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The Riemann zeta function at 0 and 1

At zero, one has ζ ( 0 ) = B 1 − = − B 1 + = − 1 2 {\displaystyle \zeta (0)={B_{1}^{-}}=-{B_{1}^{+}}=-{\tfrac {1}{2}}\!}

At 1 there is a pole, so ζ(1) is not finite but the left and right limits are: lim ε → 0 ± ζ ( 1 + ε ) = ± ∞ {\displaystyle \lim _{\varepsilon \to 0^{\pm }}\zeta (1+\varepsilon )=\pm \infty } Since it is a pole of first order, it has a complex residue lim ε → 0 ε ζ ( 1 + ε ) = 1 . {\displaystyle \lim _{\varepsilon \to 0}\varepsilon \zeta (1+\varepsilon )=1\,.}

Positive integers

Even positive integers

For the even positive integers n {\displaystyle n} , one has the relationship to the Bernoulli numbers B n {\displaystyle B_{n}} :

ζ ( n ) = ( − 1 ) n 2 + 1 ( 2 π ) n B n 2 ( n ! ) . {\displaystyle \zeta (n)=(-1)^{{\tfrac {n}{2}}+1}{\frac {(2\pi )^{n}B_{n}}{2(n!)}}\,.}

The computation of ζ ( 2 ) {\displaystyle \zeta (2)} is known as the Basel problem. The value of ζ ( 4 ) {\displaystyle \zeta (4)} is related to the Stefan–Boltzmann law and Wien approximation in physics. The first few values are given by: ζ ( 2 ) = 1 + 1 2 2 + 1 3 2 + ⋯ = π 2 6 ζ ( 4 ) = 1 + 1 2 4 + 1 3 4 + ⋯ = π 4 90 ζ ( 6 ) = 1 + 1 2 6 + 1 3 6 + ⋯ = π 6 945 ζ ( 8 ) = 1 + 1 2 8 + 1 3 8 + ⋯ = π 8 9450 ζ ( 10 ) = 1 + 1 2 10 + 1 3 10 + ⋯ = π 10 93555 ζ ( 12 ) = 1 + 1 2 12 + 1 3 12 + ⋯ = 691 π 12 638512875 ζ ( 14 ) = 1 + 1 2 14 + 1 3 14 + ⋯ = 2 π 14 18243225 ζ ( 16 ) = 1 + 1 2 16 + 1 3 16 + ⋯ = 3617 π 16 325641566250 . {\displaystyle {\begin{aligned}\zeta (2)&=1+{\frac {1}{2^{2}}}+{\frac {1}{3^{2}}}+\cdots ={\frac {\pi ^{2}}{6}}\\[4pt]\zeta (4)&=1+{\frac {1}{2^{4}}}+{\frac {1}{3^{4}}}+\cdots ={\frac {\pi ^{4}}{90}}\\[4pt]\zeta (6)&=1+{\frac {1}{2^{6}}}+{\frac {1}{3^{6}}}+\cdots ={\frac {\pi ^{6}}{945}}\\[4pt]\zeta (8)&=1+{\frac {1}{2^{8}}}+{\frac {1}{3^{8}}}+\cdots ={\frac {\pi ^{8}}{9450}}\\[4pt]\zeta (10)&=1+{\frac {1}{2^{10}}}+{\frac {1}{3^{10}}}+\cdots ={\frac {\pi ^{10}}{93555}}\\[4pt]\zeta (12)&=1+{\frac {1}{2^{12}}}+{\frac {1}{3^{12}}}+\cdots ={\frac {691\pi ^{12}}{638512875}}\\[4pt]\zeta (14)&=1+{\frac {1}{2^{14}}}+{\frac {1}{3^{14}}}+\cdots ={\frac {2\pi ^{14}}{18243225}}\\[4pt]\zeta (16)&=1+{\frac {1}{2^{16}}}+{\frac {1}{3^{16}}}+\cdots ={\frac {3617\pi ^{16}}{325641566250}}\,.\end{aligned}}}

Taking the limit n → ∞ {\displaystyle n\rightarrow \infty } , one obtains ζ ( ∞ ) = 1 {\displaystyle \zeta (\infty )=1} .

