Ramanujan–Sato series

In mathematics, a Ramanujan–Sato series[1][2] generalizes Ramanujan’s pi formulas such as,

${\displaystyle {\frac {1}{\pi }}={\frac {2{\sqrt {2}}}{99^{2}}}\sum _{k=0}^{\infty }{\frac {(4k)!}{k!^{4}}}{\frac {26390k+1103}{396^{4k}}}}$

to the form

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }s(k){\frac {Ak+B}{C^{k}}}}$

by using other well-defined sequences of integers ${\displaystyle s(k)}$ obeying a certain recurrence relation, sequences which may be expressed in terms of binomial coefficients ${\displaystyle {\tbinom {n}{k}}}$, and ${\displaystyle A,B,C}$ employing modular forms of higher levels.

Ramanujan made the enigmatic remark that there were "corresponding theories", but it was only recently that H. H. Chan and S. Cooper found a general approach that used the underlying modular congruence subgroup ${\displaystyle \Gamma _{0}(n)}$,[3] while G. Almkvist has experimentally found numerous other examples also with a general method using differential operators.[4]

Levels 1–4A were given by Ramanujan (1914),[5] level 5 by H. H. Chan and S. Cooper (2012),[3] 6A by Chan, Tanigawa, Yang, and Zudilin,[6] 6B by Sato (2002),[7] 6C by H. Chan, S. Chan, and Z. Liu (2004),[1] 6D by H. Chan and H. Verrill (2009),[8] level 7 by S. Cooper (2012),[9] part of level 8 by Almkvist and Guillera (2012),[2] part of level 10 by Y. Yang, and the rest by H. H. Chan and S. Cooper.

The notation j_n(τ) is derived from Zagier[10] and T_n refers to the relevant McKay–Thompson series.

Level 1

Examples for levels 1–4 were given by Ramanujan in his 1917 paper. Given ${\displaystyle q=e^{2\pi i\tau }}$ as in the rest of this article. Let,

${\displaystyle {\begin{aligned}j(\tau )&={\Big (}{\tfrac {E_{4}(\tau )}{\eta ^{8}(\tau )}}{\Big )}^{3}={\tfrac {1}{q}}+744+196884q+21493760q^{2}+\dots \\j^{*}(\tau )&=432\,{\frac {{\sqrt {j(\tau )}}+{\sqrt {j(\tau )-1728}}}{{\sqrt {j(\tau )}}-{\sqrt {j(\tau )-1728}}}}={\tfrac {1}{q}}-120+10260q-901120q^{2}+\dots \end{aligned}}}$

with the j-function j(τ), Eisenstein series E₄, and Dedekind eta function η(τ). The first expansion is the McKay–Thompson series of class 1A (OEIS: A007240) with a(0) = 744. Note that, as first noticed by J. McKay, the coefficient of the linear term of j(τ) almost equals ${\displaystyle 196883}$, which is the degree of the smallest nontrivial irreducible representation of the Monster group. Similar phenomena will be observed in the other levels. Define

${\displaystyle s_{1A}(k)={\tbinom {2k}{k}}{\tbinom {3k}{k}}{\tbinom {6k}{3k}}=1,120,83160,81681600,\dots }$ (OEIS: A001421)

${\displaystyle s_{1B}(k)=\sum _{j=0}^{k}{\tbinom {2j}{j}}{\tbinom {3j}{j}}{\tbinom {6j}{3j}}{\tbinom {k+j}{k-j}}(-432)^{k-j}=1,-312,114264,-44196288,\dots }$

Then the two modular functions and sequences are related by

${\displaystyle \sum _{k=0}^{\infty }s_{1A}(k)\,{\frac {1}{(j(\tau ))^{k+1/2}}}=\pm \sum _{k=0}^{\infty }s_{1B}(k)\,{\frac {1}{(j^{*}(\tau ))^{k+1/2}}}}$

if the series converges and the sign chosen appropriately, though squaring both sides easily removes the ambiguity. Analogous relationships exist for the higher levels.

Examples:

${\displaystyle {\frac {1}{\pi }}=12\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{1A}(k)\,{\frac {163\cdot 3344418k+13591409}{(-640320^{3})^{k+1/2}}},\quad j{\Big (}{\tfrac {1+{\sqrt {-163}}}{2}}{\Big )}=-640320^{3}}$

${\displaystyle {\frac {1}{\pi }}=24\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{1B}(k)\,{\frac {-3669+320{\sqrt {645}}\,(k+{\tfrac {1}{2}})}{{\big (}{-432}\,U_{645}^{3}{\big )}^{k+1/2}}},\quad j^{*}{\Big (}{\tfrac {1+{\sqrt {-43}}}{2}}{\Big )}=-432\,U_{645}^{3}=-432{\Big (}{\tfrac {127+5{\sqrt {645}}}{2}}{\Big )}^{3}}$

and ${\displaystyle U_{n}}$ is a fundamental unit. The first belongs to a family of formulas which were rigorously proven by the Chudnovsky brothers in 1989[11] and later used to calculate 10 trillion digits of π in 2011.[12] The second formula, and the ones for higher levels, was established by H.H. Chan and S. Cooper in 2012.[3]

Level 2

Using Zagier's notation[10] for the modular function of level 2,

${\displaystyle {\begin{aligned}j_{2A}(\tau )&={\Big (}{\big (}{\tfrac {\eta (\tau )}{\eta (2\tau )}}{\big )}^{12}+2^{6}{\big (}{\tfrac {\eta (2\tau )}{\eta (\tau )}}{\big )}^{12}{\Big )}^{2}={\tfrac {1}{q}}+104+4372q+96256q^{2}+1240002q^{3}+\cdots \\j_{2B}(\tau )&={\big (}{\tfrac {\eta (\tau )}{\eta (2\tau )}}{\big )}^{24}={\tfrac {1}{q}}-24+276q-2048q^{2}+11202q^{3}-\cdots \end{aligned}}}$

Note that the coefficient of the linear term of j_2A(τ) is one more than ${\displaystyle 4371}$ which is the smallest degree > 1 of the irreducible representations of the Baby Monster group. Define,

${\displaystyle s_{2A}(k)={\tbinom {2k}{k}}{\tbinom {2k}{k}}{\tbinom {4k}{2k}}=1,24,2520,369600,63063000,\dots }$ (OEIS: A008977)

${\displaystyle s_{2B}(k)=\sum _{j=0}^{k}{\tbinom {2j}{j}}{\tbinom {2j}{j}}{\tbinom {4j}{2j}}{\tbinom {k+j}{k-j}}(-64)^{k-j}=1,-40,2008,-109120,6173656,\dots }$

Then,

${\displaystyle \sum _{k=0}^{\infty }s_{2A}(k)\,{\frac {1}{(j_{2A}(\tau ))^{k+1/2}}}=\pm \sum _{k=0}^{\infty }s_{2B}(k)\,{\frac {1}{(j_{2B}(\tau ))^{k+1/2}}}}$

if the series converges and the sign chosen appropriately.

