Finite string-sum coverage from string detectors #
The finite detector reconstruction writes every finite-dimensional module as a biproduct of coefficient-valued literal string modules. A finite coefficient space is a biproduct of copies of the ground field, so the reconstruction flattens to a finite biproduct of literal string modules.
This is the direct object-coverage input for hook and cohook irreducibility; it does not pass through a separate string-or-band classification theorem.
The multiplicity with which the detector representative i occurs in
the reconstruction of N.
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One label for each literal string copy occurring in the detector reconstruction.
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A numerical enumeration of all literal string copies in the detector reconstruction.
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The literal word carried by a numerical reconstruction-copy label.
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A coefficient-valued reconstruction summand is a finite biproduct of copies of its literal string module.
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The complete reconstruction source is a single finite biproduct of
literal string modules, with nested detector/coefficient indices flattened
and enumerated by a Fin type.
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The detector reconstruction identifies a finite-dimensional module itself with a finite biproduct of literal string modules.
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Every finite-dimensional module is a finite biproduct of literal string modules. This follows directly from the detector reconstruction theorem.
The canonical right-hook projection is irreducible once the finite detector family exists.
The canonical right-cohook inclusion is irreducible once the finite detector family exists.
The canonical left-hook projection is irreducible once the finite detector family exists.
The canonical left-cohook inclusion is irreducible once the finite detector family exists.
A finite complete indecomposable skeleton makes the right-hook projection irreducible, with detector finiteness discharged internally.
A finite complete indecomposable skeleton makes the right-cohook inclusion irreducible, with detector finiteness discharged internally.
A finite complete indecomposable skeleton makes the left-hook projection irreducible, with detector finiteness discharged internally.
A finite complete indecomposable skeleton makes the left-cohook inclusion irreducible, with detector finiteness discharged internally.