Selected values for even integers

Value	Decimal expansion	Source
ζ ( 2 ) {\displaystyle \zeta (2)}	1.6449340668482264364...	OEIS: A013661
ζ ( 4 ) {\displaystyle \zeta (4)}	1.0823232337111381915...	OEIS: A013662
ζ ( 6 ) {\displaystyle \zeta (6)}	1.0173430619844491397...	OEIS: A013664
ζ ( 8 ) {\displaystyle \zeta (8)}	1.0040773561979443393...	OEIS: A013666
ζ ( 10 ) {\displaystyle \zeta (10)}	1.0009945751278180853...	OEIS: A013668
ζ ( 12 ) {\displaystyle \zeta (12)}	1.0002460865533080482...	OEIS: A013670
ζ ( 14 ) {\displaystyle \zeta (14)}	1.0000612481350587048...	OEIS: A013672
ζ ( 16 ) {\displaystyle \zeta (16)}	1.0000152822594086518...	OEIS: A013674

The relationship between zeta at the positive even integers and powers of pi may be written as

a n ζ ( 2 n ) = π 2 n b n {\displaystyle a_{n}\zeta (2n)=\pi ^{2n}b_{n}}

where a n {\displaystyle a_{n}} and b n {\displaystyle b_{n}} are coprime positive integers for all n {\displaystyle n} . These are given by the integer sequences OEIS: A002432 and OEIS: A046988, respectively, in OEIS. Some of these values are reproduced below:

coefficients

n	an	bn
1	6	1
2	90	1
3	945	1
4	9450	1
5	93555	1
6	638512875	691
7	18243225	2
8	325641566250	3617
9	38979295480125	43867
10	1531329465290625	174611
11	13447856940643125	155366
12	201919571963756521875	236364091
13	11094481976030578125	1315862
14	564653660170076273671875	6785560294
15	5660878804669082674070015625	6892673020804
16	62490220571022341207266406250	7709321041217
17	12130454581433748587292890625	151628697551

If we let η n = b n / a n {\displaystyle \eta _{n}=b_{n}/a_{n}} be the coefficient of π 2 n {\displaystyle \pi ^{2n}} as above, ζ ( 2 n ) = ∑ ℓ = 1 ∞ 1 ℓ 2 n = η n π 2 n {\displaystyle \zeta (2n)=\sum _{\ell =1}^{\infty }{\frac {1}{\ell ^{2n}}}=\eta _{n}\pi ^{2n}} then we find recursively,

η 1 = 1 / 6 η n = ∑ ℓ = 1 n − 1 ( − 1 ) ℓ − 1 η n − ℓ ( 2 ℓ + 1 ) ! + ( − 1 ) n + 1 n ( 2 n + 1 ) ! {\displaystyle {\begin{aligned}\eta _{1}&=1/6\\\eta _{n}&=\sum _{\ell =1}^{n-1}(-1)^{\ell -1}{\frac {\eta _{n-\ell }}{(2\ell +1)!}}+(-1)^{n+1}{\frac {n}{(2n+1)!}}\end{aligned}}}

This recurrence relation may be derived from that for the Bernoulli numbers.

Also, there is another recurrence:

ζ ( 2 n ) = 1 n + 1 2 ∑ k = 1 n − 1 ζ ( 2 k ) ζ ( 2 n − 2 k )  for  n > 1 {\displaystyle \zeta (2n)={\frac {1}{n+{\frac {1}{2}}}}\sum _{k=1}^{n-1}\zeta (2k)\zeta (2n-2k)\quad {\text{ for }}\quad n>1} which can be proved, using that d d x cot ⁡ ( x ) = − 1 − cot 2 ⁡ ( x ) {\displaystyle {\frac {d}{dx}}\cot(x)=-1-\cot ^{2}(x)}

