\small
\begin{center}
{\it P. Bhat,
     R. Gilmartin, 
     R. Jesik, 
     M. Kruse,
     H. Prosper,
     W. Yao} \\
\end{center}
\normalsize \nopagebreak

Although the cross section times branching ratio for the $ZH\rightarrow\lpm\bb$
final is roughly 1/3 that of the previous two channels, these events are easily
and cleanly identified.  Furthermore, given the high luminosity required for
observation in the higher rate $WH\rightarrow\ell\nu\bb$ and $ZH\rightarrow
\nn\bb$ channels, it is clear that every possible event is valuable to the
Higgs search.

       \vskip 4mm 
       \centerline{ \large \it 3a. $\lpm\bb$, QFL$^\prime$ Simulation
           and Traditional Techniques}
       \vskip 4mm 
	
The selection criteria for this channel are:
 In the $ZH\rightarrow (e^+e^-,\mu^+\mu^-)b\bar b$ channel, we select the 
 dilepton events with the following cuts.
\begin{itemize} 
      \item First lepton  $\et(\pt)>20$ GeV, $|\eta|<1.0$ 
      \item Second lepton $\et(\pt)>10$ GeV, $|\eta|<2.0$ 
      \item $| M_{Z}-M_{l^+l^-}|<15 $ GeV
      \item Two $b$-tagged jets with $\et>15$ GeV and $|\eta|<2.0$ 
\end{itemize} 
The results are included with those for the $ZH\rightarrow\nn\bb$
channel described in section {\it 2a}.

       \vskip 4mm 
       \centerline{ \large \it 1b. $\lpm\bb$, SHW Simulation 
           and Traditional Techniques} \nopagebreak
       \vskip 4mm 
       \input{zhll/zhll-shw.tex}

       \vskip 4mm 
       \centerline{ \large \it 1c. $\lpm\bb$, SHW Simulation 
           and Neural Network Techniques} \nopagebreak
       \vskip 4mm 
       \input{zhll/zhll-nn.tex}

