\batchmode
\documentstyle[12pt,epsf]{article}
\makeatletter 


\baselineskip 12pt plus 1pt minus 1pt
\parskip 12pt plus 1pt minus 1pt

\textwidth 16.5cm 
\textheight 23.8cm 
\pagestyle{plain}
\topmargin -1.6cm
\oddsidemargin -0.5cm
\parindent=3pc






\includeonly{abst,sldauth,physics,theory,select,anal,result,bib,trans1,lephnu}

\def\mathrm{\rm}\newcommand{\ra}{\mbox{$\rightarrow$}}
\newcommand{\pr}{\mbox{\small $\prime$}}
\newcommand{\half}{\mbox{$\frac{1}{2}$}}
\newcommand{\third}{\mbox{$\frac{1}{3}$}}
\newcommand{\thovsxt}{\mbox{$\frac{3}{16}$}}
\newcommand{\thoveit}{\mbox{$\frac{3}{8}$}}
\newcommand{\thovfr}{\mbox{$\frac{3}{4}$}}
\newcommand{\eitovth}{\mbox{$\frac{8}{3}$}}
\newcommand{\sxtovth}{\mbox{$\frac{16}{3}$}}
\newcommand{\onovsij}{\mbox{$\frac{1}{\sij}$}}
\newcommand{\onovsi}{\mbox{$\frac{1}{\sigma_i}$}}
\newcommand{\tn}{\mbox{$\tau$}}
\def\t{\tn}\newcommand{\tm}{\mbox{$\tau^-$}}
\newcommand{\tp}{\mbox{$\tau^+$}}
\newcommand{\nut}{\mbox{$\nu_{\tau}$}}
\newcommand{\nutb}{\mbox{$\bar{\nu}_{\tau}$}}
\newcommand{\eln}{\mbox{\rm e}}
\newcommand{\elm}{\mbox{\rm e$^-$}}
\newcommand{\elp}{\mbox{\rm e$^+$}}
\newcommand{\nue}{\mbox{$\nu_e$}}
\newcommand{\nueb}{\mbox{$\bar{\nu}_e$}}
\newcommand{\mun}{\mbox{$\mu$}}
\newcommand{\mum}{\mbox{$\mu^-$}}
\newcommand{\mup}{\mbox{$\mu^+$}}
\newcommand{\num}{\mbox{$\nu_{\mu}$}}
\newcommand{\numb}{\mbox{$\bar{\nu}_{\mu}$}}
\newcommand{\elln}{\mbox{$\ell$}}
\newcommand{\ellm}{\mbox{$\ell^-$}}
\newcommand{\ellp}{\mbox{$\ell^+$}}
\newcommand{\nul}{\mbox{$\nu_{\ell}$}}
\newcommand{\nulb}{\mbox{$\bar{\nu}_{\ell}$}}
\newcommand{\pin}{\mbox{$\pi$}}
\newcommand{\pim}{\mbox{$\pi^-$}}
\newcommand{\pip}{\mbox{$\pi^+$}}
\newcommand{\piz}{\mbox{$\pi^0$}}
\newcommand{\piK}{\mbox{$\pi$(K)}}
\newcommand{\rhon}{\mbox{$\rho$}}
\newcommand{\rhom}{\mbox{$\rho^-$}}
\newcommand{\rhop}{\mbox{$\rho^+$}}
\newcommand{\Kstn}{\mbox{\rm K$^{\ast}$}}
\newcommand{\Kstm}{\mbox{\rm K$^{\ast +}$}}
\newcommand{\Kstp}{\mbox{\rm K$^{\ast -}$}}
\newcommand{\ksh}{\mbox{\rm K$^0_s$}}
\newcommand{\Xp}{\mbox{\rm X$^+$}}
\newcommand{\Xm}{\mbox{\rm X$^-$}}
\newcommand{\aonep}{\mbox{\rm a$_1^-$}}
\newcommand{\aonem}{\mbox{\rm a$_1^+$}}
\newcommand{\Z}{\mbox{\rm Z$^0$ }}
\def\tt{\mbox{\tp \tm}}\newcommand{\tautau}{\mbox{\tp \tm}}
\newcommand{\ee}{\mbox{\elp \elm} }
\newcommand{\mumu}{\mbox{\mup \mum} }
\newcommand{\ggmm}{\mbox{$\gamma\gamma$\ra\mumu}}
\newcommand{\led}    {\elln\nulb\nut}
\newcommand{\pid}    {\piK \nut}
\newcommand{\tmu}{\mbox{\tn \ra \mun \numb \nut}}
\newcommand{\tel}{\mbox{\tn \ra \eln \nueb \nut}}
\newcommand{\tle}{\mbox{\tn \ra \elln \nulb \nut}}
\newcommand{\tpi}{\mbox{\tn \ra $\pi$ \nut}}
\newcommand{\tpiK}{\mbox{\tn \ra \piK \nut}}
\newcommand{\tro}{\mbox{\tn \ra \rhon\nut}}
\def\thp{\t \ra h\pi^0\nu}\newcommand{\tkstr}{\mbox{\tn \ra K$^{\ast}$ \nut}}
\newcommand{\taone}{\mbox{\tn \ra a$_1$\nut}}
\newcommand{\thnpiz}{\mbox{\tn \ra h $>$2\piz \nut}}
\newcommand{\eemm}{\mbox{\ee \ra \mumu} }
\newcommand{\eett}{\mbox{\ee \ra \tautau} }
\newcommand{\pzgg}{\mbox{\piz \ra $\gamma \gamma$}}
\def\p0gg{\pi ^0 \ra \gamma \gamma}\newcommand{\efswsq}