The values of the zeta function at non-negative even integers have the generating function: ∑ n = 0 ∞ ζ ( 2 n ) x 2 n = − π x 2 cot ⁡ ( π x ) = − 1 2 + π 2 6 x 2 + π 4 90 x 4 + π 6 945 x 6 + ⋯ {\displaystyle \sum _{n=0}^{\infty }\zeta (2n)x^{2n}=-{\frac {\pi x}{2}}\cot(\pi x)=-{\frac {1}{2}}+{\frac {\pi ^{2}}{6}}x^{2}+{\frac {\pi ^{4}}{90}}x^{4}+{\frac {\pi ^{6}}{945}}x^{6}+\cdots } Since lim n → ∞ ζ ( 2 n ) = 1 {\displaystyle \lim _{n\rightarrow \infty }\zeta (2n)=1} The formula also shows that for n ∈ N , n → ∞ {\displaystyle n\in \mathbb {N} ,n\rightarrow \infty } , | B 2 n | ∼ ( 2 n ) ! 2   ( 2 π ) 2 n {\displaystyle \left|B_{2n}\right|\sim {\frac {(2n)!\,2}{\;~(2\pi )^{2n}\,}}}

Odd positive integers

The sum of the harmonic series is infinite. ζ ( 1 ) = 1 + 1 2 + 1 3 + ⋯ = ∞ {\displaystyle \zeta (1)=1+{\frac {1}{2}}+{\frac {1}{3}}+\cdots =\infty \!}

The value ζ(3) is also known as Apéry's constant and has a role in the electron's gyromagnetic ratio. The value ζ(3) also appears in Planck's law. These and additional values are:

Selected values for odd integers

Value	Decimal expansion	Source
ζ ( 3 ) {\displaystyle \zeta (3)}	1.2020569031595942853...	OEIS: A002117
ζ ( 5 ) {\displaystyle \zeta (5)}	1.0369277551433699263...	OEIS: A013663
ζ ( 7 ) {\displaystyle \zeta (7)}	1.0083492773819228268...	OEIS: A013665
ζ ( 9 ) {\displaystyle \zeta (9)}	1.0020083928260822144...	OEIS: A013667
ζ ( 11 ) {\displaystyle \zeta (11)}	1.0004941886041194645...	OEIS: A013669
ζ ( 13 ) {\displaystyle \zeta (13)}	1.0001227133475784891...	OEIS: A013671
ζ ( 15 ) {\displaystyle \zeta (15)}	1.0000305882363070204...	OEIS: A013673

It is known that ζ(3) is irrational (Apéry's theorem) and that infinitely many of the numbers ζ(2n + 1) : n ∈ N {\displaystyle \mathbb {N} } , are irrational.¹ There are also results on the irrationality of values of the Riemann zeta function at the elements of certain subsets of the positive odd integers; for example, at least one of ζ(5), ζ(7), ζ(9), or ζ(11) is irrational.²

The positive odd integers of the zeta function appear in physics, specifically correlation functions of antiferromagnetic XXX spin chain.³

Most of the identities following below are provided by Simon Plouffe. They are notable in that they converge quite rapidly, giving almost three digits of precision per iteration, and are thus useful for high-precision calculations.

Plouffe stated the following identities without proof.⁴ Proofs were later given by other authors.⁵

ζ(5)

ζ ( 5 ) = 1 294 π 5 − 72 35 ∑ n = 1 ∞ 1 n 5 ( e 2 π n − 1 ) − 2 35 ∑ n = 1 ∞ 1 n 5 ( e 2 π n + 1 ) ζ ( 5 ) = 12 ∑ n = 1 ∞ 1 n 5 sinh ⁡ ( π n ) − 39 20 ∑ n = 1 ∞ 1 n 5 ( e 2 π n − 1 ) + 1 20 ∑ n = 1 ∞ 1 n 5 ( e 2 π n + 1 ) {\displaystyle {\begin{aligned}\zeta (5)&={\frac {1}{294}}\pi ^{5}-{\frac {72}{35}}\sum _{n=1}^{\infty }{\frac {1}{n^{5}(e^{2\pi n}-1)}}-{\frac {2}{35}}\sum _{n=1}^{\infty }{\frac {1}{n^{5}(e^{2\pi n}+1)}}\\\zeta (5)&=12\sum _{n=1}^{\infty }{\frac {1}{n^{5}\sinh(\pi n)}}-{\frac {39}{20}}\sum _{n=1}^{\infty }{\frac {1}{n^{5}(e^{2\pi n}-1)}}+{\frac {1}{20}}\sum _{n=1}^{\infty }{\frac {1}{n^{5}(e^{2\pi n}+1)}}\end{aligned}}}

ζ(7)

ζ ( 7 ) = 19 56700 π 7 − 2 ∑ n = 1 ∞ 1 n 7 ( e 2 π n − 1 ) {\displaystyle \zeta (7)={\frac {19}{56700}}\pi ^{7}-2\sum _{n=1}^{\infty }{\frac {1}{n^{7}(e^{2\pi n}-1)}}\!}

Note that the sum is in the form of a Lambert series.

