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The binomial family of the splitting pullback is multiplicative and bracket-preserving, and its logarithm is a derivation

Statement

Let d≥1, let (U,Uρ,A~,B~,M,K,δ,Ψh) be analytic splitting data, and use all notation of The truncated binomial family Ths,N, the truncated logarithm LN(h), its coefficient fields Xj and the truncations X[N]: the domains D(r) and Dk, the parameters b=ρ/(8N), rN=ρ/(C0MN), the binomial coefficients (sk), the difference operator Δh, the truncated family Ths,N and the truncated logarithm LN(h). Let f,g be holomorphic on D0, and put E:=D(ρ/4). For every Z∈D0 and finite k, joint local holomorphy of Ψh and Ψ0=id give a neighborhood of (0,Z) on which the first k iterates are defined and stay in D0. Define [hj](Δhkf)(Z) from this local holomorphic family. Compatible flow germs make these coefficients independent of the neighborhood; coefficient extraction makes them holomorphic on D0. On E they agree with the uniform construction at order Qj:=max⁡{2,j} for k≤j, where ∣h∣<rQj and E⊆Dk. Whenever Dj denotes a distance domain below, allocate it with order Qj; thus Dj⊆D0 even for j=0,1. For s∈C and Z∈D0 define the coefficient polynomial

Pj(s)f:=∑k=0j(sk) [hj](Δhkf),

where [hj](Δhkf):=1j!∂hj(Δhkf)∣h=0, and Pj(s)f is a polynomial of degree at most j in s with coefficients in the holomorphic functions on D0.

Then:

  1. Integer case. For all integers Q≥2, 0≤m≤Q and every ∣h∣≤rQ, Thm,Qf=f∘Ψhm (omit the zero summands with k>m to extend the finite sum) on the domain Dm allocated with order Q.
  2. Multiplicativity and bracket identity. For every j∈N and every s∈C, as identities of holomorphic functions on Dj, Pj(s)(fg)=∑j1+j2=jPj1(s)f⋅Pj2(s)g,Pj(s){f,g}=∑j1+j2=j{Pj1(s)f,  Pj2(s)g}.
  3. The logarithm is a derivation. Put Djf:=Pj′(0)f∈O(D0) (the derivative in s at s=0), so that Djf=[hj](L(h)f) for the formal logarithm L(h):=∑k≥1(−1)k+1kΔhk. Then D0=0, each Dj is a C-linear local differential operator on holomorphic functions, and Dj(fg)=Djf⋅g+f⋅Djg,Dj{f,g}={Djf, g}+{f, Djg} as functions on Dj; equivalently the coefficient of hj in L(h)(fg) and in L(h){f,g} obeys the product rule and the bracket derivation rule. Moreover Djf for h-degree j≤N agrees with the j-th coefficient of the concrete holomorphic function h↦LN(h)f restricted to ∣h∣≤rN whenever j≤N.

Moreover Djf=∑i(Djzi)∂zif for j≥1: each coefficient derivation is the coordinate vector field used in the later Hamiltonian construction.

Facts & Assumptions

Given: The analytic splitting data and all notational conventions of The truncated binomial family Ths,N, the truncated logarithm LN(h), its coefficient fields Xj and the truncations X[N]; holomorphic f,g on D0.

[L1]

Binomial algebra: the polynomial identity (1+x)m=∑k=0m(mk)xk for m∈N holds for the single operator Δh in the algebra of operators on functions holomorphic on the appropriate domains, because all powers of Δh commute; (mk)=0 for integers k>m; and dds(sk)∣s=0=(−1)k+1k for k≥1 with value 0 for k=0 (The truncated binomial family Ths,N, the truncated logarithm LN(h), its coefficient fields Xj and the truncations X[N], The factorial n! and the falling factorial nk‾, defined by recursion in N).

[L2]

Pullback calculus: (f∘Ψhm)=(f∘Ψh)∘Ψhm−1, and {f∘Ψhm,g∘Ψhm}={f,g}∘Ψhm for holomorphic f,g, by the chain rule and Hamiltonian flows and the exact splitting map preserve the complexified canonical form and the Poisson bracket clause 3; all maps involved are holomorphic (Calculus of holomorphic maps: chain rule, Wirtinger derivatives, coefficient extraction in one variable, and locally uniform limits, Complex phase domains, holomorphic maps on Cm, and the complexified canonical form and bracket).

[L3]

Domains: Dj⊆Dj′ for fixed truncation order and j≥j′, and rj≤rj′ for j≥j′; Dhkf is holomorphic on Dk for ∣h∣≤rk (The difference operator Δh=Ψh∗−id loses a controlled domain margin and is bounded by CdM∣h∣/b).

[L4]

Holomorphic functions of h: if h↦G(h) is holomorphic for ∣h∣≤r and A(h)=B(h) for all such h, then all Taylor coefficients at 0 agree; and a polynomial in s vanishing at s=0,1,2,… vanishes identically (Calculus of holomorphic maps: chain rule, Wirtinger derivatives, coefficient extraction in one variable, and locally uniform limits clause 3, Iterated Cauchy formula, power-series expansion and Cauchy estimates for functions continuous and separately holomorphic on a polydisc).