{\mbox{$\sin^2\theta_{W}^{\mbox{\small \it eff}}$}}
\def\swsq{\sin^2\theta_W}\def\cost{\cos\theta}\newcommand{\cosst}  {\cos^2\theta}
\newcommand{\cst}{\mbox{$\cos\theta$}}
\newcommand{\cstp}{\mbox{$\cos\theta^{\pr}$}}
\newcommand{\csts}{\mbox{$\cos\theta^{\ast}$}}
\newcommand{\cpsi}{\mbox{$\cos\psi$}}
\newcommand{\sspsi}{\mbox{$\sin^2\psi$}}
\newcommand{\cspsi}{\mbox{$\cos^2\psi$}}
\newcommand{\seta}{\mbox{$\sin\eta$}}
\newcommand{\ceta}{\mbox{$\cos\eta$}}
\newcommand{\cseta}{\mbox{$\cos^2\eta$}}
\newcommand{\ctsh}{\mbox{$\cos\frac{\theta^{\ast}}{2}$}}
\newcommand{\stsh}{\mbox{$\sin\frac{\theta^{\ast}}{2}$}}
\newcommand{\cstsh}{\mbox{$\cos^2\frac{\theta^{\ast}}{2}$}}
\newcommand{\sstsh}{\mbox{$\sin^2\frac{\theta^{\ast}}{2}$}}
\newcommand{\act}{\mbox{$|\cos\theta |$}}
\newcommand{\cstsq}{\mbox{$\cos^{2}\theta$}}
\newcommand{\eb}{\mbox{$E_{beam}$}}
\newcommand{\elep}{\mbox{$E_{\ell}$}}
\newcommand{\ehad}{\mbox{$E_h$}}
\newcommand{\ecm}{\mbox{$E_{cm}$}}
\def\ecma{\langle\ecm\rangle}\newcommand{\cof}{\mbox{$\chi^2/D.O.F.$}}
\newcommand{\chs}{\mbox{$\chi^2$}}
\newcommand{\xih}{\mbox{$\xi_{had}$}}
\newcommand{\xxi}{\mbox{$x_i$}}
\newcommand{\xxj}{\mbox{$x_j$}}
\newcommand{\xip}{\mbox{$x_i$}}
\newcommand{\xjp}{\mbox{$x_j$}}
\newcommand{\xp}{\mbox{$x$}}
\newcommand{\ptr}{\mbox{$p_{\scriptscriptstyle T}$}}
\newcommand{\xtr}{\mbox{$x_{\scriptscriptstyle T}$}}
\newcommand{\xtp}{\mbox{$x^{\pr}_{\scriptscriptstyle T}$}}
\newcommand{\tpr}{\mbox{$\theta^{\pr}$}}
\newcommand{\fix}{\mbox{$f_i$}}
\newcommand{\fjx}{\mbox{$f_j$}}
\newcommand{\gix}{\mbox{$g_i$}}
\newcommand{\gjx}{\mbox{$g_j$}}
\newcommand{\rxx}{\mbox{${\cal R}_i(\bar{\xxi},\xip)$}}
\newcommand{\rcc}{\mbox{${\cal C}_i(\cos\bar{\theta},\cst)$}}
\newcommand{\mhs}{\mbox{$m_h^2$}}
\newcommand{\mts}{\mbox{$m_{\tau}^2$}}
\newcommand{\mrs}{\mbox{$m_{\rho}^2$}}
\newcommand{\mpc}{\mbox{$m_{\pi^{\pm}}$}}
\newcommand{\mpz}{\mbox{$m_{\pi^0}$}}
\newcommand{\mt}{\mbox{$m_{\tau}$}}
\newcommand{\mr}{\mbox{$m_{\rho}$}}
\newcommand{\mzsq}{\mbox{$m_{\mbox \rm Z}^2$}}
\newcommand{\mz}{\mbox{$m_Z$}}
\def\mzs{s=m_Z^2}\newcommand{\lamt}{\mbox{${\cal A}_{\tau}$}}
\newcommand{\lame}{\mbox{${\cal A}_e$}}
\newcommand{\laml}{\mbox{${\cal A}_{\ell}$}}
\newcommand{\vovat}{\mbox{\rm g$_v^{\tau}$/g$_a^{\tau}$}}
\newcommand{\vovae}{\mbox{\rm g$_v^e$/g$_a^e$}}
\newcommand{\voval}{\mbox{ \rm g$_v^{\ell}$/g$_a^{\ell}$} }
\newcommand{\epstij}
{\mbox{${\cal E}^{\pm}_{ij}(\xip,\xjp,\cst)$}}
\newcommand{\epsti}
{\mbox{${\cal E}^{\pm}_{i}(\xip,\cst)$}}
\newcommand{\epsdi}{\mbox{$\epsilon_{i}(\xip,\cst)$}}
\newcommand{\epsdj}{\mbox{$\epsilon_{j}(\xjp,\cst)$}}
\def\epstpi{{\cal E}^{\pr\pm}_{i}(\xip,\cst)}\newcommand{\hi}{\mbox{$h^{\pm}_i(\xip)$}}
\newcommand{\hj}{\mbox{$h^{\pm}_j(\xjp)$}}
\newcommand{\beti}{\mbox{$\beta^{\pm}_{i} (\xip,\cst)$}}
\newcommand{\betj}{\mbox{$\beta^{\pm}_{j} (\xjp,\cst)$}}
\def\bbetij{\bar{\beta}^\pm_{ij}}\def\bbeti{\bar{\beta}^\pm_{i}}\newcommand{\bntij}{\mbox{$\beta^{non-\tau}_{ij}(\xip,\xjp,\cst)$}}
\newcommand{\bnti}{\mbox{$\beta^{non-\tau}_{i}(\xip,\cst)$}}
\newcommand{\ri}{\mbox{$r^{\pm}_i(\bar{\xxi})$}}
