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On the double tangent of projective closed curves

Thomas Blomme thomas.blomme@unige.ch Université de Neuchâtel, rue Émile Argan 11, Neuchâtel 2000, Switzerland
Abstract

We generalize a previous result by Fabricius-Bjerre [FB62] from curves in 2\mathbb{R}^{2} to curves in P2\mathbb{R}P^{2}. Applied to the case of real algebraic curves, this recovers the signed count of bitangents of quartics introduced by Larson-Vogt [LV21] and proves its positivity, conjectured by Larson-Vogt. Our method is not specific to quartics and applies to algebraic curves of any degree.

:
14N10
keywords:
Enumerative geometry, bitangents, plane algebraic curves

1 Introduction

We consider curves in 2\mathbb{R}^{2} and P2\mathbb{R}P^{2}. By curve we mean a closed immersed C1C^{1} curve which is the union of finitely many strictly convex arcs. Such a curve has a finite number of flexes (points where the curve passes through its tangent), nodes (also called double points or self-intersection) and double tangents, also called bitangents, which are lines tangent at two points of the curve. Throughout the paper, we assume all our curves to be generic in the sense that double points are simple, no tangent at a flex is tangent elsewhere, and a double tangent has only two tangency points. The normalization of the curve (desingularizing the double points) may not be connected, and its connected components are called components of the curve.

In 1962, Fabricius-Bjerre [FB62] introduced a signed count of bitangents for such curves in 2\mathbb{R}^{2}. Let C2C\subset\mathbb{R}^{2} be a curve and DD be a bitangent to CC. There are two types of bitangents according to the relative position of the curve near the tangency points (See Figure 1):

  • \circ

    exterior (type TT) if the arcs of CC near the tangency points lie on the same side of DD,

  • \circ

    interior (type SS) if the arcs of CC near the tangency points lie on opposite sides of DD.

The Fabricius-Bjerre sign of a bitangent is ++ for type TT and - for type SS. If CC has i(C)i(C) flexes and n(C)n(C) self-intersections, Fabricius-Bjerre [FB62] states that the signed count σ(C)\sigma(C) of bitangents satisfies

σ(C)=n(C)+i(C)2.\sigma(C)=n(C)+\frac{i(C)}{2}.

Although the proof of [FB62] seems to assume the curve has only one component, such an assumption is actually not necessary.

(T)(T), exterior bitangent, ++ (S)(S), interior bitangent, -
Figure 1: Types of bitangents

Our main result is to provide a generalization of the Fabricius-Bjerre count to the projective setting. To extend the sign definition, we choose a line LP2L_{\infty}\subset\mathbb{R}P^{2} and consider curves generically transverse to LL_{\infty}: no line passing through a point of CLC\cap L_{\infty} is a bitangent or tangent at a flex, which means LL_{\infty} is transverse to CC union its bitangents and tangent at flexes. Let 𝒯(C)\mathscr{T}_{\infty}(C) be the set of tangents to CC at points of CLC\cap L_{\infty}. As P2\L=2\mathbb{R}P^{2}\backslash L_{\infty}=\mathbb{R}^{2}, we choose as sign for the bitangents the well-defined Fabricius-Bjerre sign in this affine chart. Notice it depends on the choice of LL_{\infty}.

Theorem.

3.2 Let CC a curve in P2\mathbb{R}P^{2} transverse to LL_{\infty} with i(C)i(C) flexes, n(C)n(C) nodes and aa intersection points with LL_{\infty}. Then, we have the following signed count of bitangents:

σ(C)=n(C)+i(C)2+a(a2)2T𝒯(C)(|CT|1).\sigma(C)=n(C)+\frac{i(C)}{2}+\frac{a(a-2)}{2}-\sum_{T\in\mathscr{T}_{\infty}(C)}(|C\cap T|-1).

The case of [FB62] corresponds to curve such that CL=C\cap L_{\infty}=\emptyset (i.e. a=0a=0).

If 𝒞\mathscr{C} is a real algebraic curve, Plücker [Plü34, Plü39] already knew the number of complex bitangents, which only depends on the degree. However, the number of real bitangents depends on the curve. One may hope that there exists some suitable signed counts of the bitangents that is to some extent invariant. In [BBG24], Blomme-Brugallé-Garay proved the existence of a signed count only depending on the topology of the real part for curves of even degree. Prior to the latter, Larson-Vogt proved the existence of a different signed count for quartics, with some conjectures concerning so-called quadratic enrichment to more general fields. The Fabricius-Bjerre sign actually coincides with the Larson-Vogt sign [LV21] used to count real bitangents to a real quartic curve.