Examples:

${\displaystyle {\frac {1}{\pi }}=32{\sqrt {2}}\,\sum _{k=0}^{\infty }s_{2A}(k)\,{\frac {58\cdot 455k+1103}{(396^{4})^{k+1/2}}},\quad j_{2A}{\Big (}{\tfrac {1}{2}}{\sqrt {-58}}{\Big )}=396^{4}}$

${\displaystyle {\frac {1}{\pi }}=16{\sqrt {2}}\,\sum _{k=0}^{\infty }s_{2B}(k)\,{\frac {-24184+9801{\sqrt {29}}\,(k+{\tfrac {1}{2}})}{(64\,U_{29}^{12})^{k+1/2}}},\quad j_{2B}{\Big (}{\tfrac {1}{2}}{\sqrt {-58}}{\Big )}=64{\Big (}{\tfrac {5+{\sqrt {29}}}{2}}{\Big )}^{12}=64\,U_{29}^{12}}$

The first formula, found by Ramanujan and mentioned at the start of the article, belongs to a family proven by D. Bailey and the Borwein brothers in a 1989 paper.[13]

Level 3

Define,

${\displaystyle {\begin{aligned}j_{3A}(\tau )&={\Big (}{\big (}{\tfrac {\eta (\tau )}{\eta (3\tau )}}{\big )}^{6}+3^{3}{\big (}{\tfrac {\eta (3\tau )}{\eta (\tau )}}{\big )}^{6}{\Big )}^{2}={\tfrac {1}{q}}+42+783q+8672q^{2}+65367q^{3}+\dots \\j_{3B}(\tau )&={\big (}{\tfrac {\eta (\tau )}{\eta (3\tau )}}{\big )}^{12}={\tfrac {1}{q}}-12+54q-76q^{2}-243q^{3}+1188q^{4}+\dots \\\end{aligned}}}$

where ${\displaystyle 782}$ is the smallest degree > 1 of the irreducible representations of the Fischer group Fi₂₃ and,

${\displaystyle s_{3A}(k)={\tbinom {2k}{k}}{\tbinom {2k}{k}}{\tbinom {3k}{k}}=1,12,540,33600,2425500,\dots }$ (OEIS: A184423)

${\displaystyle s_{3B}(k)=\sum _{j=0}^{k}{\tbinom {2j}{j}}{\tbinom {2j}{j}}{\tbinom {3j}{j}}{\tbinom {k+j}{k-j}}(-27)^{k-j}=1,-15,297,-6495,149481,\dots }$

Examples:

${\displaystyle {\frac {1}{\pi }}=2\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{3A}(k)\,{\frac {267\cdot 53k+827}{(-300^{3})^{k+1/2}}},\quad j_{3A}{\Big (}{\tfrac {3+{\sqrt {-267}}}{6}}{\Big )}=-300^{3}}$

${\displaystyle {\frac {1}{\pi }}={\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{3B}(k)\,{\frac {12497-3000{\sqrt {89}}\,(k+{\tfrac {1}{2}})}{(-27\,U_{89}^{2})^{k+1/2}}},\quad j_{3B}{\Big (}{\tfrac {3+{\sqrt {-267}}}{6}}{\Big )}=-27\,{\big (}500+53{\sqrt {89}}{\big )}^{2}=-27\,U_{89}^{2}}$

Level 4

Define,

${\displaystyle {\begin{aligned}j_{4A}(\tau )&={\Big (}{\big (}{\tfrac {\eta (\tau )}{\eta (4\tau )}}{\big )}^{4}+4^{2}{\big (}{\tfrac {\eta (4\tau )}{\eta (\tau )}}{\big )}^{4}{\Big )}^{2}={\Big (}{\tfrac {\eta ^{2}(2\tau )}{\eta (\tau )\,\eta (4\tau )}}{\Big )}^{24}=-{\Big (}{\tfrac {\eta ((2\tau +3)/2)}{\eta (2\tau +3)}}{\Big )}^{24}={\tfrac {1}{q}}+24+276q+2048q^{2}+11202q^{3}+\dots \\j_{4C}(\tau )&={\big (}{\tfrac {\eta (\tau )}{\eta (4\tau )}}{\big )}^{8}={\tfrac {1}{q}}-8+20q-62q^{3}+216q^{5}-641q^{7}+\dots \\\end{aligned}}}$

where the first is the 24th power of the Weber modular function ${\displaystyle {\mathfrak {f}}(\tau )}$. And,

${\displaystyle s_{4A}(k)={\tbinom {2k}{k}}^{3}=1,8,216,8000,343000,\dots }$ (OEIS: A002897)

${\displaystyle s_{4C}(k)=\sum _{j=0}^{k}{\tbinom {2j}{j}}^{3}{\tbinom {k+j}{k-j}}(-16)^{k-j}=(-1)^{k}\sum _{j=0}^{k}{\tbinom {2j}{j}}^{2}{\tbinom {2k-2j}{k-j}}^{2}=1,-8,88,-1088,14296,\dots }$ (OEIS: A036917)

Examples:

${\displaystyle {\frac {1}{\pi }}=8\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{4A}(k)\,{\frac {6k+1}{(-2^{9})^{k+1/2}}},\quad j_{4A}{\Big (}{\tfrac {1+{\sqrt {-4}}}{2}}{\Big )}=-2^{9}}$