\newcommand{\ric}{\mbox{$\hat{r}^{\pm}_i(\cos\bar{\theta})$}}
\newcommand{\ptm}{\mbox{$\langle P_{\tau^-}\rangle$}}
\newcommand{\ptp}{\mbox{$\langle P_{\tau^+}\rangle$}}
\newcommand{\pta}{\mbox{$\langle P_{\tau}\rangle$}}
\newcommand{\pfa}{\mbox{$\langle P_{f}\rangle$}}
\newcommand{\ptat}{\mbox{$\langle P_{\tau}\rangle_{\theta}$}}
\newcommand{\dpta}{\mbox{$\Delta \langle P_{\tau}\rangle$}}
\newcommand{\Pt}{\mbox{\rm P$_{\tau}$}}
\newcommand{\At}{\mbox{\rm A$_{\tau}$}}
\newcommand{\Al}{\mbox{\rm A$_{\ell}$}}
\newcommand{\hnu}{\mbox{\rm h$_{\nu_{\tau}}$}}
\newcommand{\Ae}{\mbox{\rm A$_e$}}
\newcommand{\Pe}{\mbox{\it P$_e$}}
\newcommand{\ptau}   {P_{\tau}}
\def\pt{P_{\t}}\newcommand{\afb}{\mbox{\rm A$_{FB}$}}
\newcommand{\aplfb}{\mbox{\rm A$_{pol}^{FB}$}}
\newcommand{\daplfb}{\mbox{$\Delta$ \rm A$_{pol}^{FB}$}}
\newcommand{\apolf}  {\langle\ptau\rangle^F}
\newcommand{\apolb}  {\langle\ptau\rangle^B}
\newcommand{\sigp}{\mbox{$\sigma_+$}}
\newcommand{\sigm}{\mbox{$\sigma_-$}}
\newcommand{\sigr}{\mbox{$\sigma_R$}}
\newcommand{\sigl}{\mbox{$\sigma_L$}}
\newcommand{\sigtot}{\mbox{$\sigma_{tot}$}}
\newcommand{\sigtotp}{\mbox{$\sigma_{tot}^{\pr}$}}
\newcommand{\spr}{\mbox{$\sigma$}}
\newcommand{\sijp}{\mbox{$\spr_{ij}$}}
\newcommand{\sip}{\mbox{$\spr_i$}}
\def\sigpp{\sigma(++)}\def\sigpm{\sigma(+-)}\def\sigmp{\sigma(-+)}\def\sigmm{\sigma(--)}\newcommand{\sigf}   {\sigma^F}
\newcommand{\sigb}   {\sigma^B}
\newcommand{\ptrans}{\mbox{\bf p$_{\scriptscriptstyle T}$}}
\def\dsigtw{\frac{d^2\sigma_i}{d\cst\:d\xxi}}\def\dsigtwp{\frac{d^2\sip}{d\cst\:d\xip}}\def\dsigth{\frac{d^3\sij}{d\cos\theta\:d\xxi\:d\xxj}}\def\dsigthp{\frac{d^3\sijp}{d\cst\:d\xip\:d\xjp}}\def\fz{F_0(s)}\def\fo{F_1(s)}\def\ft{F_2(s)}\def\fth{F_3(s)}\newcommand{\fos}    {F_0(s)}
\newcommand{\fis}    {F_1(s)}
\newcommand{\fts}    {F_2(s)}
\newcommand{\frs}    {F_3(s)}
\def\qe{q_{e}}\def\qt{q_{\tau}}\def\ae{a_{e}}\def\at{a_{\tau}}\def\ve{v_{e}}\def\vt{v_{\tau}}\def\gv{\hat{{\sl g}}_v^{\ell}}\def\ga{\hat{{\sl g}}_a^{\ell}}\newcommand{\dzero}{\mbox{$| d_0|$}}
\newcommand{\zzero}{\mbox{$| z_0|$}}
\def\d0{|d_0|}\def\z0{|z_0|}\newcommand{\Excess}{\mbox{\rm E$_{excess}$}}
\newcommand{\dphimax}{\mbox{$\delta \phi_{max}$}}
\newcommand{\Nhl}{\mbox{\rm N$^{HC}_{hits/layer}$}}
\newcommand{\Nhc}{\mbox{\rm N$^{HC}_{layers}$}}
\newcommand{\Nhm}{\mbox{\rm N$^{HC/MU}_{layers}$}}
\newcommand{\degree} {$^\circ$}
\newcommand{\cth}    {$|\cos\theta|$}
\newcommand{\id}{identification}
\newcommand{\goro}[1]{\multicolumn{2}{c|}{#1}}
\newcommand{\bb}{\mathrm{b}\overline{\mathrm{b}}}
\def\dedx{\mbox{$\mathrm{d}E/\mathrm{d}x$}}\newcommand{\etal}{\mbox{\it et al.,}~}
\newcommand {\beq} {\begin{equation}}
\newcommand {\eeq} {\end{equation}}
\newcommand {\bea} {\begin{eqnarray}}
\newcommand {\eea} {\end{eqnarray}}
\newcommand{\ind}[1]{#1\index{#1}}
\newcommand{\Ntpair}{4552}
\newcommand{\HNU}{-0.89}
\newcommand{\HNUST}{0.21}
\newcommand{\HNUSY}{0.07}
\newcommand{\XI}{1.17}
\newcommand{\XIST}{0.35}
\newcommand{\XISY}{0.21}
\newcommand{\XIDELTA}{0.49}
\newcommand{\XIDELTAST}{0.24}
\newcommand{\XIDELTASY}{0.13}

