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Affine algebraic curves with zero Euler characteristics

Oberwolfach, 2007

Maciej Borodzik, Henryk ˙Zoł ˛adek

Institute of Mathematics, University of Warsaw

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Problem

Curve C ⊂ C2.

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Problem

Curve C ⊂ C2.

C ⊂ CP¯ 2 its closure.

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Problem

Curve C ⊂ C2.

C ⊂ CP¯ 2 its closure.

C is rational.¯

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Problem

Curve C ⊂ C2.

C ⊂ CP¯ 2 its closure.

C is rational.¯

χ(C) = 0.

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Problem

Curve C ⊂ C2.

C ⊂ CP¯ 2 its closure.

C is rational.¯

χ(C) = 0.

It follows, that either

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Problem

Curve C ⊂ C2.

C ⊂ CP¯ 2 its closure.

C is rational.¯

χ(C) = 0.

It follows, that either

• C ≃ C and C has no finite self–intersections.

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Problem

Curve C ⊂ C2.

C ⊂ CP¯ 2 its closure.

C is rational.¯

χ(C) = 0.

It follows, that either

• C ≃ C and C has no finite self–intersections.

• C has one place at infinity and one finite self–intersection.

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Known results

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Known results

If χ(C) = 1, then C is homeomorphic to a line.

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Known results

If χ(C) = 1, then C is homeomorphic to a line.

Zajdenberg–Lin theorem: C ≃ {xp = yq} with p, q coprime.

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Known results

If χ(C) = 1, then C is homeomorphic to a line.

Zajdenberg–Lin theorem: C ≃ {xp = yq} with p, q coprime.

Koras, Russell case C ≃ C and C smooth.

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Our result

It is restricted to regular curves.

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Our result

It is restricted to regular curves.

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Our result

It is restricted to regular curves.

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Our result

It is restricted to regular curves.

Conjecture: All curves are regular.

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Our result

It is restricted to regular curves.

Conjecture: All curves are regular.

Lots of evidence.

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Our result

It is restricted to regular curves.

Conjecture: All curves are regular.

Lots of evidence.

A gap in the proof.

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Two points of view

Equation

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

Parametrisation

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

Parametrisation

C = {(x(t), y(t)) ∈ C2,t ∈ CP1}

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

Parametrisation

C = {(x(t), y(t)) ∈ C2,t ∈ CP1}

genus is zero.

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

Parametrisation

C = {(x(t), y(t)) ∈ C2,t ∈ CP1}

genus is zero.

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

Parametrisation

C = {(x(t), y(t)) ∈ C2,t ∈ CP1}

genus is zero.

Singular points: x(t0) = y(t0) = 0

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Two points of view

Equation

C = {(x, y) ∈ C2 : f (x, y) = 0}

Genus is difficult.

Singular points fx (x0, y0) = fy(x0, y0) = 0

Self–intersections are singular points.

Parametrisation

C = {(x(t), y(t)) ∈ C2,t ∈ CP1}

genus is zero.

Singular points: x(t0) = y(t0) = 0

Self–intersections are difficult.

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Parametric curves

Rational curve C with one place at infinity is given by a polynomial

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Parametric curves

Rational curve C with one place at infinity is given by a polynomial

x(t) = ta + α1ta−1 + · · · + αa y(t) = tc + β1tc−1 + · · · + βc.

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Parametric curves

Rational curve C with one place at infinity is given by a polynomial

x(t) = ta + α1ta−1 + · · · + αa y(t) = tc + β1tc−1 + · · · + βc.

Any rational C with two branches at infinity is given by a polynomial in t and t−1.

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Parametric curves

Rational curve C with one place at infinity is given by a polynomial

x(t) = ta + α1ta−1 + · · · + αa y(t) = tc + β1tc−1 + · · · + βc.

Any rational C with two branches at infinity is given by a polynomial in t and t−1.

so

x(t) = ta + α1ta−1 + · · · + αa+bt−b y(t) = tc + β1tc−1 + · · · + βc+dt−d.

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δ invariant

For singular point with Milnor number µ and r branches set

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δ invariant

For singular point with Milnor number µ and r branches set

2δ = µ + r − 1.

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δ invariant

For singular point with Milnor number µ and r branches set

2δ = µ + r − 1.

If (x0, y0) is a singular point of (x(t), y(t)),

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δ invariant

For singular point with Milnor number µ and r branches set

2δ = µ + r − 1.

If (x0, y0) is a singular point of (x(t), y(t)), 2δ is the number of solutions to

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δ invariant

For singular point with Milnor number µ and r branches set

2δ = µ + r − 1.

If (x0, y0) is a singular point of (x(t), y(t)), 2δ is the number of solutions to

(x(s

1)−x(s2)

s1−s2 = 0

y(s1)−y(s2)

s1−s2 = 0 such that x(s1) = x0 i y(s1) = y0.

