Fricke transport of the good Hecke operators #
At an index n coprime to N, the Fricke operator intertwines Tₙ with
⟨n⟩⁻¹ Tₙ on forms for Γ₁(N). On a nebentypus space this gives the scalar
χ(n) when Tₙ is moved past Fricke from the source to the target character space.
The same identities hold for the Petersson-normalized Fricke operator and for cusp forms.
This relation transports good Hecke eigensystems to the inverse-nebentypus space; it is the Hecke-theoretic input to the Fricke pseudo-eigenvalue theorem for primitive forms.
References #
- T. Miyake, Modular forms, §4.6, Theorem 4.6.15.
- F. Diamond and J. Shurman, A first course in modular forms, §5.5.
At a good index, Fricke carries Tₙ to its inverse-diamond multiple on modular forms.
At a good index, Fricke carries Tₙ to its inverse-diamond multiple on cusp forms.
The Petersson normalization leaves the Fricke–Hecke intertwining relation unchanged.
The normalized Fricke–Hecke intertwining relation on cusp forms.
On M_k(N, χ), moving a good Tₙ past Fricke introduces χ(n).
The output of Fricke has nebentypus χ⁻¹.
On S_k(N, χ), moving a good Tₙ past Fricke introduces χ(n).
On a nebentypus space, the normalized Fricke operator intertwines Tₙ with χ(n)Tₙ.
No parity or reality hypothesis on χ is needed.
The normalized Fricke–Hecke relation on cusp forms with general nebentypus.
Fricke transports a good Hecke eigenrelation by multiplying its eigenvalue by χ(n)⁻¹.
The equivalence includes the zero form and does not require normalization of its coefficients.