Inmathematics, anelliptic surface is a surface that has an ellipticfibration, in other words aproper morphism with connectedfibers to analgebraic curve such that almost all fibers aresmooth curves ofgenus 1. (Over an algebraically closed field such as thecomplex numbers, these fibers areelliptic curves, perhaps without a chosen origin.) This is equivalent to thegeneric fiber being a smooth curve of genus one. This follows fromproper base change.
The surface and the base curve are assumed to be non-singular (complex manifolds orregular schemes, depending on the context). The fibers that are not elliptic curves are called thesingular fibers and were classified byKunihiko Kodaira. Both elliptic and singular fibers are important instring theory, especially inF-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 andsmooth4-manifolds. They are similar to (have analogies with, that is), elliptic curves overnumber 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, andTate'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 aminimal 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:
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 typeADE.
The intersection matrix determines the fiber type with three exceptions:
Themonodromy around each singular fiber is a well-definedconjugacy class in the group SL(2,Z) of 2 × 2 integer matrices withdeterminant 1. The monodromy describes the way the firsthomology group of a smooth fiber (which is isomorphic toZ2) 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 | |||
| II | 0 | 0 | ||
| III | affine A1 | 1728 | ||
| IV | affine A2 | 0 | ||
| I0* | affine D4 | in | ||
| Iν* (ν≥1) | affine D4+ν | if ν is even, if ν is odd | ||
| IV* | affine E6 | 0 | ||
| III* | affine E7 | 1728 | ||
| II* | affine E8 | 0 |
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 haspotential 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 thej-invariant in the table. Over the complex numbers, the curve withj-invariant 0 is the unique elliptic curve with automorphism group of order 6, and the curve withj-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 asection, called aJacobian 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, the group of components of the smooth locus is isomorphic to the center of the simply connected simple Lie group with Dynkin diagram, as listedhere.) Knowing the group structure of the singular fibers is useful for computing theMordell-Weil group of an elliptic fibration (the group of sections), in particular its torsion subgroup.
To understand how elliptic surfaces fit into theclassification of surfaces, it is important to compute thecanonical bundle of a minimal elliptic surfacef:X →S. Over the complex numbers, Kodaira proved the followingcanonical bundle formula:[2]
Here the multiple fibers off (if any) are written as, for an integermi at least 2 and a divisorDi whose coefficients have greatest common divisor equal to 1, andL is some line bundle on the smooth curveS. IfS is projective (or equivalently, compact), then thedegree ofL is determined by theholomorphic Euler characteristics ofX andS: deg(L) = χ(X,OX) − 2χ(S,OS). The canonical bundle formula implies thatKX isQ-linearly equivalent to the pullback of someQ-divisor onS; it is essential here that the elliptic surfaceX →S is minimal.
Building on work ofKenji Ueno, Takao Fujita (1986) gave a useful variant of the canonical bundle formula, showing howKX depends on the variation of the smooth fibers.[3] Namely, there is aQ-linear equivalence
where thediscriminant divisorBS is an explicit effectiveQ-divisor onS associated to the singular fibers off, and themoduli divisorMS is, wherej:S →P1 is the function giving thej-invariant of the smooth fibers. (ThusMS is aQ-linear equivalence class ofQ-divisors, using the identification between thedivisor class group Cl(S) and thePicard group Pic(S).) In particular, forS projective, the moduli divisorMS has nonnegative degree, and it has degree zero if and only if the elliptic surface is isotrivial, meaning that all the smooth fibers are isomorphic.
The discriminant divisor in Fujita's formula is defined by
wherec(p) is thelog canonical threshold. This is an explicit rational number between 0 and 1, depending on the type of singular fiber. Explicitly, the lct is 1 for a smooth fiber or type, and it is 1/m for a multiple fiber, 1/2 for, 5/6 for II, 3/4 for III, 2/3 for IV, 1/3 for IV*, 1/4 for III*, and 1/6 for II*.
The canonical bundle formula (in Fujita's form) has been generalized byYujiro Kawamata and others to families ofCalabi–Yau varieties of any dimension.[4]
Alogarithmic transformation (of orderm with centerp) of an elliptic surface or fibration turns a fiber of multiplicity 1 over a pointp of the base space into a fiber of multiplicitym. 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:LetL be the latticeZ+iZ ofC, and letE be the elliptic curveC/L. Then the projection map fromE×C toC is an elliptic fibration. We will show how to replace the fiber over 0 with a fiber of multiplicity 2.
There is an automorphism ofE×C of order 2 that maps (c,s) to (c+1/2,−s). We letX be the quotient ofE×C by this group action. We makeX into a fiber space overC by mapping (c,s) tos2. We construct an isomorphism fromX minus the fiber over 0 toE×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 fibrationX is certainly not isomorphic to the fibrationE×C over all ofC.)
Then the fibrationX has a fiber of multiplicity 2 over 0, and otherwise looks likeE×C. We say thatX is obtained by applying a logarithmic transformation of order 2 toE×C with center 0.