ζ(2n + 1)

By defining the quantities

S ± ( s ) = ∑ n = 1 ∞ 1 n s ( e 2 π n ± 1 ) {\displaystyle S_{\pm }(s)=\sum _{n=1}^{\infty }{\frac {1}{n^{s}(e^{2\pi n}\pm 1)}}}

a series of relationships can be given in the form

0 = a n ζ ( n ) − b n π n + c n S − ( n ) + d n S + ( n ) {\displaystyle 0=a_{n}\zeta (n)-b_{n}\pi ^{n}+c_{n}S_{-}(n)+d_{n}S_{+}(n)}

where an, bn, cn and dn are positive integers. Plouffe gives a table of values:

coefficients

n	an	bn	cn	dn
3	180	7	360	0
5	1470	5	3024	84
7	56700	19	113400	0
9	18523890	625	37122624	74844
11	425675250	1453	851350500	0
13	257432175	89	514926720	62370
15	390769879500	13687	781539759000	0
17	1904417007743250	6758333	3808863131673600	29116187100
19	21438612514068750	7708537	42877225028137500	0
21	1881063815762259253125	68529640373	3762129424572110592000	1793047592085750

These integer constants may be expressed as sums over Bernoulli numbers, as given in (Vepstas, 2006) below.

A fast algorithm for the calculation of Riemann's zeta function for any integer argument is given by E. A. Karatsuba.⁶⁷⁸

Negative integers

In general, for negative integers (and also zero), one has

ζ ( − n ) = ( − 1 ) n B n + 1 n + 1 {\displaystyle \zeta (-n)=(-1)^{n}{\frac {B_{n+1}}{n+1}}}

The so-called "trivial zeros" occur at the negative even integers:

ζ ( − 2 n ) = 0 {\displaystyle \zeta (-2n)=0} (Ramanujan summation)

The first few values for negative odd integers are

ζ ( − 1 ) = − 1 12 ζ ( − 3 ) = 1 120 ζ ( − 5 ) = − 1 252 ζ ( − 7 ) = 1 240 ζ ( − 9 ) = − 1 132 ζ ( − 11 ) = 691 32760 ζ ( − 13 ) = − 1 12 {\displaystyle {\begin{aligned}\zeta (-1)&=-{\frac {1}{12}}\\[4pt]\zeta (-3)&={\frac {1}{120}}\\[4pt]\zeta (-5)&=-{\frac {1}{252}}\\[4pt]\zeta (-7)&={\frac {1}{240}}\\[4pt]\zeta (-9)&=-{\frac {1}{132}}\\[4pt]\zeta (-11)&={\frac {691}{32760}}\\[4pt]\zeta (-13)&=-{\frac {1}{12}}\end{aligned}}}

However, just like the Bernoulli numbers, these do not stay small for increasingly negative odd values. For details on the first value, see 1 + 2 + 3 + 4 + · · ·.

So ζ(m) can be used as the definition of all (including those for index 0 and 1) Bernoulli numbers.

Derivatives

The derivative of the zeta function at the negative even integers is given by

ζ ′ ( − 2 n ) = ( − 1 ) n ( 2 n ) ! 2 ( 2 π ) 2 n ζ ( 2 n + 1 ) . {\displaystyle \zeta ^{\prime }(-2n)=(-1)^{n}{\frac {(2n)!}{2(2\pi )^{2n}}}\zeta (2n+1)\,.}