${\displaystyle {\frac {1}{\pi }}=16\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{4C}(k)\,{\frac {1-2{\sqrt {2}}\,(k+{\tfrac {1}{2}})}{(-16\,U_{2}^{4})^{k+1/2}}},\quad j_{4C}{\Big (}{\tfrac {1+{\sqrt {-4}}}{2}}{\Big )}=-16\,{\big (}1+{\sqrt {2}}{\big )}^{4}=-16\,U_{2}^{4}}$

Level 5

Define,

${\displaystyle {\begin{aligned}j_{5A}(\tau )&={\big (}{\tfrac {\eta (\tau )}{\eta (5\tau )}}{\big )}^{6}+5^{3}{\big (}{\tfrac {\eta (5\tau )}{\eta (\tau )}}{\big )}^{6}+22={\tfrac {1}{q}}+16+134q+760q^{2}+3345q^{3}+\dots \\j_{5B}(\tau )&={\big (}{\tfrac {\eta (\tau )}{\eta (5\tau )}}{\big )}^{6}={\tfrac {1}{q}}-6+9q+10q^{2}-30q^{3}+6q^{4}+\dots \end{aligned}}}$

and,

${\displaystyle s_{5A}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}{\tbinom {k+j}{j}}=1,6,114,2940,87570,\dots }$

${\displaystyle s_{5B}(k)=\sum _{j=0}^{k}(-1)^{j+k}{\tbinom {k}{j}}^{3}{\tbinom {4k-5j}{3k}}=1,-5,35,-275,2275,-19255,\dots }$ (OEIS: A229111)

where the first is the product of the central binomial coefficients and the Apéry numbers (OEIS: A005258)[9]

Examples:

${\displaystyle {\frac {1}{\pi }}={\frac {5}{9}}\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{5A}(k)\,{\frac {682k+71}{(-15228)^{k+1/2}}},\quad j_{5A}{\Big (}{\tfrac {5+{\sqrt {-5(47)}}}{10}}{\Big )}=-15228=-(18{\sqrt {47}})^{2}}$

${\displaystyle {\frac {1}{\pi }}={\frac {6}{\sqrt {5}}}\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{5B}(k)\,{\frac {25{\sqrt {5}}-141(k+{\tfrac {1}{2}})}{(-5{\sqrt {5}}\,U_{5}^{15})^{k+1/2}}},\quad j_{5B}{\Big (}{\tfrac {5+{\sqrt {-5(47)}}}{10}}{\Big )}=-5{\sqrt {5}}\,{\big (}{\tfrac {1+{\sqrt {5}}}{2}}{\big )}^{15}=-5{\sqrt {5}}\,U_{5}^{15}}$

Level 6

Modular functions

In 2002, Sato[7] established the first results for level > 4. It involved Apéry numbers which were first used to establish the irrationality of ${\displaystyle \zeta (3)}$. First, define,

${\displaystyle {\begin{aligned}j_{6A}(\tau )&=j_{6B}(\tau )+{\tfrac {1}{j_{6B}(\tau )}}-2=j_{6C}(\tau )+{\tfrac {64}{j_{6C}(\tau )}}+16=j_{6D}(\tau )+{\tfrac {81}{j_{6D}(\tau )}}+14={\tfrac {1}{q}}+10+79q+352q^{2}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{6B}(\tau )&={\Big (}{\tfrac {\eta (2\tau )\eta (3\tau )}{\eta (\tau )\eta (6\tau )}}{\Big )}^{12}={\tfrac {1}{q}}+12+78q+364q^{2}+1365q^{3}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{6C}(\tau )&={\Big (}{\tfrac {\eta (\tau )\eta (3\tau )}{\eta (2\tau )\eta (6\tau )}}{\Big )}^{6}={\tfrac {1}{q}}-6+15q-32q^{2}+87q^{3}-192q^{4}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{6D}(\tau )&={\Big (}{\tfrac {\eta (\tau )\eta (2\tau )}{\eta (3\tau )\eta (6\tau )}}{\Big )}^{4}={\tfrac {1}{q}}-4-2q+28q^{2}-27q^{3}-52q^{4}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{6E}(\tau )&={\Big (}{\tfrac {\eta (2\tau )\eta ^{3}(3\tau )}{\eta (\tau )\eta ^{3}(6\tau )}}{\Big )}^{3}={\tfrac {1}{q}}+3+6q+4q^{2}-3q^{3}-12q^{4}+\dots \end{aligned}}}$

J. Conway and S. Norton showed there are linear relations between the McKay–Thompson series T_n,[14] one of which was,

${\displaystyle T_{6A}-T_{6B}-T_{6C}-T_{6D}+2T_{6E}=0}$

or using the above eta quotients j_n,

${\displaystyle j_{6A}-j_{6B}-j_{6C}-j_{6D}+2j_{6E}=22}$

α Sequences

For the modular function j_6A, one can associate it with three different sequences. (A similar situation happens for the level 10 function j_10A.) Let,

${\displaystyle \alpha _{1}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}^{3}=1,4,60,1120,24220,\dots }$ (OEIS: A181418, labeled as s₆ in Cooper's paper)

${\displaystyle \alpha _{2}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}\sum _{m=0}^{j}{\tbinom {j}{m}}^{3}={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}{\tbinom {2j}{j}}=1,6,90,1860,44730,\dots }$ (OEIS: A002896)

${\displaystyle \alpha _{3}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}(-8)^{k-j}\sum _{m=0}^{j}{\tbinom {j}{m}}^{3}=1,-12,252,-6240,167580,-4726512,\dots }$

The three sequences involve the product of the central binomial coefficients ${\displaystyle c(k)={\tbinom {2k}{k}}}$ with: 1st, the Franel numbers ${\displaystyle \sum _{j=0}^{k}{\tbinom {k}{j}}^{3}}$; 2nd, OEIS: A002893, and 3rd, (-1)^k OEIS: A093388. Note that the second sequence, α₂(k) is also the number of 2n-step polygons on a cubic lattice. Their complements,

${\displaystyle \alpha '_{2}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}(-1)^{k-j}\sum _{m=0}^{j}{\tbinom {j}{m}}^{3}=1,2,42,620,12250,\dots }$

