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Green kernel of a slit plane via the square-root map

Example

Let Ω=C∖(−∞,0] be the slit plane, let a,z∈Ω with z≠a, and let   be the principal square root of Complex powers defined from a holomorphic logarithm branch, so that Re⁡w>0 for w∈Ω. Then the canonical Green kernel of The canonical Green kernel of a plane domain is gΩ(z,a)=log⁡∣z+a‾z−a∣. The kernel tends to zero at every point of the slit and at infinity. This is an unbounded domain, and no general Euclidean boundary map is used: the boundary value at the slit is read off directly from the explicit formula.

Facts & Assumptions

Given: The slit plane Ω=C∖(−∞,0], points a,z∈Ω with z≠a, and the right half-plane H={w∈C:Re⁡w>0}. Conjugates and moduli are those of Real and imaginary parts, complex conjugation, and modulus, complex domains are those of A complex domain is a nonempty connected open subset of C, and the canonical Green kernel is that of The canonical Green kernel of a plane domain.

[F1]

For a proper plane domain D and b∈D the canonical Green function gD(⋅,b), when it exists, is the pointwise least nonnegative function that is harmonic on D∖{b} and satisfies: gD(⋅,b)+log⁡∣⋅−b∣ extends harmonically across b (The canonical Green kernel of a plane domain).

[F2]

For every integer n≥1, the map Rn(z)=exp⁡(Log⁡z/n) is a biholomorphism from the slit plane onto the sector Vn={reiθ:r>0, ∣θ∣<π/n}, with inverse w↦wn; for n=2 this is a biholomorphism  :Ω→H with inverse w↦w2, and both Ω and H are complex domains (A slit-plane root branch biholomorphically parametrizes a sector, Biholomorphic maps between complex domains, Complex powers defined from a holomorphic logarithm branch).

[F3]

The function log⁡∣⋅∣ is harmonic on C∖{0} (Logarithmic modulus is harmonic off its centre), and the composition of a harmonic function with a holomorphic map is harmonic (Plane harmonicity is preserved by holomorphic and antiholomorphic changes of coordinate).

[F4]

If u is continuous on the closure of a bounded complex domain and harmonic inside, then sup⁡D‾u=sup⁡∂Du and inf⁡D‾u=inf⁡∂Du (Maximum and minimum principles for plane harmonic functions).

Verification

technique · direct
1.1F1F2F3givenalgebra

Put β:=a, so that β∈H by [F2] and Re⁡β>0. Define q(w):=log⁡∣w+β‾∣−log⁡∣w−β∣(w∈H∖{β}). The translations w↦w+β‾ and w↦w−β are holomorphic and are nonzero on H and H∖{β}, respectively; by [F3], their logarithmic moduli are harmonic on those sets. (The real part of w−β may vanish away from β, but the complex number w−β is still nonzero there.) Hence q is harmonic on H∖{β}. Writing w=u+iv with u=Re⁡w and β=α+iγ, α>0, gives ∣w+β‾∣2−∣w−β∣2=(u+α)2−(u−α)2=4uα, so ∣w+β‾∣≥∣w−β∣ with equality exactly on the imaginary axis; thus q≥0 on H. Finally q(w)+log⁡∣w−β∣=log⁡∣w+β‾∣ is harmonic across w=β, since β+β‾=2α≠0 makes w+β‾ nonvanishing near β. So q is a nonnegative logarithmic-pole candidate at β in the sense of [F1].

2.1F1step 1.1

Let k be any nonnegative logarithmic-pole candidate at β on H and put u:=k−q. On H∖{β} the function u is harmonic as a difference of harmonic functions, and it extends harmonically across β: by the defining property in [F1] both k(w)+log⁡∣w−β∣ and q(w)+log⁡∣w−β∣=log⁡∣w+β‾∣ are harmonic in a neighbourhood of β, and u is their difference off β.

2.2F2F3step 1.1

Define G(z):=q(z)=log⁡∣(z+β‾)/(z−β)∣ for z∈Ω∖{a}. Then G≥0 by step 1.1, and G is harmonic on Ω∖{a} by [F3], because  :Ω→H is holomorphic by [F2] and z=β holds exactly for z=a, by the inverse property in [F2].

