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Context:

Reading this interesting paper: (https://arxiv.org/pdf/1607.04742.pdf) ("Special values of Gauss’s hypergeometric series derived from Appell’s series F1 with closed forms" by Akihito Ebisu). We find that the author obtains a lot of values of Gauss Hypergeometric function with a new approach. In particular we have: $$\sum_{n=0}^{\infty}\frac{(3n)!(2n)!(-1)^n}{n!^5}\left(\frac{1}{8640} \right)^n=\frac{9\cdot 5^{2/3}\cdot\Gamma(1/3)^6}{100\pi^4},\tag{1}$$ $$\sum_{n=0}^{\infty}\frac{(4n)!(-1)^n}{n!^4}\left(\frac{1}{6635520} \right)^n=\frac{3\cdot 5^{1/4}\cdot\Gamma(1/4)^4}{25 \pi^3}.\tag{2}$$

Guillera obtains values of Gauss Hypergeometric function with the WZ method: (https://arxiv.org/pdf/2001.08104.pdf), and then with Clausen's formula deduces some Ramanujan series for $1/\pi$.

Updated Level 3:

From the comments of Tito Piezas III we are going to give the transformation that allows us to obtain (1) using Ebisu's values. We take this version of Clausen's formula: $$\left(\sum_{n=0}^{\infty}\frac{f(a)f(b)}{f(2b)n!}x^n\right)^2=(1-x)^{-a}\sum_{n=0}^{\infty}\frac{f(a)f(b)f(2b-a)}{f(b+1/2)f(2b)n!}\left(\frac{x^2}{4(x-1)} \right)^n\tag{3}.$$ Where $f(x)=\frac{\Gamma{(x+n)}}{\Gamma{(x)}}=(x)_{n},$ is the Pochhammer symbol. Setting $a=1/3$ and $b=1/2$ in $(3)$ we have: $$_2F_1(\frac{1}{3},\frac{1}{2};1;x)^2=\frac{1}{(1-x)^{1/3}}\sum_{n=0}^{\infty}\frac{(2n)!(3n)!}{n!^5}\left(\frac{x^2}{432(x-1)}\right)^{n}\tag{4}.$$ Now using value $(E′′.1)$ (page 11 from Ebisu's paper) and setting in $(4)$ $x=\frac{1}{5}$ we have $(1)$ which is the second formula of level 3 listed by Tito.

Concerning the second series of level 3 we find that solutions to $\frac{x^2}{432(x-1)}=-\frac{1}{8640}$ are $x=1/5$ and $x=-1/4$ so setting in $(4)$ $x=-1/4$ gives also: $$_2F_1(\frac{1}{3},\frac{1}{2};1;-\frac{1}{4})=\frac{3\cdot 20^{1/6}\Gamma{(\frac{1}{3})}^3}{10\pi^2}\tag{5}.$$ Concerning the third series of level 3 we find that solutions to $\frac{x^2}{432(x-1)}=-\frac{1}{326592}$ are $x=1/28$ and $x=-1/27$ so setting in $(4)$ $x=1/28$ gives: $$_2F_1(\frac{1}{3},\frac{1}{2};1;\frac{1}{28})=\frac{3\cdot 14^{1/3}\Gamma{(\frac{1}{3})}^3}{14\pi^2}\tag{6}.$$ Setting in $(4)$ $x=-1/27$ gives also: $$_2F_1(\frac{1}{3},\frac{1}{2};1;-\frac{1}{27})=\frac{9\cdot 2^{2/3}\Gamma{(\frac{1}{3})}^3}{28\pi^2}\tag{7}.$$

Updated Level 2:

