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Certain subrings in classical invariant theory

Nur Hamid , Masashi Kosuda and Manabu Oura

Abstract. We have studied E-polynomials which are combinato- rial analogue of Eisenstein series. In this paper, we apply this ap- proach to classical invariant theory. The corresponding subrings to E-polynomials are investigated.

1. Introduction

Eisenstein series are important in number theory. Under the correspon- dence between combinatorics and modular forms, we have introduced the notion of E-polynomials.

On the other hand, classical invariant theory plays important roles in many branches of mathematics. Igusa [2] discussed invariant theory of bi- nary forms and arithmetic invariants. The connection between the modular forms and projective invariants then was given in [3]. The structure of the graded ring of invariants of binary octavics then was given by Shioda in [8].

In this paper, we construct the analogue theory of Eisenstein series. We apply the notion to classical invariant theory. The computations are done by [1] and [6].

Let m be a positive integer. We take a ground form of degree m f =

X

m i=0

u

i

m i

ξ

1mi

ξ

i2

.

2010

Mathematics Subject Classification.

Primary 13A50; Secondary 13A02, 16W50.

Key words and phrases.

Invariant ring, E-polynomial.

33

(2)

Here we mean f is a polynomial of degree m in variables ξ

1

, ξ

2

with co- efficients u

i mi

where u

i

are variables. In some parts, we regard f as an element of C[ξ

1

, ξ

2±1

, u

±01

, u

1

, . . . , u

m

].

While ξ

1

, ξ

2

are transformed according to

1

ξ

2

) = (ξ

1

ξ

2

)A (”contragrediently”),

f changes into a form of the new variables ξ

1

, ξ

2

with the coefficients u

0

, u

1

, . . . , u

m

where

 

 

u

0

u

1

.. . u

m

 

 

 =

A

m

 

 

u

0

u

1

.. . u

m

 

 

.

We write this correspondence u

=

A

m

u for short. This gives an irre- ducible representation (A 7→

A

m

) of SL(2, C) of degree m + 1.

We let SL(2, C) operate on C[u] = C[u

0

, u

1

, . . . , u

m

] by the above rep- resentation and consider the invariant subring, say S(2, m):

S(2, m) := {J C[u] : J(u

) = J(u),

A SL(2, C)}.

It is known that S(2, m) is of finite type over C. For example, we have S(2, 2) = C[u

0

u

2

u

21

].

Let M be a graded ring such that each homogeneous part M

d

of degree d is a finite dimensional vector space over M

0

= C. We can write M as

M = M

d=0

M

d

.

The dimension formula of M is defined by the formal series X

d=0

(dim M

d

)t

d

.

(3)

The following formulas are the dimension formulas of S(2, m) for m = 2, 4, 6, 8.

S(2, 2) : X

d=0

(dim S

d

(2, 2))t

d

= 1 1 t

2

, S(2, 4) :

X

d=0

(dim S

d

(2, 4))t

d

= 1

(1 t

2

)(1 t

3

) , S(2, 6) :

X

d=0

(dim S

d

(2, 6))t

d

= 1 + t

15

(1 t

2

)(1 t

4

)(1 t

6

)(1 t

10

) , S(2, 8) :

X

d=0

(dim S

d

(2, 8))t

d

= 1 + t

8

+ t

9

+ t

10

+ t

18

Q

7

i=2

(1 t

i

) .

We refer to [7] for the dimension formulas of S(2, 2), S(2, 4), S(2, 6) and to [8] for S(2, 8).

The generators of the rings mentioned are known. For example, S(2, 4) is generated by P and Q whose explicit forms are

P = u

0

u

4

4u

1

u

3

+ 3u

22

, Q = det

 

u

0

u

1

u

2

u

1

u

2

u

3

u

2

u

3

u

4

  .

The ring S(2, 6) are generated by 5 elements J

2

, J

4

, J

6

, J

10

, and J

15

. We write the generators of S(2, 6) in Appendix A. In this paper, we deal with only invariants of even degrees. So we omit J

15

. We denote by S(2, m)

e

the even parts of S(2, m).

Let ξ

3

= ξ

1

2

. The form ξ

2m

f is a polynomial in ξ

3

with coefficients in C[u] and can be written as

X

m i=0

u

i

m i

ξ

3mi

. Let ε

1

, ε

2

, . . . , ε

m

be the roots of the equation

X

m i=0

u

i

m

i

ξ

3mi

= 0.