In the real algebraic setting, bitangents can be split or non-split according to whether the tangency points are real or complex conjugate. Given a smooth curve 𝒞\mathscr{C}, Klein’s formula [Kle76] provides a relation between the number of non-split bitangents t0(𝒞)t_{0}(\mathscr{C}) and the number of real flexes. It is possible to apply Theorem 3.2 coupled to Klein’s formula to a real algebraic curve transverse to a line LL_{\infty} and get a signed count of the bitangents: ρ(𝒞)=t0(𝒞)+σ(𝒞)\rho(\mathscr{C})=t_{0}(\mathscr{C})+\sigma(\mathbb{R}\mathscr{C}).

Theorem.

4.1 Let 𝒞\mathscr{C} be a smooth real algebraic curve of degree dd in P2\mathbb{R}P^{2} intersecting LL_{\infty} transversally at exactly aa points. Then, we have the following signed count:

ρ(𝒞)=d(d2)2+a(a2)2T𝒯(𝒞)(|𝒞T|1).\rho(\mathscr{C})=\frac{d(d-2)}{2}+\frac{a(a-2)}{2}-\sum_{T\in\mathscr{T}_{\infty}(\mathbb{R}\mathscr{C})}(|\mathbb{R}\mathscr{C}\cap T|-1).

Furthermore, the integer ρ(𝒞)\rho(\mathscr{C}) is even and non-negative

In the case of quartics non-intersecting LL_{\infty}, we recover the signed count from [LV21]. Furthermore, the non-negativity statement proves [LV21, Conjecture 2] for any degree, already proven for quartics by Kummer-McKean [KM24] through different methods. It would be very interesting to see if quadratic enrichments exist for other fields. Theorem 4.1 suggests such a count should relate a quadratic count of bitangents to the intersection points between the curves and the tangents to points at infinity.

Acknowledgments. The author is supported by the SNF grant 204125 and would like to thank Erwan Brugallé for suggesting to work on bitangents and write this paper in the first place, as well as commenting on a first version.

2 Classical Fabricius-Bjerre Theorem

Let CC be a curve in 2\mathbb{R}^{2} with components CjC_{j}. For each component, we choose a regular parametrization γj:Ij2\gamma_{j}:I_{j}\to\mathbb{R}^{2} inducing an orientation. We denote the tangent at γj(tj)\gamma_{j}(t_{j}) by D(γj(tj))=γj(tj)+γj(tj)D(\gamma_{j}(t_{j}))=\gamma_{j}(t_{j})+\mathbb{R}\gamma^{\prime}_{j}(t_{j}). We also consider the half-tangents

D+(γj(tj))=γj(tj)+>0γj(tj) and D(γj(tj))=γj(tj)+<0γj(tj).D_{+}(\gamma_{j}(t_{j}))=\gamma_{j}(t_{j})+\mathbb{R}_{>0}\gamma^{\prime}_{j}(t_{j})\text{ and }D_{-}(\gamma_{j}(t_{j}))=\gamma_{j}(t_{j})+\mathbb{R}_{<0}\gamma^{\prime}_{j}(t_{j}).

They are switched when the orientation of CC is reversed. Let t(C)t(C) (resp. s(C)s(C)) be the number of bitangents of type TT (resp. SS), so that the signed count is σ(C)=t(C)s(C)\sigma(C)=t(C)-s(C).

The following Theorem is first due to Fabricius-Bjerre [FB62] in the case where the curve CC has a unique component. For convenience of the reader, we recall its proof. We also notice that the proof also works for curves with possibly several components.

Theorem 2.1.

Let CC be a curve in 2\mathbb{R}^{2} with n(C)n(C) nodes and i(C)i(C) flexes. We have the following identity:

σ(C)=n(C)+i(C)2.\sigma(C)=n(C)+\frac{i(C)}{2}.
Proof.

