 
\documentclass[11pt,twoside]{report}
\usepackage{fancyheadings}
\usepackage{german}
\usepackage{epsfig}
\usepackage{here}
\usepackage{amsmath}
\usepackage{amssymb}
\usepackage{wrapfig} 
\usepackage{psfrag} 
\usepackage{epigraph} 
\usepackage{rotating} 
\usepackage[latin1]{inputenc}
%
%\pagestyle{headings}

% change headerstyle

% JB's header
%\fancyhf{}
%\headheight=15pt
%\renewcommand{\chaptermark}[1]
%                      {\markboth{#1}{}}
%\renewcommand{\sectionmark}[1]%
%              {\markright{\thesection\ #1}}
%\lhead[\fancyplain{}{\bfseries\thepage}]%
%                        {\fancyplain{}{\bfseries\rightmark}}
%\rhead[\fancyplain{}{\bfseries\leftmark}]%
%                        {\fancyplain{}{\bfseries\thepage}}
% end of headerstyle definition

\pagestyle{plain}
\textwidth 14cm
\textheight 27.0cm
 
\oddsidemargin   -1.5cm
\topmargin     -3.0cm
%%\setlength{\textheight}{23.0cm}
%%\setlength{\topmargin}{-0.5cm}
%%\setlength{\textwidth}{15.5cm}
%%\setlength{\oddsidemargin}{0.4cm}
%%\setlength{\evensidemargin}{0.4cm}
\pagestyle{fancyplain}
%\fancypagestyle{headings}
%\setlength{\plainheadrulewidth}{15.5cm}

