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The flow of a bounded holomorphic field on a polydisc: existence in complex time, displacement bound, holomorphy, and the composition law

Statement

In this item, a complex-time solution on an open set Ω⊆C is a holomorphic map Y:Ω→D satisfying Y′(τ)=F(Y(τ)). For a closed time disc, a solution means the restriction of such a map that is continuous on the closed disc.

Let n≥1, let D⊆Cn be open, let F:D→Cn be holomorphic in the sense of Complex phase domains, holomorphic maps on Cm, and the complexified canonical form and bracket with ∥F∥≤M everywhere on D for some M>0, let Z0∈D and let s>0 satisfy Δs(Z0)⊆D (Complex phase domains, holomorphic maps on Cm, and the complexified canonical form and bracket). Put

t0:=s8nM,Dt0:={t∈C: ∣t∣≤t0}.

Then there is a map Φ:Dt0×B(Z0,s/4)→D that is the restriction of a jointly holomorphic map on {∣t∣<3t0/2}×B(Z0,s/4), such that:

  1. Solution. For every Z∈B(Z0,s/4), t↦Φ(t,Z) solves Y′=F(Y) with Y(0)=Z for ∣t∣<3t0/2. It is the unique holomorphic solution on ∣t∣<t0 among solutions with values in B(Z,s/2). On Dt0 it satisfies ∥Φ(t,Z)−Z∥≤M∣t∣≤s/(8n).
  2. Holomorphy. Φ is holomorphic on the open set {∣t∣<t0}×B(Z0,s/4) in the sense of Complex phase domains, holomorphic maps on Cm, and the complexified canonical form and bracket, and Φ(0,Z)=Z.
  3. Composition and inverse. Repeating the construction with each initial point as a center gives a family of compatible local maps; in this clause Φ(t,Z) denotes the map in the chart centered at Z. If the two sides are defined by branches on the same connected open continuation of a solution, then Φ(s2,Φ(s1,Z))=Φ(s1+s2,Z). In particular, along the reverse continuation of the same local solution, Φ(−s1,Φ(s1,Z))=Z whenever both sides are defined.

Facts & Assumptions

Given: The open D⊆Cn, the holomorphic F with ∥F∥≤M on D, the point Z0, the radius s with Δs(Z0)⊆D, and t0=s/(8nM).

[L1]

Scalar Cauchy estimates on polydiscs (Iterated Cauchy formula, power-series expansion and Cauchy estimates for functions continuous and separately holomorphic on a polydisc): if a scalar holomorphic g is bounded by A on the distinguished boundary of a polydisc of radius r about W, then ∣∂zkg(W)∣≤A/r. Applying this to each component Fi gives ∣∂zkFi(W)∣≤4M/s whenever Δs/4(W)⊆D. Thus the Euclidean norm of the k-th column of DF(W) is at most 4nM/s. For v∈Cn, ∥DF(W)v∥≤(4nM/s)∑k∣vk∣≤(4nM/s)∥v∥, using (∑k∣vk∣)2≤n∑k∣vk∣2. This supplies the claimed vector-valued Lipschitz constant without applying a scalar estimate directly to a vector-valued map.

[L2]

Calculus of holomorphic maps (Calculus of holomorphic maps: chain rule, Wirtinger derivatives, coefficient extraction in one variable, and locally uniform limits): compositions of holomorphic maps are holomorphic with the chain rule; a locally uniform limit of holomorphic maps is holomorphic.

[L3]

Parameter integrals (A jointly continuous finite-interval parameter integral of holomorphic functions is holomorphic): a jointly continuous scalar φ:[0,1]×Ω→C whose slices are holomorphic in the complex parameter has a holomorphic integral, with differentiation under the integral when the parameter derivative is jointly continuous. For a Cn-valued integrand, apply this scalar result to each of its n components; the resulting integral is holomorphic componentwise.