To obtain $(2)$ there is not explicit value listed in Ebisu's paper but using formula (B'.1) from page 8 and setting $a=1/4$ implies: $$_2F_1(\frac{1}{4},\frac{1}{2};1;-\frac{1}{80})=\frac{20^{1/4}\Gamma{(1/4)}^2}{5\pi^{3/2}}.\tag{8}$$ Now using $(3)$ and setting $a=1/4$ and $b=1/2$ we have: $$_2F_1(\frac{1}{4},\frac{1}{2};1;x)^2=\frac{1}{(1-x)^{1/4}}\sum_{n=0}^{\infty}\frac{(4n)!}{n!^4}\left(\frac{x^2}{1024(x-1)}\right)^{n}.\tag{9}$$ Then using $(8)$ and $(9)$ we recover $(2)$ which is the second series of level 2 given by Tito. Also solutions to $\frac{x^2}{1024(x-1)}=-\frac{1}{6635520}$ are $x=-1/80$ and $x=1/81$ so putting $x=1/81$ in $(9)$ we get also: $$_2F_1(\frac{1}{4},\frac{1}{2};1;\frac{1}{81})=\frac{3\sqrt{2}\Gamma{(1/4)}^2}{10\pi^{3/2}}.\tag{10}$$

Concerning the first series of level 2 given by Tito we see that solutions to: $\frac{x^2}{1024(x-1)}=-\frac{1}{12288}$ are $x=-1/3$ and $x=1/4$ so using $(9)$ when $x=-1/3$ gives: $$_2F_1(\frac{1}{4},\frac{1}{2};1;-\frac{1}{3})=\frac{\sqrt{6}\Gamma{(1/4)}^2}{6\pi^{3/2}}.\tag{11}$$ And setting $x=1/4$ also: $$_2F_1(\frac{1}{4},\frac{1}{2};1;\frac{1}{4})=\frac{3^{1/4}\Gamma{(1/4)}^2}{3\pi^{3/2}}.\tag{12}$$

Updated Level 2': Also: $$_2F_1(\frac{1}{4},\frac{1}{2};1;-\frac{32}{49})=\frac{28^{1/4}\Gamma{(1/7)}\Gamma{(2/7)}\Gamma{(4/7)}}{8\pi^2}\tag{13},$$ and $$_2F_1(\frac{1}{4},\frac{1}{2};1;\frac{32}{81})=\frac{3\cdot 1372^{1/4}\Gamma{(1/7)}\Gamma{(2/7)}\Gamma{(4/7)}}{56\pi^2}\tag{14}.$$ So the $_3F_2$ series: $$\sum_{n=0}^{\infty}\frac{(-1)^n(4n)!}{63^{2n}n!^{4}}=\frac{3\cdot\Gamma{(1/7)}^2\Gamma{(2/7)}^2\Gamma{(4/7)}^2}{32\pi^{4}}\tag{15}.$$ With some effor one can shows the Ramanujan's series: $$\sum_{n=0}^{\infty}\frac{(-1)^n(65n+8)(4n)!}{63^{2n}n!^{4}}=\frac{9\sqrt{7}}{\pi}.\tag{16}$$


Question: So Akihito's method is less opaque than WZ method. Do you think that we can use his method and prove all the rational series known for $1/\pi$ ?


Reflections: This question can be misunderstood as to what the WZ method refers. I think this method is revolutionary and brilliant because it's "trivial" except for the fact when Carlson's theorem is needed. Also as Tito Piezas III has pointed, Jesús Guillera has proved series for $1/\pi^2$ using it and no other proofs are known till today. This method goes far beyond and deals with any hypergeometric series so you can see how magnificent it is.

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    In the paper, Akihito Ebisu had a lot of identities involving $\Gamma(1/3)$. Did you use one that directly leads to $(1)$? – Tito Piezas III Nov 01 '23 at 10:19
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    Thanks. Ah, so you went from Ebisa's $_2F_1$ to the Ramanujan-type $_3F_2$. So maybe we can do the reverse: given the five Ramanujan-type $_3F_2$ in my answer, we can find their corresponding $_2F_1$. If so, I assume some are not in Ebisa's list. – Tito Piezas III Nov 01 '23 at 12:41

1 Answers1

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The proof for the Ramanujan-Sato series $1/\pi$ for levels 1,2,3,4 has already been found by the Borwein brothers and later authors such as Chan and Cooper (who also proved the higher levels).

