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HironakaExamples.MaximalContact.Example106Stages

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:

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 #

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.

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 #

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 − x₂²z₂w₂² ∈ MC(I₂), with ∂(x₂³z₂w₂² − y₂²)/∂x₂ = 3x₂²z₂w₂².

The blow-up of q': three empty charts and the w₃-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.

No point of order 2 on the z₃-chart: ∂(x₃⁴z₃⁸w₃⁴ + x₃ − w₃²z₃)/∂x₃ = 4x₃³z₃⁸w₃⁴ + 1 and ∂(x₃³z₃⁴w₃² − y₃²)/∂z₃ = 4x₃³z₃³w₃² are incompatible.

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.