[L4]

Completeness and componentwise uniform limits. A uniformly Cauchy sequence of maps into Cn≅R2n has a pointwise limit: at each argument its 2n real coordinates are Cauchy and converge by The reals are complete, and assembling these limits gives a vector limit. A uniform tail bound in Euclidean norm passes to that limit by continuity of the norm, so convergence is uniform. Each component of a uniform limit of continuous Cn-valued maps is continuous by A uniform limit of continuous complex-valued functions is continuous; finitely many continuous components give a continuous vector map, since ∥v∥≤nmax⁡i∣vi∣. Likewise a locally uniform limit of holomorphic scalar functions is holomorphic by Locally uniform limits of holomorphic functions are holomorphic and their derivatives converge locally uniformly. For a finite vector of componentwise holomorphic functions, collect their scalar derivatives into one complex-linear map; the Euclidean norm of the vector of finitely many o(∥v∥) remainders is again o(∥v∥), so the vector map is holomorphic in the total-derivative sense.

[L5]

Integrals of continuous Cn-valued functions satisfy ∥∫01φ dσ∥≤∫01∥φ∥ dσ; the complex segment integral ∫0tψ(τ)dτ=t∫01ψ(σt) dσ is thereby controlled (For a≤b and f:[a,b]→Rm integrable when a<b, ∥∫abf∥2≤∫ab∥f∥2; for a<b, ∥f∥2 is integrable, The derivative and the Riemann integral of a vector-valued function: an intrinsic derivative and a componentwise integral).

[L7]

The vector-valued fundamental theorem of calculus gives ∫01u′(σ) dσ=u(1)−u(0) for a differentiable u:[0,1]→R2n with integrable derivative; its bounded-derivative clause says that if u is continuous and ∥u′(σ)∥≤A on (0,1), then ∥u(1)−u(0)∥≤A (If f:[a,b]→Rm is differentiable with integrable f′ then ∫abf′=f(b)−f(a); and a bounded derivative makes f Lipschitz, both clauses).

Proof

technique · constructive; Picard iteration with the contraction estimate on the polydisc $\Delta_{s/2}(Z_0)$, uniform Cauchy convergence, and slice-wise holomorphy of the limit
1.1givenL1L2L6L7

Lipschitz estimate. For every W with ∥W−Z0∥≤3s/4, the polydisc Δs/4(W) is contained in Δs(Z0)⊆D: each coordinate satisfies ∣ζk−Z0k∣≤∣Wk−Z0k∣+∣ζk−Wk∣<3s/4+s/4=s. By [L1], the operator norm of DF(W) is at most Λ=4nM/s. For W,W′∈B(Z0,3s/4) the segment u(t)=F(W′+t(W−W′)), 0≤t≤1, stays in the convex ball by [L6]; by the chain rule in [L2], its derivative is DF(W′+t(W−W′))(W−W′) and has norm at most Λ∥W−W′∥. Applying [L7] to this real-parameter curve gives ∥F(W)−F(W′)∥≤Λ∥W−W′∥. Since t0=s/(8nM), Λ=1/(2t0).

2.1givenstep 1.1L4L5L6algebra

The Picard map [construct]. Fix Z∈B(Z0,s/4) and let XZ be the set of continuous γ:Dt0→Cn with γ(0)=Z and ∥γ(t)−Z∥≤s/2 for all t∈Dt0, equipped with the supremum distance. Define Tγ by (Tγ)(t):=Z+t∫01F(γ(σt)) dσ. For γ∈XZ, the integrand is continuous; since ∥Z−Z0∥<s/4 and ∥γ(σt)−Z∥≤s/2, its values satisfy ∥γ(σt)−Z0∥<3s/4 and lie in D. Therefore ∥(Tγ)(t)−Z∥≤∣t∣M≤t0M=s/(8n)≤s/2: T maps XZ to itself. Moreover, by step 1.1 and [L5], for γ1,γ2∈XZ, ∥(Tγ1)(t)−(Tγ2)(t)∥≤∣t∣∫01Λ∥γ1(σt)−γ2(σt)∥ dσ≤t0Λ∥γ1−γ2∥∞=12∥γ1−γ2∥∞. The same construction on Dt∗ with t∗:=3t0/2 also works: t∗Λ=3/4<1 and t∗M=3s/(16n)<s/2, so the iterates have summable successive differences bounded by a geometric sequence with ratio 3/4 and remain in XZ. The coordinatewise completeness argument of [L4] gives their limit. Repeating steps 3.1--5.1 with this radius yields a solution holomorphic on ∣t∣<t∗, so the solution on Dt0 extends through its boundary.

