We deepen the study of the relations previously established by Mayer, Lewis and Zagier, and the authors, among the eigenfunctions of the transfer operators of the Gauss and the Farey maps, the solutions of the Lewis-Zagier three-term functional equation and the Maass forms on the modular surface $PSL(2,Z)ackslash HH$. In particular we introduce an ``inverse'' of the integral transform studied by Lewis and Zagier, and use it to obtain new series expansions for the Maass cusp forms and the non-holomorphic Eisenstein series restricted to the imaginary axis. As corollaries we obtain further information on the Fourier coefficients of the forms, including a new series expansion for the divisor function
We study certain types of Fuchsian groups of the first kind denoted by $R(N)$, which coincide with t...
We characterize Maass cusp forms for Hecke congruence subgroups of prime level as 1-eigenfunctions o...
We investigate the Maass wave form for Γ(0)(2) whose eigenvalue of Laplacian Δ is 1/4-π(2)/log(2)(√2...
We deepen the study of the relations previously established by Mayer, Lewis and Zagier, and the auth...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We consider complex-valued modular forms on finite upper half planes Hq and ob-tain Fourier expansio...
We consider complex-valued modular forms on finite upper half planes Hq and obtain Fourier expansion...
In this thesis the Fourier expansions of all types of GL(3) Eisenstein series for the congruence sub...
We are interested in the study of non-correlation of Fourier coefficients of Maass forms against a w...
AbstractWe give a Katok–Sarnak type correspondence for Niebur type Poincaré series and Eisenstein se...
We define canonical real analytic versions of modular forms of integral weight for the full modular ...
We define canonical real analytic versions of modular forms of integral weight for the full modular ...
We study certain types of Fuchsian groups of the first kind denoted by $R(N)$, which coincide with t...
We characterize Maass cusp forms for Hecke congruence subgroups of prime level as 1-eigenfunctions o...
We investigate the Maass wave form for Γ(0)(2) whose eigenvalue of Laplacian Δ is 1/4-π(2)/log(2)(√2...
We deepen the study of the relations previously established by Mayer, Lewis and Zagier, and the auth...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We deepen the study of the relations − previously established by Mayer, Lewis and Zagier, and the au...
We consider complex-valued modular forms on finite upper half planes Hq and ob-tain Fourier expansio...
We consider complex-valued modular forms on finite upper half planes Hq and obtain Fourier expansion...
In this thesis the Fourier expansions of all types of GL(3) Eisenstein series for the congruence sub...
We are interested in the study of non-correlation of Fourier coefficients of Maass forms against a w...
AbstractWe give a Katok–Sarnak type correspondence for Niebur type Poincaré series and Eisenstein se...
We define canonical real analytic versions of modular forms of integral weight for the full modular ...
We define canonical real analytic versions of modular forms of integral weight for the full modular ...
We study certain types of Fuchsian groups of the first kind denoted by $R(N)$, which coincide with t...
We characterize Maass cusp forms for Hecke congruence subgroups of prime level as 1-eigenfunctions o...
We investigate the Maass wave form for Γ(0)(2) whose eigenvalue of Laplacian Δ is 1/4-π(2)/log(2)(√2...