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δ invariant

For singular point with Milnor number µ and r branches set

2δ = µ + r − 1.

If (x0, y0) is a singular point of (x(t), y(t)), 2δ is the number of solutions to

double point equation

(x(s

1)−x(s2)

s1−s2 = 0

y(s1)−y(s2)

s1−s2 = 0 such that x(s1) = x0 i y(s1) = y0.

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δ invariant

For singular point with Milnor number µ and r branches set

2δ = µ + r − 1.

If (x0, y0) is a singular point of (x(t), y(t)), 2δ is the number of solutions to

(x(s

1)−x(s2)

s1−s2 = 0

y(s1)−y(s2)

s1−s2 = 0 such that x(s1) = x0 i y(s1) = y0.

For an ordinary double point we have 2δ = 2.

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Example

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Example

y2 = x3 + λx2,

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Example

y2 = x3 + λx2, λ = 2.

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Example

y2 = x3 + λx2, λ = 1.

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Example

y2 = x3 + λx2, λ = 12.

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Example

y2 = x3 + λx2, λ = 0.

One double point „hides” in a singular point. 2δ = 2.

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t,

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 1

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.99

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.98

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.97

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.96

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.95

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.94

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.93

(56)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.92

(57)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.91

(58)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.89

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.87

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.85

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.83

(62)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.81

(63)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.79

(64)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.75

(65)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.7

(66)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.65

(67)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.6

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.55

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.5

(70)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.45

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Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0.4

(72)

Another example

Curves depend on λ.

xλ(t) = t3 − 15λ2t

yλ(t) = t5 − 30λ2t3 + 10λ3t2 + 201λ4t, λ = 0

Four double points hide in a singular point (t3, t5).

Thus 2δ = 8.

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Serre formula

For a curve C of degree d we have

(74)

Serre formula

For a curve C of degree d we have g = (d − 1)(d − 2)

2 − P

δi

(75)

Serre formula

For a curve C of degree d we have g = (d − 1)(d − 2)

2 − P

δi g — genus.

(76)

Serre formula

For a curve C of degree d we have g = (d − 1)(d − 2)

2 − P

δi g — genus.

d — degree.

(77)

Serre formula

For a curve C of degree d we have g = (d − 1)(d − 2)

2 − P

δi g — genus.

d — degree.

δi — δ invariant of a singular point.

(78)

Serre formula

For a curve C of degree d we have g = (d − 1)(d − 2)

2 − P

δi g — genus.

d — degree.

δi — δ invariant of a singular point.

P — sum over all singular points and double points.

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Serre formula II

We require g = 0. Thus

X 2δi = (d − 1)(d − 2).

(80)

Serre formula II

We require g = 0. Thus

X 2δi = (d − 1)(d − 2).

For a typical curve δi correspond to ordinary double points.

(81)

Serre formula II

We require g = 0. Thus

X 2δi = (d − 1)(d − 2).

For a typical curve δi correspond to ordinary double points.

If C has no finite double points (or only one), all other points must be hidden in singular points.

(82)

Serre formula II

We require g = 0. Thus

X 2δi = (d − 1)(d − 2).

For a typical curve δi correspond to ordinary double points.

If C has no finite double points (or only one), all other points must be hidden in singular points.

Maybe at infinity.

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Codimension of a singular point.

To control the deformations of a parametric curves we introduce

(84)

Codimension of a singular point.

To control the deformations of a parametric curves we introduce the codimension.

(85)

Codimension of a singular point.

To control the deformations of a parametric curves we introduce the codimension.

Strongly resembles ¯M number of Orevkov.

(86)

Codimension of a singular point.

To control the deformations of a parametric curves we introduce the codimension.

Parametrise locally x(t) ∼ tp, y(t) ∼ tq + . . . . Write y = c1x1/p + c2x2/p + · · · + cixi/p + . . . .

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Codimension of a singular point.

To control the deformations of a parametric curves we introduce the codimension.

Parametrise locally x(t) ∼ tp, y(t) ∼ tq + . . . . Write y = c1x1/p + c2x2/p + · · · + cixi/p + . . . .

c1, c2, . . . , ci, . . . — Puiseux coefficients

(88)

Codimension of a singular point.

To control the deformations of a parametric curves we introduce the codimension.

Parametrise locally x(t) ∼ tp, y(t) ∼ tq + . . . . Write y = c1x1/p + c2x2/p + · · · + cixi/p + . . . .

c1, c2, . . . , ci, . . . — Puiseux coefficients

The local codimension ν is the number of vanishing essential Puiseux coefficients.

(89)

Codimension of a singular point.

To control the deformations of a parametric curves we introduce the codimension.

