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CONVENTIONS:
%-------------------------------------------------------------------
\documentstyle[epsfig,english,rotating,11pt,a4wide]{article}
\renewcommand{\Huge}{\huge}
\parskip12pt plus 1pt minus 1pt
\topsep0pt plus 1pt
\floatsep0pt plus 1pt
\setcounter{topnumber}{6}
\setcounter{bottomnumber}{6}
\setcounter{totalnumber}{6}
\renewcommand{\topfraction}{1}
\renewcommand{\bottomfraction}{1}
\renewcommand{\textfraction}{0}
\renewcommand{\floatpagefraction}{1}
%%%%%%%%%%%%%%%%
% Declarations %
%%%%%%%%%%%%%%%%
\newcommand {\GeV} {\rm{GeV}}
\newcommand {\MeV} {\rm{MeV}}
\newcommand {\nb} {\rm{nb}}
\newcommand {\Afbpol} {\rm{A}\!^{0,\,\ell}_{\rm {FB}}}
\newcommand {\Afbze} {\rm{A}\!^{0,\,{\rm e}}_{\rm {FB}}}
\newcommand {\Afbzf} {\rm{A}\!^{0,\,{\rm f}}_{\rm {FB}}}
\newcommand {\Afbzm} {\rm{A}\!^{0,\,\mu}_{\rm {FB}}}
\newcommand {\Afbzt} {\rm{A}\!^{0,\,\tau}_{\rm {FB}}}
\newcommand {\Afbzb} {\rm{A}\!^{0,\,{\rm b}}_{\rm {FB}}}
\newcommand {\Afbzc} {\rm{A}\!^{0,\,{\rm c}}_{\rm {FB}}}
\newcommand {\sigmaf} {\sigma_F}
\newcommand {\sigmab} {\sigma_B}
%\newcommand {\shad} {\sigma_{\rm h}^o}
%------------------------------------------------------------------
\renewcommand {\rm} {\mathrm}
\renewcommand{\thefootnote}{\fnsymbol{footnote}}
\newcommand {\nn} {\noindent}
\newcommand {\mc} {\multicolumn {2} {|c|}}
\newcommand {\mco} {\multicolumn {1} {|c|}}
\newcommand {\mccl} {\multicolumn {2} {|l|}}
\newcommand {\mcl} {\multicolumn {1} {|c||}}
\newcommand {\mcf} {\multicolumn {5} {|c|}}
\newcommand {\mcn} {\multicolumn {9} {|c|}}
\newcommand {\alfas} {\alpha_s}
\newcommand {\alfmz} {\alfas(\MZ^2)}
\newcommand {\cms} {\mbox{centre-of-mass}}
\newcommand {\xmu} {x_{\mu}}
\newcommand {\ord} {\cal O}
\newcommand {\fZg} {f^{\gamma{\rm Z}}}
\newcommand {\Lum} {\cal{L}}
%%%
\newcommand {\Zzero} {\mathrm{Z}^0}
\newcommand {\Zpole} {\mbox{Z$^0$-pole}}
\newcommand {\SM} {\mbox{Standard Model}}
\newcommand {\MZ} {M_{\mathrm{Z}}}
\newcommand {\MW} {M_{\mathrm{W}}}
\newcommand {\GF} {G_{\mathrm{F}}}
\newcommand {\Gm} {G_{\mu}}
\newcommand {\MH} {M_{\mathrm{H }}}
\newcommand {\Mt} {M_{\mathrm{t}}}
\newcommand {\Mnu} {M_{\nu}}
\newcommand {\Msnu} {M_{\tilde{\nu}}}
\newcommand {\Mmajo} {M_{\nu}(\mathrm{Majorana})}
\newcommand {\GZ} {\Gamma_{\mathrm{Z}}}
\newcommand {\Afb} {A_{\mathrm{FB}}}
\newcommand {\NF} {N_{\mathrm{F}}}