Proof

technique · direct; identify the integer family with pullbacks, compare Taylor coefficients in $h$, then use polynomiality in $s$ and differentiate at $s=0$
1.1givenL1L2L3

Local coefficients and integer case. On any sufficiently small common neighborhood, write Ψh(Z)=Z+hR(h,Z) with holomorphic R. If a holomorphic family G(h,Z) is O(hk), then G(h,Ψh(Z))−G(h,Z) is O(hk+1): factor hk and integrate the spatial derivative of the remaining family along the short segment from Z to Ψh(Z). Induction therefore gives Δhkf=O(hk) locally. We prove Thm,Mf=f∘Ψhm for 0≤m≤M and ∣h∣≤rM by induction on m. For m=0, Th0,Mf=(00)f=f. If it holds for m, then by [L1] id+Δh=Ψh∗ on the relevant domains and (1+Δh)m applied to f equals f∘Ψhm; applying id+Δh once more gives (f∘Ψhm)∘Ψh=f∘Ψhm+1 by [L2], while the binomial expansion over M≥m+1 reproduces Thm+1,Mf because (m+1k)=0 for k>m+1.

2.1givenstep 1.1L2L4L5

Multiplicativity and bracket identities at integer s. For an integer m with 0≤m≤M, both Thm,M(fg) and Thm,Mf⋅Thm,Mg equal (f∘Ψhm)(g∘Ψhm) on Dm by step 1.1; likewise Thm,M{f,g} and {Thm,Mf,Thm,Mg} both equal {f,g}∘Ψhm by step 1.1 and [L2]. At any Z∈D0, the same finite pullback identities hold as local germs for arbitrary fixed integers m,M with M≥m. Comparing Taylor coefficients in h of order j≤M on that neighborhood by [L4] and using that Δhkf contributes only at order ≥k gives, for every j and every integer m≥0 (choose an integer truncation M:=max⁡{2,m,j}, distinct from the field bound M in the splitting data), Pj(m)(fg)=∑j1+j2=jPj1(m)f⋅Pj2(m)g,Pj(m){f,g}=∑j1+j2=j{Pj1(m)f,Pj2(m)g}.

3.1givenstep 2.1L1L4

Polynomial extension. Both sides of each identity of step 2.1 are polynomials in m of degree at most j (for the j-coefficient, products of polynomials of degrees j1,j2 with j1+j2=j), and they agree at every integer m≥0; hence by [L4] they agree for every s∈C. This is clause 2.

4.1givenstep 3.1L1L3L4

Derivative at s=0. Differentiate the identities of clause 2 in s at s=0 and use [L1]: since P0(s)f=(s0)[h0](Δh0f)=f and Pj(0)f=0 for j≥1 (all coefficients (0k) vanish for k≥1), the product identity becomes Dj(fg)=Djf⋅g+f⋅Djg, and the bracket identity becomes Dj{f,g}={Djf,g}+{f,Djg}. By [L1] again, Djf=∑k=1j(−1)k+1k[hj](Δhkf)=[hj](L(h)f). Finally, L(h)≡LN(h) mod hN+1 because the two series differ by terms of order hk≥hN+1; hence for j≤N the coefficients agree, and h↦LN(h)f is holomorphic on ∣h∣≤rN by The difference operator Δh=Ψh∗−id loses a controlled domain margin and is bounded by CdM∣h∣/b clause 3, so its Taylor coefficients are the Djf.

5.1givenstep 1.1step 4.1L4algebra

Coordinate field identification. Fix Z∗∈D0. By the integer pullback identity, each Δhkf is a finite linear combination of f∘Ψhm with 0≤m≤k; for fixed m, Ψhm(Z∗) is holomorphic in h near 0, equals Z∗ at h=0, and differs from Z∗ by O(h). The Taylor expansion of f at Z∗ through total degree j has a remainder O(∥W−Z∗∥j+1), so replacing f by that Taylor polynomial changes none of the coefficients [hj](Δhkf)(Z∗) for k≤j. The product derivation rule of step 4.1 gives Dj1=0 and annihilates at Z∗ every monomial of degree at least two in Z−Z∗: split such a monomial into two factors vanishing at Z∗. Only the linear Taylor terms remain, yielding Djf(Z∗)=∑iDjzi(Z∗)∂zif(Z∗). Since Z∗ was arbitrary, this is the claimed local differential-operator formula on D0.

6.1step 1.1step 3.1step 4.1step 5.1∎

Conclusion. Clause 1 is step 1.1, clause 2 is step 3.1 and clause 3 is step 4.1 together with the C-linearity of s-differentiation at 0 and of the coefficient extraction.

Remarks

  • The key point is that the family is a polynomial in s at each h-degree, so the integer-s identities — which are the multiplicativity and bracket naturality of the pullback — extend to all complex s; differentiating at s=0 then produces the derivation identities used to build the modified Hamiltonian. No convergence of the full series ∑k(−1)k+1Δhk/k is asserted here: only the concrete truncated functions LN(h)f for ∣h∣≤rN and their coefficients of order ≤N are used.
  • All identities are on complex domains; no real-valuedness or physical interpretation is involved, and no choice principle is used.

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