The ray table of A₀ #
Setting 8.4 (local-ray-geometry.tex) for A₀: "A₀ = kP … identified with kP by
Proposition 4.14. We use its normed homogeneous ray basis." The basis of Proposition 4.14
(basisA0) consists of one vector on each nonzero deck-homogeneous piece A₀(x, y)_g; its
multiplication table is the ray table P (A0Tab), with the weight [x, y, g] ∈ W(P) of
Definition 7.1 (cls) and the degree given by the length mesh weight. Rays with the same
endpoints and the same weight are equal, since both lie in one length degree and the length
pieces of a corner are lines (lines, Lemma 3.7 for A₀). By Theorem 4.? A₀ is
representation-finite, so the table carries Setting 8.4 (A0Sys).
The basis vector of the piece (x, y, g) lies in the corner e_y A₀ e_x of the opposite
algebra, so the table has source y and target x.
The chosen deck-homogeneous vectors of Proposition 4.14.
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The rays of A₀: the nonzero deck-homogeneous pieces.
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The normed homogeneous ray basis of A₀ (Proposition 4.14).
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The identity piece of a vertex.
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Source of a ray of A₀ (the opposite convention).
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Target of a ray of A₀.
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The multiplication table of A₀.
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Idempotents and length grading of A₀ #
The vertex idempotents of A₀ as primitive idempotents.
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Vertices as indices of the idempotents of A₀.
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Weights and degrees #
The length mesh weight: every arrow has weight one.
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Products of rays #
A nonzero product of rays of A₀ is the composite piece.
The weight of a ray of A₀ in W(P).
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The length degree on W(P).
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Rays of A₀ with the same endpoints and weight are equal (one line per length
degree in each corner).
The ray table P = ray A₀ with weights in W(P).
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kP ≅ A₀ (Proposition 4.14).
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Setting 8.4 for A₀.
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Other weight lattices #
Any mesh weight Wt with values in L, with a homomorphism dg : L → ℤ recovering the
length, gives ray weights Wt.res [x, y, g] making the same table a ray table with
weights in L.
The ray weights in L'.
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The ray table of A₀ with weights in L'.
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kP ≅ A₀ for the table with weights in L'.
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Setting 8.4 for A₀ with weights in L'.