Parametrise locally x(t) ∼ tp, y(t) ∼ tq + . . . . Write y = c1x1/p + c2x2/p + · · · + cixi/p + . . . .

c1, c2, . . . , ci, . . . — Puiseux coefficients

The local codimension ν is the number of vanishing essential Puiseux coefficients.

ν is determined by the characteristic sequence and the order p.

(90)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

(91)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

(92)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

where µ Milnor number (= 2δ),

(93)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

where µ Milnor number (= 2δ), ν the local codimension

(94)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

where µ Milnor number (= 2δ), ν the local codimension

(95)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

where µ Milnor number (= 2δ), ν the local codimension

One can find all cases with an equality.

(96)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

where µ Milnor number (= 2δ), ν the local codimension

One can find all cases with an equality.

Direct calculations.

(97)

Codimension inequality

If x(t) ∼ tp, y(t) ∼ tq we have:

µ ≤ pν.

where µ Milnor number (= 2δ), ν the local codimension

One can find all cases with an equality.

Direct calculations.

Resembles Zajdenberg–Orevkov inequality.

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Example

x = t4,

y = 2t4 + t6 + 2t8 + t9

(99)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t9

y = 2x4/4 + x6/4 + 2x8/4 + x9/4.

(100)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t9 y = 2x + x3/2 + 2x2 + x9/4. c1 = c2 = c3 = c5 = c7 = 0.

(101)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t9 y = 2x + x3/2 + 2x2 + x9/4. c1 = c2 = c3 = c5 = c7 = 0.

Hence ν = 5. Also

µ = 15 + 3 = 18 ≤ 4 · 5

(102)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t9 y = 2x + x3/2 + 2x2 + x9/4. c1 = c2 = c3 = c5 = c7 = 0.

Hence ν = 5. Also

µ = 15 + 3 = 18 ≤ 4 · 5 Change 9 to 13.

(103)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t13 y = 2x + x3/2 + 2x2 + x13/4. c1 = c2 = c3 = c5 = c7 = 0.

Hence ν = 5. Also

µ = 15 + 3 = 18 ≤ 4 · 5

(104)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t13 y = 2x + x3/2 + 2x2 + x13/4. c1 = c2 = c3 = c5 = c7 = c9 = c11 = 0.

Now ν = 7. And

µ = 15 + 7 = 22 ≤ 4 · 7

(105)

Example

x = t4,

y = 2t4 + t6 + 2t8 + t13 y = 2x + x3/2 + 2x2 + x13/4. c1 = c2 = c3 = c5 = c7 = c9 = c11 = 0.

Now ν = 7. And

µ = 15 + 7 = 22 ≤ 4 · 7

The more complicated singularity, the less sharp is the inequality.

(106)

Tangent codimension

Two branches at a singular point

y = c1x1/p1 + c2x2/p1 + · · · + ckxk/p1 + . . . y = d1x1/p2 + d2x2/p2 + · · · + dlxl/p2 + . . . .

(107)

Tangent codimension

Two branches at a singular point

y = c1x1/p1 + c2x2/p1 + · · · + ckxk/p1 + . . . y = d1x1/p2 + d2x2/p2 + · · · + dlxl/p2 + . . . .

The singularity is decribed by

(108)

Tangent codimension

Two branches at a singular point

y = c1x1/p1 + c2x2/p1 + · · · + ckxk/p1 + . . . y = d1x1/p2 + d2x2/p2 + · · · + dlxl/p2 + . . . .

The singularity is decribed by

— vanishing of ν1 c’s, ν2, d’s

(109)

Tangent codimension

Two branches at a singular point

y = c1x1/p1 + c2x2/p1 + · · · + ckxk/p1 + . . . y = d1x1/p2 + d2x2/p2 + · · · + dlxl/p2 + . . . .

The singularity is decribed by

— vanishing of ν1 c’s, ν2, d’s

— and possibly some equality relations between non–vanishing c’s and d’s.

(110)

Tangent codimension

Two branches at a singular point

y = c1x1/p1 + c2x2/p1 + · · · + ckxk/p1 + . . . y = d1x1/p2 + d2x2/p2 + · · · + dlxl/p2 + . . . .

The singularity is decribed by

— vanishing of ν1 c’s, ν2, d’s

— and possibly some equality relations between non–vanishing c’s and d’s.

number of these relation νtan: the tangent codimension.

(111)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22

(112)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 Consider Puiseux expansion

(113)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6.

(114)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6.

(115)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6.

• The sign change results from chosing different root of unity of order 6.

(116)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6. Here terms at x, x2, x5/2, x3 agree.

(117)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6.

In other words, c4 = d6, c8 = d12, c10 = d15 and c12 = d18.

(118)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6. νtan = 4

(119)

Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6. Note, that c14 6= d21

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Example

Branch I x = t4

y = t8 + 3t10 + 2t14 + 5t15 Branch II x = u6

y = u12−3u15+2u21 + 3t22 y =x2 + 3x5/2 + 2x7/2 + 5x15/4

y =x2+3x5/2−2x7/2 + 4x22/6. Note, that c14 6= d21

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Codimension inequality II.

