Defining parameters
| Level: | \( N \) | \(=\) | \( 110 = 2 \cdot 5 \cdot 11 \) |
| Weight: | \( k \) | \(=\) | \( 2 \) |
| Character orbit: | \([\chi]\) | \(=\) | 110.g (of order \(5\) and degree \(4\)) |
| Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 11 \) |
| Character field: | \(\Q(\zeta_{5})\) | ||
| Newform subspaces: | \( 3 \) | ||
| Sturm bound: | \(36\) | ||
| Trace bound: | \(2\) | ||
| Distinguishing \(T_p\): | \(3\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(110, [\chi])\).
| Total | New | Old | |
|---|---|---|---|
| Modular forms | 88 | 16 | 72 |
| Cusp forms | 56 | 16 | 40 |
| Eisenstein series | 32 | 0 | 32 |
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(110, [\chi])\) into newform subspaces
| Label | Dim | $A$ | Field | CM | Traces | $q$-expansion | |||
|---|---|---|---|---|---|---|---|---|---|
| $a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | ||||||
| 110.2.g.a | $4$ | $0.878$ | \(\Q(\zeta_{10})\) | None | \(-1\) | \(4\) | \(1\) | \(1\) | \(q+(-1+\zeta_{10}-\zeta_{10}^{2}+\zeta_{10}^{3})q^{2}+\cdots\) |
| 110.2.g.b | $4$ | $0.878$ | \(\Q(\zeta_{10})\) | None | \(1\) | \(4\) | \(1\) | \(0\) | \(q+(1-\zeta_{10}+\zeta_{10}^{2}-\zeta_{10}^{3})q^{2}+(\zeta_{10}+\cdots)q^{3}+\cdots\) |
| 110.2.g.c | $8$ | $0.878$ | 8.0.682515625.5 | None | \(2\) | \(-4\) | \(-2\) | \(-1\) | \(q+(1-\beta _{2}+\beta _{3}-\beta _{7})q^{2}+(-\beta _{1}-\beta _{2}+\cdots)q^{3}+\cdots\) |
Decomposition of \(S_{2}^{\mathrm{old}}(110, [\chi])\) into lower level spaces
\( S_{2}^{\mathrm{old}}(110, [\chi]) \simeq \) \(S_{2}^{\mathrm{new}}(22, [\chi])\)\(^{\oplus 2}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(55, [\chi])\)\(^{\oplus 2}\)