\newcommand {\NB} {N_{\mathrm{B}}}
\newcommand {\Nnu} {N_\nu}
\newcommand {\RZ} {R_{\ell}}
\newcommand {\Ree} {R_{\mathrm{e}}}
\newcommand {\Rmu} {R_{\mu}}
\newcommand {\Rtau} {R_{\tau}}
\newcommand {\Rl} {R_{\ell}}
\newcommand {\rhoZ} {\rho_{\mathrm{Z}}}
\newcommand {\thw} {\theta_{\mathrm{W}}}
\newcommand {\thweff} {\theta_{\mathrm{W}}^{eff}}
\newcommand {\thwefff} {\theta_{\mathrm{W}}^{eff,\,{\rm f}}}
\newcommand {\thweffb} {\theta_{\mathrm{W}}^{eff,\,{\rm b}}}
\newcommand {\thweffl} {\theta_{\mathrm{W}}^{eff,\,\ell}}
\newcommand {\swsq} {1-\MW^2/\MZ^2}
\newcommand {\swsqeff} {\sin^2\!\thweff}
\newcommand {\swsqefff} {\sin^2\!\thwefff}
\newcommand {\swsqeffl} {\sin^2\!\theta_{eff}^{\rm {lept}}}
\newcommand {\swsqeffb} {\sin^2\!\thweffb}
\newcommand {\cwsq} {\cos^2\!\thw}
\newcommand {\swsqb} {\sin^2\!\overline{\theta}_{\mathrm{W}}}
\newcommand {\swsqbIBA} {\swsqb^{\mathrm{IBA}}}
\newcommand {\swsqbSM} {\swsqb^{\mathrm{SM}}}
\newcommand {\ff} {{\rm f}\overline{\rm f}}
\newcommand {\lept} {\ell^+\ell^-}
\newcommand {\ee} {\mathrm{e}^+\mathrm{e}^-}
\newcommand {\eeX} {\ee X}
\newcommand {\gaga} {\gamma\gamma}
\newcommand {\mumu} {\mu^+\mu^-}
\newcommand {\eeg} {\ee\gamma}
\newcommand {\mumug} {\mu^+\mu^-\gamma}
\newcommand {\tautau} {\tau^+\tau^-}
\newcommand {\eeff} {\ee\rightarrow\ff}
\newcommand {\eecc} {\ee\rightarrow\cc}
\newcommand {\eebb} {\ee\rightarrow\bb}
\newcommand {\eegg} {\ee\rightarrow \gamma\gamma}
\newcommand {\eeggg} {\ee\rightarrow \gamma\gamma\gamma}
\newcommand {\eeee} {\ee\rightarrow\ee}
\newcommand {\eeeeee} {\ee\rightarrow \ee\ee}
\newcommand {\eeeeg} {\ee\rightarrow \ee(\gamma)}
\newcommand {\eeeegg} {\ee\rightarrow \ee\gamma\gamma}
\newcommand {\eeeg} {\ee\rightarrow \mathrm{e(e)}\gamma}
\newcommand {\eemumu} {\ee\rightarrow \mu^+\mu^-}
\newcommand {\eetautau} {\ee\rightarrow \tau^+\tau^-}
\newcommand {\eehad} {\ee\rightarrow\mathrm{hadrons}}
\newcommand {\eeqq} {\ee\rightarrow {\rm q}\overline{\rm q}}
\newcommand {\eettg} {\ee\rightarrow \tau^+\tau^-\gamma}
\newcommand {\eell} {\ee\rightarrow \lept}
\newcommand {\Ztoqq} {\mathrm{Z}^0\rightarrow q\overline{q}}
\newcommand {\Ztoee} {\mathrm{Z}^0\rightarrow \ee}
\newcommand {\Ztomumu} {\mathrm{Z}^0\rightarrow \mu^+\mu^-}
\newcommand {\Ztotautau} {\mathrm{Z}^0\rightarrow \tau^+\tau^-}
\newcommand {\Ztoll} {\mathrm{Z}^0\rightarrow \lept}
\newcommand {\Nf} {\mbox{N$_{_{\mathrm{F}}}$}}
