Defining parameters
Level: | \( N \) | \(=\) | \( 1152 = 2^{7} \cdot 3^{2} \) |
Weight: | \( k \) | \(=\) | \( 2 \) |
Character orbit: | \([\chi]\) | \(=\) | 1152.v (of order \(8\) and degree \(4\)) |
Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 32 \) |
Character field: | \(\Q(\zeta_{8})\) | ||
Newform subspaces: | \( 4 \) | ||
Sturm bound: | \(384\) | ||
Trace bound: | \(23\) | ||
Distinguishing \(T_p\): | \(5\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(1152, [\chi])\).
Total | New | Old | |
---|---|---|---|
Modular forms | 832 | 84 | 748 |
Cusp forms | 704 | 76 | 628 |
Eisenstein series | 128 | 8 | 120 |
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(1152, [\chi])\) into newform subspaces
Label | Dim | $A$ | Field | CM | Traces | $q$-expansion | |||
---|---|---|---|---|---|---|---|---|---|
$a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | ||||||
1152.2.v.a | $4$ | $9.199$ | \(\Q(\zeta_{8})\) | None | \(0\) | \(0\) | \(4\) | \(-4\) | \(q+(1+\zeta_{8}+2\zeta_{8}^{2}-2\zeta_{8}^{3})q^{5}+(-1+\cdots)q^{7}+\cdots\) |
1152.2.v.b | $8$ | $9.199$ | 8.0.18939904.2 | None | \(0\) | \(0\) | \(0\) | \(8\) | \(q+(\beta _{4}-\beta _{7})q^{5}+(1-\beta _{1}-\beta _{3}+\beta _{7})q^{7}+\cdots\) |
1152.2.v.c | $32$ | $9.199$ | None | \(0\) | \(0\) | \(0\) | \(0\) | ||
1152.2.v.d | $32$ | $9.199$ | None | \(0\) | \(0\) | \(0\) | \(0\) |
Decomposition of \(S_{2}^{\mathrm{old}}(1152, [\chi])\) into lower level spaces
\( S_{2}^{\mathrm{old}}(1152, [\chi]) \cong \) \(S_{2}^{\mathrm{new}}(32, [\chi])\)\(^{\oplus 9}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(64, [\chi])\)\(^{\oplus 6}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(96, [\chi])\)\(^{\oplus 6}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(128, [\chi])\)\(^{\oplus 3}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(192, [\chi])\)\(^{\oplus 4}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(288, [\chi])\)\(^{\oplus 3}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(384, [\chi])\)\(^{\oplus 2}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(576, [\chi])\)\(^{\oplus 2}\)