Defining parameters
| Level: | \( N \) | \(=\) | \( 400 = 2^{4} \cdot 5^{2} \) |
| Weight: | \( k \) | \(=\) | \( 2 \) |
| Character orbit: | \([\chi]\) | \(=\) | 400.a (trivial) |
| Character field: | \(\Q\) | ||
| Newform subspaces: | \( 8 \) | ||
| Sturm bound: | \(120\) | ||
| Trace bound: | \(7\) | ||
| Distinguishing \(T_p\): | \(3\), \(7\) |
Dimensions
The following table gives the dimensions of various subspaces of \(M_{2}(\Gamma_0(400))\).
| Total | New | Old | |
|---|---|---|---|
| Modular forms | 78 | 11 | 67 |
| Cusp forms | 43 | 8 | 35 |
| Eisenstein series | 35 | 3 | 32 |
The following table gives the dimensions of the cuspidal new subspaces with specified eigenvalues for the Atkin-Lehner operators and the Fricke involution.
| \(2\) | \(5\) | Fricke | Total | Cusp | Eisenstein | |||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| All | New | Old | All | New | Old | All | New | Old | ||||||
| \(+\) | \(+\) | \(+\) | \(18\) | \(2\) | \(16\) | \(10\) | \(2\) | \(8\) | \(8\) | \(0\) | \(8\) | |||
| \(+\) | \(-\) | \(-\) | \(20\) | \(3\) | \(17\) | \(11\) | \(3\) | \(8\) | \(9\) | \(0\) | \(9\) | |||
| \(-\) | \(+\) | \(-\) | \(21\) | \(3\) | \(18\) | \(12\) | \(2\) | \(10\) | \(9\) | \(1\) | \(8\) | |||
| \(-\) | \(-\) | \(+\) | \(19\) | \(3\) | \(16\) | \(10\) | \(1\) | \(9\) | \(9\) | \(2\) | \(7\) | |||
| Plus space | \(+\) | \(37\) | \(5\) | \(32\) | \(20\) | \(3\) | \(17\) | \(17\) | \(2\) | \(15\) | ||||
| Minus space | \(-\) | \(41\) | \(6\) | \(35\) | \(23\) | \(5\) | \(18\) | \(18\) | \(1\) | \(17\) | ||||
Trace form
Decomposition of \(S_{2}^{\mathrm{new}}(\Gamma_0(400))\) into newform subspaces
Decomposition of \(S_{2}^{\mathrm{old}}(\Gamma_0(400))\) into lower level spaces
\( S_{2}^{\mathrm{old}}(\Gamma_0(400)) \simeq \) \(S_{2}^{\mathrm{new}}(\Gamma_0(20))\)\(^{\oplus 6}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(\Gamma_0(40))\)\(^{\oplus 4}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(\Gamma_0(50))\)\(^{\oplus 4}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(\Gamma_0(80))\)\(^{\oplus 2}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(\Gamma_0(100))\)\(^{\oplus 3}\)\(\oplus\)\(S_{2}^{\mathrm{new}}(\Gamma_0(200))\)\(^{\oplus 2}\)