%
% Macro definitions,
% field

%
% Teilchen-stuff

\def\qf{q_{\mbox{\scriptsize f}}}
%\newcommand{\Log}{\mbox{$ \log{\cal L}$}}
\newcommand{\CL}{\mbox{${\mathrm C}{\mathrm L}$}}
\newcommand{\Log}{\mbox{$ -\Delta \log  {\mathrm L}$}}
\newcommand{\OO}{\mbox{${\cal OO}$}}
\newcommand{\gz}{\mbox{$  g_1^Z$}}
%\newcommand{\Dgz}{\mbox{$\Delta {\mathrm g}_1^Z$}}
\newcommand{\Dgz}{\mbox{$\Delta  g_1^Z$}}
\newcommand{\kg}{\mbox{$\kappa_\gamma$}}
\newcommand{\Dkg}{\mbox{$\Delta\kappa_\gamma$}}
\newcommand{\kz}{\mbox{$\kappa_Z$}}
\newcommand{\Dkz}{\mbox{$\Delta \kappa_Z$}}
\newcommand{\lm}{\mbox{$\lambda_\gamma$}}
\newcommand{\lz}{\mbox{$\lambda_Z$}}
\newcommand{\xg}{\mbox{$x_\gamma$}}
\newcommand{\xz}{\mbox{$x_Z$}}
\newcommand{\ga}       {\mbox{$g_{{\mathrm A}{\mathrm l} }$}}
\newcommand{\gv}       {\mbox{$g_{{\mathrm V}{\mathrm l} }$}}
\newcommand{\swq}       {\mbox{$\sin^2 \theta_{\mathrm{W}}$}}
\newcommand{\sww}       {\mbox{$ \sigma_{{\mathrm W}{\mathrm W}}$}}
\newcommand{\U}       {\mbox{$ {\mathrm U}(1)_Y$}}
\newcommand{\Uem}       {\mbox{$ {\mathrm U}(1)_Q$}}
\newcommand{\SU}       {\mbox{$ {\mathrm S}{\mathrm U}(2)_L$}}
\newcommand{\TGV}       {Drei-Eichbosonen-Vertex}
\newcommand{\SUU}       {\mbox{$ \SU  \times \U $}}
\newcommand{\gmu}       {\mbox{$ {\mathrm G}_{\mu}$}}
\newcommand{\mw}       {\mbox{$ {\mathrm M}_{\mathrm W}$}}
\newcommand{\mz}       {\mbox{$ {\mathrm M}_{\mathrm Z}$}}
\newcommand{\mws}       {\mbox{$ {\mathrm M}_{\mathrm W}^2$}}
\newcommand{\mzs}       {\mbox{$ {\mathrm M}_{\mathrm Z}^2$}}
\newcommand{\mh}       {\mbox{$ {\mathrm M}_{\mathrm H}$}}
\newcommand{\mt}       {\mbox{$ {\mathrm M}_{\mathrm t}$}}
\newcommand{\W}        {\mbox{$ {\mathrm W}$}}
\newcommand{\Z}       {\mbox{$ {\mathrm Z}$}}
\newcommand{\Wp}       {\mbox{$ {\mathrm W}^+ $}}
\newcommand{\Wm}       {\mbox{$ {\mathrm W}^- $}}
\newcommand{\wpm}      {\mbox{$ {\mathrm W}^{\pm} $}}
\newcommand{\photon}   {\mbox{$ \gamma$}}
\newcommand{\A}        {\mbox{$ {\mathrm A}$}}
\newcommand{\ee}       {\mbox{$ {\mathrm e}^+ {\mathrm e}^-$}}
\newcommand{\ww}       {\mbox{$ {\mathrm W}^+ {\mathrm W}^-$}}
\newcommand{\zz}       {\mbox{$ {\mathrm Z} {\mathrm Z}$}}
\newcommand{\wz}       {\mbox{$ \z \w$}}
\newcommand{\wwz}      {\mbox{WWZ}}
\newcommand{\wwv}      {\mbox{WWV}}
\newcommand{\wwgamma}  {\mbox{$ {\mathrm W}{\mathrm W} \gamma $}}
\newcommand{\eeff}     {\mbox{$ \ee \rightarrow {\mathrm f} \bar{{\mathrm f}}$}}
\newcommand{\eezgammaff}     {\mbox{$ \ee \rightarrow \z /\photon \rightarrow
    {\mathrm f} \bar{{\mathrm f}}$}}
\newcommand{\eezll}     {\mbox{$ \ee \rightarrow \Z \rightarrow
    {\mathrm l} \bar{{\mathrm l}}$}}
\newcommand{\eeffff}   {\mbox{$ \ee \rightarrow {\mathrm f}_1 \bar{{\mathrm
        f}}_2 {\mathrm f}_3 \bar{{\mathrm f}}_4 $}}
\newcommand{\eewwffff} {\mbox{$ \ee \rightarrow \ww \rightarrow {\mathrm f}_1
    \bar{{\mathrm f}}_2 {\mathrm f}_3 \bar{{\mathrm f}}_4 $}}
\newcommand{\eeww}     {\mbox{$ \ee \rightarrow \ww$}}
\newcommand{\lvlv}     {\mbox{$ \ell \nu \ell \nu$}}
\newcommand{\lvqq}     {\mbox{$ \ell \nu q \bar{q}$}}
\newcommand{\lsvqq}     {\mbox{$ \ell_{s} \nu q \bar{q}$}}
\newcommand{\evqq}     {\mbox{$ e \nu q \bar{q}$}}
\newcommand{\muvqq}     {\mbox{$ \mu \nu q \bar{q}$}}
\newcommand{\lvjj}     {\mbox{$ \ell \nu j j$}}
\newcommand{\lsvjj}     {\mbox{$ \ell_{s} \nu j j$}}
