Let π:Ξβββπ₯πππ΅πΎπΌππ be a quiver representation.
The dimension vectordimββ‘πββΞπ0 of π is the function defined by quiv
(dimββ‘π)(π₯)=dimβ‘π(π₯)
where the notation is by analogy to graded dimension.
We call any vector in βΞπ0ββΞπ a dimension vector for Ξ,
since one can always