${\displaystyle \alpha '_{3}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}(8)^{k-j}\sum _{m=0}^{j}{\tbinom {j}{m}}^{3}=1,20,636,23840,991900,\dots }$

There are also associated sequences, namely the Apéry numbers,

${\displaystyle s_{6B}(k)=\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}{\tbinom {k+j}{j}}^{2}=1,5,73,1445,33001,\dots }$ (OEIS: A005259)

the Domb numbers (unsigned) or the number of 2n-step polygons on a diamond lattice,

${\displaystyle s_{6C}(k)=(-1)^{k}\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}{\tbinom {2(k-j)}{k-j}}{\tbinom {2j}{j}}=1,-4,28,-256,2716,\dots }$ (OEIS: A002895)

and the Almkvist-Zudilin numbers,

${\displaystyle s_{6D}(k)=\sum _{j=0}^{k}(-1)^{k-j}\,3^{k-3j}\,{\tfrac {(3j)!}{j!^{3}}}{\tbinom {k}{3j}}{\tbinom {k+j}{j}}=1,-3,9,-3,-279,2997,\dots }$ (OEIS: A125143)

where ${\displaystyle {\tfrac {(3j)!}{j!^{3}}}={\tbinom {2j}{j}}{\tbinom {3j}{j}}}$.

Identities

The modular functions can be related as,

${\displaystyle P=\sum _{k=0}^{\infty }\alpha _{1}(k)\,{\frac {1}{{\big (}j_{6A}(\tau ){\big )}^{k+1/2}}}=\sum _{k=0}^{\infty }\alpha _{2}(k)\,{\frac {1}{{\big (}j_{6A}(\tau )+4{\big )}^{k+1/2}}}=\sum _{k=0}^{\infty }\alpha _{3}(k)\,{\frac {1}{{\big (}j_{6A}(\tau )-32{\big )}^{k+1/2}}}}$

${\displaystyle Q=\sum _{k=0}^{\infty }s_{6B}(k)\,{\frac {1}{{\big (}j_{6B}(\tau ){\big )}^{k+1/2}}}=\sum _{k=0}^{\infty }s_{6C}(k)\,{\frac {1}{{\big (}j_{6C}(\tau ){\big )}^{k+1/2}}}=\sum _{k=0}^{\infty }s_{6D}(k)\,{\frac {1}{{\big (}j_{6D}(\tau ){\big )}^{k+1/2}}}}$

if the series converges and the sign chosen appropriately. It can also be observed that,

${\displaystyle P=Q=\sum _{k=0}^{\infty }\alpha '_{2}(k)\,{\frac {1}{{\big (}j_{6A}(\tau )-4{\big )}^{k+1/2}}}=\sum _{k=0}^{\infty }\alpha '_{3}(k)\,{\frac {1}{{\big (}j_{6A}(\tau )+32{\big )}^{k+1/2}}}}$

which implies,

${\displaystyle \sum _{k=0}^{\infty }\alpha _{2}(k)\,{\frac {1}{{\big (}j_{6A}(\tau )+4{\big )}^{k+1/2}}}=\sum _{k=0}^{\infty }\alpha '_{2}(k)\,{\frac {1}{{\big (}j_{6A}(\tau )-4{\big )}^{k+1/2}}}}$

and similarly using α₃ and α'₃.

Examples

One can use a value for j_6A in three ways. For example, starting with,

${\displaystyle \Delta =j_{6A}{\Big (}{\sqrt {\tfrac {-17}{6}}}{\Big )}=198^{2}-4=(140{\sqrt {2}})^{2}}$

and noting that ${\displaystyle 3\times 17=51}$ then,

${\displaystyle {\begin{aligned}{\frac {1}{\pi }}&={\frac {24{\sqrt {3}}}{35}}\,\sum _{k=0}^{\infty }\alpha _{1}(k)\,{\frac {51\cdot 11k+53}{(\Delta )^{k+1/2}}}\\{\frac {1}{\pi }}&={\frac {4{\sqrt {3}}}{99}}\,\sum _{k=0}^{\infty }\alpha _{2}(k)\,{\frac {17\cdot 560k+899}{(\Delta +4)^{k+1/2}}}\\{\frac {1}{\pi }}&={\frac {\sqrt {3}}{2}}\,\sum _{k=0}^{\infty }\alpha _{3}(k)\,{\frac {770k+73}{(\Delta -32)^{k+1/2}}}\\\end{aligned}}}$

as well as,

${\displaystyle {\begin{aligned}{\frac {1}{\pi }}&={\frac {12{\sqrt {3}}}{9799}}\,\sum _{k=0}^{\infty }\alpha '_{2}(k)\,{\frac {11\cdot 51\cdot 560k+29693}{(\Delta -4)^{k+1/2}}}\\{\frac {1}{\pi }}&={\frac {6{\sqrt {3}}}{613}}\,\sum _{k=0}^{\infty }\alpha '_{3}(k)\,{\frac {51\cdot 770k+3697}{(\Delta +32)^{k+1/2}}}\\\end{aligned}}}$

though the formulas using the complements apparently do not yet have a rigorous proof. For the other modular functions,

${\displaystyle {\frac {1}{\pi }}=8{\sqrt {15}}\,\sum _{k=0}^{\infty }s_{6B}(k)\,{\Big (}{\tfrac {1}{2}}-{\tfrac {3{\sqrt {5}}}{20}}+k{\Big )}{\Big (}{\frac {1}{\phi ^{12}}}{\Big )}^{k+1/2},\quad j_{6B}{\Big (}{\sqrt {\tfrac {-5}{6}}}{\Big )}={\Big (}{\tfrac {1+{\sqrt {5}}}{2}}{\Big )}^{12}=\phi ^{12}}$

${\displaystyle {\frac {1}{\pi }}={\frac {1}{2}}\,\sum _{k=0}^{\infty }s_{6C}(k)\,{\frac {3k+1}{32^{k}}},\quad j_{6C}{\Big (}{\sqrt {\tfrac {-1}{3}}}{\Big )}=32}$

