Defining parameters
Level: | \( N \) | \(=\) | \( 1100 = 2^{2} \cdot 5^{2} \cdot 11 \) |
Weight: | \( k \) | \(=\) | \( 2 \) |
Character orbit: | \([\chi]\) | \(=\) | 1100.cb (of order \(10\) and degree \(4\)) |
Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 55 \) |
Character field: | \(\Q(\zeta_{10})\) | ||
Newform subspaces: | \( 4 \) | ||
Sturm bound: | \(360\) | ||
Trace bound: | \(21\) | ||
Distinguishing \(T_p\): | \(3\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(1100, [\chi])\).
Total | New | Old | |
---|---|---|---|
Modular forms | 792 | 72 | 720 |
Cusp forms | 648 | 72 | 576 |
Eisenstein series | 144 | 0 | 144 |
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(1100, [\chi])\) into newform subspaces
Label | Dim | $A$ | Field | CM | Traces | $q$-expansion | |||
---|---|---|---|---|---|---|---|---|---|
$a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | ||||||
1100.2.cb.a | $8$ | $8.784$ | \(\Q(\zeta_{20})\) | None | \(0\) | \(0\) | \(0\) | \(0\) | \(q+(2\zeta_{20}+\zeta_{20}^{5}-\zeta_{20}^{7})q^{3}+(2\zeta_{20}+\cdots)q^{7}+\cdots\) |
1100.2.cb.b | $16$ | $8.784$ | \(\mathbb{Q}[x]/(x^{16} - \cdots)\) | None | \(0\) | \(0\) | \(0\) | \(0\) | \(q+(\beta _{2}-\beta _{6}-\beta _{10}-\beta _{12}-\beta _{13}+\beta _{14}+\cdots)q^{3}+\cdots\) |
1100.2.cb.c | $16$ | $8.784$ | \(\mathbb{Q}[x]/(x^{16} + \cdots)\) | None | \(0\) | \(0\) | \(0\) | \(0\) | \(q+(2\beta _{1}-\beta _{2}+\beta _{7}-\beta _{9}-\beta _{11}+\beta _{13}+\cdots)q^{3}+\cdots\) |
1100.2.cb.d | $32$ | $8.784$ | None | \(0\) | \(0\) | \(0\) | \(0\) |
Decomposition of \(S_{2}^{\mathrm{old}}(1100, [\chi])\) into lower level spaces
\( S_{2}^{\mathrm{old}}(1100, [\chi]) \cong \) \(S_{2}^{\mathrm{new}}(55, [\chi])\)\(^{\oplus 6}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(110, [\chi])\)\(^{\oplus 4}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(220, [\chi])\)\(^{\oplus 2}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(275, [\chi])\)\(^{\oplus 3}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(550, [\chi])\)\(^{\oplus 2}\)