\makeatother
\newenvironment{tex2html_wrap}{}{}
\setlength{\textheight}{10in}\begin{document}
\pagestyle{empty}
\newpage

{\samepage \clearpage $\t$
}


\newpage

{\samepage \clearpage $\hnu$
}


\newpage

{\samepage \clearpage $\xi$
}


\newpage

{\samepage \clearpage $\delta$
}


\newpage

{\samepage \clearpage $\tn$
}


\newpage

{\samepage \clearpage $\tpiK$
}


\newpage

{\samepage \clearpage $\tel$
}


\newpage

{\samepage \clearpage $\tmu$
}


\newpage

{\samepage \clearpage $e^+e^-\rightarrow Z^0 \rightarrow \tt$
}


\newpage

{\samepage \clearpage $\Ntpair$
}


\newpage

{\samepage \clearpage $\mbox{\rm h$_{\nu_{\tau}}$}=-0.89 \pm 0.21 \pm \HNUSY$
}


\newpage

{\samepage \clearpage $\xi=1.17 \pm 0.35 \pm \XISY$
}


\newpage

{\samepage \clearpage $\xi\delta= 0.49 \pm 0.24 \pm \XIDELTASY$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $^{(29)}$
}


\newpage

{\samepage \clearpage $^{(14)}$
}


\newpage

{\samepage \clearpage $^{(26)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(27)\dagger}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(32)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(10)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(11)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(2)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(22)}$
}


\newpage

{\samepage \clearpage $^{(21)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(11)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(13)}$
}


\newpage

{\samepage \clearpage $^{(6)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(12)}$
}


\newpage

{\samepage \clearpage $^{(23)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(23)(a)}$
}


\newpage

{\samepage \clearpage $^{(21)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(3)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(8)}$
}


\newpage

{\samepage \clearpage $^{(25)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(13)}$
}


\newpage

{\samepage \clearpage $^{(13)}$
}


\newpage

{\samepage \clearpage $^{(23)}$
}


\newpage

{\samepage \clearpage $^{(9)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(14)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(22)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(25)}$
}


\newpage

{\samepage \clearpage $^{(14)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(29)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(17)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(29)}$
}


\newpage

{\samepage \clearpage $^{(25)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(3)}$
}


\newpage

{\samepage \clearpage $^{(32)}$
}


\newpage

{\samepage \clearpage $^{(8)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(19)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(26)}$
}


\newpage

{\samepage \clearpage $^{(14)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(26)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(17)}$
}


\newpage

{\samepage \clearpage $^{(10)}$
}


\newpage

{\samepage \clearpage $^{(18)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(10)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(21)}$
}


\newpage

{\samepage \clearpage $^{(6)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(22)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(22)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(22)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(12)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(8)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(10)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(8)}$
}


\newpage

{\samepage \clearpage $^{(19)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(30)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(13)(b)}$
}


\newpage

{\samepage \clearpage $^{(13)}$
}


\newpage

{\samepage \clearpage $^{(12)}$
}


\newpage

{\samepage \clearpage $^{(23)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(32)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(30)}$
}


\newpage

{\samepage \clearpage $^{(18)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(11)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(15)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(32)}$
}


\newpage

{\samepage \clearpage $^{(11)}$
}


\newpage

{\samepage \clearpage $^{(3)}$
}


\newpage

{\samepage \clearpage $^{(15)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(15)}$
}


\newpage

{\samepage \clearpage $^{(1)}$
}


\newpage

{\samepage \clearpage $^{(17)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(29)}$
}


\newpage

{\samepage \clearpage $^{(19)}$
}


\newpage

{\samepage \clearpage $^{(19)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(23)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(30)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(23)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(3)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(25)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^{(9)}$
}


\newpage

{\samepage \clearpage $^{(5)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(21)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(6)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(29)}$
}


\newpage

{\samepage \clearpage $^{(32)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(1)}$
}