${\displaystyle {\frac {1}{\pi }}=2{\sqrt {3}}\,\sum _{k=0}^{\infty }s_{6D}(k)\,{\frac {4k+1}{81^{k+1/2}}},\quad j_{6D}{\Big (}{\sqrt {\tfrac {-1}{2}}}{\Big )}=81}$

Level 7

Define

${\displaystyle s_{7A}(k)=\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}{\tbinom {2j}{k}}{\tbinom {k+j}{j}}=1,4,48,760,13840,\dots }$ (OEIS: A183204)

and,

${\displaystyle {\begin{aligned}j_{7A}(\tau )&={\Big (}{\big (}{\tfrac {\eta (\tau )}{\eta (7\tau )}}{\big )}^{2}+7{\big (}{\tfrac {\eta (7\tau )}{\eta (\tau )}}{\big )}^{2}{\Big )}^{2}={\tfrac {1}{q}}+10+51q+204q^{2}+681q^{3}+\dots \\j_{7B}(\tau )&={\big (}{\tfrac {\eta (\tau )}{\eta (7\tau )}}{\big )}^{4}={\tfrac {1}{q}}-4+2q+8q^{2}-5q^{3}-4q^{4}-10q^{5}+\dots \end{aligned}}}$

Example:

${\displaystyle {\frac {1}{\pi }}={\frac {\sqrt {7}}{22^{3}}}\,\sum _{k=0}^{\infty }s_{7A}(k)\,{\frac {11895k+1286}{(-22^{3})^{k}}},\quad j_{7A}{\Big (}{\tfrac {7+{\sqrt {-427}}}{14}}{\Big )}=-22^{3}+1=-(39{\sqrt {7}})^{2}}$

No pi formula has yet been found using j_7B.

Level 8

Define,

${\displaystyle {\begin{aligned}j_{4B}(\tau )&={\big (}j_{2A}(2\tau ){\big )}^{1/2}={\tfrac {1}{q}}+52q+834q^{3}+4760q^{5}+24703q^{7}+\dots \\&={\Big (}{\big (}{\tfrac {\eta (\tau )\,\eta ^{2}(4\tau )}{\eta ^{2}(2\tau )\,\eta (8\tau )}}{\big )}^{4}+4{\big (}{\tfrac {\eta ^{2}(2\tau )\,\eta (8\tau )}{\eta (\tau )\,\eta ^{2}(4\tau )}}{\big )}^{4}{\Big )}^{2}={\Big (}{\big (}{\tfrac {\eta (2\tau )\,\eta (4\tau )}{\eta (\tau )\,\eta (8\tau )}}{\big )}^{4}-4{\big (}{\tfrac {\eta (\tau )\,\eta (8\tau )}{\eta (2\tau )\,\eta (4\tau )}}{\big )}^{4}{\Big )}^{2}\\j_{8A'}(\tau )&={\big (}{\tfrac {\eta (\tau )\,\eta ^{2}(4\tau )}{\eta ^{2}(2\tau )\,\eta (8\tau )}}{\big )}^{8}={\tfrac {1}{q}}-8+36q-128q^{2}+386q^{3}-1024q^{4}+\dots \\j_{8A}(\tau )&={\big (}{\tfrac {\eta (2\tau )\,\eta (4\tau )}{\eta (\tau )\,\eta (8\tau )}}{\big )}^{8}={\tfrac {1}{q}}+8+36q+128q^{2}+386q^{3}+1024q^{4}+\dots \\j_{8B}(\tau )&={\big (}j_{4A}(2\tau ){\big )}^{1/2}={\big (}{\tfrac {\eta ^{2}(4\tau )}{\eta (2\tau )\,\eta (8\tau )}}{\big )}^{12}={\tfrac {1}{q}}+12q+66q^{3}+232q^{5}+639q^{7}+\dots \end{aligned}}}$

The expansion of the first is the McKay–Thompson series of class 4B (and is the square root of another function). The fourth is also the square root of another function. Let,

${\displaystyle s_{4B}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}4^{k-2j}{\tbinom {k}{2j}}{\tbinom {2j}{j}}^{2}={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {k}{j}}{\tbinom {2k-2j}{k-j}}{\tbinom {2j}{j}}=1,8,120,2240,47320,\dots }$

${\displaystyle s_{8A'}(k)=(-1)^{k}\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}{\tbinom {2j}{k}}^{2}=1,-4,40,-544,8536,\dots }$

${\displaystyle s_{8B}(k)=\sum _{j=0}^{k}{\tbinom {2j}{j}}^{3}{\tbinom {2k-4j}{k-2j}}=1,2,14,36,334,\dots }$

where the first is the product[2] of the central binomial coefficient and a sequence related to an arithmetic-geometric mean (OEIS: A081085),

Examples:

${\displaystyle {\frac {1}{\pi }}={\frac {2{\sqrt {2}}}{13}}\,\sum _{k=0}^{\infty }s_{4B}(k)\,{\frac {70\cdot 99\,k+579}{(16+396^{2})^{k+1/2}}},\qquad j_{4B}{\Big (}{\tfrac {1}{4}}{\sqrt {-58}}{\Big )}=396^{2}}$

${\displaystyle {\frac {1}{\pi }}={\frac {\sqrt {-2}}{70}}\,\sum _{k=0}^{\infty }s_{4B}(k)\,{\frac {58\cdot 13\cdot 99\,k+6243}{(16-396^{2})^{k+1/2}}}}$

${\displaystyle {\frac {1}{\pi }}=2{\sqrt {2}}\,\sum _{k=0}^{\infty }s_{8A'}(k)\,{\frac {-222+377{\sqrt {2}}\,(k+{\tfrac {1}{2}})}{{\big (}4(1+{\sqrt {2}})^{12}{\big )}^{k+1/2}}},\qquad j_{8A'}{\Big (}{\tfrac {1}{4}}{\sqrt {-58}}{\Big )}=4(1+{\sqrt {2}})^{12},\quad j_{8A}{\Big (}{\tfrac {1}{4}}{\sqrt {-58}}{\Big )}=4(99+13{\sqrt {58}})^{2}=4U_{58}^{2}}$

${\displaystyle {\frac {1}{\pi }}={\frac {\sqrt {3/5}}{16}}\,\sum _{k=0}^{\infty }s_{8B}(k)\,{\frac {210k+43}{(64)^{k+1/2}}},\qquad j_{4B}{\Big (}{\tfrac {1}{4}}{\sqrt {-7}}{\Big )}=64}$

though no pi formula is yet known using j_8A(τ).

