi ≥ j i=0 βi.

Definition: For LR-tableaux Γ = [γ(0), . . . , γ(s)], ˜ Γ = [˜ γ(0), . . . , ˜ γ(s)], we say Γ ≤part ˜ Γ if for each i, γ(i)≤part˜ γ(i). Example:

1 1 1 2

>part

1 1 2 1

>part

1 2 1 1 [321,3321,4321] [321,4221,4321] [321,4311,4321]

Definition: By ≤box we denote the transitive closure of the relation

  • n T β

α,γ given by exchanging two boxes such that the smaller entry

moves up. Theorem: ≤box implies ≤∗

closure implies ≤part.

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Main result: The algebraic orders

For Γ, ˜ Γ ∈ T β

α,γ define: ◮ Γ ≤ext ˜

Γ, if there are X ∈ VΓ, ˜ X ∈ V˜

Γ with X ≤ext ˜

X, (In particular, X ≤ext ˜ X if ˜ X = ˜ X1 ⊕ ˜ X2 and there is a short exact sequence 0 → ˜ X1 → X → ˜ X2 → 0.)

◮ Γ ≤deg ˜

Γ, if there are X, ˜ X such that X ≤deg ˜ X. (Recall X ≤deg ˜ X if O ˜

X ⊂ OX.) ◮ Γ ≤hom ˜

Γ, if there are X, ˜ X with X ≤hom ˜ X, (equivalently, for all T, dim Hom(X, T) ≤ dim Hom( ˜ X, T).

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Main result: The algebraic orders

For Γ, ˜ Γ ∈ T β

α,γ define: ◮ Γ ≤ext ˜

Γ, if there are X ∈ VΓ, ˜ X ∈ V˜

Γ with X ≤ext ˜

X, (In particular, X ≤ext ˜ X if ˜ X = ˜ X1 ⊕ ˜ X2 and there is a short exact sequence 0 → ˜ X1 → X → ˜ X2 → 0.)

◮ Γ ≤deg ˜

Γ, if there are X, ˜ X such that X ≤deg ˜ X. (Recall X ≤deg ˜ X if O ˜

X ⊂ OX.) ◮ Γ ≤hom ˜

Γ, if there are X, ˜ X with X ≤hom ˜ X, (equivalently, for all T, dim Hom(X, T) ≤ dim Hom( ˜ X, T). Note 1: As for modules, ≤ext implies ≤deg implies ≤hom. Note 2: Since O ˜

X ⊂ V˜ Γ and OX ⊂ VΓ, ≤deg implies ≤closure.

Theorem: ≤ext implies ≤closure implies ≤hom−pic (the restriction of ≤hom to pickets T).

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Main result: How the partial orders are related

Theorem: For LR-tableaux Γ, ˜ Γ of the same shape, the following implications hold. ≤part ≤∗

hom

≤∗

closure

≤∗

deg

≤∗

ext

≤box ↓ ↓ ւ ց ց ւ

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SLIDE 25

Main result: How the partial orders are related

Theorem: For LR-tableaux Γ, ˜ Γ of the same shape, the following implications hold. ≤part ≤∗

hom

≤∗

closure

≤∗

deg

≤∗

ext

≤box ↓ ↓ ւ ց ց ւ Corollary: The closure relation is a partial order controlled combinatorially and algebraically (note ≤part is equivalent to ≤hom−pic).

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SLIDE 26

Main result: How the partial orders are related

Theorem: For LR-tableaux Γ, ˜ Γ of the same shape, the following implications hold. ≤part ≤∗

hom

≤∗

closure

≤∗

deg

≤∗

ext

≤box ↓ ↓ ւ ց ց ւ Corollary: The closure relation is a partial order controlled combinatorially and algebraically (note ≤part is equivalent to ≤hom−pic). Theorem (KS 2012): Suppose α is a partition with all parts at most 2. All partially ordered sets are equivalent.

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Proof: The closure relation implies the part relation, always

Theorem: If V˜

Γ ∩ VΓ = ∅ then Γ ≤part ˜

Γ. Proof: We assume Γ≤part˜ Γ to define a closed subset U ⊂ Vβ

α,γ

such that the following conditions hold: VΓ ⊂ U and U ∩ V˜

Γ = ∅

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SLIDE 28

Proof: The closure relation implies the part relation, always

Theorem: If V˜

Γ ∩ VΓ = ∅ then Γ ≤part ˜

Γ. Proof: We assume Γ≤part˜ Γ to define a closed subset U ⊂ Vβ

α,γ

such that the following conditions hold: VΓ ⊂ U and U ∩ V˜

Γ = ∅

For the closure of U we use the following Lemma: Suppose M is a set of monomorphisms between vector spaces A, B. For subspaces U ⊂ A, V ⊂ B, and for n ∈ N, the condition dim(f (U) ∩ V ) ≥ n defines a closed subset in M. Proof:

◮ The condition rank(f ) > m defines an open subset in

Hom(A, B)

◮ The condition dim f (U)+V V

> m defines an open subset in Hom(A, B)

◮ The subset defined by dim f (U) f (U)∩V > m is open ◮ On M, the subset given by dim(f (U) ∩ V ) < n is open

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SLIDE 29

Summary

◮ Set-Up: Given partitions α, β, γ, the short exact sequences

0 → Nα → Nβ → Nγ → 0 form a constructible subset Vβ

α,γ of

an affine variety.

◮ Motivation: Varieties of type Vβ α,γ occur in applications and

are of interest geometrically.

◮ Fact: Each variety Vβ α,γ has cβ α,γ irreducible components VΓ

where cβ

α,γ is the Littlewood-Richardson coefficient. ◮ Aim: Study the closure relation given by V˜ Γ ∩ VΓ = ∅. ◮ Example: In case α1 ≤ 2, the closure relation is known. ◮ Main result: The closure relation is under control

combinatorially (≤box implies ≤∗

closure implies ≤part) and

algebraically (≤∗

ext implies ≤∗ closure implies ≤hom−pic). ◮ Proof: We showed the Key-Lemma for ≤∗ closure implies ≤part.

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SLIDE 30

Summary

◮ Set-Up: Given partitions α, β, γ, the short exact sequences

0 → Nα → Nβ → Nγ → 0 form a constructible subset Vβ

α,γ of

an affine variety.

◮ Motivation: Varieties of type Vβ α,γ occur in applications and

are of interest geometrically.

◮ Fact: Each variety Vβ α,γ has cβ α,γ irreducible components VΓ

where cβ

α,γ is the Littlewood-Richardson coefficient. ◮ Aim: Study the closure relation given by V˜ Γ ∩ VΓ = ∅. ◮ Example: In case α1 ≤ 2, the closure relation is known. ◮ Main result: The closure relation is under control

combinatorially (≤box implies ≤∗

closure implies ≤part) and

algebraically (≤∗

ext implies ≤∗ closure implies ≤hom−pic). ◮ Proof: We showed the Key-Lemma for ≤∗ closure implies ≤part.

Thank You!