Defining parameters
Level: | \( N \) | \(=\) | \( 1110 = 2 \cdot 3 \cdot 5 \cdot 37 \) |
Weight: | \( k \) | \(=\) | \( 2 \) |
Character orbit: | \([\chi]\) | \(=\) | 1110.u (of order \(4\) and degree \(2\)) |
Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 111 \) |
Character field: | \(\Q(i)\) | ||
Newform subspaces: | \( 6 \) | ||
Sturm bound: | \(456\) | ||
Trace bound: | \(7\) | ||
Distinguishing \(T_p\): | \(7\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(1110, [\chi])\).
Total | New | Old | |
---|---|---|---|
Modular forms | 472 | 96 | 376 |
Cusp forms | 440 | 96 | 344 |
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.u.a | $4$ | $8.863$ | \(\Q(\zeta_{8})\) | None | \(0\) | \(0\) | \(0\) | \(-8\) | \(q-\zeta_{8}^{3}q^{2}+(-\zeta_{8}+\zeta_{8}^{2}+\zeta_{8}^{3})q^{3}+\cdots\) |
1110.2.u.b | $4$ | $8.863$ | \(\Q(\zeta_{8})\) | None | \(0\) | \(0\) | \(0\) | \(16\) | \(q+\zeta_{8}q^{2}+(-\zeta_{8}-\zeta_{8}^{2}+\zeta_{8}^{3})q^{3}+\cdots\) |
1110.2.u.c | $4$ | $8.863$ | \(\Q(\zeta_{8})\) | None | \(0\) | \(0\) | \(0\) | \(-16\) | \(q-\zeta_{8}^{3}q^{2}+(\zeta_{8}-\zeta_{8}^{2}-\zeta_{8}^{3})q^{3}-\zeta_{8}^{2}q^{4}+\cdots\) |
1110.2.u.d | $4$ | $8.863$ | \(\Q(\zeta_{8})\) | None | \(0\) | \(0\) | \(0\) | \(8\) | \(q-\zeta_{8}^{3}q^{2}+(\zeta_{8}+\zeta_{8}^{2}-\zeta_{8}^{3})q^{3}-\zeta_{8}^{2}q^{4}+\cdots\) |
1110.2.u.e | $40$ | $8.863$ | None | \(0\) | \(0\) | \(0\) | \(-24\) | ||
1110.2.u.f | $40$ | $8.863$ | None | \(0\) | \(0\) | \(0\) | \(24\) |
Decomposition of \(S_{2}^{\mathrm{old}}(1110, [\chi])\) into lower level spaces
\( S_{2}^{\mathrm{old}}(1110, [\chi]) \cong \)