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TauCeti.RingTheory.FormalGroup.Logarithm.InfiniteHeight

Formal group laws of infinite height are additive #

Let p be a prime and let F be a commutative formal group law over a commutative ring R with [p]_F = 0. Then p = 0 in R, since p is the linear coefficient of [p]_F, so no logarithm in the sense of FormalGroup.log is available. Nevertheless F is strictly isomorphic to the additive formal group law, along a coordinate that is unique once normalised: there is a unique power series

g(X) = X + βˆ‘_{i β‰₯ 2} aα΅’ Xⁱ with a_{pᡏ} = 0 for every k β‰₯ 1

such that g(F(X, Y)) = g(X) + g(Y). Over a field of characteristic p, the condition [p]_F = 0 says that F has height ⊀, so the formal group laws of infinite height are exactly those isomorphic to the additive one. For p = 2 this is Quillen's normalised logarithm of a formal group law of exponent two, FormalGroup.exponentTwoLog. No coefficient field and no further hypothesis on R is used: it may have nilpotents or be the zero ring.

The power series g is constructed degree by degree. If g is additive along F up to degree n, the error Φ(X, Y) = g(F(X, Y)) - g(X) - g(Y) is the homomorphism defect of g from F to the additive formal group law, so its degree-n part is r C_n for the Lazard cocycle C_n = ((X + Y)ⁿ - Xⁿ - Yⁿ) / d_n (FormalGroup.exists_homogeneousComponent_homDefect_eq_smul_lazardCocycle).

Each step leaves the coefficients in lower degrees, and those in degrees pᡏ, unchanged, and g is the limit of these approximations. Uniqueness is the fact that a nonzero homomorphism to the additive formal group law has order a power of p (FormalGroup.exists_order_eq_pow_of_natCast_eq_zero).

Main results #

References #

theorem FormalGroup.logarithm_unique_of_natCast_eq_zero {R : Type u_1} [CommRing R] (F : FormalGroup R) {p : β„•} (hp : Nat.Prime p) (hpR : ↑p = 0) {g g' : PowerSeries R} (hβ‚€ : PowerSeries.constantCoeff g = 0) (h₁ : (PowerSeries.coeff 1) g = 1) (hpow : βˆ€ (k : β„•), 0 < k β†’ (PowerSeries.coeff (p ^ k)) g = 0) (hg : PowerSeries.subst F.toPowerSeries g = PowerSeries.subst (MvPowerSeries.X 0) g + PowerSeries.subst (MvPowerSeries.X 1) g) (hβ‚€' : PowerSeries.constantCoeff g' = 0) (h₁' : (PowerSeries.coeff 1) g' = 1) (hpow' : βˆ€ (k : β„•), 0 < k β†’ (PowerSeries.coeff (p ^ k)) g' = 0) (hg' : PowerSeries.subst F.toPowerSeries g' = PowerSeries.subst (MvPowerSeries.X 0) g' + PowerSeries.subst (MvPowerSeries.X 1) g') :
g = g'

Uniqueness of the normalised logarithm in characteristic p. Let p be a prime with p = 0 in R, and let F be a formal group law over R, not necessarily commutative. Two power series g, g' = X + β‹― without terms of degree pᡏ, k β‰₯ 1, that are additive along F agree.

Indeed g - g' is a homomorphism from F to the additive formal group law, and a nonzero such homomorphism has order a power of p.

The normalised logarithm of a formal group law of infinite height. Let p be a prime and let F be a commutative formal group law over a commutative ring R with [p]_F = 0. There is a unique power series g(X) = X + βˆ‘_{i β‰₯ 2} aα΅’ Xⁱ with a_{pᡏ} = 0 for every k β‰₯ 1 such that g(F(X, Y)) = g(X) + g(Y).

A formal group law of infinite height is additive. If p is a prime and F is a commutative formal group law with [p]_F = 0, then F is strictly isomorphic to the additive formal group law.

Formal group laws of infinite height are the additive ones. Over a field K of characteristic p, a commutative formal group law has height ⊀ exactly when it is isomorphic to the additive formal group law.