§ 8. Convergence of the Hausdorff series (ultrametric case)
In this paragraph we assume that K is a non-discrete complete valued field of characteristic zero, with an ultrametric absolute value. We denote by p the characteristic of the residue field of K (Commutative Algebra, Chapter VI, § 3, no. 2). If p=0, we write a=∣p∣; we know (Commutative Algebra, Chapter VI, § 6, nos. 2 and 3) that 0<a<1 and that there exists one and only one valuation v on K with values in R whose restriction to Q is the p-adic valuation vp and which is such that ∣x∣=av(x) for all x∈K. Also we write: (1) θ=p−11.
If p=0, we denote by a a real number such that 0<a<1 and by v a valuation on K with values in R such that ∣x∣=av(x) for all x∈K (loc. cit.). Then v(x)=0 for x∈Q∗. Also we write:
θ=0.
1. p-adic upper bounds of the series exp, log and H
In this no. we assume that p=0.
Lemma 1
Let n be an integer ⩾0 and let n=n0+n1p+⋯+nkpk, with 0⩽ni⩽p−1, be the p-adic expansion of n. Let S(n)=n0+n1+⋯+nk. Then*
vp(n!)=p−1n−S(n).
vp(n!)=∑i=1nvp(i) and the number of integers i between 1 and n for which vp(i)⩾j is equal to the integral part [n/pj] of n/pj. Then
vp(n!)=j⩾0∑j([n/pj]−[n/pj+1])=j⩾1∑[n/pj].
As [n/pj]=∑i⩾jnipi−j, the lemma follows.
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v(n)⩽v(n!)⩽(n−1)θ and v(n)⩽(logn)/(logp) for every integer n⩾1. v(n!)=vp(n!)=(n−S(n))θ⩽(n−1)θ by Lemma 1. On the other hand, n⩾pv(n), whence v(n)⩽(logn)/(logp). Let I={U,V} be a set of two elements and let
H=r,s⩾0∑Hr,s(U,V)∈L^Q(I)
be the Hausdorff series (§ 6, no. 4, Definition 1). Let Z(p) be the local ring of Z relative to the prime ideal (p) and (eb)b∈B a basis of LZ(p)(I) over Z (§ 2, no. 11, Theorem 1). It is also a basis of LQ(I) over Q.
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Let f be the integer such that f≤(r+s−1)θ<f+1. Relation (4) is equivalent to vp(λb)≥−f for all b∈B, that is Hr,s∈p−fLZ(p). But this is equivalent also by (5) to Hr,s∈p−fAZ(p)(I).
By formula (11) of § 6, no. 4, it suffices to show that, for every integer m≥1 and all integers r1,…,rm,s1,…,sm such that
r1+⋯+rm=r,s1+⋯+sm=s,
ri+si≥1for 1≤i≤m,
we have
vp(m!r!…rm!s1!…sm!)≤f.
But by Lemma 2, vp(ri!si!)≤(ri+si−1)θ and vp(m!)≤vp(m!)≤(m−1)θ; the left hand side of (7) is therefore bounded above by
θ(m−1+i=1∑m(ri+si−1))=θ(r+s−1);
as it is an integer, it is ≤f, which completes the proof.
2. Normed Lie algebras
Definition 1
A normed Lie algebra over K* is a Lie algebra with a norm such that
∥x+y∥≤sup(∥x∥,∥y∥)
∥[x,y]∥≤∥x∥⋅∥y∥
for all x,y in g.
Throughout the rest of this paragraph, g denotes a complete normed Lie algebra.
For every finite set I we define as in § 7, no. 1 a continuous Lie algebra homomorphism u↦u~ of L^(I) into P^(gI;g). We see as in § 7 that if u=∑vuv, with uv∈Lv(I) for v∈NI, then u~=∑vu~v, where u~v is the polynomial mapping (ti)i∈I↦uv((ti)) defined in § 2, no. 4. The composition formula (2) of § 7, no. 1, remains valid.
3. Group defined by a complete normed Lie algebra
Let H=∑r,s≥0Hr,s∈L^({U,V}) be the Hausdorff series (§ 6, no. 4, Definition 1). We shall show that the corresponding formal power series with continuous components
H~=r,s≥0∑H~r,s∈P^(g×g,g)
is convergent (Differentiable and Analytic Manifolds, R, 4.1.1).
Let r≥0,s≥0 be such that r+s=0 and let ∥H~r,s∥ be the norm of the continuous polynomial H~r,s (Differentiable and Analytic Manifolds, R, Appendix, no. 2).
Let B be a Hall set relative to I and let Hr,s=∑b∈Bλbeb be the decomposition of Hr,s with respect to the corresponding basis of L({U,V}). Then
∣λb∣≤a−(r+s−1)θ.
