Defining parameters
Level: | \( N \) | \(=\) | \( 260 = 2^{2} \cdot 5 \cdot 13 \) |
Weight: | \( k \) | \(=\) | \( 2 \) |
Character orbit: | \([\chi]\) | \(=\) | 260.bj (of order \(12\) and degree \(4\)) |
Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 260 \) |
Character field: | \(\Q(\zeta_{12})\) | ||
Newform subspaces: | \( 3 \) | ||
Sturm bound: | \(84\) | ||
Trace bound: | \(10\) | ||
Distinguishing \(T_p\): | \(3\), \(17\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(260, [\chi])\).
Total | New | Old | |
---|---|---|---|
Modular forms | 184 | 184 | 0 |
Cusp forms | 152 | 152 | 0 |
Eisenstein series | 32 | 32 | 0 |
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(260, [\chi])\) into newform subspaces
Label | Dim | $A$ | Field | CM | Traces | $q$-expansion | |||
---|---|---|---|---|---|---|---|---|---|
$a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | ||||||
260.2.bj.a | $4$ | $2.076$ | \(\Q(\zeta_{12})\) | \(\Q(\sqrt{-1}) \) | \(2\) | \(0\) | \(4\) | \(0\) | \(q+(-\zeta_{12}+\zeta_{12}^{2}+\zeta_{12}^{3})q^{2}-2\zeta_{12}q^{4}+\cdots\) |
260.2.bj.b | $4$ | $2.076$ | \(\Q(\zeta_{12})\) | \(\Q(\sqrt{-1}) \) | \(2\) | \(0\) | \(4\) | \(0\) | \(q+(-\zeta_{12}+\zeta_{12}^{2}+\zeta_{12}^{3})q^{2}-2\zeta_{12}q^{4}+\cdots\) |
260.2.bj.c | $144$ | $2.076$ | None | \(-6\) | \(0\) | \(-24\) | \(0\) |