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Shifted log-Gamma branch is independent of the shift

Statement

For every z∈Ω=C∖(−∞,0], the value ℓ(z) in Log-Gamma branch on the slit plane is independent of the integer m≥0 with Re⁡(z+m)>0, is holomorphic on Ω, and satisfies eℓ(z)=Γ(z).

Facts & Assumptions

Given: z∈Ω and the branch definitions Log-Gamma branch on the right half-plane and Log-Gamma branch on the slit plane.

[F1]

Weierstrass log-Gamma series converges to a Gamma branch: eℓ+(w)=Γ(w) and ℓ+ is holomorphic for Re⁡w>0.

[F2]

The Gamma functional equation: if Re⁡w>0, then Γ(w+1)=wΓ(w).

[F3]

Gamma functional equation away from the poles: the same functional equation holds when w is not a nonpositive integer.

[F6]

A differentiable map on a connected open Euclidean set has zero derivative exactly when it is constant: a holomorphic function with zero derivative on a connected open domain is constant.

[F7]

exp⁡(z+w)=exp⁡z exp⁡w, and the complex exponential extends the real exponential and The complex exponential by its power series: exp⁡(u+v)=exp⁡(u)exp⁡(v) and exp⁡(0)=1. In particular, exp⁡(−v) is the reciprocal of exp⁡(v).

[F9]

Real and imaginary parts, complex conjugation, and modulus, Real and complex modulus product and triangle inequalities, and Every path-connected space is connected, and every path component lies inside a component: the right half-plane is open, since if x=Re⁡w0>0 and ∣w−w0∣<x, then Re⁡w≥x−∣Re⁡(w−w0)∣≥x−∣w−w0∣>0. For w0,w1 in it, γ(t)=(1−t)w0+tw1 has positive real part and ∣γ(t)−γ(s)∣=∣t−s∣∣w1−w0∣, which proves continuity by the metric definition. The half-plane contains 1 and is open and connected.

[F10]

Complex differentiability is equivalent to real total differentiability together with a complex-linear derivative, with ∂zˉf=0, or with the Cauchy–Riemann equations: under C≅R2, a complex-differentiable function is totally differentiable and its real derivative is multiplication by its complex derivative; in particular, H′=0 implies DH=0.

Proof

1.1F1F2F4F5F6F7F8F9F10algebra

For Re⁡w>0, the function H(w)=ℓ+(w+1)−ℓ+(w)−Log⁡w is holomorphic by [F1]. The functional equation [F2], branch identity [F1], and exp⁡(Log⁡w)=w from [F4] give exp⁡(ℓ+(w+1))=exp⁡(ℓ+(w)+Log⁡w). By [F7], exp⁡(H(w))=1. Differentiating this identity by [F5] gives exp⁡(H(w))H′(w)=0, hence H′(w)=0. By [F10], the real derivative of H vanishes; the right half-plane is nonempty, open, and connected by [F9], so [F6] makes H constant there. For positive real w, all three terms are real by the defining series for ℓ+ and the real logarithm, so [F8] and exp⁡(H(w))=1 imply H(w)=log⁡1=0. Therefore ℓ+(w+1)=ℓ+(w)+Log⁡w throughout the right half-plane.

2.1givenstep 1.1algebra

If m2>m1 are both admissible shifts, then w=z+m1 has positive real part, as do w,w+1,…,w+(m2−m1−1). Iterating step 1.1 gives ℓ+(z+m2)−∑j=0m2−1Log⁡(z+j)=ℓ+(z+m1)−∑j=0m1−1Log⁡(z+j), so the definition is independent of m. Locally m can be fixed, making the formula holomorphic; independence makes these local formulas agree.

3.1F1F3step 2.1algebra∎

Exponentiating the formula with any admissible m gives eℓ(z)=Γ(z+m)/∏j=0m−1(z+j) by [F1]. None of the factors vanishes because z∈Ω. Iterating [F3] downward therefore identifies this quotient with Γ(z).

Depends on

Used by

Cited to discharge well-definedness by Log-Gamma branch on the slit plane.

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