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Proceedings of the 44th Symposium on Ring Theory and ...

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( B Ω ; wt, ε i , ϕ i , ẽ i , ˜f i<br />

)<br />

27 ∗ crystal<br />

structure <br />

Q Ω R Ω Ω 0<br />

R Ω 0<br />

Ω<br />

<br />

<br />

A ([3],[17]) <br />

<br />

5.5. Open problems.<br />

<br />

Problem 1D E Z N ≥0 crystal structure <br />

B = ⊔ d IrrΛ(d) Z N ≥0 N = |∆+ |<br />

Ψ : B ∼ → Z N ≥0<br />

Γ = (I, Ω) Dynkin quiverA <br />

D E B crystal structure Ψ Ω Z N ≥0 <br />

<br />

A <br />

Z N ≥0 crystal structure <br />

Problem 2Tame case<br />

B ∼ = B(∞) loop quiver Γ Dynkin case <br />

tame Γ extended Dynkin Lie <str<strong>on</strong>g>the</str<strong>on</strong>g>ory<br />

side “affine case” <br />

B(∞) <br />

Λ(d) <br />

<br />

Problem 3Rigid crystals<br />

<br />

variety <str<strong>on</strong>g>of</str<strong>on</strong>g> nilpotent representati<strong>on</strong>s Λ(d) G(d)-<br />

dimensi<strong>on</strong> vector d nilpotent P (Γ)-module <br />

<br />

Λ(d) IrrΛ(d) <br />

27 ẽ i <br />

(<br />

ẽ i a Ω =<br />

R Ω Ω 0<br />

◦ ẽ i ◦ R Ω0<br />

Ω<br />

)<br />

(a Ω ) (a Ω ∈ B Ω )<br />

ẽ i B Ω0 ẽ i <br />

5.2 explicit formula RΩ Ω 0<br />

R Ω 0<br />

Ω<br />

<br />

<br />

–191–

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