• Source: Dedekind eta function

In mathematics, the Dedekind eta function, named after Richard Dedekind, is a modular form of weight 1/2 and is a function defined on the upper half-plane of complex numbers, where the imaginary part is positive. It also occurs in bosonic string theory.




Definition


For any complex number τ with Im(τ) > 0, let q = e2πiτ; then the eta function is defined by,




η
(
τ
)
=

e



π
i
τ

12




∏

n
=
1


∞



(

1
−

e

2
n
π
i
τ



)

=

q


1
24




∏

n
=
1


∞



(

1
−

q

n



)

.


{\displaystyle \eta (\tau )=e^{\frac {\pi i\tau }{12}}\prod _{n=1}^{\infty }\left(1-e^{2n\pi i\tau }\right)=q^{\frac {1}{24}}\prod _{n=1}^{\infty }\left(1-q^{n}\right).}


Raising the eta equation to the 24th power and multiplying by (2π)12 gives




Δ
(
τ
)
=
(
2
π

)

12



η

24


(
τ
)


{\displaystyle \Delta (\tau )=(2\pi )^{12}\eta ^{24}(\tau )}


where Δ is the modular discriminant. The presence of 24 can be understood by connection with other occurrences, such as in the 24-dimensional Leech lattice.
The eta function is holomorphic on the upper half-plane but cannot be continued analytically beyond it.

The eta function satisfies the functional equations








η
(
τ
+
1
)



=

e



π
i

12



η
(
τ
)
,




η

(

−


1
τ



)




=


−
i
τ



η
(
τ
)
.







{\displaystyle {\begin{aligned}\eta (\tau +1)&=e^{\frac {\pi i}{12}}\eta (\tau ),\\\eta \left(-{\frac {1}{\tau }}\right)&={\sqrt {-i\tau }}\,\eta (\tau ).\,\end{aligned}}}


In the second equation the branch of the square root is chosen such that √−iτ = 1 when τ = i.
More generally, suppose a, b, c, d are integers with ad − bc = 1, so that




τ
↦



a
τ
+
b


c
τ
+
d





{\displaystyle \tau \mapsto {\frac {a\tau +b}{c\tau +d}}}


is a transformation belonging to the modular group. We may assume that either c > 0, or c = 0 and d = 1. Then




η

(



a
τ
+
b


c
τ
+
d



)

=
ϵ
(
a
,
b
,
c
,
d
)


(

c
τ
+
d

)



1
2



η
(
τ
)
,


{\displaystyle \eta \left({\frac {a\tau +b}{c\tau +d}}\right)=\epsilon (a,b,c,d)\left(c\tau +d\right)^{\frac {1}{2}}\eta (\tau ),}


where




ϵ
(
a
,
b
,
c
,
d
)
=


{




e



b
i
π

12





c
=
0
,

d
=
1
,





e

i
π

(




a
+
d


12
c



−
s
(
d
,
c
)
−


1
4



)





c
>
0.








{\displaystyle \epsilon (a,b,c,d)={\begin{cases}e^{\frac {bi\pi }{12}}&c=0,\,d=1,\\e^{i\pi \left({\frac {a+d}{12c}}-s(d,c)-{\frac {1}{4}}\right)}&c>0.\end{cases}}}


Here s(h,k) is the Dedekind sum




s
(
h
,
k
)
=

∑

n
=
1


k
−
1




n
k



(




h
n

k


−

⌊



h
n

k


⌋

−


1
2



)

.


{\displaystyle s(h,k)=\sum _{n=1}^{k-1}{\frac {n}{k}}\left({\frac {hn}{k}}-\left\lfloor {\frac {hn}{k}}\right\rfloor -{\frac {1}{2}}\right).}


Because of these functional equations the eta function is a modular form of weight ⁠1/2⁠ and level 1 for a certain character of order 24 of the metaplectic double cover of the modular group, and can be used to define other modular forms. In particular the modular discriminant of Weierstrass with





ω

2


=
τ

ω

1




{\displaystyle \omega _{2}=\tau \omega _{1}}


can be defined as




Δ
(
τ
)
=
(
2
π

ω

1



)

12


η
(
τ

)

24





{\displaystyle \Delta (\tau )=(2\pi \omega _{1})^{12}\eta (\tau )^{24}\,}


and is a modular form of weight 12. Some authors omit the factor of (2π)12, so that the series expansion has integral coefficients.
The Jacobi triple product implies that the eta is (up to a factor) a Jacobi theta function for special values of the arguments:




η
(
τ
)
=

∑

n
=
1


∞


χ
(
n
)
exp
⁡

(



π
i

n

2


τ

12


)

,


{\displaystyle \eta (\tau )=\sum _{n=1}^{\infty }\chi (n)\exp \left({\frac {\pi in^{2}\tau }{12}}\right),}


where χ(n) is "the" Dirichlet character modulo 12 with χ(±1) = 1 and χ(±5) = −1. Explicitly,




η
(
τ
)
=

e



π
i
τ

12



ϑ

(




τ
+
1

2


;
3
τ

)

.