\newcommand{\evjj}     {\mbox{$ e\nu jj$}}
\newcommand{\muvjj}     {\mbox{$ \mu\nu jj$}}
\newcommand{\tauvjj}     {\mbox{$ \tau\nu jj$}}
\newcommand{\evev}     {\mbox{$ e\nu e\nu $}}
\newcommand{\evmuv}     {\mbox{$ e\nu \mu\nu $}}
\newcommand{\evtauv}     {\mbox{$ e\nu \tau\nu $}}
\newcommand{\muvmuv}     {\mbox{$ \mu\nu \mu\nu $}}
\newcommand{\muvtauv}     {\mbox{$ \mu\nu \tau\nu $}}
\newcommand{\tauvtauv}     {\mbox{$ \tau\nu \tau\nu $}}
\newcommand{\eeee}     {\mbox{$ \ee\ee$}}
\newcommand{\evud}     {\mbox{$ {\mathrm e}^- \bar{\nu}_e {\mathrm u}
    \bar{{\mathrm d}}$}}
\newcommand{\qqqq}     {\mbox{$ q q q q$}}
\newcommand{\jjjj}     {\mbox{$ j j j j$}}
\newcommand{\ppbar}    {\mbox{$ {\mathrm p} \bar{{\mathrm p}} $}}
\newcommand{\pantip}   {\mbox{$ {\mathrm p} \bar{{\mathrm p}} $}}
\newcommand{\gev}      {\mbox{GeV}}
\newcommand{\gevp}      {\mbox{$\mbox{GeV}/\mathrm{c}$ }}
\newcommand{\mev}      {\mbox{MeV}}
\newcommand{\tev}      {\mbox{TeV}}
\newcommand{\nb}       {\mbox{nb}}
\newcommand{\nbinv}    {\mbox{nb$^{-1}$}}
\newcommand{\pb}       {\mbox{pb}}
\newcommand{\pbinv}    {\mbox{pb$^{-1}$}}
\newcommand{\pantiptowgamma}      {\mbox{$ \pantip\rightarrow\w\gamma $}}
\newcommand{\lv}       {\mbox{$ \ell \nu$}}
\newcommand{\qqbar}    {\mbox{$ q \bar{q}$}}
\newcommand{\vt}       {\vartheta}
\newcommand{\lmg}{\lambda_\gamma}
\newcommand{\pvl}{{\vec p}_l}
\newcommand{\pvlb}{{\vec p}_{\bar{l}}}
\newcommand{\pvn}{{\vec p}_{\nu}}
\newcommand{\pvnb}{{\vec p}_{\bar{\nu}}}
\newcommand{\gti}{\tilde{g}_i}
\newcommand{\gtj}{\tilde{g}_j}
\newcommand{\gai}{\gamma_i}
\newcommand{\sz}{{S}_0(\Omega)}
\newcommand{\sone}{{S}_{1,i}(\Omega)}
\newcommand{\stwo}{{S}_{2,ij}(\Omega)}
\newcommand{\stz}{\tilde{S}_0(\Omega)}
\newcommand{\stone}{\tilde{S}_{1,i}(\Omega)}
\newcommand{\sttwo}{\tilde{S}_{2,ij}(\Omega)}
\newcommand{\sstz}{\tilde{S}_0}
\newcommand{\sstone}{\tilde{S}_{1,i}}
\newcommand{\ssttwo}{\tilde{S}_{2,ij}}
\newcommand{\sstoneeq}{\tilde{S}_{1,j}}
\newcommand{\ssttwoeq}{\tilde{S}_{2,jk}}
\newcommand{\ssz}{{S}_0}
\newcommand{\ssone}{{S}_{1,i}}
\newcommand{\sstwo}{{S}_{2,ij}}
\newcommand{\ssoneeq}{{S}_{1,j}}
\newcommand{\sstwoeq}{{S}_{2,jk}}
\newcommand{\dsig}{\frac{d \sigma}{d \Omega}}
\newcommand{\dsigr}{\frac{d \sigma^R}{d \Omega^R}}
\newcommand{\oi}{{\cal O}_i}
\newcommand{\oidata}{\langle \oi \rangle }
\newcommand{\ojdata}{\langle \oj \rangle }
\newcommand{\oj}{{\cal O}_j}
\newcommand{\oti}{\tilde{\cal O}_i}
\newcommand{\otj}{\tilde{\cal O}_j}
\newcommand{\ot}{\tilde{\cal O}}
\newcommand{\non}{\nonumber\\}
\newcommand{\Orja}{\Omega^R,l, \nu, j_1, j_2}
\newcommand{\Orjb}{\Omega^R,l, \nu, j_2, j_1}
%\newcommand{\Orj2j1}{\Omega^{rek}_{l \mu j_{2} j_{1}}}
\newcommand{\Pe}{\mbox{${\cal P}_{e \nu jj}$}}
\newcommand{\Pmu}{\mbox{${\cal P}_{\mu \nu jj}$}}

\newcommand{\D}        {\displaystyle}
\newcommand{\T}        {\textstyle}
\newcommand{\TS}        {\scriptstyle}

\newcommand{\myrule}{\rule[-4.mm]{0mm}{11mm} }
\newcommand{\smallrule}{\rule[-3.mm]{0mm}{8mm} }
\newcommand{\scarletstrobes}{\clearpage{\pagestyle{empty}\cleardoublepage}}
\def\notp{{\hbox{$p$}\kern-5.87pt{/}\ }}
\def\notpz{{\hbox{$p_3$}\kern-8.87pt{/}\ }}
\def\notpt{{\hbox{$p_t$}\kern-8.87pt{/}\ }}
\def\notE{{\hbox{$E$}\kern-5.87pt{/}\ }}

%%% Local Variables: 
%%% mode: latex
%%% TeX-master: "dr"
%%% End: 
