Defining parameters
Level: | \( N \) | \(=\) | \( 9 = 3^{2} \) |
Weight: | \( k \) | \(=\) | \( 40 \) |
Character orbit: | \([\chi]\) | \(=\) | 9.a (trivial) |
Character field: | \(\Q\) | ||
Newform subspaces: | \( 5 \) | ||
Sturm bound: | \(40\) | ||
Trace bound: | \(2\) | ||
Distinguishing \(T_p\): | \(2\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{40}(\Gamma_0(9))\).
Total | New | Old | |
---|---|---|---|
Modular forms | 41 | 17 | 24 |
Cusp forms | 37 | 16 | 21 |
Eisenstein series | 4 | 1 | 3 |
The following table gives the dimensions of the cuspidal new subspaces with specified eigenvalues for the Atkin-Lehner operators and the Fricke involution.
\(3\) | Dim |
---|---|
\(+\) | \(7\) |
\(-\) | \(9\) |
Trace form
Decomposition of \(S_{40}^{\mathrm{new}}(\Gamma_0(9))\) into newform subspaces
Label | Dim | $A$ | Field | CM | Traces | A-L signs | $q$-expansion | ||||
---|---|---|---|---|---|---|---|---|---|---|---|
$a_{2}$ | $a_{3}$ | $a_{5}$ | $a_{7}$ | 3 | |||||||
9.40.a.a | $1$ | $86.706$ | \(\Q\) | \(\Q(\sqrt{-3}) \) | \(0\) | \(0\) | \(0\) | \(54\!\cdots\!40\) | $+$ | \(q-2^{39}q^{4}+54595696320612740q^{7}+\cdots\) | |
9.40.a.b | $3$ | $86.706$ | \(\mathbb{Q}[x]/(x^{3} - \cdots)\) | None | \(-548856\) | \(0\) | \(-17\!\cdots\!90\) | \(-17\!\cdots\!44\) | $-$ | \(q+(-182952+\beta _{1})q^{2}+(90692993728+\cdots)q^{4}+\cdots\) | |
9.40.a.c | $3$ | $86.706$ | \(\mathbb{Q}[x]/(x^{3} - \cdots)\) | None | \(-533574\) | \(0\) | \(53\!\cdots\!30\) | \(-15\!\cdots\!28\) | $-$ | \(q+(-177858+\beta _{1})q^{2}+(319147551244+\cdots)q^{4}+\cdots\) | |
9.40.a.d | $3$ | $86.706$ | \(\mathbb{Q}[x]/(x^{3} - \cdots)\) | None | \(1107000\) | \(0\) | \(-93\!\cdots\!90\) | \(13\!\cdots\!04\) | $-$ | \(q+(369000+\beta _{1})q^{2}+(335300075200+\cdots)q^{4}+\cdots\) | |
9.40.a.e | $6$ | $86.706$ | \(\mathbb{Q}[x]/(x^{6} - \cdots)\) | None | \(0\) | \(0\) | \(0\) | \(33\!\cdots\!80\) | $+$ | \(q+\beta _{1}q^{2}+(532022999032+\beta _{3})q^{4}+\cdots\) |
Decomposition of \(S_{40}^{\mathrm{old}}(\Gamma_0(9))\) into lower level spaces
\( S_{40}^{\mathrm{old}}(\Gamma_0(9)) \cong \) \(S_{40}^{\mathrm{new}}(\Gamma_0(1))\)\(^{\oplus 3}\)\(\oplus\)\(S_{40}^{\mathrm{new}}(\Gamma_0(3))\)\(^{\oplus 2}\)