{\displaystyle \eta (\tau )=e^{\frac {\pi i\tau }{12}}\vartheta \left({\frac {\tau +1}{2}};3\tau \right).}


The Euler function








ϕ
(
q
)



=

∏

n
=
1


∞



(

1
−

q

n



)







=

q

−


1
24




η
(
τ
)
,






{\displaystyle {\begin{aligned}\phi (q)&=\prod _{n=1}^{\infty }\left(1-q^{n}\right)\\&=q^{-{\frac {1}{24}}}\eta (\tau ),\end{aligned}}}


has a power series by the Euler identity:




ϕ
(
q
)
=

∑

n
=
−
∞


∞


(
−
1

)

n



q



3

n

2


−
n

2



.


{\displaystyle \phi (q)=\sum _{n=-\infty }^{\infty }(-1)^{n}q^{\frac {3n^{2}-n}{2}}.}


Note that by using Euler Pentagonal number theorem for





I


(
τ
)
>
0


{\displaystyle {\mathfrak {I}}(\tau )>0}

, the eta function can be expressed as




η
(
τ
)
=

∑

n
=
−
∞


∞



e

π
i
n



e

3
π
i


(

n
+


1
6



)


2


τ


.


{\displaystyle \eta (\tau )=\sum _{n=-\infty }^{\infty }e^{\pi in}e^{3\pi i\left(n+{\frac {1}{6}}\right)^{2}\tau }.}


This can be proved by using



x
=
2
π
i
τ


{\displaystyle x=2\pi i\tau }

in Euler Pentagonal number theorem with the definition of eta function.
Because the eta function is easy to compute numerically from either power series, it is often helpful in computation to express other functions in terms of it when possible, and products and quotients of eta functions, called eta quotients, can be used to express a great variety of modular forms.
The picture on this page shows the modulus of the Euler function: the additional factor of q⁠1/24⁠ between this and eta makes almost no visual difference whatsoever. Thus, this picture can be taken as a picture of eta as a function of q.




Combinatorial identities


The theory of the algebraic characters of the affine Lie algebras gives rise to a large class of previously unknown identities for the eta function. These identities follow from the Weyl–Kac character formula, and more specifically from the so-called "denominator identities". The characters themselves allow the construction of generalizations of the Jacobi theta function which transform under the modular group; this is what leads to the identities. An example of one such new identity is




η
(
8
τ
)
η
(
16
τ
)
=

∑



m
,
n
∈

Z



m
≤

|

3
n

|





(
−
1

)

m



q

(
2
m
+
1

)

2


−
32

n

2






{\displaystyle \eta (8\tau )\eta (16\tau )=\sum _{m,n\in \mathbb {Z} \atop m\leq |3n|}(-1)^{m}q^{(2m+1)^{2}-32n^{2}}}


where q = e2πiτ is the q-analog or "deformation" of the highest weight of a module.




Special values


From the above connection with the Euler function together with the special values of the latter, it can be easily deduced that








η
(
i
)



=



Γ

(


1
4


)



2

π


3
4










η

(




1
2



i

)




=



Γ

(


1
4


)




2


7
8




π


3
4










η
(
2
i
)



=



Γ

(


1
4


)




2


11
8




π


3
4










η
(
3
i
)



=



Γ

(


1
4


)



2


3

3





(

3
+
2


3



)



1
12




π


3
4










η
(
4
i
)



=






−
1
+


2




4




Γ

(


1
4


)




2


29
16




π


3
4










η

(

e



2
π
i

3



)




=

e

−



π
i

24









3

8




Γ


(


1
3


)



