OAI/AlgebraicGeometry/StableCoordinate/DeterminantWeights.lean
20 declarations, 0 contain sorry, 0 declared as axioms
Fiber weights on the actual determinant quotient
The Laurent coaction is induced by the exact weights (1,1,-1,-1,0) on
a,d,b,c,u. We establish the final weight contradiction in the actual
quotient ring, not just in an abstract polynomial algebra: an element in
the image of k[a,d,u] with negative fiber weight is zero.
- theorem
OAI.StableCoordinate.DeterminantWeights.relation_fiber_homogeneousline 28Source documentation
The determinant relation is homogeneous of fiber weight zero.
theorem relation_fiber_homogeneous : (relation k).IsWeightedHomogeneous Obstruction.fiberWeight 0 := by … - def
OAI.StableCoordinate.DeterminantWeights.fiberCoactionline 43Source documentation
The genuine fiber-weight coaction on
k[a,d,b,c,u]/(ac-bd-1).def fiberCoaction : C k →ₐ[k] LaurentPolynomial (C k) := …
- theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_generatorline 48 - theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_aline 53 - theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_dline 56 - theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_bline 59 - theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_cline 62 - theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_uline 65 - theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_abline 70Source documentation
The first quadric coordinate
x=abis fixed by fiber scaling.@[simp] theorem fiberCoaction_ab : fiberCoaction k (a k * b k) = AddMonoidAlgebra.single 0 (a k * b k) := by …Mentions: OAI.StableCoordinate.DeterminantWeights.fiberCoaction
- theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_dcline 76Source documentation
The second quadric coordinate
y=dcis fixed by fiber scaling.@[simp] theorem fiberCoaction_dc : fiberCoaction k (d k * c k) = AddMonoidAlgebra.single 0 (d k * c k) := by …Mentions: OAI.StableCoordinate.DeterminantWeights.fiberCoaction
- theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_dbline 82Source documentation
The third quadric coordinate
z=dbis fixed by fiber scaling.@[simp] theorem fiberCoaction_db : fiberCoaction k (d k * b k) = AddMonoidAlgebra.single 0 (d k * b k) := by …Mentions: OAI.StableCoordinate.DeterminantWeights.fiberCoaction
- theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_of_mem_quadric_adjoinline 88Source documentation
Every polynomial in the four base quadric coordinates is fiber-invariant.
theorem fiberCoaction_of_mem_quadric_adjoin {q : C k} (hq : q ∈ Algebra.adjoin k (Set.range ![a k * b k, d k * c k, d k * b k, u k])) : fiberCoaction k q = AddMonoidAlgebra.single 0 q := by …Mentions: OAI.StableCoordinate.DeterminantWeights.fiberCoaction
- theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_mk_of_homogeneousline 102Source documentation
Homogeneous images in the quotient satisfy the corresponding Laurent weight identity.
theorem fiberCoaction_mk_of_homogeneous {p : P k} {n : ℤ} (hp : p.IsWeightedHomogeneous Obstruction.fiberWeight n) : fiberCoaction k (mk k p) = AddMonoidAlgebra.single n (mk k p) := …Mentions: OAI.StableCoordinate.Obstruction.fiberWeight, OAI.StableCoordinate.DeterminantWeights.fiberCoaction
- theorem
OAI.StableCoordinate.DeterminantWeights.fiberCoaction_mem_nonnegative_of_mem_baseRangeline 109Source documentation
Membership in the polynomial subalgebra generated by
a,d,ugives only nonnegative fiber powers.theorem fiberCoaction_mem_nonnegative_of_mem_baseRange {q : C k} (hq : q ∈ (baseMap (k := k)).range) : … - theorem
OAI.StableCoordinate.DeterminantWeights.eq_zero_of_mem_baseRange_of_negative_weightline 127Source documentation
The final rigidity obstruction in the actual determinant quotient, stated directly using its fiber coaction.
theorem eq_zero_of_mem_baseRange_of_negative_weight {q : C k} (hq : q ∈ (baseMap (k := k)).range) {n : ℤ} (hn : n < 0) … - theorem
OAI.StableCoordinate.DeterminantWeights.eq_zero_of_mem_baseRange_of_homogeneous_representativeline 136Source documentation
The same obstruction for the image definition of a homogeneous quotient piece. This is the interface consumed by a quotient grading.
theorem eq_zero_of_mem_baseRange_of_homogeneous_representative {q : C k} (hq : q ∈ (baseMap (k := k)).range) {n : ℤ} (hn : n < 0) … - theorem
OAI.StableCoordinate.DeterminantWeights.no_nonzero_baseRange_weight_neg_twoline 146Source documentation
In particular, the nonzero coefficient of fiber weight
-2required by the source's final step cannot lie ink[a,d,u].theorem no_nonzero_baseRange_weight_neg_two {q : C k} (hq0 : q ≠ 0) (hq : q ∈ (baseMap (k := k)).range) : … - theorem
OAI.StableCoordinate.DeterminantWeights.eq_zero_of_mem_baseRange_of_mem_homogeneous_pieceline 154Source documentation
Image-submodule form of the final obstruction; this matches the standard grading on a quotient by a homogeneous relation.
theorem eq_zero_of_mem_baseRange_of_mem_homogeneous_piece {q : C k} (hq : q ∈ (baseMap (k := k)).range) {n : ℤ} (hn : n < 0) … - theorem
OAI.StableCoordinate.DeterminantWeights.coefficient_weight_neg_twoline 163Source documentation
Both terms of the source coefficient
c*D(b)-b*D(c)have fiber weight-2wheneverDpreserves the fiber weights ofbandc.theorem coefficient_weight_neg_two {r s : C k} (hr : fiberCoaction k r = AddMonoidAlgebra.single (-1) r) (hs : fiberCoaction k s = AddMonoidAlgebra.single (-1) s) : fiberCoaction k (c k * r - b k * s) = AddMonoidAlgebra.single (-2) (c k * r - b k * s) := by …Mentions: OAI.StableCoordinate.DeterminantWeights.fiberCoaction
- theorem
OAI.StableCoordinate.DeterminantWeights.coefficient_eq_zero_of_mem_baseRangeline 175Source documentation
Final coefficient vanishing, ready to combine with the determinant coefficient's nonvanishing for a nonzero derivation.
theorem coefficient_eq_zero_of_mem_baseRange {r s : C k} (hr : fiberCoaction k r = AddMonoidAlgebra.single (-1) r) (hs : fiberCoaction k s = AddMonoidAlgebra.single (-1) s) (hq : c k * r - b k * s ∈ (baseMap (k := k)).range) : …Mentions: OAI.StableCoordinate.DeterminantWeights.fiberCoaction