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TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-16
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On a positively oriented circle about a, the integral of (z-a)^m is zero for every integer m except -1, and is 2 pi i for m=-1

Statement

Let a∈C, r>0, and γ(t)=a+rexp⁡(it) for 0≤t≤2π. For every integer m, ∫γ(z−a)m dz={2πi,m=−1,0,m≠−1.

Facts & Assumptions

Given: The positively oriented circle γ and an integer m.

[L1]

On a piecewise-C1 contour, the Riemann–Stieltjes integral agrees with ∫f(γ(t))γ′(t) dt (For piecewise-C1 contours the Riemann–Stieltjes integral agrees with the parametric complex integral and the published real line integrals).

[L2]

Negative integer powers are defined exactly for nonzero complex bases (Integer powers in the complex field).

[L3]

The complex exponential is entire with derivative itself and satisfies exp⁡(z+w)=exp⁡zexp⁡w (The complex exponential is entire and its complex derivative is itself, exp⁡(z+w)=exp⁡z exp⁡w, and the complex exponential extends the real exponential).

[L4]

For real x,y, exp⁡(x+iy)=ex(cos⁡y+isin⁡y) and ∣exp⁡(x+iy)∣=ex; in particular eiπ+1=0 (exp⁡(x+iy)=ex(cos⁡y+isin⁡y), ∣exp⁡(x+iy)∣=ex, and eiπ+1=0).

[L5]

If a real function G is differentiable on [a,b] and G′ is integrable, then ∫abG′=G(b)−G(a) (The second fundamental theorem: if G is differentiable on [a,b] with G′=f and f is integrable, then ∫abf=G(b)−G(a)).

[L6]

Proof

technique · cases
1.1L1L2L3algebra

Since r>0, γ(t)−a≠0, so all integer powers in [L2] are defined. By [L1] and [L3], the integrand becomes irm+1exp⁡(i(m+1)t).

2.1assume-case exceptionalstep 1.1algebra

If m=−1, the expression in step 1.1 is the constant i, whose integral from 0 to 2π is 2πi.

2.2assume-case regularstep 1.1L3L4L5L6algebra

If m≠−1, an antiderivative is rm+1exp⁡(i(m+1)t)/(m+1) by [L3]. Apply the real theorem [L5] to its two components using [L6]; the complex integral is the endpoint difference rm+1(exp⁡(2πi(m+1))−1)/(m+1). Write k:=m+1, a nonzero integer. For k>0 the addition law in [L3] gives exp⁡(2πik)=exp⁡(iπ)2k, and exp⁡(iπ)=−1 by [L4], so exp⁡(2πik)=(−1)2k=1; for k<0 the addition law gives exp⁡(2πik)exp⁡(−2πik)=exp⁡(0)=1 with exp⁡(−2πik)=1 by the previous case, so again exp⁡(2πik)=1. The endpoint difference is therefore 0.

3.1step 2.1step 2.2cases-exhaustive∎

The integer cases m=−1 and m≠−1 are exhaustive, proving the formula.

Depends on

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Sources