3
2





2
π









{\displaystyle {\begin{aligned}\eta (i)&={\frac {\Gamma \left({\frac {1}{4}}\right)}{2\pi ^{\frac {3}{4}}}}\\[6pt]\eta \left({\tfrac {1}{2}}i\right)&={\frac {\Gamma \left({\frac {1}{4}}\right)}{2^{\frac {7}{8}}\pi ^{\frac {3}{4}}}}\\[6pt]\eta (2i)&={\frac {\Gamma \left({\frac {1}{4}}\right)}{2^{\frac {11}{8}}\pi ^{\frac {3}{4}}}}\\[6pt]\eta (3i)&={\frac {\Gamma \left({\frac {1}{4}}\right)}{2{\sqrt[{3}]{3}}\left(3+2{\sqrt {3}}\right)^{\frac {1}{12}}\pi ^{\frac {3}{4}}}}\\[6pt]\eta (4i)&={\frac {{\sqrt[{4}]{-1+{\sqrt {2}}}}\,\Gamma \left({\frac {1}{4}}\right)}{2^{\frac {29}{16}}\pi ^{\frac {3}{4}}}}\\[6pt]\eta \left(e^{\frac {2\pi i}{3}}\right)&=e^{-{\frac {\pi i}{24}}}{\frac {{\sqrt[{8}]{3}}\,\Gamma \left({\frac {1}{3}}\right)^{\frac {3}{2}}}{2\pi }}\end{aligned}}}





Eta quotients


Eta quotients are defined by quotients of the form





∏

0
<
d
∣
N


η
(
d
τ

)


r

d






{\displaystyle \prod _{0eta (d\tau )^{r_{d}}}


where d is a non-negative integer and rd is any integer. Linear combinations of eta quotients at imaginary quadratic arguments may be algebraic, while combinations of eta quotients may even be integral. For example, define,








j
(
τ
)



=


(



(



η
(
τ
)


η
(
2
τ
)



)


8


+

2

8




(



η
(
2
τ
)


η
(
τ
)



)


16



)


3







j

2
A


(
τ
)



=


(



(



η
(
τ
)


η
(
2
τ
)



)


12


+

2

6




(



η
(
2
τ
)


η
(
τ
)



)


12



)


2







j

3
A


(
τ
)



=


(



(



η
(
τ
)


η
(
3
τ
)



)


6


+

3

3




(



η
(
3
τ
)


η
(
τ
)



)


6



)


2







j

4
A


(
τ
)



=


(



(



η
(
τ
)


η
(
4
τ
)



)


4


+

4

2




(



η
(
4
τ
)


η
(
τ
)



)


4



)


2


=


(




η

2


(
2
τ
)


η
(
τ
)

η
(
4
τ
)



)


24








{\displaystyle {\begin{aligned}j(\tau )&=\left(\left({\frac {\eta (\tau )}{\eta (2\tau )}}\right)^{8}+2^{8}\left({\frac {\eta (2\tau )}{\eta (\tau )}}\right)^{16}\right)^{3}\\[6pt]j_{2A}(\tau )&=\left(\left({\frac {\eta (\tau )}{\eta (2\tau )}}\right)^{12}+2^{6}\left({\frac {\eta (2\tau )}{\eta (\tau )}}\right)^{12}\right)^{2}\\[6pt]j_{3A}(\tau )&=\left(\left({\frac {\eta (\tau )}{\eta (3\tau )}}\right)^{6}+3^{3}\left({\frac {\eta (3\tau )}{\eta (\tau )}}\right)^{6}\right)^{2}\\[6pt]j_{4A}(\tau )&=\left(\left({\frac {\eta (\tau )}{\eta (4\tau )}}\right)^{4}+4^{2}\left({\frac {\eta (4\tau )}{\eta (\tau )}}\right)^{4}\right)^{2}=\left({\frac {\eta ^{2}(2\tau )}{\eta (\tau )\,\eta (4\tau )}}\right)^{24}\end{aligned}}}


with the 24th power of the Weber modular function 𝔣(τ). Then,








j

(



1
+


−
163



2


)




=
−

640320

3


,



e

π


163







≈

640320

3


+
743.99999999999925
…





j

2
A



(



−
58

2


)




=

396

4


,



e

π


58







≈

396

4


−
104.00000017
…





j

3
A



(



1
+


−


89
3





2


)




=
−

300

3


,



e

π



89
3








≈

300

3


+
41.999971
…





j

4
A



(



−
7

2


)




