Properties

Label 1000.2.bh
Level $1000$
Weight $2$
Character orbit 1000.bh
Rep. character $\chi_{1000}(3,\cdot)$
Character field $\Q(\zeta_{100})$
Dimension $5920$
Newform subspaces $1$
Sturm bound $300$
Trace bound $0$

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Defining parameters

Level: \( N \) \(=\) \( 1000 = 2^{3} \cdot 5^{3} \)
Weight: \( k \) \(=\) \( 2 \)
Character orbit: \([\chi]\) \(=\) 1000.bh (of order \(100\) and degree \(40\))
Character conductor: \(\operatorname{cond}(\chi)\) \(=\) \( 1000 \)
Character field: \(\Q(\zeta_{100})\)
Newform subspaces: \( 1 \)
Sturm bound: \(300\)
Trace bound: \(0\)

Dimensions

The following table gives the dimensions of various subspaces of \(M_{2}(1000, [\chi])\).

Total New Old
Modular forms 6080 6080 0
Cusp forms 5920 5920 0
Eisenstein series 160 160 0

Trace form

\( 5920 q - 40 q^{2} - 80 q^{3} - 40 q^{4} - 40 q^{6} - 40 q^{8} - 80 q^{9} + O(q^{10}) \) \( 5920 q - 40 q^{2} - 80 q^{3} - 40 q^{4} - 40 q^{6} - 40 q^{8} - 80 q^{9} - 40 q^{10} - 80 q^{11} - 40 q^{12} - 40 q^{14} - 40 q^{16} - 80 q^{17} - 40 q^{18} - 80 q^{19} - 40 q^{20} - 40 q^{22} - 50 q^{24} - 80 q^{25} - 30 q^{26} - 80 q^{27} - 40 q^{28} - 40 q^{30} - 40 q^{32} - 80 q^{33} - 40 q^{34} - 80 q^{35} - 40 q^{36} - 10 q^{38} - 90 q^{40} - 80 q^{41} + 60 q^{42} - 80 q^{43} - 110 q^{44} - 40 q^{46} - 170 q^{48} - 100 q^{49} + 50 q^{50} - 60 q^{51} - 130 q^{52} + 90 q^{54} - 40 q^{56} - 80 q^{57} + 30 q^{58} - 80 q^{59} - 140 q^{60} + 10 q^{62} - 70 q^{64} - 80 q^{65} - 40 q^{66} - 80 q^{67} - 40 q^{68} - 40 q^{70} - 70 q^{72} - 80 q^{73} - 50 q^{74} - 80 q^{75} - 30 q^{76} - 10 q^{78} - 40 q^{80} - 80 q^{81} - 80 q^{82} - 80 q^{83} - 120 q^{84} - 40 q^{86} - 160 q^{88} + 20 q^{89} - 190 q^{90} - 80 q^{91} - 140 q^{92} - 200 q^{94} - 40 q^{96} - 160 q^{97} - 200 q^{98} - 100 q^{99} + O(q^{100}) \)

Decomposition of \(S_{2}^{\mathrm{new}}(1000, [\chi])\) into newform subspaces

Label Char Prim Dim $A$ Field CM Minimal twist Traces Sato-Tate $q$-expansion
$a_{2}$ $a_{3}$ $a_{5}$ $a_{7}$
1000.2.bh.a 1000.bh 1000.ah $5920$ $7.985$ None 1000.2.bh.a \(-40\) \(-80\) \(0\) \(0\) $\mathrm{SU}(2)[C_{100}]$