\newcommand {\Nb} {\mbox{N$_{_{\mathrm{B}}}$}}
\newcommand {\Gee} {\Gamma_{\rm {ee}}}
\newcommand {\Gpig} {\Gamma_{\pi^0\gamma}}
\newcommand {\Ggg} {\Gamma_{\gamma\gamma}}
\newcommand {\Gggg} {\Gamma_{\gamma\gamma\gamma}}
\newcommand {\Gmumu} {\Gamma_{\mu\mu}}
\newcommand {\Gtautau} {\Gamma_{\tau\tau}}
\newcommand {\Ginv} {\Gamma_{\mathrm{inv}}}
\newcommand {\Ghad} {\Gamma_{\mathrm{had}}}
\newcommand {\Gnu} {\Gamma_{\nu\nu}}
\newcommand {\GnuSM} {\Gnu^{\mathrm{SM}}}
\newcommand {\Gll} {\Gamma_{\ell\ell}}
\newcommand {\Gff} {\Gamma_{\mathrm{f}\overline{\mathrm{f}}}}
\newcommand {\Gqq} {\Gamma_{\mathrm{q}\overline{\mathrm{q}}}}
\newcommand {\Gtot} {\Gamma_{\mathrm{tot}}}
\newcommand {\Cagz} {C^{a}_{\gamma \mathrm{Z}}}
\newcommand {\Csgz} {C^{s}_{\gamma \mathrm{Z}}}
\newcommand {\Cazz} {C^{a}_{\mathrm{ZZ}}}
\newcommand {\Cszz} {C^{s}_{\mathrm{ZZ}}}
\newcommand {\Kagz} {\kappa^{a}_{\gamma \mathrm{Z}}}
\newcommand {\Ksgz} {\kappa^{s}_{\gamma \mathrm{Z}}}
\newcommand {\Kazz} {\kappa^{a}_{\mathrm{ZZ}}}
\newcommand {\Kszz} {\kappa^{s}_{\mathrm{ZZ}}}
\newcommand {\roots} {\sqrt{s}}
\newcommand {\pT} {p_{\mathrm{T}}}
\newcommand {\up} {^}
\newcommand {\abscosthe} {|\cos\theta|}
\newcommand {\costh} {\cos\theta}
\newcommand {\dsum} {\Sigma |d_\circ|}
\newcommand {\zsum} {\Sigma z_\circ}
\newcommand {\sint} {\mbox{$\sin\theta}}
\newcommand {\cost} {\mbox{$\cos\theta$}}
\newcommand {\mcost} {\mbox{$|\cos\theta|$}}
\newcommand {\epair} {\mbox{$e^{+}e^{-}$}}
\newcommand {\mupair} {\mbox{$\mu^{+}\mu^{-}$}}
\newcommand {\taupair} {\mbox{$\tau^{+}\tau^{-}$}}
\newcommand {\pf} {\mbox{$\cal P_{\rm f}$}}
\newcommand {\cosstar} {\mbox{$\cos\theta^*$}}
\newcommand {\ptau} {\mbox{$\cal P_{\tau}$}}
\newcommand {\ALR} {\mbox{$A_{\rm {LR}}$}}
\newcommand {\AFBpf} {\mbox{$A_{\rm {FB}}^{\cal P_{\rm f}}$}}
\newcommand {\AFBtau} {\mbox{$A_{\rm {FB}}^{\cal P_{\tau}}$}}
\newcommand {\AFBpol} {\mbox{$A_{\rm {FB}}^{\rm {pol}}$}}
\newcommand {\cAe} {\mbox{$\cal A_{\rm e}$}}
\newcommand {\cAt} {\mbox{$\cal A_{\tau}$}}
\newcommand {\cAf} {\mbox{$\cal A_{\rm f}$}}
\newcommand {\cAq} {\mbox{$\cal A_{\rm q}$}}
\newcommand {\cAl} {\mbox{$\cal A_{\ell}$}}
\newcommand {\cAb} {\mbox{$\cal A_{\rm b}$}}
\newcommand {\cAtau} {\mbox{$\cal A_{\tau}$}}
\newcommand {\Gbb} {\Gamma_{{\rm b}\overline {\rm b}}}
\newcommand {\Gcc} {\Gamma_{{\rm c}\overline {\rm c}}}
\newcommand {\Gdd} {\Gamma_{{\rm d}\overline {\rm d}}}