The first few values of which are

ζ ′ ( − 2 ) = − ζ ( 3 ) 4 π 2 ζ ′ ( − 4 ) = 3 4 π 4 ζ ( 5 ) ζ ′ ( − 6 ) = − 45 8 π 6 ζ ( 7 ) ζ ′ ( − 8 ) = 315 4 π 8 ζ ( 9 ) . {\displaystyle {\begin{aligned}\zeta ^{\prime }(-2)&=-{\frac {\zeta (3)}{4\pi ^{2}}}\\[4pt]\zeta ^{\prime }(-4)&={\frac {3}{4\pi ^{4}}}\zeta (5)\\[4pt]\zeta ^{\prime }(-6)&=-{\frac {45}{8\pi ^{6}}}\zeta (7)\\[4pt]\zeta ^{\prime }(-8)&={\frac {315}{4\pi ^{8}}}\zeta (9)\,.\end{aligned}}}

One also has

ζ ′ ( 0 ) = − 1 2 ln ⁡ ( 2 π ) ζ ′ ( − 1 ) = 1 12 − ln ⁡ A ζ ′ ( 2 ) = 1 6 π 2 ( γ + ln ⁡ 2 − 12 ln ⁡ A + ln ⁡ π ) {\displaystyle {\begin{aligned}\zeta ^{\prime }(0)&=-{\frac {1}{2}}\ln(2\pi )\\[4pt]\zeta ^{\prime }(-1)&={\frac {1}{12}}-\ln A\\[4pt]\zeta ^{\prime }(2)&={\frac {1}{6}}\pi ^{2}(\gamma +\ln 2-12\ln A+\ln \pi )\end{aligned}}}

where A is the Glaisher–Kinkelin constant. The first of these identities implies that the regularized product of the reciprocals of the positive integers is 1 / 2 π {\displaystyle 1/{\sqrt {2\pi }}} , thus the amusing "equation" ∞ ! = 2 π {\displaystyle \infty !={\sqrt {2\pi }}} .⁹

From the logarithmic derivative of the functional equation,

2 ζ ′ ( 1 / 2 ) ζ ( 1 / 2 ) = log ⁡ ( 2 π ) + π cos ⁡ ( π / 4 ) 2 sin ⁡ ( π / 4 ) − Γ ′ ( 1 / 2 ) Γ ( 1 / 2 ) = log ⁡ ( 2 π ) + π 2 + 2 log ⁡ 2 + γ . {\displaystyle 2{\frac {\zeta '(1/2)}{\zeta (1/2)}}=\log(2\pi )+{\frac {\pi \cos(\pi /4)}{2\sin(\pi /4)}}-{\frac {\Gamma '(1/2)}{\Gamma (1/2)}}=\log(2\pi )+{\frac {\pi }{2}}+2\log 2+\gamma \,.}

Selected derivatives

Value	Decimal expansion	Source
ζ ′ ( 3 ) {\displaystyle \zeta '(3)}	−0.19812624288563685333...	OEIS: A244115
ζ ′ ( 2 ) {\displaystyle \zeta '(2)}	−0.93754825431584375370...	OEIS: A073002
ζ ′ ( 0 ) {\displaystyle \zeta '(0)}	−0.91893853320467274178...	OEIS: A075700
ζ ′ ( − 1 2 ) {\displaystyle \zeta '(-{\tfrac {1}{2}})}	−0.36085433959994760734...	OEIS: A271854
ζ ′ ( − 1 ) {\displaystyle \zeta '(-1)}	−0.16542114370045092921...	OEIS: A084448
ζ ′ ( − 2 ) {\displaystyle \zeta '(-2)}	−0.030448457058393270780...	OEIS: A240966
ζ ′ ( − 3 ) {\displaystyle \zeta '(-3)}	+0.0053785763577743011444...	OEIS: A259068
ζ ′ ( − 4 ) {\displaystyle \zeta '(-4)}	+0.0079838114502686242806...	OEIS: A259069
ζ ′ ( − 5 ) {\displaystyle \zeta '(-5)}	−0.00057298598019863520499...	OEIS: A259070
ζ ′ ( − 6 ) {\displaystyle \zeta '(-6)}	−0.0058997591435159374506...	OEIS: A259071
ζ ′ ( − 7 ) {\displaystyle \zeta '(-7)}	−0.00072864268015924065246...	OEIS: A259072
ζ ′ ( − 8 ) {\displaystyle \zeta '(-8)}	+0.0083161619856022473595...	OEIS: A259073

Series involving ζ(n)

The following sums can be derived from the generating function: ∑ k = 2 ∞ ζ ( k ) x k − 1 = − ψ 0 ( 1 − x ) − γ {\displaystyle \sum _{k=2}^{\infty }\zeta (k)x^{k-1}=-\psi _{0}(1-x)-\gamma } where ψ0 is the digamma function.

