1629 — The Mixed Fourth Cumulant Requires a Canonical Quantum Gram Companion
Objective
Construct the smallest quantum phase-space positivity object that contains the two fourth moments entering Entry 1627's residual and retains the canonical commutator before taking an associated grade.
Operator basis
Scale the canonical pair by
and define
Use the operator column
For every positive density matrix, its Gram object
is positive semidefinite.
Exact commutator entry
The canonical relation gives
Writing
the Gram matrix is
The imaginary entry is forced; omitting it would forget the quantum normal direction.
Determinant inequality
The Schur complement gives
The real mixed entry contains the Weyl-ordered fourth moment needed by Entry 1627. It is controlled only together with .
Finite unboundedness test
At the fixed lower data
every real lies on the determinant boundary after choosing
The checker verifies 5,670 positive-semidefinite integer packets and 201 such unbounded mixed-moment witnesses.
Narrow result
Positive semidefiniteness of this truncated Gram object is necessary, not sufficient, for extension to a full quantum state.
Architectural consequence
The coefficient object is intrinsically multi-grade and noncommutative:
- the fourth-cumulant coordinate;
- its companion fourth moment;
- the commutator-fixed imaginary extension;
- the lower covariance block.
Projecting to alone destroys the positivity constraint. This is coefficient complexity over the existing labelled carrier, not evidence for a new carrier cell.
Durable artifacts
research/benincasa/checkers/quantum_fourth_moment_gram.rsresearch/benincasa/results/quantum-fourth-moment-gram.jsonresearch/benincasa/quantum-fourth-moment-gram.md
Next falsifier
Test extension of this Gram packet to the full degree-four Weyl moment matrix with basis
Compute whether the Entry 1627 residual functional remains unbounded on fixed covariance fibers after all degree-four commutator and positivity constraints are imposed. If it does, degree-six/eight moments are required; if bounded, derive the sharp bound without fitting.