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Next: Bibliography Up: Sample LATEX document Previous: Preliminaries

Some sample theorems


\begin{lemma}
Let's put here exactly what we need to prove the next theorem.
\end{lemma}


\begin{thm}
Let $f$\ be a nonzero element of $S_{k/2}(4N,\psi)$. Then
there exi...
...umber of square-free positive integers $t$ such that $\Sh_t(f) \ne 0$.
\end{thm}

The proof which is below is correct, but unmotivated. Perhaps we can find an alternate proof which provides more insight

Proof. If $ \Sh_t(f) = 0$ for all but a finite number of square-free positive integers $ t$, then by lemma:squareclasses the Fourier coefficients of $ f$ are supported on only a finite number of square classes. By Theorem 3 of [3] the weight of $ f$ must be $ 1/2$ of $ 3/2$ and at weight $ 3/2$ must be in the span of the theta series $ h_\psi$, contrary to assumption. $ \qedsymbol$

By thm:nonzerolifts, we see that it we can always find nonzero Shimura lifts.


\begin{defn}
A horse is a horse of course, of course, but noone can talk to a horse
of course \dots.
\end{defn}

Here we have some displayed and aligned equations.

Here is an unnumbered displayed equation:

$\displaystyle T(m) T(n) = \sum_{d \mid (m,n)} d^{k-1}\chi(d) T(mn/d^2).$    

Here is a numbered displayed equation:

$\displaystyle T(m) T(n) = \sum_{d \mid (m,n)} d^{k-1}\chi(d) T(mn/d^2).$ (1)

Here is the same expression, but inline and not displayed. Notice it is set smaller and the summation indeices are placed differently: $ T(m) T(n) = \sum_{d \mid (m,n)} d^{k-1}\chi(d) T(mn/d^2).$ Note I need to use $ to surround my formula when in an inline mode.

For an aligned display we have

$\displaystyle \Lambda_N(s;f)$ $\displaystyle = \left(\frac{2\pi}{\sqrt N}\right)^{-s} \Gamma(s) L(s;f)$    
$\displaystyle \Lambda_M(s;g)$ $\displaystyle = \left(\frac{2\pi}{\sqrt M}\right)^{-s} \Gamma(s) L(s;g)$    

A numbered version is given by

$\displaystyle \Lambda_N(s;f)$ $\displaystyle = \left(\frac{2\pi}{\sqrt N}\right)^{-s} \Gamma(s) L(s;f)$ (2)
$\displaystyle \Lambda_M(s;g)$ $\displaystyle = \left(\frac{2\pi}{\sqrt M}\right)^{-s} \Gamma(s) L(s;g)$ (3)

A version with only one number associated to the group of equations is given by

\begin{displaymath}\begin{split}\Lambda_N(s;f) &= \left(\frac{2\pi}{\sqrt N}\rig...
...t(\frac{2\pi}{\sqrt M}\right)^{-s} \Gamma(s) L(s;g) \end{split}\end{displaymath} (4)

Something with cases

$\displaystyle \phi_p(s) = \begin{cases}\left(\frac{1 - b(p) p^{-s} + \psi(p) p^...
...\right) &\qquad \text{if } p\mid L\\  1&\qquad\text{if } p \nmid L. \end{cases}$    

This should be more than enough displayed equations for the average person. Gosh, I sure hope this paper gets accepted. More remarks of little permanent consequence.


\begin{thm}Suppose that $N$\ is an odd positive integer and $\psi$\ is an
even ...
...hen
$S^+_{k/2}(4N,\psi)_K \subset S^+_{k/2}(4N,\psi)$.
\end{enumerate}\end{thm}

Let's get the other references in now. See [1] and [2].


next up previous
Next: Bibliography Up: Sample LATEX document Previous: Preliminaries
Thomas R. Shemanske 2000-07-07