On each component CjC_{j} of CC, we consider the function fj(tj)=|D+(γj(tj))C||D(γj(tj))C|f_{j}(t_{j})=|D_{+}(\gamma_{j}(t_{j}))\cap C|-|D_{-}(\gamma_{j}(t_{j}))\cap C| giving the difference between the number of intersection points of the curve and the two half-tangents.

If D(γj(tj))D(\gamma_{j}(t_{j})) is transverse to CC outside its tangency point γj(tj)\gamma_{j}(t_{j}), intersection points deform continously in a neighborhood of tjt_{j}. It follows that fjf_{j} is locally constant near tjt_{j}. Thus, fjf_{j} is locally constant outside the values of tjt_{j} where γj(tj)\gamma_{j}(t_{j}) is a flex, a node, or D(γj(tj))D(\gamma_{j}(t_{j})) is a bitangent. Let Jj(t)=fj(tj+)f(tj)J_{j}(t)=f_{j}(t_{j}^{+})-f(t_{j}^{-}) be the value of the jump at tjt_{j}, where tj±t_{j}^{\pm} denotes the limit on the two sides of tt. The jump function JjJ_{j} takes the following values:

  • \circ

    Assume γj(tj)\gamma_{j}(t_{j}) is a node. When crossing the node, passing from tjt_{j}^{-} to tj+t_{j}^{+}, one intersection point passes from D+(γj(tj))D_{+}(\gamma_{j}(t_{j}^{-})) to D(γj(tj+))D_{-}(\gamma_{j}(t_{j}^{+})). Thus, we have Jj(tj)=2J_{j}(t_{j})=-2.

  • \circ

    Assume γj(tj)\gamma_{j}(t_{j}) is a flex of CjC_{j}. Here, when crossing the flex, we also have an intersection point passing from D+(γj(tj))D_{+}(\gamma_{j}(t_{j}^{-})) to D(γj(tj+))D_{-}(\gamma_{j}(t_{j}^{+})), so that Jj(tj)=2J_{j}(t_{j})=-2.

  • \circ

    Assume that the tangent D(γj(tj))D(\gamma_{j}(t_{j})) is a bitangent: D(γj(tj))=D(γk(tk))D(\gamma_{j}(t_{j}))=D(\gamma_{k}(t^{\prime}_{k})) for some kk and tkt^{\prime}_{k}. Assume this bitangent is of type TT. When passing from tjt_{j}^{-} to tj+t_{j}^{+}, we have two possibilities:

    • -

      If γk(tk)D+(γj(tj))\gamma_{k}(t^{\prime}_{k})\in D_{+}(\gamma_{j}(t_{j})), we gain two intersection points in D+(γj(tj))D_{+}(\gamma_{j}(t_{j})).

    • -

      If γ(tk)D(γj(tj))\gamma(t^{\prime}_{k})\in D_{-}(\gamma_{j}(t_{j})), we lose two intersection points in D(γj(tj))D_{-}(\gamma_{j}(t_{j})).

    In any case, we get that Jj(tj)=2J_{j}(t_{j})=2.

  • \circ

    Assuming the bitangent to be of type SS, we get similarly Jj(tj)=2J_{j}(t_{j})=-2.

As for each component we have fj(0)=fj(1)f_{j}(0)=f_{j}(1), we have

0=jfj(1)fj(0)=jtj:Jj(tj)0Jj(tj).0=\sum_{j}f_{j}(1)-f_{j}(0)=\sum_{j}\sum_{t_{j}:J_{j}(t_{j})\neq 0}J_{j}(t_{j}).

Grouping together the parameters giving the same node or bitangent, we deduce the following relation:

4t(C)4s(C)4n(C)2i(C)=0,4t(C)-4s(C)-4n(C)-2i(C)=0,

which is the desired identity. ∎

3 A projective Fabricius-Bjerre Theorem

We now aim to generalize the result by considering curves in P2\mathbb{R}P^{2}. To do so, let LL_{\infty} be a line in P2\mathbb{R}P^{2} and consider curves generically transverse to LL_{\infty}, which means the following: no line passing through a point of CLC\cap L_{\infty} is a bitangent or tangent at a flex. Recall that 𝒯(C)\mathscr{T}_{\infty}(C) is the set of tangents to CC at points of CLC\cap L_{\infty}. As P2\L=2\mathbb{R}P^{2}\backslash L_{\infty}=\mathbb{R}^{2}, we can use the Fabricius-Bjerre sign in this affine chart and make the associated signed count of bitangents. All constructions depend on the choice of this line LL_{\infty}. If LL is a line distinct from LL_{\infty}, we denote by pLp_{L} the unique intersection point between LL and LL_{\infty}.

