The example states of the monomial procedure #
Concrete states of Hironaka/Resolution/Algebraic/Monomial/State.lean on which the procedure of
[Kol07, 111, Step 3] is computed, and the maximal-multiplicity procedure that
[Kol07, Example 112] refutes. The computations themselves are in
HironakaExamples/Monomial/Example112.lean (which is imported by the root) and in
HironakaExamples/MonomialState.lean and HironakaExamples/MonomialRestrict.lean.
example112 m hm: the surface of [Kol07, Example 112], two curvesE¹, E²meeting at one point, both with exponentm + 1.maxMultChoice,maxMultRun,maxMultFaces,example112OtherPath: the maximal-multiplicity procedure that Kollár dismisses at the start of Step 3 (blow up the locus of highest multiplicity; "this, however, does not work, not even for surfaces"). It is defined here only to be computed against, not used by the procedure: the faces of maximal sum≥ m(maxMultFaces), with the lexicographically largest label tuple as the tie-break (Kollár'sE² ∩ E³); the centres of the other tie-break, which gives the same exponents by symmetry, are listed asexample112OtherPath.threePhase:n = 3,m = 8, one component per label, exponents4, 9, 3, 6, maximal faces{0}and{1, 2, 3}, an instance in which all three phases act.splitX,splitU: the example showing why the components of a member must carry their own exponents (the deviation recorded inHironaka/Resolution/Algebraic/Monomial/State.lean), in its fine, labelled form: the four linesV(x), V(x-1)(label0),V(y), V(y-1)(label1) of𝔸²with the exponents1, 0, 1, 0ofI = (xy),m = 1, onX = 𝔸²and onU = D((x-1)(y-1));coarseX,coarseU: the same example with one exponent per member, the minimum over its components, as the members of [Kol07, Definition–Lemma 110] are printed (not assumed irreducible): exponents0, 0onXand1, 1onU. Not in the sources.
Example 112 #
The surface of [Kol07, Example 112]: E¹, E² two curves intersecting at a point with
a₁ = a₂ = m + 1, as a state with components 0, 1 (labels 0, 1, the curves E¹, E²), nerve
{0}, {1}, {0, 1}, exponents m + 1, n = 2.
Equations
Instances For
The maximal-multiplicity choice ([Kol07, 111, Step 3], the "usual method" that Kollár
rejects), defined for the computations only: the faces of maximal sum ≥ m, with the
lexicographically largest label tuple as the tie-break (Kollár's E² ∩ E³ in Example 112; the
other tie-break gives the same exponents by symmetry).
Equations
- One or more equations did not get rendered due to their size.
Instances For
k steps of the maximal-multiplicity procedure: the final state and the list of centres, in
order.
Equations
Instances For
The maximal-multiplicity locus before the tie-break: the faces of maximal sum ≥ m
(Kollár's "highest multiplicity locus"); maxMultChoice is its tie-break.
Equations
Instances For
The centres of six steps of the maximal-multiplicity procedure on Example 112 under the
other tie-break (the lexicographically smallest label tuple): the point {0, 1}, then {0, 2}
(Kollár's E¹ ∩ E³ instead of E² ∩ E³), then the unique maximizers {2, 3}, {3, 4},
{4, 5}, {5, 6}; the exponents come out the same by symmetry.
Equations
Instances For
The three-phase instance #
An instance in which all three phases act: n = 3, m = 8, one component per label,
exponents 4, 9, 3, 6, maximal faces {0} and {1, 2, 3}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The split example #
The fine split of the boundary E¹ = V(x(x-1)), E² = V(y(y-1)) of 𝔸²: the four lines
V(x), V(x-1) (label 0) and V(y), V(y-1) (label 1) with the exponents 1, 0, 1, 0 of
I = (xy) along them, m = 1; the nerve is the four double points.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The same on U = D((x-1)(y-1)): the components 1, 3 (V(x-1), V(y-1)) are dead, the
nerve is {0}, {2}, {0, 2}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The coarse split, one exponent per member as in [Kol07, Definition–Lemma 110] with members
not assumed irreducible: on X = 𝔸², E¹ = V(x(x-1)), E² = V(y(y-1)) with the coarse exponents
c_j = min_D ord_D (xy) = 0, 0; m = 1; nerve {0}, {1}, {0, 1}.
Equations
Instances For
The coarse split on U = D((x-1)(y-1)): E¹|_U = V(x) and E²|_U = V(y) are irreducible,
so the coarse exponents are 1, 1.