(4)

We can write

X

m i=1

ε

i

= m

1 u

1

u

0

, .. .

X

i1<i2<···<ir

ε

i1

ε

i2

· · · ε

ir

= ( 1)

r

m

r u

r

u

0

, .. .

ε

1

ε

2

· · · ε

m

= ( 1)

m

m

m u

m

u

0

.

In order to obtain the useful construction of invariants, we shall interpret the ground form as

f = u

0

Y

m i=1

1

ε

i

ξ

2

) .

As usual, we denote by S

n

the symmetric group of degree n. The following lemma gives a construction of invariants we expected (cf. [2, 9]).

Lemma 1.1. An expression of the form u

r0

X

i

ε

j

)(ε

k

ε

l

) . . . ,

in which every ε

i

appears r times in each product and which is symmetric in ε

1

, ε

2

, . . . , ε

m

can be considered as an invariant of degree r.

2. Results

Let g be a positive integer. We start with a ground form of degree 2g + 2 f =

2g+2

X

i=0

u

i

2g + 2 i

ξ

(2g+2)1 i

ξ

i2

= u

0 2g+2

Y

i=1

1

ε

i

ξ

2

) .

We would like to concentrate on one type of invariants we shall define now.

We fix the following polynomial

φ

2n

= u

2n0

1

ε

2

)

2n

3

ε

4

)

2n

. . .

2g+1

ε

2g+2

)

2n

.

(5)

We denote by G the symmetric group of degree 2g + 2. The group G acts on the polynomial ring C[ε

1

, . . . , ε

2g+2

] as F (. . . , ε

i

, . . . )

σ

= F(. . . , ε

iσ

, . . . ).

Let G

φ2n

be the stabilizer of φ

2n

, that is, elements of G which preserve φ

2n

. Proposition 2.1. The group G

φ2n

can be generated by the (g + 1) + 2 elements

(1 2), (3 4), . . . , (2g + 1 2g + 2), (1 3)(2 4), (1 3 5 . . . 2g + 1)(2 4 . . . 2g + 2)

and is isomorphic to C

2g+1

o S

g+1

. In particular, G

φ2n

does not depend on n.

Proof. The elements given in Proposition 2.1 are in G

φ2n

. Conversely, since (ε

i

ε

j

)

2n

= (ε

j

ε

i

)

2n

, the first g + 1 elements can be obtained by interchanging of two indexes in each parenthesis. These interchanging are isomorphic to C

2g+1

. Let ˜ 1, ˜ 2, . . . , g ] + 1 represent (1 2), (3 4), . . . , (g + 1 g + 2), respectively. Then, the additional two generators come from the generators of the set of all permutations of { ˜ 1, ˜ 2, . . . , g ] + 1 } . This set is isomorphic to S

g+1

and its generators are (˜ 1 ˜ 2) and (˜ 1 ... g ] + 1) which represent (1 2)(3 4) and (1 3 . . . 2g + 1)(2 4 . . . 2g + 2), respectively.

For simplicity, we denote by K for G

φ2n

and by κ the cardinality of K\G.

The number κ for g = 1, 2, 3 is 3, 15, 105, respectively.

Set

ψ

2n

= X

K\G∋σ

φ

σ2n

,

which is actually an element of degree 2n in S(2, 2g + 2) by Lemma 1.1.

We call the polynomial ψ

2n

by an E-polynomial. We shall denote by A

g

the ring generated by ψ

2n

(n = 1, 2, . . . ) over C. The ring A

g

is a subring of the invariant ring S(2, 2g + 2).

Theorem 2.2. The ring A

g

is finitely generated over C. More precisely the elements ψ

2

, ψ

4

, . . . , ψ

generate the ring A

g

.

Proof. Since the second assertion implies the first, we shall show the second.

Let σ

1

, σ

2

, . . . , σ

κ

be a set of representatives of K \ G. For each σ

i

, the

(6)

polynomial φ

σ2ni

can be written as

φ

σ2ni

= B

i2n

where

B

i

= (u

0

1

ε

2

) (ε

3

ε

4

) . . .

