In mathematics, an elliptic surface is a surface that has an elliptic fibration, in other words a proper morphism with connected fibers to an algebraic curve such that almost all fibers are smooth curves of genus 1. (Over an algebraically closed field such as the complex numbers, these fibers are elliptic curves, perhaps without a chosen origin.) This is equivalent to the generic fiber being a smooth curve of genus one. This follows from proper base change.
The surface and the base curve are assumed to be non-singular (complex manifolds or regular schemes, depending on the context). The fibers that are not elliptic curves are called the singular fibers and were classified by Kunihiko Kodaira. Both elliptic and singular fibers are important in string theory, especially in F-theory.
Elliptic surfaces form a large class of surfaces that contains many of the interesting examples of surfaces, and are relatively well understood in the theories of complex manifolds and smooth 4-manifolds. They are similar to (have analogies with, that is), elliptic curves over number fields.
Most of the fibers of an elliptic fibration are (non-singular) elliptic curves. The remaining fibers are called singular fibers: there are a finite number of them, and each one consists of a union of rational curves, possibly with singularities or non-zero multiplicities (so the fibers may be non-reduced schemes). Kodaira and Néron independently classified the possible fibers, and Tate's algorithm can be used to find the type of the fibers of an elliptic curve over a number field.
The following table lists the possible fibers of a minimal elliptic fibration. ("Minimal" means roughly one that cannot be factored through a "smaller" one; precisely, the singular fibers should contain no smooth rational curves with self-intersection number −1.) It gives:
Kodaira | Néron | Components | Intersection matrix | Dynkin diagram | Fiber | |
---|---|---|---|---|---|---|
I0 | A | 1 (elliptic) | 0 | |||
I1 | B1 | 1 (with double point) | 0 | |||
I2 | B2 | 2 (2 distinct intersection points) | affine A1 | |||
Iv (v≥2) | Bv | v (v distinct intersection points) | affine Av-1 | |||
mIv (v≥0, m≥2) | Iv with multiplicity m | |||||
II | C1 | 1 (with cusp) | 0 | |||
III | C2 | 2 (meet at one point of order 2) | affine A1 | |||
IV | C3 | 3 (all meet in 1 point) | affine A2 | |||
I0* | C4 | 5 | affine D4 | |||
Iv* (v≥1) | C5,v | 5+v | affine D4+v | |||
IV* | C6 | 7 | affine E6 | |||
III* | C7 | 8 | affine E7 | |||
II* | C8 | 9 | affine E8 |
This table can be found as follows. Geometric arguments show that the intersection matrix of the components of the fiber must be negative semidefinite, connected, symmetric, and have no diagonal entries equal to −1 (by minimality). Such a matrix must be 0 or a multiple of the Cartan matrix of an affine Dynkin diagram of type ADE.