=

2

12


,



e

π


7







≈

2

12


−
24.06
…






{\displaystyle {\begin{aligned}j\left({\frac {1+{\sqrt {-163}}}{2}}\right)&=-640320^{3},&e^{\pi {\sqrt {163}}}&\approx 640320^{3}+743.99999999999925\dots \\[6pt]j_{2A}\left({\frac {\sqrt {-58}}{2}}\right)&=396^{4},&e^{\pi {\sqrt {58}}}&\approx 396^{4}-104.00000017\dots \\[6pt]j_{3A}\left({\frac {1+{\sqrt {-{\frac {89}{3}}}}}{2}}\right)&=-300^{3},&e^{\pi {\sqrt {\frac {89}{3}}}}&\approx 300^{3}+41.999971\dots \\[6pt]j_{4A}\left({\frac {\sqrt {-7}}{2}}\right)&=2^{12},&e^{\pi {\sqrt {7}}}&\approx 2^{12}-24.06\dots \end{aligned}}}


and so on, values which appear in Ramanujan–Sato series.
Eta quotients may also be a useful tool for describing bases of modular forms, which are notoriously difficult to compute and express directly. In 1993 Basil Gordon and Kim Hughes proved that if an eta quotient ηg of the form given above, namely




∏

0
<
d
∣
N


η
(
d
τ

)


r

d






{\displaystyle \prod _{0eta (d\tau )^{r_{d}}}

satisfies





∑

0
<
d
∣
N


d

r

d


≡
0


(
mod

24
)



and



∑

0
<
d
∣
N




N
d



r

d


≡
0


(
mod

24
)

,


{\displaystyle \sum _{0

then ηg is a weight k modular form for the congruence subgroup Γ0(N) (up to holomorphicity) where




k
=


1
2



∑

0
<
d
∣
N



r

d


.


{\displaystyle k={\frac {1}{2}}\sum _{0

This result was extended in 2019 such that the converse holds for cases when N is coprime to 6, and it remains open that the original theorem is sharp for all integers N. This also extends to state that any modular eta quotient for any level n congruence subgroup must also be a modular form for the group Γ(N). While these theorems characterize modular eta quotients, the condition of holomorphicity must be checked separately using a theorem that emerged from the work of Gérard Ligozat and Yves Martin:
If ηg is an eta quotient satisfying the above conditions for the integer N and c and d are coprime integers, then the order of vanishing at the cusp ⁠c/d⁠ relative to Γ0(N) is






N
24



∑

0
<
δ

|

N





gcd


(

d
,
δ

)


2



r

δ




gcd

(

d
,


N
δ



)

d
δ



.


{\displaystyle {\frac {N}{24}}\sum _{0<\delta |N}{\frac {\gcd \left(d,\delta \right)^{2}r_{\delta }}{\gcd \left(d,{\frac {N}{\delta }}\right)d\delta }}.}


These theorems provide an effective means of creating holomorphic modular eta quotients, however this may not be sufficient to construct a basis for a vector space of modular forms and cusp forms. A useful theorem for limiting the number of modular eta quotients to consider states that a holomorphic weight k modular eta quotient on Γ0(N) must satisfy





∑

0
<
d
∣
N



|


r

d



|

≤

∏

p
∣
N




(



p
+
1


p
−
1



)


min


(


2
,


ord


p


(
N
)


)




,


{\displaystyle \sum _{0

where ordp(N) denotes the largest integer m such that pm divides N.
These results lead to several characterizations of spaces of modular forms that can be spanned by modular eta quotients. Using the graded ring structure on the ring of modular forms, we can compute bases of vector spaces of modular forms composed of




C



{\displaystyle \mathbb {C} }

-linear combinations of eta-quotients. For example, if we assume N = pq is a semiprime then the following process can be used to compute an eta-quotient basis of Mk(Γ0(N)).

A collection of over 6300 product identities for the Dedekind Eta Function in a canonical, standardized form is available at the Wayback machine of Michael Somos' website.




See also


Chowla–Selberg formula
Ramanujan–Sato series
q-series
Weierstrass's elliptic functions
Partition function
Kronecker limit formula
Affine Lie algebra




References






Further reading


Apostol, Tom M. (1990). Modular functions and Dirichlet Series in Number Theory. Graduate Texts in Mathematics. Vol. 41 (2nd ed.). Springer-Verlag. ch. 3. ISBN 3-540-97127-0.
Koblitz, Neal (1993). Introduction to Elliptic Curves and Modular Forms. Graduate Texts in Mathematics. Vol. 97 (2nd ed.). Springer-Verlag. ISBN 3-540-97966-2.

Kata Kunci Pencarian:

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• Teorema dasar aljabar
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• Grup abelian bebas
• Dedekind eta function
• Eta function
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