Kollár's Example 106, the order-2 run continues: the blow-ups of q and of q' #
In [Kol07, Example 106], after the blow-up of the origin the transform I₁ on the z-chart,
I₁ = (x₁³z₁ − y₁², z₁(x₁⁴z₁ + x₁ − w₁³)), has order 2 at the origin q ∈ E₁ of that chart
(HironakaExamples/MaximalContact/Example106Charts.lean), against Kollár's sentence "the order has
dropped to 1", which holds on his x-chart only. This file follows the order-2 run two stages
further, computed exactly in ℚ:
- blowing up
q, thex₂-,y₂- andz₂-charts have no point of order2, while on thew₂-chartI₂ = (x₂³z₂w₂² − y₂², z₂(x₂⁴z₂w₂⁴ + x₂ − w₂²))has order exactly2at its originq', its onlyℚ-point of order2, which lies on the strict transformsH₂ = (y₂)andH₂' = (y₂ − x₂²z₂w₂²)(y₂,y₂ − x₂²z₂w₂² ∈ MC(I₂)); - blowing up
q', again only thew₃-chart has a point of order2, its origin, forI₃ = (x₃³z₃w₃⁴ − y₃², z₃(x₃⁴z₃w₃⁸ + x₃ − w₃)), insideH₃ = (y₃)andH₃' = (y₃ − x₃²z₃w₃⁴).
So the order-2 run of Example 106 continues for at least three stages; its length is not
computed here. The ℚ-point arguments read the value and the first partials of the generators at
the point (vanish_of_mem_m4_sq).
The blow-up of q: the x₂-, y₂-, z₂-charts are empty #
The marked transforms of the generators of I₁ on the x₂-chart.
No point of order 2 on the x₂-chart: ∂(x₂²z₂ − y₂²)/∂y₂ = −2y₂ and ∂/∂z₂ = x₂² force
x₂ = y₂ = 0, and then ∂(z₂(x₂⁴z₂ + 1 − w₂³x₂²))/∂z₂ = 1.
The marked transforms on the y₂-chart.
No point of order 2 on the y₂-chart: x₂³y₂²z₂ = 1 and ∂/∂y₂ = 2x₂³y₂z₂ = 0 are
incompatible.
The marked transforms on the z₂-chart.
No point of order 2 on the z₂-chart: ∂(x₂⁴z₂⁴ + x₂ − w₂³z₂²)/∂x₂ = 4x₂³z₂⁴ + 1 and
∂(x₂³z₂² − y₂²)/∂z₂ = 2x₂³z₂ are incompatible.
The blow-up of q: the w₂-chart carries the point q' of order 2 #
The marked transforms on the w₂-chart and the strict transforms of H₁, H₁'.
I₂ has order exactly 2 at its origin q'.
Every ℚ-point of order ≥ 2 on the w₂-chart is its origin: ∂/∂y₂ = −2y₂,
∂(x₂³z₂w₂² − y₂²)/∂z₂ = x₂³w₂², and the partials of the second generator finish the two cases
x₂ = 0, w₂ = 0.
q' ∈ H₂: y₂ ∈ MC(I₂).
q' ∈ H₂': y₂ − x₂²z₂w₂² ∈ MC(I₂), with ∂(x₂³z₂w₂² − y₂²)/∂x₂ = 3x₂²z₂w₂².
The blow-up of q': three empty charts and the w₃-chart #
The marked transforms of the generators of I₂ on the x₃-chart.
No point of order 2 on the x₃-chart: ∂(x₃⁴z₃w₃² − y₃²)/∂z₃ = x₃⁴w₃² forces x₃ = 0 or
w₃ = 0, and then ∂(z₃(x₃⁸z₃w₃⁴ + 1 − w₃²x₃))/∂z₃ = 1.
The marked transforms on the y₃-chart.
No point of order 2 on the y₃-chart: x₃³y₃⁴z₃w₃² = 1 and ∂/∂y₃ = 4x₃³y₃³z₃w₃² = 0 are
incompatible.
The marked transforms on the z₃-chart.
No point of order 2 on the z₃-chart: ∂(x₃⁴z₃⁸w₃⁴ + x₃ − w₃²z₃)/∂x₃ = 4x₃³z₃⁸w₃⁴ + 1 and
∂(x₃³z₃⁴w₃² − y₃²)/∂z₃ = 4x₃³z₃³w₃² are incompatible.
The marked transforms on the w₃-chart and the strict transforms of H₂, H₂'.
I₃ has order exactly 2 at its origin.
Every ℚ-point of order ≥ 2 on the w₃-chart is its origin:
∂(x₃³z₃w₃⁴ − y₃²)/∂z₃ = x₃³w₃⁴ splits the cases x₃ = 0 and w₃ = 0, which
∂(z₃(x₃⁴z₃w₃⁸ + x₃ − w₃))/∂x₃ = 4x₃³z₃²w₃⁸ + z₃ and ∂/∂z₃ = 2x₃⁴z₃w₃⁸ + x₃ − w₃ finish.
The origin of the w₃-chart lies on H₃: y₃ ∈ MC(I₃).
The origin of the w₃-chart lies on H₃': y₃ − x₃²z₃w₃⁴ ∈ MC(I₃).