"Half-integral weight modular forms"의 두 판 사이의 차이

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imported>Pythagoras0
imported>Pythagoras0
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==articles==
 
==articles==
* http://arxiv.org/abs/1507.00518
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* Chen, Bin, and Jie Wu. “Non-Vanishing and Sign Changes of Hecke Eigenvalues for Half-Integral Weight Cusp Forms.” arXiv:1512.08400 [math], December 28, 2015. http://arxiv.org/abs/1512.08400.
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* Lau, Yuk-Kam, Emmanuel Royer, and Jie Wu. “Sign of Fourier Coefficients of Modular Forms of Half Integral Weight.” arXiv:1507.00518 [math], July 2, 2015. http://arxiv.org/abs/1507.00518.
 
* http://www.worldscientific.com/doi/abs/10.1142/S1793042110003484
 
* http://www.worldscientific.com/doi/abs/10.1142/S1793042110003484
 
* http://link.springer.com/article/10.1007%2Fs00013-013-0492-5
 
* http://link.springer.com/article/10.1007%2Fs00013-013-0492-5

2015년 12월 29일 (화) 00:35 판

introduction

 

 

 

\(\Gamma_0(N) = \left\{ \begin{pmatrix} a & b \\ c & d \end{pmatrix} \in SL_2(\mathbf{Z}) : \begin{pmatrix} a & b \\ c & d \end{pmatrix} \equiv \begin{pmatrix} {*} & {*} \\ 0 & {*} \end{pmatrix} \pmod{N} \right\}\)

 

 

\(\Gamma_0(4)\)

generated by \(-I, T, ST^{-4}S\)

 

Define

\(\epsilon_d = \begin{cases} 1 \mbox{ if }d\equiv 1 \pmod{4} \\i \mbox{ if } d\equiv 3 \pmod{4} \end{cases}\)

\(\sqrt z\) has branch in \((-\pi/2, \pi/2]\)

 

Define

\(j(\gamma, z)=(\frac{c}{d})\epsilon_d^{-1}\sqrt{cz+d}\) for \(\gamma \in \Gamma_0(4)\)

 

Check

\(j(\alpha\beta,z)=j(\alpha,\beta z)j(\beta,z)\)

\(j(\gamma, z)^2=\begin{cases} {cz+d} \mbox{ if }d\equiv 1 \pmod{4} \\ -(cz+d) \mbox{ if } d\equiv 3 \pmod{4} \end{cases}\)

 

action

For \(\xi=(\alpha, \phi(z))\) and function \(f\) on the upper half plane

\(f(z)|[\xi]_{k/2}:=f(\alpha z)\phi(z)^{-k}\)

 

 

unary theta functions of weight 1/2

 

 

theta functions of weight 3/2

related items

 

expositions

articles