2g+1

ε

2g+2

))

σi

. Thus, the polynomial ψ

2n

has the form

ψ

2n

= B

12n

+ B

22n

+ · · · + B

κ2n

for n = 1, 2, . . . . By applying the fundamental theorem of symmetric func- tions to our situation, we see that A

g

is generated by ψ

2

, ψ

4

, . . . , ψ

.

The natural question arising from Theorem 2.2 is if we can find the minimal generators of A

g

. On this point, we have the following theorem.

Theorem 2.3. (1) A

1

is generated by ψ

2

, ψ

6

and coincides with S(2, 4)

e

. (2) A

2

is generated by ψ

2

, ψ

4

, ψ

6

, ψ

10

and coincides with S(2, 6)

e

. (3) A

3

is strictly smaller than S(2, 8)

e

.

Proof. We prove Theorem 2.3 by showing the relationship with the known generators. Starting from g = 1, the polynomials ψ

2

and ψ

6

can be ex- pressed in P and Q as

ψ

2

= 24 · P,

ψ

6

= 2

7

· 3 · 11 · P

3

2

8

· 3

4

· Q

2

.

Now we continue for g = 2. By J

2

, J

4

, J

6

, and J

10

, the polynomials ψ

2

, ψ

4

, ψ

6

, and ψ

10

can be expressed as

ψ

2

= 2

4

· 3 · 5 · J

2

,

ψ

4

= 2

3

· 3 · 5 · 71 · J

22

+ 2

5

· 3

3

· 5

3

· J

4

,

ψ

6

= −2

5

· 3

3

· 5 · 7

2

· J

23

2

7

· 3

5

· 5

3

· 7J

2

J

4

+ 2

3

· 3 · 5

4

· 13 · J

6

, ψ

10

= 2

5

· 3

3

· 5 · 17 · 15287 · J

25

2

8

· 3

5

· 5

4

· 29 · 199 · J

23

J

4

+ 2

3

· 3 · 5

5

· 37 · 857J

22

J

6

2

9

· 3

7

· 5

6

· 229J

2

J

42

+ 2

5

· 3

3

· 5

6

· 2207 · J

4

J

6

2

5

· 3

6

· 5

6

· 31 · J

10

.

(7)

For g = 3, the dimension formula of S(2, 8) is X

d=0

(dim S

d

(2, 8))t

d

= 1 + t

8

+ t

9

+ t

10

+ t

18

Q

7

i=2

(1 t

i

)

= 1 + t

2

+ t

3

+ 2t

4

+ 2t

5

+ 4t

6

+ 4t

7

+ 7t

8

+ · · · . The dimension of S(2, 8) of degree 8 is 7. However, the dimension of A

3

of degree 8 is at most 5.

For the comparation of the dimension formula, we give an example for g = 2. The dimension formula of S(2, 6) is

1 + t

15

(1 t

2

)(1 t

4

)(1 t

6

)(1 t

10

) , while the dimension formula of A

2

is

1

(1 t

2

)(1 t

4

)(1 t

6

)(1 t

10

) .

In the paper [5], the relation between the ring S(2, 2g +2) and the weight enumerators of some codes was discussed. In Appendix B, we give the relations between the weight enumerators and E-polynomials for g = 1, 2.

Acknowledgment. This work was supported by JSPS KAKENHI Grant Numbers 17K05164, 19K03398. The first named author was also supported by the Research Institute for Mathematical Sciences, an International Joint Usage/Research Center located in Kyoto University. We would like to thank Prof. Hajime Tanaka for his comments.

References

[1] W. Bosma, J. Cannon, C. Playoust, The Magma algebra system I: The user language, J. Symbolic Comput., 24(1997), No. 3-4, 235–265.

[2] J. Igusa, Arithmetic variety of moduli for genus two, Ann. of Math., 72(1960), No. 3, 612-649.

[3] J. Igusa, On Siegel modular forms of genus two, Amer. J. Math.,

84(1962), 175-200.

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[4] J. Igusa, Modular forms and projective invariants, Amer. J. Math., 89(1967), 817-855.

[5] M. Oura, Observation on the weight enumerators from classical in- variant theory. Comment. Math. Univ. St. Pauli, 54 (2005), No. 1, 1-15.

[6] SageMath, the Sage Mathematics Software System (Version 8.1), The Sage Developers, 2017, https://www.sagemath.org.