3.1givenstep 2.1L1L2L3L4

Iterates. For each initial value Z, put γ0(t,Z):=Z and γm+1(⋅,Z):=T(γm(⋅,Z)); all γm(⋅,Z) lie in XZ by step 2.1, and ∥γm+1(⋅,Z)−γm(⋅,Z)∥∞≤2−m∥γ1(⋅,Z)−γ0(⋅,Z)∥∞≤2−mt0M. Joint continuity in (t,Z) follows by induction: γ0(t,Z)=Z is continuous, and if γm is jointly continuous then (σ,t,Z)↦F(γm(σt,Z)) is continuous; on each compact parameter neighborhood its σ-integral is continuous by uniform continuity. Each γm is also holomorphic on Dt0 in the variable t: γ0 is constant; if γm is holomorphic then t↦γm(σt) and its composition with F are holomorphic for each σ by [L2]. The parameter integral in the definition of T is holomorphic componentwise by [L3], so every component of Tγm is holomorphic in t; the finite-dimensional assembly described in [L4] makes the vector map holomorphic. For fixed t, the same induction shows that each component of γm(t,⋅) is holomorphic in each coordinate of Z: apply [L3] separately to each output component and each input coordinate. Thus the iterates are continuous and separately holomorphic in the variables needed below.

4.1givenstep 3.1L1L2L4

Uniform convergence. By step 3.1, (γm) is uniformly Cauchy on Dt0×B(Z0,s/4): ∥γm′−γm∥∞≤2−m+1t0M for m′≥m. By the coordinatewise completeness argument in [L4], it converges uniformly to a map Φ; the componentwise continuity argument in [L4] makes Φ continuous. It satisfies ∥Φ(t,Z)−Z∥≤s/2, indeed ≤M∣t∣≤s/(8n), and Φ(0,Z)=Z. For fixed Z, each component of t↦Φ(t,Z) is a locally uniform limit of holomorphic functions, so it is holomorphic by [L4]; the same applies to each output component with t fixed and one complex coordinate of Z varying. At any point of the open product choose a polydisc contained in it. Each scalar component is continuous and separately holomorphic there, so Iterated Cauchy formula, power-series expansion and Cauchy estimates for functions continuous and separately holomorphic on a polydisc makes that component holomorphic in the total-derivative sense; the finite-dimensional assembly in [L4] then makes Φ a holomorphic Cn-valued map.

5.1givenstep 4.1L2L3L5L7

Fixed point and differential equation. T is Lipschitz with constant 1/2 on XZ by step 2.1, so TΦ=lim⁡mTγm=lim⁡mγm+1=Φ uniformly. Put G(t):=F(Φ(t,Z)), which is holomorphic with continuous derivative on ∣t∣<t0 by step 4.1 and [L2]. The fixed-point identity is Φ(t,Z)=Z+t∫01G(σt) dσ. By the derivative formula in [L3], applied componentwise, ddtΦ(t,Z)=∫01G(σt) dσ+t∫01σG′(σt) dσ=∫01ddσ(σG(σt)) dσ=G(t)=F(Φ(t,Z)), where the penultimate equality is [L7] applied to the R2n-valued curve σ↦σG(σt). The fixed-point identity also gives Φ(0,Z)=Z and, by [L5], ∥Φ(t,Z)−Z∥≤M∣t∣≤s/(8n). This proves clause 1 except uniqueness, and clause 2.

6.1givenstep 2.1step 5.1L6discharge-construct∎

Uniqueness and composition. Two solutions in the prescribed curve ball obey the contraction inequality of step 2.1 and coincide. More generally, two local solutions through any point agree on a sufficiently small time disc by that same argument centred at the point; the set of times of agreement is both relatively open and closed in a connected common continuation, hence they agree there. For fixed s1, the curves t↦Φ(s1+t,Z) and t↦Φ(t,Φ(s1,Z)) have the same initial value and derivative F wherever both are defined. Local uniqueness, followed by this continuation argument, proves the qualified composition rule and, with t=−s1, the inverse rule. This proves all three clauses.

Remarks

  • The lemma is local by design: the time radius t0=s/(8nM) shrinks with the size of the field and with the complex margin, and the initial-data ball is B(Z0,s/4). Applying it at each point gives compatible local solution maps. Continued branches are used on specified connected time domains; the local construction does not select a single-valued global maximal flow.
  • Clause 1's uniqueness is asserted among solutions with values in the ball B(Z,s/2), which is what the contraction proof gives; no global uniqueness of complex-time solutions outside that ball is claimed.

Depends on

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