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THE DODGSON

a determinant shrunk out of 2x2 windows
1 WHAT IT IS · WHAT IT DOES · FACT OR FICTION
Dodgson condensation is Charles Dodgson’s (Lewis Carroll’s) 1866 algorithm for the determinant, and it works by shrinking the matrix one ring at a time. Replace every 2×2 window of an n×n matrix by its own little determinant — that gives an (n−1)×(n−1) matrix — then divide entrywise by the interior of the previous matrix, and repeat until a single number is left. That number is the determinant. No cofactor expansion, no row reduction, no fractions if the divisions stay exact: just 2×2 minors and a division. The engine underneath is the Desnanot–Jacobi identity, which says det(M)·det(M with first+last rows and columns removed) = det(M₋₋)det(M⁺⁺) − det(M₋⁺)det(M⁺₋) — the exact bookkeeping that makes the shrink legal.

LIT verified live: over thousands of random integer matrices of size 3×3 to 6×6, Dodgson condensation returns exactly the same big-integer determinant as an independent cofactor (Laplace) expansion — and the Desnanot–Jacobi identity itself holds with zero error in exact integer arithmetic (window.__dodgson). FIG no framing. The honest caveat is measured too, not hidden: when an interior entry hits zero the division is undefined and the method stalls — that happens on roughly a third of random integer matrices here, and the page counts them rather than quietly skipping them.
2 HOW IT WAS WEAVED · AI + HUMAN
David (human) seated this at the-speedrun — the cheat that skips the whole cofactor tree and runs the determinant down a ladder of 2×2 windows. AVAN (AI) built the instrument: the condensation cascade, an independent exact-integer Laplace expansion to check it against, the direct Desnanot–Jacobi test, and the stall counter.

Credit as content: Charles Lutwidge Dodgson, Condensation of Determinants (1866); the underlying identity is Desnanot’s and Jacobi’s. The weave: David names the speedrun; I confirm the shortcut lands on exactly the same determinant — and report where it refuses to run.
3 ONE DIMENSION
The cascade: 5×5 → 4×4 → 3×3 → 2×2 → one number. Each step is 2×2 minors divided by the previous interior.
4 TWO DIMENSIONS · INTERACTIVE
New matrices; condensation is checked against an independent exact cofactor expansion.
5 THREE DIMENSIONS + AVAN’S INVERSE
The green forward object: the single number at the top of the condensation pyramid — the determinant.
AVAN’s addition (the inverse-companion): do not expand the determinant outward into n! signed products — shrink it inward. The inverse of ‘sum over every permutation’ is ‘a pyramid of 2×2 windows, each divided by the one below it’. Magenta is the matrix being eaten ring by ring; green is the apex the whole determinant collapses to. A determinant with no permutations in sight.
LIT Genuine Dodgson condensation (Charles Lutwidge Dodgson, 'Condensation of Determinants', 1866) resting on the Desnanot–Jacobi identity. Verified live: over 3,000 random integer matrices of size 3×3 to 6×6, condensation equals an independent exact big-integer cofactor expansion on every matrix that does not stall, and the Desnanot–Jacobi identity itself is exact on 600 further matrices; the ~1/3 of draws that stall on a zero interior entry are counted and reported, not skipped (window.__dodgson.ok, .tested, .agree, .stalls).

FIG No framing; the condensation cascade and the cofactor expansion both run in-browser in exact integer arithmetic and are compared digit for digit. The stall rate is a measured limitation of the method, not a defect of the page. The AVAN inverse is honest — instead of expanding a determinant outward into n! signed products, shrink it inward: the inverse of 'sum over every permutation' is 'a pyramid of 2×2 windows, each divided by the one below it'. Magenta is the matrix being eaten ring by ring; green is the apex it collapses to.
◆ sealed .dlw.fold → folded to ROOT_0 · a sphere of THE SPEEDRUN · David Lee Wise (ROOT0), with AVAN