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Appendix: Hypergeometric functions [024C]

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Appendix: Hypergeometric functions

Recall that the hypergeometric function F12​[a,b;c;z]\,{}_{2}F_{1}[a,b;c;z] is defined by

2F1[a,b;c;z]=∑n=0∞(a)n​(b)nn!​(c)nzn\,_{2}F_{1}[a,b;c;z]=\sum_{n=0}^{\infty}\frac{(a)_{n}(b)_{n}}{n!(c)_{n}}z^{n} (38)

where

(α)n:=α(α+1)(α+2)⋯(α+n−1),(α)0=1(\alpha)_{n}:=\alpha(\alpha+1)(\alpha+2)\cdots(\alpha+n-1),\quad(\alpha)_{0}=1

and we assume that c∉ℤ≤0c\notin\mathbb{Z}_{\leq 0}. It is a standard fact that the hypergeometric series converges when |z|<1|z|<1 and when Re⁡(c−a−b)>0{\rm Re}(c-a-b)>0 is also converges when z=1z=1; see for instance [1, Chapter 1].

We start from the elementary Taylor expansion

(1−y)−β=∑k=0∞(β)kk!​yk,|y|<1.(1-y)^{-\beta}=\sum_{k=0}^{\infty}\frac{(\beta)_{k}}{k!}y^{k},\quad|y|<1.
Lemma 5.2.

For x≥1x\geq 1 we have

∫1x(1−y−2)−1/ndy=x2F1[−12,1n;12;x−2]−2F1[−12,1n;12;1].\int_{1}^{x}(1-y^{-2})^{-1/n}dy=x\,_{2}F_{1}[-\frac{1}{2},\frac{1}{n};\frac{1}{2};x^{-2}]-\,_{2}F_{1}[-\frac{1}{2},\frac{1}{n};\frac{1}{2};1].
Proof.

We compute

∫1x(1−y−2)−1/ndy=∫1x∑k=0∞(1n)kk!y−2​kdy=y∑k=0∞(1n)kk!y−2​k(−2​k+1)|y=1y=x.\displaystyle\int_{1}^{x}(1-y^{-2})^{-1/n}dy=\int_{1}^{x}\sum_{k=0}^{\infty}\frac{(\frac{1}{n})_{k}}{k!}y^{-2k}dy=y\sum_{k=0}^{\infty}\frac{(\frac{1}{n})_{k}}{k!}\frac{y^{-2k}}{(-2k+1)}\bigg|_{y=1}^{y=x}.

The Lemma follows from the observation (−12)k(12)k=−12​k−1.\frac{(-\frac{1}{2})_{k}}{(\frac{1}{2})_{k}}=-\frac{1}{2k-1}. ∎

Proposition 5.3.

Let n≥3n\geq 3. Suppose gg satisfies the ODE

dd​y​(gy)=1y2​(1−yn)12,0<y<1,\frac{d}{dy}\left(\frac{g}{y}\right)=\frac{1}{y^{2}(1-y^{n})^{\frac{1}{2}}},\qquad 0<y<1,

together with the initial conditions g⁡(0)=−1,g′​(0)=0g(0)=-1,g^{\prime}(0)=0. Then we have

g(y)=−2F1[12,−1n;n−1n;yn].g(y)=-\,_{2}F_{1}[\frac{1}{2},-\frac{1}{n};\frac{n-1}{n};y^{n}].

In particular

g(1)=limy→1g(y)=−2F1[12,−1n;n−1n;1]=−Γ⁡(n−1n)​πΓ⁡(n−22​n).g(1)=\lim_{y\to 1}g(y)=-\,_{2}F_{1}[\frac{1}{2},-\frac{1}{n};\frac{n-1}{n};1]=-\frac{\Gamma(\frac{n-1}{n})\sqrt{\pi}}{\Gamma(\frac{n-2}{2n})}.
Proof.

Integrating

y−2(1−yn)−1/2=∑k=0∞(12)kk!yn​k−2,y^{-2}(1-y^{n})^{-1/2}=\sum_{k=0}^{\infty}\frac{(\frac{1}{2})_{k}}{k!}y^{nk-2},

and utilizing the initial conditions to fix the leading coefficients,

g⁡(y)=∑k=0∞(12)kk!​yn​kn​k−1.g(y)=\sum_{k=0}^{\infty}\frac{(\frac{1}{2})_{k}}{k!}\frac{y^{nk}}{nk-1}.

The formula for g⁡(y)g(y) follows from the observation −1n​k−1=(−1n)k(n−1n)k.\frac{-1}{nk-1}=\frac{(-\frac{1}{n})_{k}}{(\frac{n-1}{n})_{k}}. The evaluation of g⁡(1)g(1) appeals to Gauss’ hypergeometric theorem [1, Section 1.3]:

Lemma 5.4.

For a,b,ca,b,c with Re⁡(c−a−b)>0{\rm Re}(c-a-b)>0 we have

F12​[a,b;c;1]=Γ⁡(c)​Γ​(c−a−b)Γ⁡(c−a)​Γ​(c−b).\,{}_{2}F_{1}[a,b;c;1]=\frac{\Gamma(c)\Gamma(c-a-b)}{\Gamma(c-a)\Gamma(c-b)}.

∎

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