The intersection matrix determines the fiber type with three exceptions:
The monodromy around each singular fiber is a well-defined conjugacy class in the group SL(2,Z) of 2 × 2 integer matrices with determinant 1. The monodromy describes the way the first homology group of a smooth fiber (which is isomorphic to Z2) changes as we go around a singular fiber. Representatives for these conjugacy classes associated to singular fibers are given by:[1]
Fiber | Intersection matrix | Monodromy | j-invariant | Group structure on smooth locus | |
---|---|---|---|---|---|
Iν | affine Aν-1 | \begin{pmatrix}1&\nu\ 0&1\end{pmatrix} | infty | Z/\nu x C* | |
II | 0 | \begin{pmatrix}1&1\ -1&0\end{pmatrix} | 0 | C | |
III | affine A1 | \begin{pmatrix}0&1\ -1&0\end{pmatrix} | 1728 | Z/2 x C | |
IV | affine A2 | \begin{pmatrix}0&1\ -1&-1\end{pmatrix} | 0 | Z/3 x C | |
I0* | affine D4 | \begin{pmatrix}-1&0\ 0&-1\end{pmatrix} | in C | (Z/2)2 x C | |
Iν* (ν≥1) | affine D4+ν | \begin{pmatrix}-1&-\nu\ 0&-1\end{pmatrix} | infty | (Z/2)2 x C Z/4 x C | |
IV* | affine E6 | \begin{pmatrix}-1&-1\ 1&0\end{pmatrix} | 0 | Z/3 x C | |
III* | affine E7 | \begin{pmatrix}0&-1\ 1&0\end{pmatrix} | 1728 | Z/2 x C | |
II* | affine E8 | \begin{pmatrix}0&-1\ 1&1\end{pmatrix} | 0 | C |
For singular fibers of type II, III, IV, I0*, IV*, III*, or II*, the monodromy has finite order in SL(2,Z). This reflects the fact that an elliptic fibration has potential good reduction at such a fiber. That is, after a ramified finite covering of the base curve, the singular fiber can be replaced by a smooth elliptic curve. Which smooth curve appears is described by the j-invariant in the table. Over the complex numbers, the curve with j-invariant 0 is the unique elliptic curve with automorphism group of order 6, and the curve with j-invariant 1728 is the unique elliptic curve with automorphism group of order 4. (All other elliptic curves have automorphism group of order 2.)
For an elliptic fibration with a section, called a Jacobian elliptic fibration, the smooth locus of each fiber has a group structure. For singular fibers, this group structure on the smooth locus is described in the table, assuming for convenience that the base field is the complex numbers. (For a singular fiber with intersection matrix given by an affine Dynkin diagram
\tilde{\Gamma}
\Gamma
To understand how elliptic surfaces fit into the classification of surfaces, it is important to compute the canonical bundle of a minimal elliptic surface f: X → S. Over the complex numbers, Kodaira proved the following canonical bundle formula:[2]
*(L) ⊗ | |
K | |
X=f |
OS(\sumi(mi-1)Di).
*(p | |
f | |
i)=m |
iDi
Building on work of Kenji Ueno, Takao Fujita (1986) gave a useful variant of the canonical bundle formula, showing how KX depends on the variation of the smooth fibers.[3] Namely, there is a Q-linear equivalence
KX\sim\bf
*(K | |
f | |
S+B |
S+MS),
(1/12)j*O(1)
The discriminant divisor in Fujita's formula is defined by
BS=\sump\in(1-c(p))[p]
lct(X,f*(p))
I\nu
{}mI\nu
* | |
I | |
\nu |
The canonical bundle formula (in Fujita's form) has been generalized by Yujiro Kawamata and others to families of Calabi–Yau varieties of any dimension.[4]
A logarithmic transformation (of order m with center p) of an elliptic surface or fibration turns a fiber of multiplicity 1 over a point p of the base space into a fiber of multiplicity m. It can be reversed, so fibers of high multiplicity can all be turned into fibers of multiplicity 1, and this can be used to eliminate all multiple fibers.
Logarithmic transformations can be quite violent: they can change the Kodaira dimension, and can turn algebraic surfaces into non-algebraic surfaces.
Example:Let L be the lattice Z+iZ of C, and let E be the elliptic curve C/L. Then the projection map from E×C to C is an elliptic fibration. We will show how to replace the fiber over 0 with a fiber of multiplicity 2.
There is an automorphism of E×C of order 2 that maps (c,s) to (c+1/2, -s). We let X be the quotient of E×C by this group action. We make X into a fiber space over C by mapping (c,s) to s2. We construct an isomorphism from X minus the fiber over 0 to E×C minus the fiber over 0 by mapping (c,s) to (c-log(s)/2πi,s2). (The two fibers over 0 are non-isomorphic elliptic curves, so the fibration X is certainly not isomorphic to the fibration E×C over all of C.)
Then the fibration X has a fiber of multiplicity 2 over 0, and otherwise looks like E×C. We say that X is obtained by applying a logarithmic transformation of order 2 to E×C with center 0.