Semi-invariant of a quiver
{{No footnotes|date=June 2020}}
In mathematics, given a quiver Q with set of vertices Q0 and set of arrows Q1, a representation of Q assigns a vector space Vi to each vertex and a linear map V(α): V(s(α)) → V(t(α)) to each arrow α, where s(α), t(α) are the starting and the ending vertices of α. Given an element d ∈ Q0, the set of representations of Q with dim Vi = d(i) for each i has a vector space structure.
It is naturally endowed with an action of the algebraic group Πi∈Q0 GL(d(i)) by simultaneous base change. Such action induces one on the ring of functions. The ones which are invariants up to a character of the group are called semi-invariants. They form a ring whose structure reflects representation-theoretical properties of the quiver.
Definitions
Let Q = (Q0,Q1,s,t) be a quiver. Consider a dimension vector d, that is an element in Q0. The set of d-dimensional representations is given by
:
Once fixed bases for each vector space Vi this can be identified with the vector space
:
Such affine variety is endowed with an action of the algebraic group GL(d) := Πi∈Q0 GL(d(i)) by simultaneous base change on each vertex:
:
GL(\mathbf{d}) \times \operatorname{Rep}(Q,\mathbf{d}) & \longrightarrow & \operatorname{Rep}(Q,\mathbf{d})\\
\Big((g_i), (V_i, V(\alpha))\Big) & \longmapsto & (V_i,g_{t(\alpha)}\cdot V(\alpha)\cdot g_{s(\alpha)}^{-1} )
\end{array}
By definition two modules M,N ∈ Rep(Q,d) are isomorphic if and only if their GL(d)-orbits coincide.
We have an induced action on the coordinate ring k[Rep(Q,d)] by defining:
:
GL(\mathbf{d}) \times k[\operatorname{Rep}(Q,\mathbf{d})] & \longrightarrow & k[\operatorname{Rep}(Q,\mathbf{d})]\\
(g, f) & \longmapsto & g\cdot f(-):=f(g^{-1}. -)
\end{array}
= Polynomial invariants =
An element f ∈ k[Rep(Q,d)] is called an invariant (with respect to GL(d)) if g⋅f = f for any g ∈ GL(d). The set of invariants
:
is in general a subalgebra of k[Rep(Q,d)].
== Example ==
Consider the 1-loop quiver Q:
For d = (n) the representation space is End(kn) and the action of GL(n) is given by usual conjugation. The invariant ring is
:
where the cis are defined, for any A ∈ End(kn), as the coefficients of the characteristic polynomial
:
= Semi-invariants =
In case Q has neither loops nor cycles, the variety k[Rep(Q,d)] has a unique closed orbit corresponding to the unique d-dimensional semi-simple representation, therefore any invariant function is constant.
Elements which are invariants with respect to the subgroup SL(d) := Πi∈Q0 SL(d(i)) form a ring, SI(Q,d), with a richer structure called ring of semi-invariants. It decomposes as
:
where
:
A function belonging to SI(Q,d)σ is called semi-invariant of weight σ.
== Example ==
Consider the quiver Q:
:
Fix d = (n,n). In this case k[Rep(Q,(n,n))] is congruent to the set of n-by-n matrices: M(n). The function defined, for any B ∈ M(n), as detu(B(α)) is a semi-invariant of weight (u,−u) in fact
:
The ring of semi-invariants equals the polynomial ring generated by det, i.e.
:
Characterization of representation type through semi-invariant theory
For quivers of finite representation-type, that is to say Dynkin quivers, the vector space k[Rep(Q,d)] admits an open dense orbit. In other words, it is a prehomogenous vector space. Sato and Kimura described the ring of semi-invariants in such case.
= Sato–Kimura theorem =
Let Q be a Dynkin quiver, d a dimension vector. Let Σ be the set of weights σ such that there exists fσ ∈ SI(Q,d)σ non-zero and irreducible. Then the following properties hold true.
i) For every weight σ we have dimk SI(Q,d)σ ≤ 1.
ii) All weights in Σ are linearly independent over .
iii) SI(Q,d) is the polynomial ring generated by the fσ's, σ ∈ Σ.
Furthermore, we have an interpretation for the generators of this polynomial algebra. Let O be the open orbit, then k[Rep(Q,d)] \ O = Z1 ∪ ... ∪ Zt where each Zi is closed and irreducible. We can assume that the Zis are arranged in increasing order with respect to the codimension so that the first l have codimension one and Zi is the zero-set of the irreducible polynomial f1, then SI(Q,d) = k[f1, ..., fl].
== Example ==
In the example above the action of GL(n,n) has an open orbit on M(n) consisting of invertible matrices. Then we immediately recover SI(Q,(n,n)) = k[det].
Skowronski–Weyman provided a geometric characterization of the class of tame quivers (i.e. Dynkin and Euclidean quivers) in terms of semi-invariants.
= Skowronski–Weyman theorem =
Let Q be a finite connected quiver. The following are equivalent:
i) Q is either a Dynkin quiver or a Euclidean quiver.
ii) For each dimension vector d, the algebra SI(Q,d) is complete intersection.
iii) For each dimension vector d, the algebra SI(Q,d) is either a polynomial algebra or a hypersurface.
== Example ==
Consider the Euclidean quiver Q:
Pick the dimension vector d = (1,1,1,1,2). An element V ∈ k[Rep(Q,d)] can be identified with a quadruple (A1, A2, A3, A4) of matrices in M(1,2). Call Di,j the function defined on each V as det(Ai,Aj). Such functions generate the ring of semi-invariants:
:
See also
References
- {{Citation | last1=Derksen | first1= H.| last2=Weyman | first2=J. | title=Semi-invariants of quivers and saturation for Littlewood–Richardson coefficients. | url=http://www.ams.org/journals/jams/2000-13-03/S0894-0347-00-00331-3/home.html|mr=1758750 | year=2000 | journal=J. Amer. Math. Soc. | issue=13 | pages=467–479 | volume=3| doi= 10.1090/S0894-0347-00-00331-3| doi-access=free }}
- {{Citation | last1=Sato | first1= M.| last2=Kimura | first2=T. | title=A classification of irreducible prehomogeneous vector spaces and their relative invariants. | url=http://projecteuclid.org/euclid.nmj/1118796150|mr=0430336 | year=1977 | journal=Nagoya Math. J. | pages=1–155 | volume=65| doi= 10.1017/S0027763000017633| doi-access=free }}
- {{Citation | last1=Skowronski | first1= A.| last2=Weyman | first2=J. | title=The algebras of semi-invariants of quivers. |mr=1800533 | year=2000 | journal=Transform. Groups | issue=4 | pages=361–402 | volume=5 | doi=10.1007/bf01234798| s2cid= 120708005}}