Let LL be a second line in P2\mathbb{R}P^{2}, different from LL_{\infty}. Before getting to the generalization of Theorem 2.1, we provide a signed count of the tangents to CC passing through pLp_{L}. Let DD be a tangent to CC passing through pLp_{L}. The set P2(DLL)\mathbb{R}P^{2}\setminus(D\cup L_{\infty}\cup L) has three connected components, each one adjacent to two of the lines. Let UU the connected component in which CC is contained near its tangency point with DD: U¯D\overline{U}\supset D. We set:

  • \circ

    if U¯L\overline{U}\supset L (the concavity of CC is toward LL), the sign is ϵL(D)=+1\epsilon_{L}(D)=+1;

  • \circ

    if U¯L\overline{U}\supset L_{\infty} (the concavity of CC is toward LL_{\infty}), the sign is ϵL(D)=1\epsilon_{L}(D)=-1.

If LL is itself tangent to CC, we set ϵL(L)=0\epsilon_{L}(L)=0. We consider the signed count of tangents to CC passing through pLp_{L}:

σL(C)=DpLϵL(D).\sigma_{L}(C)=\sum_{D\ni p_{L}}\epsilon_{L}(D).
Lemma 3.1.

Assume LCL=L\cap C\cap L_{\infty}=\emptyset. The signed count of tangents to CC passing through pLp_{L} has the following value:

σL(C)=|CL||CL|.\sigma_{L}(C)=|C\cap L|-|C\cap L_{\infty}|.

Furthermore, if L𝒯(C)L\in\mathscr{T}_{\infty}(C) is tangent of CC at some point of CLC\cap L_{\infty}, then

σL(C)=1+|CL||CL|.\sigma_{L}(C)=1+|C\cap L|-|C\cap L_{\infty}|.
Proof.

First assume that pLCp_{L}\notin C. We consider the projection from CC to the pencil 𝒫P1\mathcal{P}\simeq\mathbb{R}P^{1} of lines passing through pLp_{L}:

π:pC(ppL)𝒫,\pi:p\in C\longmapsto(pp_{L})\in\mathcal{P},

where (ppL)(pp_{L}) is the unique line passing through pp and pLp_{L}. The pencil 𝒫\mathcal{P} contains the lines LL and LL_{\infty}, which split 𝒫\mathcal{P} into segments 𝒫0\mathcal{P}_{0} and 𝒫1\mathcal{P}_{1}, which we both orient from LL to LL_{\infty}.

A coordinate function on 𝒫0\mathcal{P}_{0} (resp. 𝒫1\mathcal{P}_{1}) induces a Morse function on π1(𝒫0)C\pi^{-1}(\mathcal{P}_{0})\subset C. Its critical points correspond precisely to points in CC whose tangent belongs to 𝒫\mathcal{P}, and the sign ϵL\epsilon_{L} actually coincides with the index. Therefore, for 𝒫0\mathcal{P}_{0}, we have that

|π1(L)||π1(L)|=2D𝒫0ϵL(D),|\pi^{-1}(L)|-|\pi^{-1}(L_{\infty})|=2\sum_{D\in\mathcal{P}_{0}}\epsilon_{L}(D),

where the sum is over the tangent to CC belonging to 𝒫0\mathcal{P}_{0}. As π1(L)=CL\pi^{-1}(L)=C\cap L and π1(L)=CL\pi^{-1}(L_{\infty})=C\cap L_{\infty}, adding the identities for 𝒫0\mathcal{P}_{0} and 𝒫1\mathcal{P}_{1} yields the count σL(C)\sigma_{L}(C) and its value.

If L=TL=T is the tangent line to a point pTCLp_{T}\in C\cap L_{\infty}, the projection π\pi is not a priori defined at pTp_{T}. As CC is tangent to TT at pTp_{T}, π\pi extends by continuity with π(pT)=T𝒫\pi(p_{T})=T\in\mathcal{P}. We then proceed as before, with the only difference that π1(L)=(CL)\{pT}\pi^{-1}(L_{\infty})=(C\cap L_{\infty})\backslash\{p_{T}\}, yielding the 11 discrepancy. ∎

We can now give the projective version of Fabricius-Bjerre.

