A nonzero integer polynomial of bidegree at most can cancel the first Taylor coefficients of the Fredholm series. Functional transcendence makes the resulting analytic function nonzero. If and were both algebraic, the relation would keep the auxiliary values in one fixed number field. Their Absolute logarithmic Weil height is at most , whereas their chosen absolute value is . The Liouville height inequality forces , contradicting its quadratic lower bound for sufficiently large .
Let be a number field and an elliptic curve. Heights measure the arithmetic size of points, and turn the finite quotient supplied by the Weak Mordell-Weil theorem into finite generation. For a projective point define the Absolute logarithmic Weil height
using the usual normalized absolute values and local degrees . The product formula makes this independent of scaling and of enlarging . For a Short Weierstrass form put and . Over , if in lowest terms, .
The finiteness property is Northcott theorem: for bounded height and bounded degree over there are only finitely many algebraic numbers. One sees the mechanism from the height-Mahler measure formula. If has degree and height at most , its primitive integral minimal polynomial has Mahler measure . Expanding its product of linear factors bounds every coefficient by . Only finitely many integral polynomials satisfy this bound, and each has finitely many roots. Thus a height bound gives only finitely many -coordinates in the fixed number field , and each gives at most two points of , besides .
To understand multiplication, the doubling formula gives
Its homogeneous numerator and denominator have degree four. They have no common projective zero: at infinity the numerator is nonzero, and at a root of the numerator equals , since it is . Nonsingularity excludes a common root of . The coordinate doubling map is therefore a degree-four morphism of the projective line.
The general height growth under a morphism of the projective line is for a fixed degree- morphism. Here is why the error is bounded independently of . At a place , normalize its homogeneous coordinates to have maximum norm . The fixed homogeneous forms have uniformly bounded norm. They also have a positive lower bound: the normalized coordinate space is compact over , and their common zero set is empty. Outside finitely many places their coefficients are integral and their reduction has no common zero, making both bounds . Homogeneity and summation over places then give the asserted height estimate. Consequently there is a fixed with
Define the canonical height of an elliptic curve by the conventional normalization
The successive approximants differ by at most , so the limit exists and
Thus canonical height retains Northcott finiteness, while replacing the bounded-error doubling rule by an exact one.
We also need the height parallelogram identity. It follows from the symmetric-square proof of the naive height parallelogram estimate, which we give explicitly using the supplied addition formulae. For , the unordered pair is represented by the binary quadratic , where
These forms define the biquadratic morphism for elliptic sums and differences. They have no common zero. If , the two projective coordinates agree. On the finite diagonal , and , so simultaneous vanishing would violate nonsingularity. At the homogeneous is nonzero. This also handles and sums or differences equal to , for which the affine fractions alone would be inappropriate.
The same local norm argument as above, now using bidegree , gives
On the other hand the binary quadratic is the product of two linear factors for and . At nonarchimedean places coefficient maximum norms multiply exactly: scale each factor to norm and reduce; the product of the two nonzero residue polynomials remains nonzero. This is multiplicativity of the nonarchimedean polynomial norm. At archimedean places the norms are comparable up to fixed constants, by the coefficient triangle inequality and compactness of normalized linear factors. Therefore
Combining the estimates proves the naive-height parallelogram relation with a uniform error. Apply it to , divide by , and pass to the limit to obtain
As in the polarization argument of (a), this makes quadratic, with the canonical height pairing
A torsion point has canonical height zero because its multiples have bounded naive height. Conversely, if , then all have bounded naive height. Northcott finiteness makes two equal, giving for some . Thus canonical height vanishes exactly on torsion. In particular the torsion subgroup is finite, since the comparison with naive height bounds the heights of all its points.
We can now prove the Mordell-Weil theorem. The Weak Mordell-Weil theorem, as explained in Question 2(ii), makes finite. Choose representatives and put . Every can be written . The parallelogram identity and nonnegativity give
Iterating this height descent makes the height at step at most , so after finitely many steps it is at most . There are only finitely many points of that height by Northcott and the naive-height comparison. Reversing shows that every point is an integer combination of the finitely many representatives and this finite bounded-height set. Therefore
On the resulting free part the canonical height pairing is positive definite. Its nonnegativity extends from rational vectors to real vectors by density. If a nonzero real vector were in its kernel, in a basis of the free part round to integer vectors . Their rounding errors are uniformly bounded, and would be uniformly bounded. The vectors are unbounded and therefore include infinitely many distinct vectors, contradicting Northcott finiteness. Thus there is no real null vector. Heights consequently support quantitative point searches, tests of independence, and the regulator of an elliptic curve, in addition to providing the descent that proves finite generation.
Galois cohomology and the finite division quotient. Let be a number field, with its profinite topology, and a discrete continuous -module. Its Galois cohomology is continuous group cohomology. In degrees zero and one,
Thus a crossed homomorphism measures the failure of a choice to be Galois-invariant, and changing the choice changes the cocycle by a coboundary. A short exact sequence of such modules gives a long exact sequence in group cohomology. The connecting map sends an invariant element to the cocycle obtained by lifting it and comparing its Galois translates.
For an elliptic curve and , multiplication by is surjective on and has kernel . The Kummer exact sequence of an elliptic curve therefore gives
Explicitly, choose and set . Replacing changes this by a coboundary; replacing by , , does not change it. If its class is zero, some torsion translate of is Galois-invariant, so . This proves injectivity of the Kummer map of an elliptic curve.