Level 9

Define,

${\displaystyle {\begin{aligned}j_{3C}(\tau )&={\big (}j(3\tau ))^{1/3}=-6+{\big (}{\tfrac {\eta ^{2}(3\tau )}{\eta (\tau )\,\eta (9\tau )}}{\big )}^{6}-27{\big (}{\tfrac {\eta (\tau )\,\eta (9\tau )}{\eta ^{2}(3\tau )}}{\big )}^{6}={\tfrac {1}{q}}+248q^{2}+4124q^{5}+34752q^{8}+\dots \\j_{9A}(\tau )&={\big (}{\tfrac {\eta ^{2}(3\tau )}{\eta (\tau )\,\eta (9\tau )}}{\big )}^{6}={\tfrac {1}{q}}+6+27q+86q^{2}+243q^{3}+594q^{4}+\dots \\\end{aligned}}}$

The expansion of the first is the McKay–Thompson series of class 3C (and related to the cube root of the j-function), while the second is that of class 9A. Let,

${\displaystyle s_{3C}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}(-3)^{k-3j}{\tbinom {k}{j}}{\tbinom {k-j}{j}}{\tbinom {k-2j}{j}}={\tbinom {2k}{k}}\sum _{j=0}^{k}(-3)^{k-3j}{\tbinom {k}{3j}}{\tbinom {2j}{j}}{\tbinom {3j}{j}}=1,-6,54,-420,630,\dots }$

${\displaystyle s_{9A}(k)=\sum _{j=0}^{k}{\tbinom {k}{j}}^{2}\sum _{m=0}^{j}{\tbinom {k}{m}}{\tbinom {j}{m}}{\tbinom {j+m}{k}}=1,3,27,309,4059,\dots }$

where the first is the product of the central binomial coefficients and OEIS: A006077 (though with different signs).

Examples:

${\displaystyle {\frac {1}{\pi }}={\frac {-{\boldsymbol {i}}}{9}}\sum _{k=0}^{\infty }s_{3C}(k)\,{\frac {602k+85}{(-960-12)^{k+1/2}}},\quad j_{3C}{\Big (}{\tfrac {3+{\sqrt {-43}}}{6}}{\Big )}=-960}$

${\displaystyle {\frac {1}{\pi }}=6\,{\boldsymbol {i}}\,\sum _{k=0}^{\infty }s_{9A}(k)\,{\frac {4-{\sqrt {129}}\,(k+{\tfrac {1}{2}})}{{\big (}-3{\sqrt {3U_{129}}}{\big )}^{k+1/2}}},\quad j_{9A}{\Big (}{\tfrac {3+{\sqrt {-43}}}{6}}{\Big )}=-3{\sqrt {3}}{\big (}53{\sqrt {3}}+14{\sqrt {43}}{\big )}=-3{\sqrt {3U_{129}}}}$

Level 10

Modular functions

Define,

${\displaystyle {\begin{aligned}j_{10A}(\tau )&=j_{10B}(\tau )+{\tfrac {16}{j_{10B}(\tau )}}+8=j_{10C}(\tau )+{\tfrac {25}{j_{10C}(\tau )}}+6=j_{10D}(\tau )+{\tfrac {1}{j_{10D}(\tau )}}-2={\tfrac {1}{q}}+4+22q+56q^{2}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{10B}(\tau )&={\Big (}{\tfrac {\eta (\tau )\eta (5\tau )}{\eta (2\tau )\eta (10\tau )}}{\Big )}^{4}={\tfrac {1}{q}}-4+6q-8q^{2}+17q^{3}-32q^{4}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{10C}(\tau )&={\Big (}{\tfrac {\eta (\tau )\eta (2\tau )}{\eta (5\tau )\eta (10\tau )}}{\Big )}^{2}={\tfrac {1}{q}}-2-3q+6q^{2}+2q^{3}+2q^{4}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{10D}(\tau )&={\Big (}{\tfrac {\eta (2\tau )\eta (5\tau )}{\eta (\tau )\eta (10\tau )}}{\Big )}^{6}={\tfrac {1}{q}}+6+21q+62q^{2}+162q^{3}+\dots \end{aligned}}}$

${\displaystyle {\begin{aligned}j_{10E}(\tau )&={\Big (}{\tfrac {\eta (2\tau )\eta ^{5}(5\tau )}{\eta (\tau )\eta ^{5}(10\tau )}}{\Big )}={\tfrac {1}{q}}+1+q+2q^{2}+2q^{3}-2q^{4}+\dots \end{aligned}}}$

Just like the level 6, there are also linear relations between these,

${\displaystyle T_{10A}-T_{10B}-T_{10C}-T_{10D}+2T_{10E}=0}$

or using the above eta quotients j_n,

${\displaystyle j_{10A}-j_{10B}-j_{10C}-j_{10D}+2j_{10E}=6}$

β Sequences

Let,

${\displaystyle \beta _{1}(k)=\sum _{j=0}^{k}{\tbinom {k}{j}}^{4}=1,2,18,164,1810,\dots }$ (OEIS: A005260, labeled as s₁₀ in Cooper's paper)

${\displaystyle \beta _{2}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {2j}{j}}^{-1}{\tbinom {k}{j}}\sum _{m=0}^{j}{\tbinom {j}{m}}^{4}=1,4,36,424,5716,\dots }$

${\displaystyle \beta _{3}(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {2j}{j}}^{-1}{\tbinom {k}{j}}(-4)^{k-j}\sum _{m=0}^{j}{\tbinom {j}{m}}^{4}=1,-6,66,-876,12786,\dots }$

their complements,

${\displaystyle \beta _{2}'(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {2j}{j}}^{-1}{\tbinom {k}{j}}(-1)^{k-j}\sum _{m=0}^{j}{\tbinom {j}{m}}^{4}=1,0,12,24,564,2784,\dots }$

${\displaystyle \beta _{3}'(k)={\tbinom {2k}{k}}\sum _{j=0}^{k}{\tbinom {2j}{j}}^{-1}{\tbinom {k}{j}}(4)^{k-j}\sum _{m=0}^{j}{\tbinom {j}{m}}^{4}=1,10,162,3124,66994,\dots }$

and,

${\displaystyle s_{10B}(k)=1,-2,10,-68,514,-4100,33940,\dots }$

${\displaystyle s_{10C}(k)=1,-1,1,-1,1,23,-263,1343,-2303,\dots }$

${\displaystyle s_{10D}(k)=1,3,25,267,3249,42795,594145,\dots }$

though closed-forms are not yet known for the last three sequences.

