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=0u
im i
ξ
1m−iξ
i2.
2010
Mathematics Subject Classification.Primary 13A50; Secondary 13A02, 16W50.
Key words and phrases.
Invariant ring, E-polynomial.
33
Here we mean f is a polynomial of degree m in variables ξ
1, ξ
2with co- efficients u
i miwhere u
iare 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
2are transformed according to
(ξ
1ξ
2) = (ξ
1′ξ
′2)A (”contragrediently”),
f changes into a form of the new variables ξ
1′, ξ
′2with the coefficients u
′0, u
′1, . . . , u
′mwhere
u
′0u
′1.. . u
′m
=
A
m
u
0u
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
0u
2− u
21].
Let M be a graded ring such that each homogeneous part M
dof degree d is a finite dimensional vector space over M
0= C. We can write M as
M = M
∞ d=0M
d.
The dimension formula of M is defined by the formal series X
∞d=0
(dim M
d)t
d.
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
18Q
7i=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
0u
4− 4u
1u
3+ 3u
22, Q = det
u
0u
1u
2u
1u
2u
3u
2u
3u
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)
ethe even parts of S(2, m).
Let ξ
3= ξ
1/ξ
2. The form ξ
2−mf is a polynomial in ξ
3with coefficients in C[u] and can be written as
X
m i=0u
im i
ξ
3m−i. Let ε
1, ε
2, . . . , ε
mbe the roots of the equation
X
m i=0u
im
i
ξ
3m−i= 0.
We can write
X
m i=1ε
i= − m
1 u
1u
0, .. .
X
i1<i2<···<ir
ε
i1ε
i2· · · ε
ir= ( − 1)
rm
r u
ru
0, .. .
ε
1ε
2· · · ε
m= ( − 1)
mm
m u
mu
0.
In order to obtain the useful construction of invariants, we shall interpret the ground form as
f = u
0Y
m i=1(ξ
1− ε
iξ
2) .
As usual, we denote by S
nthe 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
r0X
(ε
i− ε
j)(ε
k− ε
l) . . . ,
in which every ε
iappears r times in each product and which is symmetric in ε
1, ε
2, . . . , ε
mcan 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
i2g + 2 i
ξ
(2g+2)1 −iξ
i2= u
0 2g+2Y
i=1
(ξ
1− ε
iξ
2) .
We would like to concentrate on one type of invariants we shall define now.
We fix the following polynomial
φ
2n= u
2n0(ε
1− ε
2)
2n(ε
3− ε
4)
2n. . . (ε
2g+1− ε
2g+2)
2n.
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
φ2nbe the stabilizer of φ
2n, that is, elements of G which preserve φ
2n. Proposition 2.1. The group G
φ2ncan 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+1o S
g+1. In particular, G
φ2ndoes 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+1and 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
φ2nand 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
2nby an E-polynomial. We shall denote by A
gthe ring generated by ψ
2n(n = 1, 2, . . . ) over C. The ring A
gis a subring of the invariant ring S(2, 2g + 2).
Theorem 2.2. The ring A
gis finitely generated over C. More precisely the elements ψ
2, ψ
4, . . . , ψ
2κgenerate the ring A
g.
Proof. Since the second assertion implies the first, we shall show the second.
Let σ
1, σ
2, . . . , σ
κbe a set of representatives of K \ G. For each σ
i, the
polynomial φ
σ2nican be written as
φ
σ2ni= B
i2nwhere
B
i= (u
0(ε
1− ε
2) (ε
3− ε
4) . . . (ε
2g+1− ε
2g+2))
σi. Thus, the polynomial ψ
2nhas the form
ψ
2n= B
12n+ B
22n+ · · · + B
κ2nfor n = 1, 2, . . . . By applying the fundamental theorem of symmetric func- tions to our situation, we see that A
gis generated by ψ
2, ψ
4, . . . , ψ
2κ.
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
1is generated by ψ
2, ψ
6and coincides with S(2, 4)
e. (2) A
2is generated by ψ
2, ψ
4, ψ
6, ψ
10and coincides with S(2, 6)
e. (3) A
3is 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
2and ψ
6can 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
10can 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
2J
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
23J
4+ 2
3· 3 · 5
5· 37 · 857J
22J
6− 2
9· 3
7· 5
6· 229J
2J
42+ 2
5· 3
3· 5
6· 2207 · J
4J
6− 2
5· 3
6· 5
6· 31 · J
10.
