How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
The free Hopf module over a group algebra
Example
Let be any group, a field, and a -vector space. Write for the vector space of finite formal sums of elements of , with multiplication extended from . Give it the Hopf structure , , and on each . On use the free action and coaction. Then its coinvariants are , , and the inverse decomposition sends to .
Facts & Assumptions
Given: A group , a field , and a -vector space .
A right-right Hopf module has compatibility and coinvariants (Right-right Hopf modules and coinvariants).
The free structure on is and (The free right-right Hopf module on a vector space).
The projection is , and the inverse theorem map is (The coinvariant projection of a right-right Hopf module, The fundamental theorem of right-right Hopf modules).
Verification
Multiplication on is associative and unital because the group multiplication is; on each basis element, and . Coassociativity and both counit identities hold on since and . Finally, , so both antipode equations hold on each basis vector. All structure identities extend by linearity or bilinearity to finite sums, making a Hopf algebra.
Every has finite support and can be written ; the coefficients are unique because applying , where extracts the -coefficient, recovers . If is coinvariant, then . Applying shows for . Conversely is coinvariant, so the coinvariants are exactly .
For and , the free structure gives , while the compatibility right side is . Bilinearity extends this equality to every , so the pair is a Hopf module.
For a basis tensor , . Hence and . Finite-sum linearity gives the formulas on every element; these are the projection and inverse decomposition from [F3].
Depends on
Used by
Nothing in the library uses this result yet.
Dependency tree · two levels
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