Identities

The modular functions can be related as,[15]

${\displaystyle U=\sum _{k=0}^{\infty }\beta _{1}(k)\,{\frac {1}{(j_{10A}(\tau ))^{k+1/2}}}=\sum _{k=0}^{\infty }\beta _{2}(k)\,{\frac {1}{(j_{10A}(\tau )+4)^{k+1/2}}}=\sum _{k=0}^{\infty }\beta _{3}(k)\,{\frac {1}{(j_{10A}(\tau )-16)^{k+1/2}}}}$

${\displaystyle V=\sum _{k=0}^{\infty }s_{10B}(k)\,{\frac {1}{(j_{10B}(\tau ))^{k+1/2}}}=\sum _{k=0}^{\infty }s_{10C}(k)\,{\frac {1}{(j_{10C}(\tau ))^{k+1/2}}}=\sum _{k=0}^{\infty }s_{10D}(k)\,{\frac {1}{(j_{10D}(\tau ))^{k+1/2}}}}$

if the series converges. In fact, it can also be observed that,

${\displaystyle U=V=\sum _{k=0}^{\infty }\beta _{2}'(k)\,{\frac {1}{(j_{10A}(\tau )-4)^{k+1/2}}}=\sum _{k=0}^{\infty }\beta _{3}'(k)\,{\frac {1}{(j_{10A}(\tau )+16)^{k+1/2}}}}$

Since the exponent has a fractional part, the sign of the square root must be chosen appropriately though it is less an issue when j_n is positive.

Examples

Just like level 6, the level 10 function j_10A can be used in three ways. Starting with,

${\displaystyle j_{10A}{\Big (}{\sqrt {\tfrac {-19}{10}}}{\Big )}=76^{2}}$

and noting that ${\displaystyle 5\times 19=95}$ then,

${\displaystyle {\begin{aligned}{\frac {1}{\pi }}&={\frac {5}{\sqrt {95}}}\,\sum _{k=0}^{\infty }\beta _{1}(k)\,{\frac {408k+47}{(76^{2})^{k+1/2}}}\\{\frac {1}{\pi }}&={\frac {1}{17{\sqrt {95}}}}\,\sum _{k=0}^{\infty }\beta _{2}(k)\,{\frac {19\cdot 1824k+3983}{(76^{2}+4)^{k+1/2}}}\\{\frac {1}{\pi }}&={\frac {1}{6{\sqrt {95}}}}\,\,\sum _{k=0}^{\infty }\beta _{3}(k)\,\,{\frac {19\cdot 646k+1427}{(76^{2}-16)^{k+1/2}}}\\\end{aligned}}}$

as well as,

${\displaystyle {\begin{aligned}{\frac {1}{\pi }}&={\frac {5}{481{\sqrt {95}}}}\,\sum _{k=0}^{\infty }\beta _{2}'(k)\,{\frac {19\cdot 10336k+22675}{(76^{2}-4)^{k+1/2}}}\\{\frac {1}{\pi }}&={\frac {5}{181{\sqrt {95}}}}\,\sum _{k=0}^{\infty }\beta _{3}'(k)\,{\frac {19\cdot 3876k+8405}{(76^{2}+16)^{k+1/2}}}\end{aligned}}}$

though the ones using the complements do not yet have a rigorous proof. A conjectured formula using one of the last three sequences is,

${\displaystyle {\frac {1}{\pi }}={\frac {\boldsymbol {i}}{\sqrt {5}}}\,\sum _{k=0}^{\infty }s_{10C}(k){\frac {10k+3}{(-5^{2})^{k+1/2}}},\quad j_{10C}{\Big (}{\tfrac {1+\,{\boldsymbol {i}}}{2}}{\Big )}=-5^{2}}$

which implies there might be examples for all sequences of level 10.

Level 11

Define the McKay–Thompson series of class 11A,

${\displaystyle j_{11A}(\tau )=(1+3F)^{3}+({\tfrac {1}{\sqrt {F}}}+3{\sqrt {F}})^{2}={\tfrac {1}{q}}+6+17q+46q^{2}+116q^{3}+\dots }$

where,

${\displaystyle F={\tfrac {\eta (3\tau )\,\eta (33\tau )}{\eta (\tau )\,\eta (11\tau )}}}$

and,

${\displaystyle s_{11A}(k)=1,\,4,\,28,\,268,\,3004,\,36784,\,476476,\dots }$

No closed-form in terms of binomial coefficients is yet known for the sequence but it obeys the recurrence relation,

${\displaystyle (k+1)^{3}s_{k+1}=2(2k+1)(5k^{2}+5k+2)s_{k}\,-\,8k(7k^{2}+1)s_{k-1}\,+\,22k(k-1)(2k-1)s_{k-2}}$

with initial conditions s(0) = 1, s(1) = 4.

Example:[16]

${\displaystyle {\frac {1}{\pi }}={\frac {\boldsymbol {i}}{22}}\sum _{k=0}^{\infty }s_{11A}(k)\,{\frac {221k+67}{(-44)^{k+1/2}}},\quad j_{11A}{\Big (}{\tfrac {1+{\sqrt {-17/11}}}{2}}{\Big )}=-44}$

Higher levels

As pointed out by Cooper,[16] there are analogous sequences for certain higher levels.