Theorem 3.2.

Let CC be a curve in P2\mathbb{R}P^{2} transverse to LL_{\infty} with aa intersection points. We have the following signed count of bitangents:

σ(C)=n(C)+i(C)2+a(a2)2T𝒯(C)(|CT|1).\sigma(C)=n(C)+\frac{i(C)}{2}+\frac{a(a-2)}{2}-\sum_{T\in\mathscr{T}_{\infty}(C)}(|C\cap T|-1).
Proof.

We proceed as in the affine case, considering a parametrization γj:IjP2\gamma_{j}:I_{j}\to\mathbb{R}P^{2} of each component of CC and the functions

fj(tj)=|D+(γj(tj))C||D(γj(tj))C|.f_{j}(t_{j})=|D_{+}(\gamma_{j}(t_{j}))\cap C|-|D_{-}(\gamma_{j}(t_{j}))\cap C|.

Outside a finite number of values, fjf_{j} is locally constant. Let Jj(tj)=f(tj+)f(tj)J_{j}(t_{j})=f(t_{j}^{+})-f(t_{j}^{-}) be the jump function. On one side, we have the same jumps as for the compact curves:

  • \circ

    Jj(tj)=2J_{j}(t_{j})=2 if γj(tj)\gamma_{j}(t_{j}) is node or a flex, or if D(γj(tj))D(\gamma_{j}(t_{j})) is a bitangent of type TT;

  • \circ

    Jj(tj)=2J_{j}(t_{j})=-2 if D(γj(tj))D(\gamma_{j}(t_{j})) is a bitangent of type SS.

However, we have now new jump points when γj(tj)L\gamma_{j}(t_{j})\in L_{\infty} or if D(γj(tj))pTD(\gamma_{j}(t_{j}))\ni p_{T} for T𝒯(C)T\in\mathscr{T}_{\infty}(C).

  • \circ

    Assume γj(tj)L\gamma_{j}(t_{j})\in L_{\infty}. In particular, D(γj(tj))=T𝒯(C)D(\gamma_{j}(t_{j}))=T\in\mathscr{T}_{\infty}(C). Going from tjt_{j}^{-} to tj+t_{j}^{+}, all intersection points between CC and the tangent beside the tangency point move from DD_{-} to D+D_{+}. Therefore, we have Jj(tj)=2(|CT|1)J_{j}(t_{j})=2(|C\cap T|-1). The 1-1 is for the tangency point, not counted in the process.

  • \circ

    Assume that D(γj(tj))pTD(\gamma_{j}(t_{j}))\ni p_{T} for some T𝒯(C)T\in\mathscr{T}_{\infty}(C). Depending on the concavity of CC at γj(tj)\gamma_{j}(t_{j}), the intersection point near pTp_{T} passes from D+(γj(tj))D_{+}(\gamma_{j}(t_{j}^{-})) to D(γj(tj+))D_{-}(\gamma_{j}(t_{j}^{+})) or conversely: we have Jj(tj)=2ϵT(D(γj(tj)))=±2J_{j}(t_{j})=2\epsilon_{T}(D(\gamma_{j}(t_{j})))=\pm 2.

As 0=fj(1)fj(0)=tj:Jj(t)0Jj(tj)0=f_{j}(1)-f_{j}(0)=\sum_{t_{j}:J_{j}(t)\neq 0}J_{j}(t_{j}), summing over the various components and grouping together the parameters corresponding to bitangents and nodes, we get the following identity:

4t(C)4s(C)2i(C)4n(C)+2T𝒯(C)(|TC|1)+T𝒯(C)DpT2ϵT(D)=0.4t(C)-4s(C)-2i(C)-4n(C)+2\sum_{T\in\mathscr{T}_{\infty}(C)}(|T\cap C|-1)+\sum_{T\in\mathscr{T}_{\infty}(C)}\sum_{D\ni p_{T}}2\epsilon_{T}(D)=0.

We recognize the signed count σT(C)\sigma_{T}(C) computed in Lemma 3.1. Replacing its expression, we get that

4σ(C)2i(C)4n(C)+4(|TC|1)2a(a2)=0.4\sigma(C)-2i(C)-4n(C)+4\sum(|T\cap C|-1)-2a(a-2)=0.