\newpage

{\samepage \clearpage $^{(2)}$
}


\newpage

{\samepage \clearpage $^{(3)}$
}


\newpage

{\samepage \clearpage $^{(4)}$
}


\newpage

{\samepage \clearpage $^{(5)}$
}


\newpage

{\samepage \clearpage $^{(6)}$
}


\newpage

{\samepage \clearpage $^{(7)}$
}


\newpage

{\samepage \clearpage $^{(8)}$
}


\newpage

{\samepage \clearpage $^{(9)}$
}


\newpage

{\samepage \clearpage $^{(10)}$
}


\newpage

{\samepage \clearpage $^{(11)}$
}


\newpage

{\samepage \clearpage $^{(12)}$
}


\newpage

{\samepage \clearpage $^{(13)}$
}


\newpage

{\samepage \clearpage $^{(14)}$
}


\newpage

{\samepage \clearpage $^{(15)}$
}


\newpage

{\samepage \clearpage $^{(16)}$
}


\newpage

{\samepage \clearpage $^{(17)}$
}


\newpage

{\samepage \clearpage $^{(18)}$
}


\newpage

{\samepage \clearpage $^{(19)}$
}


\newpage

{\samepage \clearpage $^{(20)}$
}


\newpage

{\samepage \clearpage $^{(21)}$
}


\newpage

{\samepage \clearpage $^{(22)}$
}


\newpage

{\samepage \clearpage $^{(23)}$
}


\newpage

{\samepage \clearpage $^{(24)}$
}


\newpage

{\samepage \clearpage $^{(25)}$
}


\newpage

{\samepage \clearpage $^{(26)}$
}


\newpage

{\samepage \clearpage $^{(27)}$
}


\newpage

{\samepage \clearpage $^{(28)}$
}


\newpage

{\samepage \clearpage $^{(29)}$
}


\newpage

{\samepage \clearpage $^{(30)}$
}


\newpage

{\samepage \clearpage $^{(31)}$
}


\newpage

{\samepage \clearpage $^{(32)}$
}


\newpage

{\samepage \clearpage $^{(33)}$
}


\newpage

{\samepage \clearpage $^\dagger$
}


\newpage

{\samepage \clearpage $^{(a)}$
}


\newpage

{\samepage \clearpage $^{(b)}$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $\Z$
}


\newpage

{\samepage \clearpage \begin{eqnarray}% latex2html id marker 1678
\label{dspmdcst}
 \frac{1}{\mbox{$\sigma_{tot}$}}\frac{d\mbox{$\sigma_L$}}{d\mbox{$\cos\theta$}} & = & \mbox{$\frac{3}{16}$}
 {(1+\mbox{\rm A$_{\tau}$})[(1-\mbox{\rm A$_e$}\Pe)(1+\mbox{$\cos^{2}\theta$})+2(\mbox{\rm A$_e$}-\mbox{\it P$_e$})\cst],} \nonumber \\ 
 \frac{1}{\mbox{$\sigma_{tot}$}}\frac{d\mbox{$\sigma_R$}}{d\mbox{$\cos\theta$}} & = & \mbox{$\frac{3}{16}$}
 {(1-\mbox{\rm A$_{\tau}$})[(1-\mbox{\rm A$_e$}\Pe)(1+\mbox{$\cos^{2}\theta$})-2(\mbox{\rm A$_e$}-\mbox{\it P$_e$})\cst],}
 \end{eqnarray}
}


\newpage

{\samepage \clearpage % latex2html id marker 2476
$\theta$
}


\newpage

{\samepage \clearpage $\tm$
}


\newpage

{\samepage \clearpage $\tp$
}


\newpage

{\samepage \clearpage $\Pe$
}


\newpage

{\samepage \clearpage $\Ae$
}


\newpage

{\samepage \clearpage $\At$
}


\newpage

{\samepage \clearpage \begin{equation}\mbox{\rm A$_{\ell}$}=\frac{2\hat{{\sl g}}_v^{\ell}/\hat{{\sl g}}_a^{\ell}}{1+(\hat{{\sl g}}_v^{\ell}/\hat{{\sl g}}_a^{\ell})^2},
\end{equation}
}


\newpage

{\samepage \clearpage $\hat{{\sl g}}_v^{\ell}/\ga$
}


\newpage

{\samepage \clearpage \begin{equation}% latex2html id marker 1727
P_\tau(\mbox{$\cos\theta$},\mbox{\it P$_e$})=
\frac{\frac{d\mbox{$\sigma_R$}}{d\mbox{$\cos\theta$}}-\frac{d\mbox{$\sigma_L$}}{d\mbox{$\cos\theta$}} }{\frac{d\mbox{$\sigma_R$}}{d\mbox{$\cos\theta$}}
+ \frac{d\mbox{$\sigma_L$}}{d\mbox{$\cos\theta$}}}=
-\frac{ \mbox{\rm A$_{\tau}$} + 2 \frac{\mbox{\rm A$_e$} - \mbox{\it P$_e$}}{{\mbox 1} - \mbox{\rm A$_e$}\Pe} \frac{\mbox{$\cos\theta$}}
{ 1 + \cos^2\theta}}
{1 + 2 \mbox{\rm A$_{\tau}$} \frac{ \mbox{\rm A$_e$} - \mbox{\it P$_e$}}{{\mbox 1} - \mbox{\rm A$_e$} \mbox{\it P$_e$}}
 \frac{\mbox{$\cos\theta$}}{ 1 + \cos^2\theta}}.
\end{equation}
}