The whole group need not be finite. The crucial restriction is ramification. Let contain the finite primes of bad reduction of an elliptic curve and those dividing . At , good reduction and prime-to-residue-characteristic multiplication imply that every division point of a local point is in an unramified extension, by the formal-group lifting argument. Thus every global Kummer class restricts trivially to inertia there.
Choose a finite Galois extension containing and the th roots of unity, and enlarge to include its ramified primes. Over , the torsion module is constant and can be identified with . By Kummer theory,
For classes unramified outside the primes above , valuations outside must be divisible by . Their restriction images therefore lie in , the square of an S-unramified power class group. Its finiteness can be seen without assuming the Mordell-Weil theorem: the finiteness of S-unramified Kummer classes follows from
The S-unit group is finitely generated by the Dirichlet unit theorem and its valuations at . The localized ideal class group is a quotient of the ordinary ideal class group of , which is finite by the finiteness of the ideal class group. The Minkowski bound for ideal classes supplies an integral ideal of bounded norm in each class, and only finitely many integral ideals have bounded norm.
The kernel of restriction from to is also finite: a cocycle trivial after restriction can, after subtracting a coboundary, be made to factor through the finite group . There are only finitely many maps from that group to the finite module . This is the finite-extension kernel of a Kummer map mechanism. Consequently the possible Kummer classes form a finite set, proving
This is the Weak Mordell-Weil theorem. Imposing membership in the local Kummer image at every place refines the finite unramified collection to the n-Selmer group. Its relation with the obstruction to a globally rational point is
where the last group is the -torsion of the Tate–Shafarevich group. Thus local solubility gives a finite computable upper bound but can leave a genuine global obstruction.
Heights and finite generation. For the other essay, normalize the absolute values on a field so that the product formula holds. The Absolute logarithmic Weil height of is
At the infinite places the local degrees are one or two and the usual real or complex modulus is used. The product formula makes this independent of scaling; it is also unchanged by extending . Over , using coprime integral coordinates gives , the naive height on the projective line. The Northcott theorem says that points of bounded height and bounded field degree form a finite set; in particular this holds over the fixed field . One way to see the finiteness is the height-Mahler measure formula: for an algebraic number of degree , the coefficients of its primitive minimal integer polynomial are bounded by binomial factors times . Bounds on and therefore leave only finitely many integer polynomials and hence only finitely many algebraic numbers.
Set for , and . Since has degree two, bounded gives only finitely many points of . The height growth under a morphism of the projective line states that a degree- morphism gives . The upper bound follows from its homogeneous coordinate polynomials; the lower bound follows from their having no common zero, using a resultant identity at each place. Applied to the degree-four duplication map, it gives a uniform constant with
Consequently is Cauchy: the absolute difference of consecutive terms is at most . Define the canonical height of an elliptic curve by
It is nonnegative and satisfies . The factor one-half is the conventional normalization for the divisor , since the first-coordinate height belongs to .
The addition-divisor identity also gives the bounded-error height identity
uniformly in . This is the height form of the identity for the sum and difference pullbacks of the line bundle associated to ; it includes points where the affine addition formulas have a zero denominator. Apply it to , divide by , and take the limit. Thus satisfies the parallelogram law, and its polarization is a bilinear form, the height pairing. Nonnegativity implies the Cauchy-Schwarz inequality for that pairing, by evaluating its nonnegative quadratic polynomial on for all integers and approximating real ratios by rational numbers. In particular
These properties do not presuppose finite generation. Bounded canonical height gives a finite set by the bounded difference and the Northcott theorem. Torsion points have canonical height zero. Conversely, if , all have bounded naive height, so two coincide; their difference makes torsion. Thus the height detects precisely the free part, once finite generation is proved.
Use the Weak Mordell-Weil theorem with and choose finitely many coset representatives . Write , and put . The height inequality yields
Iteration enters the finite set , since after steps the height is at most . Unwinding expresses every point using that finite set and the . This proves the canonical-height proof of Mordell-Weil finite generation and hence
The Fundamental theorem of finitely generated abelian groups supplies this decomposition. The Mordell-Weil theorem combines a finite quotient from arithmetic Galois cohomology with a contracting height descent; either ingredient alone would not establish finite generation.
For
the chord-and-tangent group law gives, for distinct nonopposite points and ,
For doubling, replace the slope by
The point at infinity is the identity and .
Let the -coordinates of be . Applying the addition formula with and gives
Substituting and simplifying yields
Multiplying the two addition formulas and eliminating in the same way gives
These identities are the algebraic source of two parallelogram laws. Applied to pullbacks of the pole divisor of , they imply
for isogenies of elliptic curves. Together with , this makes the degree a quadratic form. Applied to the Absolute logarithmic Weil height of the four -coordinates, with bounded terms removed by passage to the limit defining the canonical height of an elliptic curve, they similarly give
A suitable theorem is the Baker lower bound for a homogeneous linear form in logarithms. Let be nonzero algebraic numbers with chosen logarithms and let
Choose to bound the degree-normalized Absolute logarithmic Weil height of and , and put . If , then
where is an effectively computable constant depending only on and the degree of the number field generated by the .