Hom-dimension weights and the two unit equations #
Once the Hom-dimension matrix and the mesh matrix are inverse, a row represented
by a label P satisfies the paper's column equation Phi^T d = e_P, while a
column represented by I satisfies Phi d = e_I. Nonzero maps from P, or
to I, make the corresponding integral weights strictly positive.
The integer Hom-dimension row represented by P.
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The integer Hom-dimension column represented by I.
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The additive extension of a represented Hom row evaluates every object by the dimension of its Hom space from the representing object.
The additive extension of a represented Hom column evaluates every object by the dimension of its Hom space to the representing object.
A strictly positive label weight has zero additive extension exactly on zero objects.
The Euler defect of a label weight on the chosen left mesh.
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Weighted row sum of the paper-oriented mesh matrix.
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The row of Hom dimensions represented by P satisfies the manuscript's
unit-column equation Phi^T d = e_P.
The column of Hom dimensions represented by I satisfies the manuscript's
unit-row equation Phi d = e_I.
The categorical left-mesh defect of a represented Hom column is the Kronecker delta at its representing label. This is the literal opposite unit equation used at Iyama's injective boundary.
A single weight identified with both the source Hom row and the sink Hom
column satisfies the two unit equations in Proposition factor-structure of
the frozen manuscript.
Nonzero maps from P to every chosen indecomposable make its Hom row a
strictly positive integral weight.
Nonzero maps from every chosen indecomposable to I make its Hom column a
strictly positive integral weight.