Similar series

R. Steiner found examples using Catalan numbers ${\displaystyle C_{k}}$,

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-n})}^{2}{\frac {(4z)k+(2^{4(n-2)+2}-(4n-3)z)}{2^{4k}}}(z\in \mathbb {Z} ,n\geq 2,n\in \mathbb {N} )}$

and for this a modular form with a second periodic for k exists: ${\displaystyle k={\frac {1}{16}}((-20-12{\boldsymbol {i}})+16n),k={\frac {1}{16}}((-20+12{\boldsymbol {i}})+16n)}$. Other similar series are

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-2})}^{2}{\frac {3k+{\frac {1}{4}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {(4z+1)k-z}{2^{4k}}}(z\in \mathbb {Z} )}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {-1k+{\frac {1}{2}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {0k+{\frac {1}{4}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {{\frac {k}{5}}+{\frac {1}{5}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {{\frac {k}{3}}+{\frac {1}{6}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {{\frac {k}{2}}+{\frac {1}{8}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {2k-{\frac {1}{4}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k-1})}^{2}{\frac {3k-{\frac {1}{2}}}{2^{4k}}}}$

${\displaystyle {\frac {1}{\pi }}=\sum _{k=0}^{\infty }{(2C_{k})}^{2}{\frac {{\frac {k}{16}}+{\frac {1}{16}}}{2^{4k}}}}$

with the last (comments in OEIS: A013709) found by using a linear combination of higher parts of Wallis-Lambert series for 4/Pi and Euler series for the circumference of an ellipse.

Using the definition of Catalan numbers with the gamma function the first and last for example give the identities

${\displaystyle {\frac {1}{4}}=\sum _{k=0}^{\infty }{\left({\frac {\Gamma ({\frac {1}{2}}+k)}{\Gamma (2+k)}}\right)}^{2}\left(4zk-(4n-3)z+2^{4(n-2)+2}\right)(z\in \mathbb {Z} ,n\geq 2,n\in \mathbb {N} )}$

...

${\displaystyle 4=\sum _{k=0}^{\infty }{\left({\frac {\Gamma ({\frac {1}{2}}+k)}{\Gamma (2+k)}}\right)}^{2}(k+1)}$.

The last is also equivalent to,

${\displaystyle {\frac {1}{\pi }}={\frac {1}{4}}\sum _{k=0}^{\infty }{\frac {{\binom {2k}{k}}^{2}}{k+1}}\,{\frac {1}{2^{4k}}}}$

and is related to the fact that,

${\displaystyle \pi =\lim _{k\rightarrow \infty }{\frac {2^{4k}}{k{2k \choose k}^{2}}}}$

which is a consequence of Stirling's approximation.

See also

• Chudnovsky algorithm
• Borwein's algorithm

References

1. Chan, Heng Huat; Chan, Song Heng; Liu, Zhiguo (2004). "Domb's numbers and Ramanujan–Sato type series for 1/π". Advances in Mathematics. 186 (2): 396–410. doi:10.1016/j.aim.2003.07.012.
2. Almkvist, Gert; Guillera, Jesus (2013). "Ramanujan–Sato-Like Series". In Borwein, J.; Shparlinski, I.; Zudilin, W. (eds.). Number Theory and Related Fields. Springer Proceedings in Mathematics & Statistics. vol 43. New York: Springer. pp. 55–74. doi:10.1007/978-1-4614-6642-0_2. ISBN 978-1-4614-6641-3.
3. Chan, H. H.; Cooper, S. (2012). "Rational analogues of Ramanujan's series for 1/π" (PDF). Mathematical Proceedings of the Cambridge Philosophical Society. 153 (2): 361–383. doi:10.1017/S0305004112000254.
4. Almkvist, G. (2012). "Some conjectured formulas for 1/π coming from polytopes, K3-surfaces and Moonshine". arXiv:1211.6563. Cite journal requires |journal= (help)
5. Ramanujan, S. (1914). "Modular equations and approximations to π". Quart. J. Math. Oxford. 45.
6. Chan; Tanigawa; Yang; Zudilin (2011). "New analogues of Clausen's identities arising from the theory of modular forms". Advances in Mathematics. 228 (2): 1294–1314. doi:10.1016/j.aim.2011.06.011.
7. Sato, T. (2002). "Apéry numbers and Ramanujan's series for 1/π". Abstract of a Talk Presented at the Annual Meeting of the Mathematical Society of Japan.
8. Chan, H.; Verrill, H. (2009). "The Apéry numbers, the Almkvist–Zudilin Numbers, and new series for 1/π". Mathematical Research Letters. 16 (3): 405–420. doi:10.4310/MRL.2009.v16.n3.a3.
9. Cooper, S. (2012). "Sporadic sequences, modular forms and new series for 1/π". Ramanujan Journal. 29 (1–3): 163–183. doi:10.1007/s11139-011-9357-3.
10. Zagier, D. (2000). "Traces of Singular Moduli" (PDF): 15–16. Cite journal requires |journal= (help)
11. Chudnovsky, David V.; Chudnovsky, Gregory V. (1989), "The Computation of Classical Constants", Proceedings of the National Academy of Sciences of the United States of America, 86 (21): 8178–8182, doi:10.1073/pnas.86.21.8178, ISSN 0027-8424, JSTOR 34831, PMC 298242, PMID 16594075.
12. Yee, Alexander; Kondo, Shigeru (2011), 10 Trillion Digits of Pi: A Case Study of summing Hypergeometric Series to high precision on Multicore Systems, Technical Report, Computer Science Department, University of Illinois, hdl:2142/28348.
13. Borwein, J. M.; Borwein, P. B.; Bailey, D. H. (1989). "Ramanujan, modular equations, and approximations to pi; Or how to compute one billion digits of pi" (PDF). Amer. Math. Monthly. 96 (3): 201–219. doi:10.1080/00029890.1989.11972169.
14. Conway, J.; Norton, S. (1979). "Monstrous Moonshine". Bulletin of the London Mathematical Society. 11 (3): 308–339 [p. 319]. doi:10.1112/blms/11.3.308.
15. S. Cooper, "Level 10 analogues of Ramanujan’s series for 1/π", Theorem 4.3, p.85, J. Ramanujan Math. Soc. 27, No.1 (2012)
16. Cooper, S. (December 2013). "Ramanujan's theories of elliptic functions to alternative bases, and beyond" (PDF). Askey 80 Conference.

External links

• Franel numbers
• McKay–Thompson series
• Approximations to Pi via the Dedekind eta function