\newpage

{\samepage \clearpage $|\cst|$
}


\newpage

{\samepage \clearpage \begin{figure}% latex2html id marker 790
[htbp]
\label{jimsplot}
\epsfysize=10cm.
\epsffile[80 420 722 720 ]{ptau.eps}
\caption{Tau polarization vs  production angle
 with and without beam polarization.}
\end{figure}
}


\newpage

{\samepage \clearpage \begin{eqnarray}\frac{1}{\Gamma}\frac{d\Gamma_L}{dx} = f(x)+g(x),\nonumber \\ 
\frac{1}{\Gamma}\frac{d\Gamma_R}{dx} = f(x)-g(x).
\end{eqnarray}
}


\newpage

{\samepage \clearpage \begin{eqnarray}f(x) & = & 1,\nonumber \\ 
g(x) & = & \mbox{\rm h$_{\nu_{\tau}}$} \frac{2x-1-\mbox{$m_h^2$}/\mbox{$m_{\tau}^2$}}{1-\mbox{$m_h^2$}/\mbox{$m_{\tau}^2$}},
\end{eqnarray}
}


\newpage

{\samepage \clearpage $\mts$
}


\newpage

{\samepage \clearpage $\mhs$
}


\newpage

{\samepage \clearpage $x$
}


\newpage

{\samepage \clearpage $x=\frac{E_{\pi}}{E_{\mbox{$\tau$}}}$
}


\newpage

{\samepage \clearpage $\rho$
}


\newpage

{\samepage \clearpage $\tle$
}


\newpage

{\samepage \clearpage \begin{eqnarray}\label{fgleptons}
f(x)    &=& f_1+ \rho \cdot f_2,\nonumber \\ 
g(x)    &=& \xi (g_1+ \delta \cdot g_2),
\end{eqnarray}
}


\newpage

{\samepage \clearpage \begin{eqnarray}f_1  &=& 2-6x^2+4x^3 ,\nonumber \\ 
f_2  &=& \frac{4}{9}(-1+9x^2-8x^3),\nonumber \\ 
g_1  &=&-\frac{2}{3}+4x-6x^2+\frac{8}{3}x^3 ,\;\; {\mbox and}\\ 
g_2  &=& \frac{4}{9}(1-12x+27x^2-16x^3)].\nonumber
\end{eqnarray}
}


\newpage

{\samepage \clearpage $x=\frac{E_{\ell}}{E_{\mbox{$\tau$}}}$
}


\newpage

{\samepage \clearpage \begin{eqnarray}% latex2html id marker 1771
\label{fitfunction}
\frac{1}{\sigma}\frac{d^2\sigma(x,\mbox{$\cos\theta$},\mbox{\it P$_e$})}{dx d\mbox{$\cos\theta$}} = 
\frac{d\mbox{$\sigma_L$}}{d\mbox{$\cos\theta$}}\frac{1}{\Gamma}\frac{d\Gamma_L}{dx}+
\frac{d\mbox{$\sigma_R$}}{d\mbox{$\cos\theta$}}\frac{1}{\Gamma}\frac{d\Gamma_R}{dx}.
\end{eqnarray}
}


\newpage

{\samepage \clearpage \begin{equation}% latex2html id marker 1780
\frac{1}{\sigma}\frac{d^2\sigma(x,\mbox{$\cos\theta$},\mbox{\it P$_e$})}{dx d\mbox{$\cos\theta$}} =
f(x)-P_{\t}(\mbox{$\cos\theta$},\mbox{\it P$_e$})\cdot g(x),
\end{equation}
}


\stepcounter{section}
\newpage

{\samepage \clearpage $^{-1}$
}


\newpage

{\samepage \clearpage $^{-1}$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $15^\circ$
}


\newpage

{\samepage \clearpage $^2$
}


\newpage

{\samepage \clearpage $20^\circ$
}


\newpage

{\samepage \clearpage $\Theta_{\rm miss}$
}


\newpage

{\samepage \clearpage $|\cos\Theta_{\rm miss}| < 0.88$
}


\newpage

{\samepage \clearpage $E_{\rm CM}$
}


\newpage

{\samepage \clearpage $0.45\ E_{\rm CM}$
}


\newpage

{\samepage \clearpage $0.33\ E_{\rm CM}$
}


\newpage

{\samepage \clearpage $Z^0$
}


\newpage

{\samepage \clearpage $Z^0\rightarrow hadrons$
}


\newpage

{\samepage \clearpage \begin{figure}% latex2html id marker 865
[htbp]
\label{fig-eff}
\epsfysize=18cm.
\epsffile[50 150 600 650 ]{eff_bg.eps}
\caption{The MC estimated selection efficiency and background 
fractions versus scaled
energy for tau decays to pions (a,b), muons (c,d), and electrons (e,f).}
\end{figure}
}


