Defining parameters
Level: | \( N \) | \(=\) | \( 840 = 2^{3} \cdot 3 \cdot 5 \cdot 7 \) |
Weight: | \( k \) | \(=\) | \( 2 \) |
Character orbit: | \([\chi]\) | \(=\) | 840.j (of order \(2\) and degree \(1\)) |
Character conductor: | \(\operatorname{cond}(\chi)\) | \(=\) | \( 40 \) |
Character field: | \(\Q\) | ||
Newform subspaces: | \( 6 \) | ||
Sturm bound: | \(384\) | ||
Trace bound: | \(3\) | ||
Distinguishing \(T_p\): | \(11\), \(13\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(840, [\chi])\).
Total | New | Old | |
---|---|---|---|
Modular forms | 200 | 72 | 128 |
Cusp forms | 184 | 72 | 112 |
Eisenstein series | 16 | 0 | 16 |
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(840, [\chi])\) into newform subspaces
Label | Dim | $A$ | Field | CM | Traces | $q$-expansion | |||
---|---|---|---|---|---|---|---|---|---|
$a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | ||||||
840.2.j.a | $2$ | $6.707$ | \(\Q(\sqrt{-1}) \) | None | \(-2\) | \(-2\) | \(-4\) | \(0\) | \(q+(-1-i)q^{2}-q^{3}+2iq^{4}+(-2+\cdots)q^{5}+\cdots\) |
840.2.j.b | $2$ | $6.707$ | \(\Q(\sqrt{-1}) \) | None | \(-2\) | \(2\) | \(-4\) | \(0\) | \(q+(-1+i)q^{2}+q^{3}-2iq^{4}+(-2+\cdots)q^{5}+\cdots\) |
840.2.j.c | $2$ | $6.707$ | \(\Q(\sqrt{-1}) \) | None | \(2\) | \(-2\) | \(4\) | \(0\) | \(q+(1+i)q^{2}-q^{3}+2iq^{4}+(2+i)q^{5}+\cdots\) |
840.2.j.d | $2$ | $6.707$ | \(\Q(\sqrt{-1}) \) | None | \(2\) | \(2\) | \(4\) | \(0\) | \(q+(1+i)q^{2}+q^{3}+2iq^{4}+(2+i)q^{5}+\cdots\) |
840.2.j.e | $32$ | $6.707$ | None | \(-2\) | \(-32\) | \(0\) | \(0\) | ||
840.2.j.f | $32$ | $6.707$ | None | \(2\) | \(32\) | \(0\) | \(0\) |
Decomposition of \(S_{2}^{\mathrm{old}}(840, [\chi])\) into lower level spaces
\( S_{2}^{\mathrm{old}}(840, [\chi]) \cong \) \(S_{2}^{\mathrm{new}}(40, [\chi])\)\(^{\oplus 4}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(120, [\chi])\)\(^{\oplus 2}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(280, [\chi])\)\(^{\oplus 2}\)