∑ k = 2 ∞ ( ζ ( k ) − 1 ) = 1 ∑ k = 1 ∞ ( ζ ( 2 k ) − 1 ) = 3 4 ∑ k = 1 ∞ ( ζ ( 2 k + 1 ) − 1 ) = 1 4 ∑ k = 2 ∞ ( − 1 ) k ( ζ ( k ) − 1 ) = 1 2 {\displaystyle {\begin{aligned}\sum _{k=2}^{\infty }(\zeta (k)-1)&=1\\[4pt]\sum _{k=1}^{\infty }(\zeta (2k)-1)&={\frac {3}{4}}\\[4pt]\sum _{k=1}^{\infty }(\zeta (2k+1)-1)&={\frac {1}{4}}\\[4pt]\sum _{k=2}^{\infty }(-1)^{k}(\zeta (k)-1)&={\frac {1}{2}}\end{aligned}}}

Series related to the Euler–Mascheroni constant (denoted by γ) are ∑ k = 2 ∞ ( − 1 ) k ζ ( k ) k = γ ∑ k = 2 ∞ ζ ( k ) − 1 k = 1 − γ ∑ k = 2 ∞ ( − 1 ) k ζ ( k ) − 1 k = ln ⁡ 2 + γ − 1 {\displaystyle {\begin{aligned}\sum _{k=2}^{\infty }(-1)^{k}{\frac {\zeta (k)}{k}}&=\gamma \\[4pt]\sum _{k=2}^{\infty }{\frac {\zeta (k)-1}{k}}&=1-\gamma \\[4pt]\sum _{k=2}^{\infty }(-1)^{k}{\frac {\zeta (k)-1}{k}}&=\ln 2+\gamma -1\end{aligned}}}

and using the principal value ζ ( k ) = lim ε → 0 ζ ( k + ε ) + ζ ( k − ε ) 2 {\displaystyle \zeta (k)=\lim _{\varepsilon \to 0}{\frac {\zeta (k+\varepsilon )+\zeta (k-\varepsilon )}{2}}} which of course affects only the value at 1, these formulae can be stated as

∑ k = 1 ∞ ( − 1 ) k ζ ( k ) k = 0 ∑ k = 1 ∞ ζ ( k ) − 1 k = 0 ∑ k = 1 ∞ ( − 1 ) k ζ ( k ) − 1 k = ln ⁡ 2 {\displaystyle {\begin{aligned}\sum _{k=1}^{\infty }(-1)^{k}{\frac {\zeta (k)}{k}}&=0\\[4pt]\sum _{k=1}^{\infty }{\frac {\zeta (k)-1}{k}}&=0\\[4pt]\sum _{k=1}^{\infty }(-1)^{k}{\frac {\zeta (k)-1}{k}}&=\ln 2\end{aligned}}}

and show that they depend on the principal value of ζ(1) = γ .

Nontrivial zeros

Main article: Riemann hypothesis

Zeros of the Riemann zeta except negative even integers are called "nontrivial zeros". The Riemann hypothesis states that the real part of every nontrivial zero must be ⁠1/2⁠. In other words, all known nontrivial zeros of the Riemann zeta are of the form z = ⁠1/2⁠ + yi where y is a real number. The following table contains the decimal expansion of Im(z) for the first few nontrivial zeros:

Selected nontrivial zeros

Decimal expansion of Im(z)	Source
14.134725141734693790...	OEIS: A058303
21.022039638771554992...	OEIS: A065434
25.010857580145688763...	OEIS: A065452
30.424876125859513210...	OEIS: A065453
32.935061587739189690...	OEIS: A192492
37.586178158825671257...	OEIS: A305741
40.918719012147495187...	OEIS: A305742
43.327073280914999519...	OEIS: A305743
48.005150881167159727...	OEIS: A305744
49.773832477672302181...	OEIS: A306004