\newpage

{\samepage \clearpage $10^o$
}


\newpage

{\samepage \clearpage $a_1$
}


\newpage

{\samepage \clearpage $E_{EM}/p < 0.3$
}


\newpage

{\samepage \clearpage % latex2html id marker 2658
$|cos\theta|<0.62$
}


\newpage

{\samepage \clearpage % latex2html id marker 2660
$0.62<|cos\theta|<0.74$
}


\newpage

{\samepage \clearpage $|\cst| < 0.62$
}


\newpage

{\samepage \clearpage $0.62 < |\cst| < 0.74$
}


\newpage

{\samepage \clearpage $|\cst| < 0.74$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $\cst$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$},\cst$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} > 0$
}


\newpage

{\samepage \clearpage % latex2html id marker 2694
$\mbox{$\cos\theta$} < 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} < 0$
}


\newpage

{\samepage \clearpage % latex2html id marker 2698
$\mbox{$\cos\theta$}>0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} > 0$
}


\newpage

{\samepage \clearpage % latex2html id marker 2702
$\mbox{$\cos\theta$}>0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} < 0$
}


\newpage

{\samepage \clearpage % latex2html id marker 2706
$\mbox{$\cos\theta$} < 0$
}


\newpage

{\samepage \clearpage $\xi\delta$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} < 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} > 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} < 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} > 0$
}


\newpage

{\samepage \clearpage \begin{figure}% latex2html id marker 875
[hbp]
\label{fig-pispect}
\epsfysize=17cm.
\epsffile[ 100 170 400 570]{lepphoton_pi.eps}
\caption{$\tpiK$ decay energy spectra: (a) The sum of the
spectra for pions in the forward direction with beam polarization
$\mbox{\it P$_e$} < 0$ and in the backward direction with $\mbox{\it P$_e$} > 0$;
(b) The sum of the spectra for pions in the backward direction with
$\mbox{\it P$_e$} < 0$ and in the forward direction with $\mbox{\it P$_e$} > 0$.  In each case
the points are data and the histogram is from Monte Carlo.}
\end{figure}
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} < 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} > 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} < 0$
}


\newpage

{\samepage \clearpage $\mbox{\it P$_e$} > 0$
}


\newpage

{\samepage \clearpage \begin{figure}% latex2html id marker 880
[hbp]
\label{fig-leptspect}
\epsfysize=17cm.
\epsffile[ 100 170 400  570 ]{lepphoton_lep.eps}
 
\caption{$\tle$ decay energy spectra from
(a) Monte Carlo, and   (b) the SLD data.    For both histograms, the
solid line is the sum of the
spectra for leptons in the forward direction with beam polarization
$\mbox{\it P$_e$} < 0$ and in the backward direction with $\mbox{\it P$_e$} > 0$, and the
dashed line is the sum of the spectra for leptons in the backward direction
with $\mbox{\it P$_e$} < 0$ and in the forward direction with $\mbox{\it P$_e$} > 0$.}
\end{figure}
}


\newpage

{\samepage \clearpage \begin{equation}% latex2html id marker 1805
\label{ML}
W=-2\ln{\cal L}=-2\sum_{n=1}^N \ln \left\{ \frac{1}{\mbox{$\spr_i$}}
\frac{d^2\mbox{$\spr_i$}}{d\mbox{$\cos\theta$}\:d\mbox{$x_i$}} \right\}_n,
\end{equation}
}


\newpage

{\samepage \clearpage ${\cal L}$
}


\newpage

{\samepage \clearpage $i=1-3$
}


\newpage

{\samepage \clearpage $i$
}


\newpage

{\samepage \clearpage \begin{eqnarray}% latex2html id marker 1811
\label{corcso}
\frac{16}{3}\frac{1}{\mbox{$\spr_i$}}\frac{d^2\mbox{$\spr_i$}}{d\mbox{$\cos\theta$} \:d\mbox{$x_i$}  } & = & \sum_{hel=\pm}\{
\mbox{${\cal E}^{\pm}_{i}(\mbox{$x_i$},\mbox{$\cos\theta$} )$} {\cal U}^{\pm}(\mbox{$\cos\theta$}) \nonumber \\ 
&  \times &[\mbox{$\epsilon_{i}(\mbox{$x_i$},\mbox{$\cos\theta$} )$}{\cal V}^{\pm}_i(\mbox{$x_i$})+\beti] \}  \\ 
 & + & \mbox{$\beta^{non-\tau}_{i}(\mbox{$x_i$},\mbox{$\cos\theta$} )$}.\nonumber
\end{eqnarray}
}


\newpage

{\samepage \clearpage $\epsti$
}


\newpage

{\samepage \clearpage $\mu$
}


\newpage

{\samepage \clearpage $\pi$
}


\newpage

{\samepage \clearpage $\epsdi$
}


\newpage

{\samepage \clearpage $\beti$
}


\newpage

{\samepage \clearpage $\bnti$
}


\newpage

{\samepage \clearpage ${\cal V}^{\pm}_i(\mbox{$x_i$})$
}


\newpage

{\samepage \clearpage $V^{\pm}_i(\bar{\mbox{$x_i$}})$
}


\newpage

{\samepage \clearpage \begin{eqnarray}\label{vxd}
{\cal V}^{\pm}_i(\mbox{$x_i$}) & =& \int_0^1 V^{\pm}(\bar{\mbox{$x_i$}})\mbox{$r^{\pm}_i(\bar{\mbox{$x_i$}})$}\rxx
d\bar{\mbox{$x_i$}},
\nonumber \\ 
V^{\pm}_i(\bar{\mbox{$x_i$}})& = & \mbox{$f_i$}(\bar{\mbox{$x_i$}})\pm\mbox{$g_i$}(\bar{\mbox{$x_i$}}).
\end{eqnarray}
}