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
18Q
7i=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
3of 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
2is
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.
[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.
Appendix A Generators of S(2, 6)
These are the generators of S(2, 6) taken from [7].
J
2= u
0u
6− 6u
1u
5+ 15u
2u
4− 10u
23,
J
4= det
u
0u
1u
2u
3u
1u
2u
3u
4u
2u
3u
4u
5u
3u
4u
5u
6
,
J
6= det
b
0b
1b
2b
1b
2b
3b
2b
3b
4
,
J
10= u
0c
3− 6u
1bc
2+ 3u
2(ac + 4b
2)c − 4u
3(3abc + 2b
3) + 3u
4a(ac + 4b
2) − 6u
5a
2b + u
6a
3,
where
b
0= 6(u
0u
4− 4u
1u
3+ 3u
22), b
1= 3(u
0u
5− 3u
1u
4+ 2u
2u
3), b
2= u
0u
6− 9u
2u
4+ 8u
23, b
3= 3(u
1u
6− 3u
2u
5+ 2u
3u
4), b
4= 6(u
2u
6− 4u
3u
5+ 3u
24),
a = 2(u
0u
2u
6− 3u
0u
3u
5+ 2u
0u
24− u
21u
6+ 3u
1u
2u
5− u
1u
3u
4− 3u
22u
4+ 2u
2u
23),
b = u
0u
3u
6− u
0u
4u
5− u
1u
2u
6− 8u
1u
3u
5+ 9u
1u
24+ 9u
22u
5− 17u
2u
3u
4+ 8u
33,
c = 2(u
0u
4u
6− u
0u
25− 3u
1u
3u
6+ 3u
1u
4u
5+ 2u
22u
6− u
2u
3u
5− 3u
2u
24+ 2u
23u
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
n2means the number of nonzero x
i. The inner
product of two elements x, y ∈ F
n2is defined by x · y := X
x
iy
i∈ F
2.
The dual code C
⊥of C is defined by the subspace of F
n2whose 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
−1ψ
2, e
ρ(W
g(1)24) = 2
−5· 11 · ψ
23− 2
−3· 7ψ
6.
For g = 2, the relation between the weight enumerators and E-polynomials
are the following.
e
ρ(W
e(2)8) = 2
−4ψ
22− 3 · 2
−3ψ
4, e
ρ(W
g(2)24) = 2
−153
25
−113
−231
−120129ψ
62− 2
−14513
−231
−159651ψ
24ψ
4+ 2
−137 · 13
−231
−1809ψ
23ψ
6− 2
−93 · 5
−17 · 11 · 31
−1ψ
2ψ
10+ 2
−113 · 13
−231
−165287ψ
22ψ
24+ 2
−127 · 13
−229 · 31
−1149ψ
2ψ
4ψ
6− 2
−103 · 11ψ
43+ 2
−73
27 · 13
−2ψ
62, e
ρ(W
(2)d+24
) = 2
−105
−113
−231
−16323ψ
26− 2
−913
−231
−112143ψ
24ψ
4− 2
−103 · 13
−231
−1683ψ
23ψ
6+ 2
−63 · 5
−111 · 31
−1ψ
2ψ
10+ 2
−103
213
−231
−147 · 379ψ
22ψ
24− 2
−913
−231
−12089ψ
2ψ
4ψ
6− 2
−93 · 11ψ
34− 2
−53
213
−2ψ
62, e
ρ(W
(2)d+32
) = 2
−165
−113
−231
−120507ψ
28− 2
−133
−17 · 13
−223 · 31
−1271ψ
62ψ
4− 2
−115
−113
−223 · 31
−1227ψ
25ψ
6+ 2
−133
−113
−215541ψ
24ψ
24+ 2
−93
−113
−231
−14679ψ
23ψ
4ψ
6+ 2
−75
−113
−131
−1173ψ
32ψ
10− 2
−117 · 13
−231
−127743ψ
22ψ
34− 2
−613
−231
−1139ψ
22ψ
26+ 2
−93
−113
−231
−12129ψ
2ψ
24ψ
6− 2
−613
−131
−1107ψ
2ψ
4ψ
10+ 2
−123 · 43ψ
44+ 2
−513
−231
−1281ψ
4ψ
26+ 2
−13 · 5
−113
−131
−1ψ
6ψ
10,
e ρ(W
(2)d+40