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Hecke operator
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=== Explicit formula === Let {{math|''M''<sub>''m''</sub>}} be the set of {{math|2Γ2}} integral matrices with [[determinant]] {{math|''m''}} and {{math|1=''Γ'' = ''M''<sub>1</sub>}} be the full [[modular group]] {{math|''SL''(2, '''Z''')}}. Given a modular form {{math|''f''(''z'')}} of weight {{math|''k''}}, the {{math|''m''}}th Hecke operator acts by the formula : <math> T_m f(z) = m^{k-1}\sum_{\left(\begin{smallmatrix}a & b\\ c & d\end{smallmatrix}\right)\in\Gamma\backslash M_m}(cz+d)^{-k}f\left(\frac{az+b}{cz+d}\right), </math> where {{math|''z''}} is in the [[upper half-plane]] and the normalization constant {{math|''m''<sup>''k''−1</sup>}} assures that the image of a form with integer Fourier coefficients has integer Fourier coefficients. This can be rewritten in the form : <math> T_m f(z) = m^{k-1}\sum_{a,d>0, ad=m}\frac{1}{d^k}\sum_{b \pmod d} f\left(\frac{az+b}{d}\right), </math> which leads to the formula for the Fourier coefficients of {{math|1=''T''<sub>''m''</sub>(''f''(''z'')) = Ξ£ ''b''<sub>''n''</sub>''q''<sup>''n''</sup>}} in terms of the Fourier coefficients of {{math|1=''f''(''z'') = Ξ£ ''a''<sub>''n''</sub>''q''<sup>''n''</sup>}}: : <math> b_n = \sum_{r>0, r|(m,n)}r^{k-1}a_{mn/r^2}.</math> One can see from this explicit formula that Hecke operators with different indices commute and that if {{math|1=''a''<sub>0</sub> = 0}} then {{math|1=''b''<sub>0</sub> = 0}}, so the subspace {{math|''S''<sub>''k''</sub>}} of cusp forms of weight {{math|''k''}} is preserved by the Hecke operators. If a (non-zero) cusp form {{math|''f''}} is a [[Eigenform|simultaneous eigenform]] of all Hecke operators {{math|''T''<sub>''m''</sub>}} with eigenvalues {{math|''λ''<sub>''m''</sub>}} then {{math|1=''a''<sub>''m''</sub> = ''λ''<sub>''m''</sub>''a''<sub>1</sub>}} and {{math|''a''<sub>1</sub> β 0}}. Hecke eigenforms are '''normalized''' so that {{math|1=''a''<sub>1</sub> = 1}}, then : <math> T_m f = a_m f, \quad a_m a_n = \sum_{r>0, r|(m,n)}r^{k-1}a_{mn/r^2},\ m,n\geq 1. </math> Thus for normalized cuspidal Hecke eigenforms of integer weight, their Fourier coefficients coincide with their Hecke eigenvalues.
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