Defining parameters
Level: | \( N \) | \(=\) | \( 1110 = 2 \cdot 3 \cdot 5 \cdot 37 \) |
Weight: | \( k \) | \(=\) | \( 2 \) |
Character orbit: | \([\chi]\) | \(=\) | 1110.bb (of order \(6\) and degree \(2\)) |
Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 185 \) |
Character field: | \(\Q(\zeta_{6})\) | ||
Newform subspaces: | \( 5 \) | ||
Sturm bound: | \(456\) | ||
Trace bound: | \(5\) | ||
Distinguishing \(T_p\): | \(7\), \(11\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(1110, [\chi])\).
Total | New | Old | |
---|---|---|---|
Modular forms | 472 | 80 | 392 |
Cusp forms | 440 | 80 | 360 |
Eisenstein series | 32 | 0 | 32 |
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(1110, [\chi])\) into newform subspaces
Label | Dim | $A$ | Field | CM | Traces | $q$-expansion | |||
---|---|---|---|---|---|---|---|---|---|
$a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | ||||||
1110.2.bb.a | $4$ | $8.863$ | \(\Q(\zeta_{12})\) | None | \(0\) | \(0\) | \(-4\) | \(0\) | \(q+(-\zeta_{12}+\zeta_{12}^{3})q^{2}-\zeta_{12}q^{3}+(1+\cdots)q^{4}+\cdots\) |
1110.2.bb.b | $4$ | $8.863$ | \(\Q(\zeta_{12})\) | None | \(0\) | \(0\) | \(-2\) | \(0\) | \(q+(\zeta_{12}-\zeta_{12}^{3})q^{2}+\zeta_{12}q^{3}+(1-\zeta_{12}^{2}+\cdots)q^{4}+\cdots\) |
1110.2.bb.c | $4$ | $8.863$ | \(\Q(\zeta_{12})\) | None | \(0\) | \(0\) | \(2\) | \(0\) | \(q+(-\zeta_{12}+\zeta_{12}^{3})q^{2}-\zeta_{12}q^{3}+(1+\cdots)q^{4}+\cdots\) |
1110.2.bb.d | $28$ | $8.863$ | None | \(0\) | \(0\) | \(2\) | \(0\) | ||
1110.2.bb.e | $40$ | $8.863$ | None | \(0\) | \(0\) | \(2\) | \(0\) |
Decomposition of \(S_{2}^{\mathrm{old}}(1110, [\chi])\) into lower level spaces
\( S_{2}^{\mathrm{old}}(1110, [\chi]) \cong \) \(S_{2}^{\mathrm{new}}(185, [\chi])\)\(^{\oplus 4}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(370, [\chi])\)\(^{\oplus 2}\)