Properties

Label 1620.1
Level 1620
Weight 1
Dimension 120
Nonzero newspaces 8
Newform subspaces 22
Sturm bound 139968
Trace bound 10

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Defining parameters

Level: \( N \) = \( 1620 = 2^{2} \cdot 3^{4} \cdot 5 \)
Weight: \( k \) = \( 1 \)
Nonzero newspaces: \( 8 \)
Newform subspaces: \( 22 \)
Sturm bound: \(139968\)
Trace bound: \(10\)

Dimensions

The following table gives the dimensions of various subspaces of \(M_{1}(\Gamma_1(1620))\).

Total New Old
Modular forms 2394 456 1938
Cusp forms 234 120 114
Eisenstein series 2160 336 1824

The following table gives the dimensions of subspaces with specified projective image type.

\(D_n\) \(A_4\) \(S_4\) \(A_5\)
Dimension 108 0 12 0

Trace form

\( 120q + 4q^{4} + O(q^{10}) \) \( 120q + 4q^{4} + 6q^{10} + 4q^{13} + 6q^{14} + 8q^{16} + 10q^{25} + 6q^{29} - 6q^{34} + 4q^{37} - 10q^{40} - 30q^{41} - 16q^{46} - 4q^{52} + 6q^{56} - 4q^{58} - 10q^{61} - 26q^{64} - 18q^{69} - 10q^{70} + 8q^{73} + 6q^{76} + 24q^{80} - 32q^{82} + 36q^{84} - 10q^{94} - 4q^{97} + O(q^{100}) \)

Decomposition of \(S_{1}^{\mathrm{new}}(\Gamma_1(1620))\)

We only show spaces with odd parity, since no modular forms exist when this condition is not satisfied. Within each space \( S_k^{\mathrm{new}}(N, \chi) \) we list the newforms together with their dimension.

Label \(\chi\) Newforms Dimension \(\chi\) degree
1620.1.b \(\chi_{1620}(809, \cdot)\) None 0 1
1620.1.c \(\chi_{1620}(811, \cdot)\) None 0 1
1620.1.f \(\chi_{1620}(1459, \cdot)\) 1620.1.f.a 1 1
1620.1.f.b 1
1620.1.f.c 1
1620.1.f.d 1
1620.1.f.e 4
1620.1.g \(\chi_{1620}(161, \cdot)\) None 0 1
1620.1.l \(\chi_{1620}(973, \cdot)\) 1620.1.l.a 2 2
1620.1.l.b 2
1620.1.m \(\chi_{1620}(323, \cdot)\) 1620.1.m.a 8 2
1620.1.o \(\chi_{1620}(701, \cdot)\) None 0 2
1620.1.p \(\chi_{1620}(379, \cdot)\) 1620.1.p.a 4 2
1620.1.p.b 4
1620.1.p.c 4
1620.1.p.d 4
1620.1.p.e 4
1620.1.s \(\chi_{1620}(271, \cdot)\) None 0 2
1620.1.t \(\chi_{1620}(269, \cdot)\) None 0 2
1620.1.v \(\chi_{1620}(217, \cdot)\) 1620.1.v.a 4 4
1620.1.v.b 4
1620.1.w \(\chi_{1620}(107, \cdot)\) 1620.1.w.a 8 4
1620.1.w.b 8
1620.1.w.c 8
1620.1.z \(\chi_{1620}(89, \cdot)\) None 0 6
1620.1.ba \(\chi_{1620}(91, \cdot)\) None 0 6
1620.1.bc \(\chi_{1620}(341, \cdot)\) None 0 6
1620.1.bf \(\chi_{1620}(19, \cdot)\) 1620.1.bf.a 6 6
1620.1.bf.b 6
1620.1.bh \(\chi_{1620}(143, \cdot)\) None 0 12
1620.1.bj \(\chi_{1620}(37, \cdot)\) None 0 12
1620.1.bl \(\chi_{1620}(29, \cdot)\) None 0 18
1620.1.bn \(\chi_{1620}(31, \cdot)\) None 0 18
1620.1.bp \(\chi_{1620}(79, \cdot)\) 1620.1.bp.a 18 18
1620.1.bp.b 18
1620.1.bq \(\chi_{1620}(41, \cdot)\) None 0 18
1620.1.bt \(\chi_{1620}(23, \cdot)\) None 0 36
1620.1.bu \(\chi_{1620}(13, \cdot)\) None 0 36

Decomposition of \(S_{1}^{\mathrm{old}}(\Gamma_1(1620))\) into lower level spaces

\( S_{1}^{\mathrm{old}}(\Gamma_1(1620)) \cong \) \(S_{1}^{\mathrm{new}}(\Gamma_1(108))\)\(^{\oplus 4}\)\(\oplus\)\(S_{1}^{\mathrm{new}}(\Gamma_1(135))\)\(^{\oplus 6}\)\(\oplus\)\(S_{1}^{\mathrm{new}}(\Gamma_1(180))\)\(^{\oplus 3}\)\(\oplus\)\(S_{1}^{\mathrm{new}}(\Gamma_1(324))\)\(^{\oplus 2}\)\(\oplus\)\(S_{1}^{\mathrm{new}}(\Gamma_1(405))\)\(^{\oplus 3}\)\(\oplus\)\(S_{1}^{\mathrm{new}}(\Gamma_1(540))\)\(^{\oplus 2}\)