Andrew Odlyzko computed the first 2 million nontrivial zeros accurate to within 4×10−9, and the first 100 zeros accurate within 1000 decimal places. See their website for the tables and bibliographies.¹⁰¹¹ A table of about 103 billion zeros with high precision (of ±2−102≈±2·10−31) is available for interactive access and download (although in a very inconvenient compressed format) via LMFDB.¹²

Ratios

Although evaluating particular values of the zeta function is difficult, often certain ratios can be found by inserting particular values of the gamma function into the functional equation

ζ ( s ) = 2 s π s − 1 sin ⁡ ( π s 2 ) Γ ( 1 − s ) ζ ( 1 − s ) {\displaystyle \zeta (s)=2^{s}\pi ^{s-1}\sin \left({\frac {\pi s}{2}}\right)\Gamma (1-s)\zeta (1-s)}

We have simple relations for half-integer arguments

ζ ( 3 / 2 ) ζ ( − 1 / 2 ) = − 4 π ζ ( 5 / 2 ) ζ ( − 3 / 2 ) = − 16 π 2 3 ζ ( 7 / 2 ) ζ ( − 5 / 2 ) = 64 π 3 15 ζ ( 9 / 2 ) ζ ( − 7 / 2 ) = 256 π 4 105 {\displaystyle {\begin{aligned}{\frac {\zeta (3/2)}{\zeta (-1/2)}}&=-4\pi \\{\frac {\zeta (5/2)}{\zeta (-3/2)}}&=-{\frac {16\pi ^{2}}{3}}\\{\frac {\zeta (7/2)}{\zeta (-5/2)}}&={\frac {64\pi ^{3}}{15}}\\{\frac {\zeta (9/2)}{\zeta (-7/2)}}&={\frac {256\pi ^{4}}{105}}\end{aligned}}}

Other examples follow for more complicated evaluations and relations of the gamma function. For example a consequence of the relation

Γ ( 3 4 ) = ( π 2 ) 1 4 AGM ⁡ ( 2 , 1 ) 1 2 {\displaystyle \Gamma \left({\tfrac {3}{4}}\right)=\left({\tfrac {\pi }{2}}\right)^{\tfrac {1}{4}}{\operatorname {AGM} \left({\sqrt {2}},1\right)}^{\tfrac {1}{2}}}

is the zeta ratio relation

ζ ( 3 / 4 ) ζ ( 1 / 4 ) = 2 π ( 2 − 2 ) AGM ⁡ ( 2 , 1 ) {\displaystyle {\frac {\zeta (3/4)}{\zeta (1/4)}}=2{\sqrt {\frac {\pi }{(2-{\sqrt {2}})\operatorname {AGM} \left({\sqrt {2}},1\right)}}}}

where AGM is the arithmetic–geometric mean. In a similar vein, it is possible to form radical relations, such as from

Γ ( 1 5 ) 2 Γ ( 1 10 ) Γ ( 3 10 ) = 1 + 5 2 7 10 5 4 {\displaystyle {\frac {\Gamma \left({\frac {1}{5}}\right)^{2}}{\Gamma \left({\frac {1}{10}}\right)\Gamma \left({\frac {3}{10}}\right)}}={\frac {\sqrt {1+{\sqrt {5}}}}{2^{\tfrac {7}{10}}{\sqrt[{4}]{5}}}}}

the analogous zeta relation is

ζ ( 1 / 5 ) 2 ζ ( 7 / 10 ) ζ ( 9 / 10 ) ζ ( 1 / 10 ) ζ ( 3 / 10 ) ζ ( 4 / 5 ) 2 = ( 5 − 5 ) ( 10 + 5 + 5 ) 10 ⋅ 2 3 10 {\displaystyle {\frac {\zeta (1/5)^{2}\zeta (7/10)\zeta (9/10)}{\zeta (1/10)\zeta (3/10)\zeta (4/5)^{2}}}={\frac {(5-{\sqrt {5}})\left({\sqrt {10}}+{\sqrt {5+{\sqrt {5}}}}\right)}{10\cdot 2^{\tfrac {3}{10}}}}}