4 Applications to real algebraic curves

Let 𝒞\mathscr{C} be a generic smooth real algebraic curve in P2\mathbb{R}P^{2} of degree d2d\geqslant 2. In particular, the real part 𝒞\mathbb{R}\mathscr{C} is a curve in our sense. If LL is a real line tangent to 𝒞\mathscr{C} at two points, there are two possibilities:

  • \circ

    the split bitangents if the tangency points are real,

  • \circ

    the non-split bitangents if the tangency points are complex conjugate.

Actually, the number of non-split bitangents t0(𝒞)t_{0}(\mathscr{C}) is related to the number of real flexes i(𝒞)i(\mathbb{R}\mathscr{C}) via Klein’s formula [Kle76]:

t0(𝒞)+i(𝒞)2=d(d2)2.t_{0}(\mathscr{C})+\frac{i(\mathbb{R}\mathscr{C})}{2}=\frac{d(d-2)}{2}.

We consider the following signed count of bitangents to 𝒞\mathscr{C}:

ρ(𝒞)=t0(𝒞)+σ(𝒞).\rho(\mathscr{C})=t_{0}(\mathscr{C})+\sigma(\mathbb{R}\mathscr{C}).

The first term deals with non-split bitangents (thus counted with a positive sign), and the second term with the split bitangents, counted with the Fabricius-Bjerre sign. The curve being smooth, we have n(𝒞)=0n(\mathbb{R}\mathscr{C})=0. Coupling Klein’s formula with Theorem 3.2, we get the following.

Theorem 4.1.

Let 𝒞\mathscr{C} be a generic smooth real algebraic curve of degree dd in P2\mathbb{R}P^{2} with aa intersection points with LL_{\infty}. Then, we have the following signed count:

ρ(𝒞)=d(d2)2+a(a2)2T𝒯(𝒞)(|𝒞T|1).\rho(\mathscr{C})=\frac{d(d-2)}{2}+\frac{a(a-2)}{2}-\sum_{T\in\mathscr{T}_{\infty}(\mathbb{R}\mathscr{C})}(|\mathbb{R}\mathscr{C}\cap T|-1).

Furthermore, this count is even and non-negative.

Theorem 4.1 actually proves [LV21, Conjecture 2] and generalizes it for curves of any degree. This conjecture was already proved by Kummer-McKean [KM24] by a different method in the case of quartics.

Proof.

As advertised, the signed count is a consequence of Theorem 3.2 and Klein’s formula. We now prove the count is even and non-negative. By Bezout’s theorem, for each tangent TT, we have that

|T𝒞|1d2.|T\cap\mathbb{R}\mathscr{C}|-1\leqslant d-2.

Summing over all the tangents of 𝒯(𝒞)\mathscr{T}_{\infty}(\mathbb{R}\mathscr{C}), we have the following lower bound:

ρ(𝒞)d(d2)2+a(a2)2a(d2)=(da)(da2)20,\rho(\mathscr{C})\geqslant\frac{d(d-2)}{2}+\frac{a(a-2)}{2}-a(d-2)=\frac{(d-a)(d-a-2)}{2}\geqslant 0,

since by Bezout’s theorem, da1d-a\neq 1. For the parity, Bezout’s Theorem also tells us that damod2d\equiv a\mod 2 and |T𝒞|1dmod 2|T\cap\mathbb{R}\mathscr{C}|-1\equiv d\ \mathrm{mod}\ 2 since the tangency points count twice. Therefore,

ρ(𝒞)\displaystyle\rho(\mathscr{C})\equiv a2+d22adadmod 2\displaystyle\frac{a^{2}+d^{2}}{2}-a-d-ad\ \mathrm{mod}\ 2
\displaystyle\equiv a2d22mod 2.\displaystyle\frac{a^{2}-d^{2}}{2}\ \mathrm{mod}\ 2.

As admod 2a\equiv d\ \mathrm{mod}\ 2, we get a2d2mod 4a^{2}\equiv d^{2}\ \mathrm{mod}\ 4 and we conclude. ∎

Assuming 𝒞\mathscr{C} has no real point on LL_{\infty}, i.e. a=0a=0, the signed count in this particular case is

ρ(𝒞)=d(d2)2.\rho(\mathscr{C})=\frac{d(d-2)}{2}.
Example 4.2.