[7] I. Schur, Vorlesungen ¨ uber Invariantentheorie, Bearbeitet und heraus- gegeben von Helmut Grunsky, Die Grundlehren der mathematischen Wissenschaften, Band 143 Springer-Verlag, Berlin-New York 1968.

[8] T. Shioda, On the graded ring of invariants of binary octavics, Amer.

J. Math., 89(1967), 1022-1046.

[9] S. Tsuyumine, On Siegel modular forms of degree three, Amer. J.

Math., 108(1986), 755-862.

[10] H. Weyl, The classical groups. Their invariants and representations,

Princeton University Press, Princeton, N.J., 1939.

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Appendix A Generators of S(2, 6)

These are the generators of S(2, 6) taken from [7].

J

2

= u

0

u

6

6u

1

u

5

+ 15u

2

u

4

10u

23

,

J

4

= det

 

 

u

0

u

1

u

2

u

3

u

1

u

2

u

3

u

4

u

2

u

3

u

4

u

5

u

3

u

4

u

5

u

6

 

 

,

J

6

= det

 

b

0

b

1

b

2

b

1

b

2

b

3

b

2

b

3

b

4

  ,

J

10

= u

0

c

3

6u

1

bc

2

+ 3u

2

(ac + 4b

2

)c 4u

3

(3abc + 2b

3

) + 3u

4

a(ac + 4b

2

) 6u

5

a

2

b + u

6

a

3

,

where

b

0

= 6(u

0

u

4

4u

1

u

3

+ 3u

22

), b

1

= 3(u

0

u

5

3u

1

u

4

+ 2u

2

u

3

), b

2

= u

0

u

6

9u

2

u

4

+ 8u

23

, b

3

= 3(u

1

u

6

3u

2

u

5

+ 2u

3

u

4

), b

4

= 6(u

2

u

6

4u

3

u

5

+ 3u

24

),

a = 2(u

0

u

2

u

6

3u

0

u

3

u

5

+ 2u

0

u

24

u

21

u

6

+ 3u

1

u

2

u

5

u

1

u

3

u

4

3u

22

u

4

+ 2u

2

u

23

),

b = u

0

u

3

u

6

u

0

u

4

u

5

u

1

u

2

u

6

8u

1

u

3

u

5

+ 9u

1

u

24

+ 9u

22

u

5

17u

2

u

3

u

4

+ 8u

33

,

c = 2(u

0

u

4

u

6

u

0

u

25

3u

1

u

3

u

6

+ 3u

1

u

4

u

5

+ 2u

22

u

6

u

2

u

3

u

5

3u

2

u

24

+ 2u

23

u

4

).

Appendix B Weight Enumerators

We recall coding theory. A code C of length n means a subspace of F

n2

.

The weight wt(x) of x F

n2

means the number of nonzero x

i

. The inner

(10)

product of two elements x, y F

n2

is defined by x · y := X

x

i

y

i

F

2

.

The dual code C

of C is defined by the subspace of F

n2

whose elements are orthogonal to every element of C. If C = C

, then we call C self-dual. The code C is called doubly even if the weight of any element in C is equivalent to 0 modulo 4. The weight enumerator of C in genus g is defined by

W

C(g)

:= W

C(g)

(x

a

| a F

g2

) = X

c1,...,cg∈C

Y

a∈Fg2

x

naa(c1,...,cg)

where

n

a

(c

1

, . . . , c

g

) = |{ i | (c

1i

, . . . , c

gi

) = a }| .

Let ρ e be the combination of the Brou´ e-Enguehard map T h and Igusa’s homomorphism ρ. In other word, we can say

e

ρ(W

C(g)

) = ρ(T h(W

C(g)

))

for a code C. We omit the detail of ρ e and only say that ρ e maps the weight enumerators in genus g to the ring S(2, 2g+2). The reader who is interested in the detail of ρ e can refer to [5]. For every code C used here, the expression of ρ(W e

C(g)

) is taken from [5].

We start with g = 1. The weight enumerators of some codes are related to E-polynomials by the following relations.

e

ρ(W

e(1)8

) = 2

1

ψ

2

, e

ρ(W

g(1)24

) = 2

5

· 11 · ψ

23

2

3

·

6

.

