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Lecture notes for Introduction to Representation Theory

Lecture notes for Introduction to Representation Theory

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These two corollaries show that there are only finitely many indecomposable representations<br />

(since there are only finitely many roots) and that the dimension vec<strong>to</strong>r of each of them is a positive<br />

root. The last statement of Gabriel’s theorem follows from<br />

Corollary 5.37. For every positive root ϕ, there is an indecomposable representation V with<br />

Proof. Consider the sequence<br />

d(V ) = ϕ.<br />

s n ϕ, s n−1 s n ϕ, . . .<br />

Consider the first element of this sequence which is a negative root (this has <strong>to</strong> happen by Lemma<br />

5.33) and look at one step be<strong>for</strong>e that, calling this element α. So α is a positive root and s i α is a<br />

negative root <strong>for</strong> some i. But since the s i only change one coordinate, we get<br />

and<br />

α = ϕ i<br />

(s q . . . s n−1 s n )ϕ = ϕ i .<br />

We let C (i) be the representation having dimension vec<strong>to</strong>r ϕ i . Then we define<br />

This is an indecomposable representation and<br />

V = F n − F n<br />

−<br />

−1 . . . F q − C (i) .<br />

d(V ) = ϕ.<br />

Example 5.38. Let us demonstrate by example how reflection func<strong>to</strong>rs work. Consider the quiver<br />

D 4 with the orientation of all arrows <strong>to</strong>wards the node (which is labeled by 4). Start with the<br />

1-dimensional representation V 4 sitting at the 4-th vertex. Apply <strong>to</strong> V 4 the func<strong>to</strong>r F 3 − F 2 − F 1 − .<br />

This yields<br />

F 1 − F 2 − F 3 − V 4 = V 1 + 2 + 3 + 4<br />

.<br />

Now applying F 4 − we get<br />

F 4 − F 1 − F 2 − F 3 − V 4 = V 1 + 2 + 3 +2 4<br />

.<br />

Note that this is exactly the inclusion of 3 lines in<strong>to</strong> the plane, which is the most complicated<br />

indecomposable representation of the D 4 quiver.<br />

5.9 Problems<br />

Problem 5.39. Let Q n be the cyclic quiver of length n, i.e., n vertices connected by n oriented edges<br />

<strong>for</strong>ming a cycle. Obviously, the classification of indecomposable representations of Q 1 is given by<br />

the Jordan normal <strong>for</strong>m theorem. Obtain a similar classification of indecomposable representations<br />

of Q 2 . In other words, classify pairs of linear opera<strong>to</strong>rs A : V ⊃ W and B : W ⊃ V up <strong>to</strong><br />

isomorphism. Namely:<br />

(a) Consider the following pairs (<strong>for</strong> n ⊂ 1):<br />

1) E n, : V = W = C n , A is the Jordan block of size n with eigenvalue ∂, B = 1 (∂ C).<br />

2) E n,≤ : is obtained from E n,0 by exchanging V with W and A with B.<br />

96

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