\newpage

{\samepage \clearpage % latex2html id marker 2830
${\cal U}^{\pm}(\mbox{$\cos\theta$})$
}


\newpage

{\samepage \clearpage $U^{\pm}(\bar{\mbox{$x_i$}})$
}


\newpage

{\samepage \clearpage \begin{eqnarray}% latex2html id marker 1854
\label{uxd}
{\cal U}^{\pm}(\mbox{$\cos\theta$}) & = & \int_{-1}^1 U^{\pm}(\cos\bar{\theta})\mbox{$\hat{r}^{\pm}_i(\cos\bar{\theta})$}
\mbox{${\cal C}_i(\cos\bar{\theta},\mbox{$\cos\theta$})$} d\cos\bar{\theta},\\ 
U^{\pm}(\cos\bar{\theta})& = & (1 - \mbox{\it P$_e$} \mbox{\rm A$_e$})(1 \pm \mbox{\rm A$_{\tau}$})(1+\cos\bar{
\theta}^2) + 2(\mbox{\rm A$_e$} - \mbox{\it P$_e$})
(\mbox{\rm A$_{\tau}$} \pm 1) \cos\bar{\theta}.\nonumber
\end{eqnarray}
}


\newpage

{\samepage \clearpage $\rxx$
}


\newpage

{\samepage \clearpage $\rcc$
}


\newpage

{\samepage \clearpage $\xxi$
}


\newpage

{\samepage \clearpage $\bar{\mbox{$x_i$}}$
}


\newpage

{\samepage \clearpage % latex2html id marker 2864
$\cos\bar{\theta}$
}


\newpage

{\samepage \clearpage $\ri$
}


\newpage

{\samepage \clearpage $\ric$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $\mbox{\rm h$_{\nu_{\tau}}$}=-0.89\pm0.21(stat)$
}


\newpage

{\samepage \clearpage $\xi=1.17 \pm 0.35 (stat)$
}


\newpage

{\samepage \clearpage $\xi\delta= 0.49 \pm 0.24 (stat)$
}


\newpage

{\samepage \clearpage $\Al$
}


\newpage

{\samepage \clearpage \begin{table}% latex2html id marker 943
[htb]
\begin{center}
\begin{tabular}{lccccccc} \hline\hline
       & && $\Delta h_\nu$ & && $\Delta\xi$ & $\Delta(\xi\delta)$ \\  \hline
  $\tau$ selection      & && 0.01 && & 0.03 & 0.05 \\ 
  Final-state selection & && 0.05 && & 0.02 & 0.01 \\ 
  $\tau$ background     & && 0.01 && & 0.03 & 0.02 \\ 
  Non-$\tau$ background & && 0.01 && & 0.03 & 0.04 \\ 
  Radiative corrections & && 0.02 && & 0.10 & 0.02 \\ 
$\cos\theta$ resolution & && 0.01 && & 0.05 & 0.02 \\ 
  $x$ resolution        & && 0.01 && & 0.07 & 0.06 \\ 
  Beam energy           & && 0.02 && & 0.04 & 0.05 \\ 
  Beam polarization     & && 0.01 && & 0.02 & 0.01 \\ 
  $A_e$, $A_\tau$       & && 0.01 && & 0.03 & 0.02 \\ 
  $\rho$ fixed          & &&      && & 0.14 & 0.07 \\  \hline
  TOTAL                 & && 0.07 && & 0.21 & 0.13 \\  \hline\hline
 
\end{tabular}
\caption[y]{Systematic uncertainties.}
\label{systab}
\end{center}
\end{table}
}


\newpage

{\samepage \clearpage $\pi^{\pm} $
}


\newpage

{\samepage \clearpage $\pi^0$
}


\newpage

{\samepage \clearpage \begin{eqnarray*}h_\nu & = & -0.89 \pm 0.21 (stat)\pm 0.07 (syst), \\ 
     \ \\ 
             \xi   & = &\ \ \ 1.17 \pm 0.35 (stat)\pm  0.21 (syst),
\;\;{\mbox and} \\ 
     \ \\ 
      \xi\delta & = &\ \ \ 0.49 \pm 0.24 (stat)\pm 0.13
 (syst).
\end{eqnarray*}
}


\newpage

{\samepage \clearpage $3 \over 4$
}


\newpage

{\samepage \clearpage ${\cal O}(\alpha)$
}


\newpage

{\samepage \clearpage $\mbox{\rm A$_{\tau}$}=0.1418 \pm 0.0075$
}


\newpage

{\samepage \clearpage $\mbox{\rm A$_{\ell}$}=0.1464 \pm 0.0039$
}


\newpage

{\samepage \clearpage $\mbox{\rm A$_e$}=0.1551 \pm 0.0040$
}


\newpage

{\samepage \clearpage $A_{LR}$
}


\newpage

{\samepage \clearpage $\mbox{\rm A$_{\ell}$}=0.15075 \pm 0.0028$
}


\newpage

{\samepage \clearpage $\pi^-\pi^+$
}



\end{document}