Further reading

• Ciaurri, Óscar; Navas, Luis M.; Ruiz, Francisco J.; Varona, Juan L. (May 2015). "A Simple Computation of ζ(2k)". The American Mathematical Monthly. 122 (5): 444–451. arXiv:1209.5030. doi:10.4169/amer.math.monthly.122.5.444. JSTOR 10.4169/amer.math.monthly.122.5.444. S2CID 207521195.
• Simon Plouffe, "Identities inspired from Ramanujan Notebooks Archived 2009-01-30 at the Wayback Machine", (1998).
• Simon Plouffe, "Identities inspired by Ramanujan Notebooks part 2 PDF Archived 2011-09-26 at the Wayback Machine" (2006).
• Vepstas, Linas (2006). "On Plouffe's Ramanujan identities" (PDF). The Ramanujan Journal. 27 (3): 387–408. arXiv:math.NT/0609775. doi:10.1007/s11139-011-9335-9. S2CID 8789411.
• Zudilin, Wadim (2001). "One of the Numbers ζ(5), ζ(7), ζ(9), ζ(11) Is Irrational". Russian Mathematical Surveys. 56 (4): 774–776. Bibcode:2001RuMaS..56..774Z. doi:10.1070/RM2001v056n04ABEH000427. MR 1861452. S2CID 250734661. PDF PDF Russian PS Russian
• Nontrival zeros reference by Andrew Odlyzko:
  • Bibliography
  • Tables

References

1. Rivoal, T. (2000). "La fonction zeta de Riemann prend une infinité de valeurs irrationnelles aux entiers impairs". Comptes Rendus de l'Académie des Sciences, Série I. 331 (4): 267–270. arXiv:math/0008051. Bibcode:2000CRASM.331..267R. doi:10.1016/S0764-4442(00)01624-4. S2CID 119678120. /wiki/Tanguy_Rivoal ↩

2. W. Zudilin (2001). "One of the numbers ζ(5), ζ(7), ζ(9), ζ(11) is irrational". Russ. Math. Surv. 56 (4): 774–776. Bibcode:2001RuMaS..56..774Z. doi:10.1070/rm2001v056n04abeh000427. S2CID 250734661. /wiki/Bibcode_(identifier) ↩

3. Boos, H.E.; Korepin, V.E.; Nishiyama, Y.; Shiroishi, M. (2002). "Quantum correlations and number theory". J. Phys. A. 35 (20): 4443–4452. arXiv:cond-mat/0202346. Bibcode:2002JPhA...35.4443B. doi:10.1088/0305-4470/35/20/305. S2CID 119143600.. /wiki/ArXiv_(identifier) ↩

4. "Identities for Zeta(2*n+1)". http://www.plouffe.fr/simon/identities.html ↩

5. "Formulas for Odd Zeta Values and Powers of Pi". https://cs.uwaterloo.ca/journals/JIS/VOL14/Lopatto/lopatto2.html ↩

6. Karatsuba, E. A. (1995). "Fast calculation of the Riemann zeta function ζ(s) for integer values of the argument s". Probl. Perdachi Inf. 31 (4): 69–80. MR 1367927. https://www.mathnet.ru/php/archive.phtml?wshow=paper&jrnid=ppi&paperid=294&option_lang=eng ↩

7. E. A. Karatsuba: Fast computation of the Riemann zeta function for integer argument. Dokl. Math. Vol.54, No.1, p. 626 (1996). ↩

8. E. A. Karatsuba: Fast evaluation of ζ(3). Probl. Inf. Transm. Vol.29, No.1, pp. 58–62 (1993). ↩

9. Muñoz García, E.; Pérez Marco, R. (2008), "The Product Over All Primes is 4 π 2 {\displaystyle 4\pi ^{2}} ", Commun. Math. Phys. (277): 69–81. ↩

10. Odlyzko, Andrew. "Tables of zeros of the Riemann zeta function". Retrieved 7 September 2022. http://www.dtc.umn.edu/~odlyzko/zeta_tables/index.html ↩

11. Odlyzko, Andrew. "Papers on Zeros of the Riemann Zeta Function and Related Topics". Retrieved 7 September 2022. http://www.dtc.umn.edu/~odlyzko/doc/zeta.html ↩

12. LMFDB: Zeros of ζ(s) https://www.lmfdb.org/zeros/zeta/ ↩