3.1F1F4step 1.1step 2.1algebra

Fix R>∣β∣ and δ∈(0,α/2), where α=Re⁡β, and set D:={w:Re⁡w>δ, ∣w∣<R}, a bounded complex domain with D‾⊆H. By step 2.1 the function −u is harmonic on D and continuous on D‾, so its supremum on D‾ is attained on ∂D by [F4]. On the circular arc {∣w∣=R, Re⁡w≥δ} one has ∣w+β‾∣≤R+∣β∣ and ∣w−β∣≥R−∣β∣>0, hence −u=q−k≤q≤log⁡R+∣β∣R−∣β∣=:cR, because k≥0 and q≥0. On the vertical segment {Re⁡w=δ, ∣w∣≤R} one has −u≤q and, since ∣w−β∣≥α/2 there, ∣w+β‾∣−∣w−β∣=∣w+β‾∣2−∣w−β∣2∣w+β‾∣+∣w−β∣=4δα∣w+β‾∣+∣w−β∣≤4δαα/2=8δ, so q=log⁡(1+∣w+β‾∣−∣w−β∣∣w−β∣)≤8δα/2=16δα. Therefore −u≤max⁡{cR,16δ/α} on D. Letting δ↓0 for fixed w∈H with R>∣w∣ gives −u(w)≤cR, and letting R→∞ gives −u(w)≤0, since cR=log⁡(1+2∣β∣R−∣β∣)→0. Hence k≥q on H, and q is the canonical Green kernel gH(⋅,β) of the half-plane by [F1].

3.2F1F2F3step 2.2algebra

The function G has the logarithmic pole at a. For z∈Ω∖{a} the factorization z−a=(z−β)(z+β) of [F2] gives log⁡∣z−β∣=log⁡∣z−a∣−log⁡∣z+β∣, hence G(z)+log⁡∣z−a∣=log⁡∣z+β‾∣+log⁡∣z+β∣=log⁡∣z+2(Re⁡β)z+∣β∣2∣, and the holomorphic function h(z):=z+2(Re⁡β)z+∣β∣2 on Ω satisfies h(a)=4βRe⁡β≠0. So z↦log⁡∣h(z)∣ is harmonic on a neighbourhood of a by [F3], and G+log⁡∣⋅−a∣ extends harmonically across a. Together with steps 1.1 and 2.2 this shows that G is a nonnegative logarithmic-pole candidate at a on Ω.

4.1F1F2F3step 3.1step 2.2step 3.2algebra

Leastness on Ω: let k be any nonnegative logarithmic-pole candidate at a on Ω and define K(w):=k(w2) for w∈H. Then K≥0, and K is harmonic on H∖{β} by [F3], since w↦w2 is holomorphic by [F2] and w2=a holds exactly for w=β. Moreover, for w≠β the identity w2−a=(w−β)(w+β) gives K(w)+log⁡∣w−β∣=(k(w2)+log⁡∣w2−a∣)−log⁡∣w+β∣, where k(⋅)+log⁡∣⋅−a∣ is harmonic near a by [F1], so its composition with w↦w2 is harmonic near β, and log⁡∣w+β∣ is harmonic near β because 2β≠0. Thus K is a nonnegative logarithmic-pole candidate at β on H, and step 3.1 gives K≥q on H. For z∈Ω, writing z=w2 with w=z∈H by [F2], we obtain k(z)=K(w)≥q(w)=G(z). Hence every candidate dominates G, so G is the pointwise least candidate and gΩ(z,a)=G(z)=log⁡∣(z+a‾)/(z−a)∣ by [F1].

5.1F2step 1.1step 4.1algebra

Boundary limits on the slit. Let ζ≤0 and let zn∈Ω with zn→ζ; put wn:=zn∈H. Since wn2=zn, the identity 2(Re⁡wn)2=∣wn∣2+Re⁡(wn2)=∣zn∣+Re⁡zn gives Re⁡wn→0 because ∣zn∣+Re⁡zn→∣ζ∣+ζ=0 for ζ≤0. Consequently ∣wn+β‾∣2−∣wn−β∣2=4(Re⁡wn)(Re⁡β)→0 by step 1.1, while ∣wn−β∣≥Re⁡β−Re⁡wn≥Re⁡β/2 for all large n; hence the quotient ∣wn+β‾∣/∣wn−β∣ tends to 1 and gΩ(zn,a)=q(wn)→0. So the kernel has limit 0 at every point of the slit (−∞,0]=∂Ω.

6.1givenstep 1.1step 4.1algebra∎

Limit at infinity. For ∣z∣>4∣β∣2 one has ∣w∣=∣z∣>2∣β∣, so 0≤gΩ(z,a)=q(w)≤log⁡∣w∣+∣β∣∣w∣−∣β∣=log⁡(1+2∣β∣∣w∣−∣β∣)≤2∣β∣∣w∣−∣β∣, which tends to 0 as ∣z∣→∞. Thus the kernel vanishes at the slit and at infinity, as claimed; all of the above is an explicit choice-free calculation, the boundary behaviour being read off from the formula z↦q(z) rather than from any Euclidean boundary correspondence.

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