For conics, i.e. d=2d=2, the tangents at 𝒞L\mathbb{R}\mathscr{C}\cap L_{\infty} have no further intersection points, so that the signed count is 0+000+0-0, compatible with the fact there is no bitangent.

We now assume 𝒞\mathscr{C} is a cubic curve: the degree is 33. Klein’s formula tells us that there are 33 real flexes. The number of tangents at 𝒞L\mathbb{R}\mathscr{C}\cap L_{\infty} is either 11 or 33. Furthermore, for any real tangent line LL, by Bezout’s theorem, L𝒞L\cap\mathscr{C} has three points counted with multiplicity. The tangency point counts for 22. Thus, the remaining point is real, and we get |L𝒞|1=1|L\cap\mathbb{R}\mathscr{C}|-1=1. In the end, if a=1a=1 we get 32121\frac{3}{2}-\frac{1}{2}-1, and if a=3a=3 we get 32+323\frac{3}{2}+\frac{3}{2}-3, which is compatible with the absence of bitangent in this case as well. \lozenge

Example 4.3.

The first interesting case is the case of quartic curves. Assuming transversality, a quartic may have a=0,2a=0,2 or 44 real intersection points with LL_{\infty}.

  • \triangleright

    If a=0a=0, the real locus is compact in 2\mathbb{R}^{2}, and we recover the signed count from [LV21].

  • \triangleright

    If r=2r=2, we have tangents at points of LL_{\infty}. The signed count is

    ρ(𝒞)=4(|T1𝒞|1)(|T2𝒞|1).\rho(\mathscr{C})=4-(|T_{1}\cap\mathbb{R}\mathscr{C}|-1)-(|T_{2}\cap\mathbb{R}\mathscr{C}|-1).

    Thanks to Bezout’s theorem, we have that |T𝒞|12|T\cap\mathbb{R}\mathscr{C}|-1\leqslant 2 for every tangent TT to CC. Thus, ρ(𝒞)0\rho(\mathscr{C})\geqslant 0 and the count may take the values 0,2,40,2,4.

  • \triangleright

    If r=4r=4, we now a have 44 asymptotic lines, and we get

    ρ(𝒞)=4+4(42)214(|Tj𝒞|1)=814(|Tj𝒞|1).\rho(\mathscr{C})=4+\frac{4(4-2)}{2}-\sum_{1}^{4}(|T_{j}\cap\mathbb{R}\mathscr{C}|-1)=8-\sum_{1}^{4}(|T_{j}\cap\mathbb{R}\mathscr{C}|-1).

    We conclude similarly than ρ(𝒞)0\rho(\mathscr{C})\geqslant 0 and can take the values 0,2,4,6,80,2,4,6,8.

\lozenge

Using the generalization of Klein’s formula [Sch04] to curves with nodes and cusp, we can generalize the signed count to real algebraic curves with nodes.

Proposition 4.4.

Let 𝒞\mathscr{C} be a degree dd real nodal algebraic curve in 2\mathbb{P}^{2} with NN nodes (both real and complex), nn_{\mathbb{R}} real nodes, ii real flexes and aa intersection points with LL_{\infty}. Then, we have the following signed count:

ρ(𝒞)=nN+d(d2)2+a(a2)2T(|CT|1)\rho(\mathscr{C})=n_{\mathbb{R}}-N+\frac{d(d-2)}{2}+\frac{a(a-2)}{2}-\sum_{T}(|C\cap T|-1)
Proof.

Let n0n_{0} be the number of real isolated nodes and n2n_{2} the number of hyperbolic nodes, so that n=n0+n2n_{\mathbb{R}}=n_{0}+n_{2}. Klein’s formula for nodal curves [Sch04] states as follows:

d+i+2t0=d(d1)2N+2n0,d+i+2t_{0}=d(d-1)-2N+2n_{0},

while Theorem 3.2 gives

σ(𝒞)=n2+i2+a(a2)2T(|CT|1).\sigma(\mathbb{R}\mathscr{C})=n_{2}+\frac{i}{2}+\frac{a(a-2)}{2}-\sum_{T}(|C\cap T|-1).

We conclude as in Theorem 4.1. ∎

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