But it is the general proof for Ramanujan-type series for $1/\pi^2, 1/\pi^3,$ etc. that has proved elusive, and Guillera used the WZ method to prove some of the $1/\pi^2.$ The unique $1/\pi^3$ and $1/\pi^4$ are still unproven.

However, there seems to be some missing details in the OP's post. The sums above involve the generalized hypergeometric function $_pF_q$,

\begin{align} \sum_{n=0}^{\infty}\frac{(3n)!(2n)!}{n!^5}\,x^n &=\,_3F_2\Big(\tfrac13,\tfrac23,\tfrac12;1,1;108x\Big)\\ \sum_{n=0}^{\infty}\frac{(4n)!}{n!^4}\,x^n &=\,_3F_2\Big(\tfrac14,\tfrac34,\tfrac12;1,1;256x\Big)\end{align}

not the usual Gauss hypergeometric function $_2F_1$ or Appell's function $\text{F}_1$ both discussed in Akihito Ebisu's paper. For example, we have the OP's,

$$\,_3F_2\Big(\tfrac13,\tfrac23,\tfrac12;1,1;\color{blue}{\tfrac{-1\;}{80}}\Big) = \frac{9\cdot 5^{2/3}\cdot\Gamma(1/3)^6}{100\cdot\pi^{4}}$$

since $108x = \frac{-1\,}{80}.$ But in the paper we have,

$$\,_2F_1\Big(\tfrac13,\tfrac23;\tfrac76;\color{blue}{\tfrac5{32}}\Big) = \frac{\sqrt3\cdot\Gamma(1/3)^6}{20\cdot\pi^{3}}$$

and similar identities, and the paper does not seem to specify how to transform one blue number to the other blue number, nor say the identities are related to series for $1/\pi$.

So unless the transformation is clarified, then the appearance of $\Gamma(1/3)$ may only be coincidence, and Ebisu's paper was not intended to prove any series for $1/\pi$.


Addendum:

Just in case there is indeed a general transformation, then there are several $_3F_2$ waiting to be expressed as a $_2F_1$, namely,

Level 2.

$$\sum_{n=0}^{\infty}\frac{(4n)!}{n!^4}\left(\frac{-1}{3\cdot64^2} \right)^n\,=\,\frac{2^{-1/2}}{\,3^{5/4}}\times\frac{\Gamma(1/4)^4}{\pi^3}$$

$$\sum_{n=0}^{\infty}\frac{(4n)!}{n!^4}\left(\frac{-1}{5\cdot1152^2} \right)^n=\frac{3}{5^{7/4}}\times\frac{\Gamma(1/4)^4}{\pi^3}$$

Level 3.

$$\sum_{n=0}^{\infty}\frac{(3n)!(2n)!\,}{n!^5}\left(\frac{-1}{3\cdot4^3} \right)^n=\frac{1}{3^{3/3}}\times\frac{3\,\Gamma(1/3)^6}{4\pi^4}$$

$$\sum_{n=0}^{\infty}\frac{(3n)!(2n)!}{n!^5}\left(\frac{-1}{5\cdot12^3} \right)^n=\frac{3}{5^{4/3}}\times\frac{3\,\Gamma(1/3)^6}{4\pi^4}$$

$$\sum_{n=0}^{\infty}\frac{(3n)!(2n)!}{n!^5}\left(\frac{-1}{7\cdot36^3} \right)^n=\frac{9}{7^{5/3}}\times\frac{3\,\Gamma(1/3)^6}{4\pi^4}$$

How to transform the negative numbers into the blue numbers of a $_2F_1$ is the big question.