\newcommand {\Guu} {\Gamma_{{\rm u}\overline {\rm u}}}
\newcommand {\Gss} {\Gamma_{{\rm s}\overline {\rm s}}}
\newcommand {\blX} {\rm b \rightarrow \ell X}
\newcommand {\BrblX} {Br(\blX)}
\newcommand {\chiB} {\chi_{\rm B}}
\newcommand {\All} {\mbox{$A_{\mathrm{FB}}^{\ell\ell}$}}
\newcommand {\Aff} {\mbox{$A_{\mathrm{FB}}^{{\rm f}\overline{\rm f}}$}}
\newcommand {\A} {\mbox{$A_{\mathrm{FB}}$}}
\newcommand {\qq} {\mathrm{q}\overline{\mathrm{q}}}
\newcommand {\pp} {\mbox{$\mathrm{p}\overline{\mathrm{p}}$}}
\newcommand {\gal} {g_l^a}
\newcommand {\gvl} {g_l^v}
\newcommand {\gae} {g_e^a}
\newcommand {\gve} {g_e^v}
\newcommand {\gamu} {g_\mu^a}
\newcommand {\gvmu} {g_\mu^v}
\newcommand {\gatau} {g_\tau^a}
\newcommand {\gvtau} {g_\tau^v}
\newcommand {\gavsq} {(\gal)^2(\gvl)^2}
\newcommand {\gahat} {\left.\hat{g}_a\right.}
\newcommand {\gvhat} {\left.\hat{g}_v\right.}
\newcommand {\gaf} {\left.{g}^{\mathrm{f}}_a\right.}
\newcommand {\gvf} {\left.{g}^{\mathrm{f}}_v\right.}
\newcommand {\Itf} {I^3_{\rm f}}
\newcommand {\Qf} {Q_{\rm f}}
\newcommand {\Qq} {Q_{\rm q}}
\newcommand {\Qb} {Q_{\rm b}}
\newcommand {\rhof} {\rho_{\rm f}}
\newcommand {\so} {s_0^2}
\newcommand {\co} {c_0^2}
\newcommand {\gahate} {g_{{A}_{\rm e}}}
\newcommand {\gvhate} {g_{{V}_{\rm e}}}
\newcommand {\gahatf} {g_{{A}_{\rm f}}}
\newcommand {\gvhatf} {g_{{V}_{\rm f}}}
\newcommand {\gahatmu} {g_{{A}_{\mu}}}
\newcommand {\gvhatmu} {g_{{V}_{\mu}}}
\newcommand {\gahattau} {g_{{A}_{\tau}}}
\newcommand {\gvhattau} {g_{{V}_{\tau}}}
\newcommand {\gahatl} {g_{{A}_{\ell}}}
\newcommand {\gvhatl} {g_{{V}_{\ell}}}
%
\newcommand {\HI} {\mbox{$60 \le \MH~[{\rm {GeV}}] \le 1000$}}
\newcommand {\tI} {\mbox{$90 \le \Mt~[{\rm {GeV}}] \le 200$}}
\newcommand {\Nqqg} {N_{\qq\gamma}}
\newcommand {\Fqqg} {\cal{F}_{\qq\gamma}}
\def\avQfb{{\langle \mbox{\rm Q}_{\mbox{\rm FB}} \rangle}}
%------------------------------------------------------------------
\def\lt{\raisebox{0.2ex}{$<$}}
\def\gt{\raisebox{0.2ex}{$>$}}
\def\avthe{$\overline{\theta}$}
\def\avphi{$\overline{\phi}$}
\def\main{$\overline{\rm MAIN}$}
\def\delphi{${\mit\Delta}\phi$}
\newcommand{\fullskip}{\vskip 16cm}
\newcommand{\halfskip}{\vskip 8cm}
\newcommand{\quarskip}{\vskip 6cm}
\newcommand{\abitskip}{\vskip 0.5cm}
\def\stat{\rm{stat}}
\def\syst{\rm{syst}}
%------------------------------------------------------------------------------
%