This is trivial for p=0, for λb∈Q; and it follows from Proposition 1 of no. 1 for p=0.
Moreover,
∥e~b∥≤1for b∈B.
We show more generally by induction on n that, for every alternant b of degree n in the two indeterminates U and V (§ 2, no. 6), ∥b~∥≤1. If n=1, b~ is one of the projections of g×g onto g and hence is of norm ≤1; if n>1, there exist two alternants b1 and b2 of degrees <n such that b=[b1,b2]. As the mapping γ:(x,y)↦[x,y] of g×g into g is bilinear of norm ≤1, we have (Differentiable and Analytic Manifolds, R, Appendix, no. 4)
∥b~∥=∥γ∘(b~1,b~2)∥≤∥b~1∥⋅∥b~2∥≤1.
Relations (11) and (12) imply the lemma.
Proposition 2
The formal power series H~ is a convergent series (Differentiable and Analytic Manifolds, R, 4.1.1). If G is the ball {x∈g∣∥x∥<aθ}, the domain of absolute convergence of H~ (Differentiable and Analytic Manifolds, R, 4.1.3) contains G×G.
This function is called the Hausdorff function of g.
Let (x,y)∈G×G. Then
∥H~r,s(x,y)∥≤sup(∥x∥,∥y∥)∥h(x,y)∥≤sup(∥x∥,∥y∥).
(17) follows immediately from (16) and (16) is trivial for r=s=0; if r≥1, then
∥H~r,s(x,y)∥≤∥H~r,s∥∥x∥r∥y∥s
≤∥x∥(aθ∥x∥)r−1(aθ∥y∥)s
≤∥x∥;
we argue similarly if s≥1.
In particular, ∥h(x,y)∥<aθ for (x,y)∈G×G.
Proposition 3
Let G be the ball {x∈g∣∥x∥<aθ}. The analytic mapping*
h:G×G→G
makes G into a group in which 0 is the identity element and −x is the inverse of x for all x∈G. Moreover, if R is a real number such that 0<R<aθ, the ball
{x∈g∣∥x∥<R}
(resp. {x∈g∣∥x∥≤R}) is an open subgroup of G.
As H(U,−U)=0 and H(0,U)=H(U,0)=U, h(x,−x)=0 and
h(0,x)=h(x,0)=x
for all x∈G. It therefore remains to prove the associativity formula
4. Exponential in complete normed associative algebras
In this no. A will denote a unital associative algebra with a norm x↦∥x∥ satisfying the conditions:
∥x+y∥≤sup(∥x∥,∥y∥)∥xy∥≤∥x∥⋅∥y∥∥1∥=1
for x,y in A, and complete with this norm. The results of the second and third paragraphs of § 7, no. 3, remain valid.
We take I={U} and consider the images e~ and l~ of the series e(U)=∑n≥1n!Un and l(U)=∑n≥1(−1)n−1nUn in P^(A;A). Then:
(n!Un)∼≤a−(n−1)θ
(nUn)∼≤a−logplogn
by Lemma 2 of no. 1. Hence the radius of absolute convergence of the series e~ (resp. l~) is ≥aθ (resp. ≥1) (Differentiable and Analytic Manifolds, R, 4.1.3). For R>0, let GR={x∈A∣∥x∥<R}; we write G=G0. The series e~ (resp. l~) defines an analytic mapping eA (resp. lA) of G (resp. G1) into A. We write:
(we omit the index A when no confusion can arise). For x∈GR and n≥1,
nxn≤n!xn<Rna−(n−1)θ=R(aθR)n−1
and hence eA(GR)⊂GR, lA(GR)⊂GR for R≤aθ.
Proposition 4
Let R be a real number such that 0<R≤aθ. The mapping expA defines an analytic isomorphism of GR onto 1+GR and the inverse isomorphism is the restriction of logA to 1+GR.
If A is given the bracket [x,y]=xy−yx, A becomes a complete normed Lie algebra, for ∥xy−yx∥≤sup(∥xy∥,∥yx∥)≤∥x∥⋅∥y∥. Proposition 2 of no. 3 implies that the domain of absolute convergence of H~ contains G×G and H~ therefore defines an analytic function h:G×G→A; then
h(x,y)=r,s≥0∑Hr,s(x,y).
Proposition 5
For x, y in G,
expA⋅expAy=expAh(x,y).
eUeV=eH(U,V) and hence
m∘(1+ϵ~,1+ϵ~)=(1+ϵ~)∘H~
in H~(A×A;A) (where m denotes multiplication on A). The proposition then follows from Proposition 2, Lemma 3 and Differentiable and Analytic Manifolds, R, 4.1.5.
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