Two branches.

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

νtan — tangent codimension.

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

νtan — tangent codimension.

2δ ≤ (p1 + p2)(ν1 + ν2 + νtan + 1).

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

νtan — tangent codimension.

2δ ≤ (p1 + p2)(ν1 + ν2 + νtan+1).

This +1 is very inconvenient. We can get rid of it almost all cases.

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

νtan — tangent codimension.

2δ ≤ (p1 + p2)(ν1 + ν2 + νtan + 1).

Assume q1 and q2 are orders of y.

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

νtan — tangent codimension.

2δ ≤ (p1 + p2)(ν1 + ν2 + νtan + 1).

Assume q1 and q2 are orders of y.

For q2p1 6= q1p2, the intersection index of branches is fixed:

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Codimension inequality II.

Two branches.

p1, p2 — orders of x.

ν1, ν2 — local codimensions.

νtan — tangent codimension.

2δ ≤ (p1 + p2)(ν1 + ν2 + νtan + 1).

Assume q1 and q2 are orders of y.

For q2p1 6= q1p2, the intersection index of branches is fixed:

it equals min(q1p2, q2p1) — leads to better estimate.

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External codimension

For the singularity with one branch

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

The subspace of curves with such singularity in the space curves x = tp + · · · + a0,

y = tq + b1tq−1 + . . . for p, q sufficiently large has codimension ext ν.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

If we swap x with y, the codimension may change.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

For x = t4, y = t8 + t9, we have ext ν = 8. For x = t8 + t9, y = t4 we have ext ν = 9.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

The codimension is minimal if ord x =multiplicity.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

If we have 2 branches with ext ν1, ext ν2, ext ν = ext ν1 + ext ν2 + νtan(12) + 2.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

If we have 2 branches with ext ν1, ext ν2, ext ν = ext ν1 + ext ν2 + νtan(12) + 2.

Additional 2 comes from the condition x(t0) = x(t1), y(t0) = y(t1).

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

If we have 2 branches with ext ν1, ext ν2, ext ν = ext ν1 + ext ν2 + νtan(12) + 2.

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External codimension

For the singularity with one branch ext ν = ν + p − 2.

We have p − 1 condition on x, ν on y and can move parameter t.

If we have 2 branches with ext ν1, ext ν2, ext ν = ext ν1 + ext ν2 + νtan(12) + 2.

Definition for more branches is similar.

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External codimension II

Setup

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0. E the reduced exceptional divisor.

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

K is the projection of the canonical divisor onto the subgroup of P ic( ˜X) ⊗ Q spanned by

components of E.

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

D = ˜C + E.

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

D = ˜C + E.

Let ¯M = K(K + D): modified Orevkov ¯M number.

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

D = ˜C + E.

Let ¯M = K(K + D): modified Orevkov ¯M number.

In fact ¯M = K(K + D) + # branches − 1.

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

D = ˜C + E.

Let ¯M = K(K + D): modified Orevkov ¯M number.

Proposition. For a given singular curve C ⊂ C2, if orders of x at C all branches are multiplicities, then

ext ν = K(K + D).

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External codimension II

Setup

(C, x0) is a curve on a surface X.

C ⊂ ˜˜ X resolution of singular point x0.

D = ˜C + E.

Let ¯M = K(K + D): modified Orevkov ¯M number.

Proposition. For a given singular curve C ⊂ C2, if orders of x at C all branches are multiplicities, then

ext ν = K(K + D).

The proof follows from calculating both quantities in terms of Eisenbud–Neumann diagrams.

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Regularity I

Space Cura,c of curves with one place at infitity

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Regularity I

Space Cura,c of curves with one place at infitity

x = ta + α1ta−1 + α2ta−2 + · · · + αa y = tc + β1tc−1 + · · · + βc

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Regularity I

Space Cura,c of curves with one place at infitity has dimension a + c.

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Regularity I

Space Cura,c of curves with one place at infitity has dimension a + c.

Space Curva,b,c,d of curves with two branches at infinity

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Regularity I

Space Cura,c of curves with one place at infitity has dimension a + c.

Space Curva,b,c,d of curves with two branches at infinity

x = ta + α1ta−1 + α2ta−2 + · · · + αa+bt−b y = tc + β1tc−1 + · · · + βc+dt−d

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Regularity I

Space Cura,c of curves with one place at infitity has dimension a + c.

Space Curva,b,c,d of curves with two branches at infinity has dimension a + b + c + d.

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Regularity I

Space Cura,c of curves with one place at infitity has dimension a + c.

Space Curva,b,c,d of curves with two branches at infinity has dimension a + b + c + d.

a, b, c and d need not be positive. We will discuss it later.

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