For g = 2, the relation between the weight enumerators and E-polynomials

(11)

are the following.

e

ρ(W

e(2)8

) = 2

4

ψ

22

3 · 2

3

ψ

4

, e

ρ(W

g(2)24

) = 2

15

3

2

5

1

13

2

31

1

20129ψ

62

2

14

513

2

31

1

59651ψ

24

ψ

4

+ 2

13

7 · 13

2

31

1

809ψ

23

ψ

6

2

9

3 · 5

1

7 · 11 · 31

1

ψ

2

ψ

10

+ 2

11

3 · 13

2

31

1

65287ψ

22

ψ

24

+ 2

12

7 · 13

2

29 · 31

1

149ψ

2

ψ

4

ψ

6

2

10

3 · 11ψ

43

+ 2

7

3

2

7 · 13

2

ψ

62

, e

ρ(W

(2)

d+24

) = 2

10

5

1

13

2

31

1

6323ψ

26

2

9

13

2

31

1

12143ψ

24

ψ

4

2

10

3 · 13

2

31

1

683ψ

23

ψ

6

+ 2

6

3 · 5

1

11 · 31

1

ψ

2

ψ

10

+ 2

10

3

2

13

2

31

1

47 · 379ψ

22

ψ

24

2

9

13

2

31

1

2089ψ

2

ψ

4

ψ

6

2

9

3 · 11ψ

34

2

5

3

2

13

2

ψ

62

, e

ρ(W

(2)

d+32

) = 2

16

5

1

13

2

31

1

20507ψ

28

2

13

3

1

7 · 13

2

23 · 31

1

271ψ

62

ψ

4

2

11

5

1

13

2

23 · 31

1

227ψ

25

ψ

6

+ 2

13

3

1

13

2

15541ψ

24

ψ

24

+ 2

9

3

1

13

2

31

1

4679ψ

23

ψ

4

ψ

6

+ 2

7

5

1

13

1

31

1

173ψ

32

ψ

10

2

11

7 · 13

2

31

1

27743ψ

22

ψ

34

2

6

13

2

31

1

139ψ

22

ψ

26

+ 2

9

3

1

13

2

31

1

2129ψ

2

ψ

24

ψ

6

2

6

13

1

31

1

107ψ

2

ψ

4

ψ

10

+ 2

12

3 · 43ψ

44

+ 2

5

13

2

31

1

281ψ

4

ψ

26

+ 2

1

3 · 5

1

13

1

31

1

ψ

6

ψ

10

,

e ρ(W

(2)

d+40

) = 31

2

(2

18

3

1

5

1

13

2

267941ψ

210

2

16

3

1

13

2

606959 ψ

82

ψ

4

2

18

3

1

13

2

1877033 ψ

27

ψ

6

+ 2

18

3

1

13

2

281

2

541 ψ

26

ψ

24

+ 2

14

5

1

13

1

17 · 4871 ψ

25

ψ

10

+ 2

17

3

1

13

2

2207 · 5779 ψ

25

ψ

4

ψ

6

2

−17

5 · 13

−1

903827 ψ

24

ψ

43

2

−14

3

−1

5 · 13

−2

107209 ψ

42

ψ

26

2

16

3

1

5 · 13

2

17 · 59 · 4957ψ

23

ψ

24

ψ

6

2

12

7 · 13

1

7187 ψ

32

ψ

4

ψ

10

+ 2

16

3 · 5 · 13

2

37 · 205187ψ

22

ψ

44

+ 2

12

3

1

5 · 13

2

271919 ψ

22

ψ

4

ψ

62

+ 2

9

13

1

17 · 43ψ

22

ψ

6

ψ

10

+ 2

15

5 · 7 · 13

2

79319ψ

2

ψ

34

ψ

6

+ 2

12

3 · 13

1

181 · 293 ψ

2

ψ

42

ψ

10

2

15

3

3

19 · 31

2

ψ

54

2

12

3

1

5 · 13

2

71 · 6719ψ

24

ψ

62

2

8

13

1

17 · 293ψ

4

ψ

6

ψ

10

+ 2

6

3 · 5

1

41ψ

210

).

(12)

Nur Hamid

Mathematics Education,

Universitas Nurul Jadid, Probolinggo INDONESIA

e-mail: [email protected] Masashi Kosuda

Yamanashi University JAPAN

e-mail: [email protected] Manabu Oura

Institute of Science and Engineering Kanazawa University

JAPAN

e-mail: [email protected]

(Received May 14, 2020)

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