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  \begin{center}
    \begin{tabular}{|l|c|l|p{9cm}|}
     \hline
     Variable & type & Dim & Description \\ 
     \hline\hline
       \verb+x_rot_abr+ & s & m & dispersive position $x_{fp}$ at the focal
       plane corrected for spectrometer aberations\\  \hline
       \verb+x_rot_kin+ & s & m & dispersive position $x_{fp}$ at the focal
       plane corrected for spectrometer aberations and for deviations of the
       nuclear recoil momentum \footnote{This correction is different for
       electrons and protons. It makes only sense to use it for the hadron arm
       in case of H(e,e'p)} \\  \hline
       \verb+th_rot+ & s & rad & angle $\theta$ of the particle track
       in the focal plane in the dispersive direction wrt the {\it local}
       central ray \\  \hline
       \verb+th_dp+ & s & rad & angle $\theta$ of the particle track
       in the focal plane in the dispersive direction wrt the detector plane
       \\  \hline
       \verb+y_rot+ & s & m & non-dispersive position $y$ in the
       focal plane \\  \hline
       \verb+ph_rot+ & s & rad & angle $\phi$ of the particle track
       in the non-dispersive plane at the focal plane \\  \hline
       \verb+ph_dp+ & s & rad & angle $\phi$ of the particle track
       in the focal plane in the non-dispersive direction wrt the detector
       plane \\  \hline
       \verb+p+ & s & MeV/c & momentum of the particle after exiting the
       target corrected for spectrometer aberations\\  \hline
       \verb+p_kin+ & s & MeV/c & momentum of the particle after exiting the
       target corrected for spectrometer aberations and for deviations of the
       nuclear recoil momentum \\  \hline
       \verb+dp+ & s & & like \verb+p+ but relative to the centralray \\  \hline
       \verb+dp_kin+ & s & & like \verb+p_kin+ but relative to the central
       ray \\  \hline
       \verb+th_tg+ & s & rad & angle $\theta_{tg}$ of the particle track
       in the dispersive plane at the scattering point at the target\\  \hline
       \verb+y_tg+ & s & m & non-dispersive position $y_{tg}$ at the
       scattering point at the target \\  \hline
       \verb+ph_tg+ & s & rad & angle $\phi_{tg}$ of the particle track
       in the non-dispersive plane at the scattering point at the
       target \\  \hline
       \verb+path_diff+ & s & m & difference n path length for this track and
       the central ray through the spectrometer. \\  \hline
       \verb+track+* & s & & number of reconstructed particle tracks. \\  \hline
    \end{tabular}
  \end{center}
  
    \label{tab:var2}
\end{table}
}

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    \begin{tabular}{|l|c|p{1.5cm}|p{1.0cm}|p{7.5cm}|}
    \hline
    Variable & type & Detector & Dim & Description \\ 
    \hline\hline
    \verb+hitpat+* & s &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     & hitpattern of wire plane, see description in section \ref{sec:Hitp}
     \\  \hline
    \verb+clus+ & s &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     & number of clusters in the wire plane \\  \hline
    \verb+tdc+ & a &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     {\sc tdc} chan & {\sc tdc} values of drift times in wire plane \\  \hline
    \verb+coars+ & s & 
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     & wire number with the shortest drift time in cluster used in the
     selected track \\  \hline
    \verb+slope+ & s &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     & slope of selected track through wire plane \\  \hline
    \verb+pos+ & s &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     m & position where seleted track passed through the wire plane given
     in the local wire plane coordinate system \\  \hline
    \verb+chisq+ & s &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+ &
     & reduced $\chi ^2$ of fit to the drift times in the wire plane \\  \hline
    \end{tabular}
  \end{center}
  
    \label{tab:var3a}
\end{table}
}

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  \begin{center}
    \begin{tabular}{|l|c|p{2.3cm}|p{0.5cm}|p{7.5cm}|}
    \hline
    Variable & type & Detector & Dim & Description \\ 
    \hline\hline
    \verb+mult+* & s &
     \verb+spec_s.u1+
     \verb+spec_s.v1+
     \verb+spec_s.u2+
     \verb+spec_s.v2+
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_s.aero+
     \verb+spec_s.gas+
     \verb+spec_e.preshow+
     \verb+spec_e.show+
     \verb+spec_h.s3+ &
     & number of hits on detector \\  \hline
    \verb+hp_l+* & a &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     & paddle hit pattern for photo multipliers on the left side \\  \hline
    \verb+hp_r+* & a &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     & paddle hit pattern for photo multipliers on the right side \\  \hline
    \verb+adc+ & a &
     \verb+spec_s.aero+
     \verb+spec_s.gas+
     \verb+spec_e.preshow+
     \verb+spec_e.show+ & 
     & {\sc adc} of Cherenkov mirrors or shower blocks \\  \hline
    \verb+adc_l+ & a &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     & {\sc adc} of scintillator paddles on the left side \\  \hline
    \verb+adc_r+ & a &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     & {\sc adc} of scintillator paddles on the right side \\  \hline
    \verb+tdc_l+ & a &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     & {\sc tdc} of scintillator paddles on the left side \\  \hline
    \verb+tdc_r+ & a &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     & {\sc tdc} of scintillator paddles on the right side \\  \hline
    \verb+x_scint+ & s &
     \verb+spec_s.s1+
     \verb+spec_s.s2+
     \verb+spec_h.s3+ &
     m & x coordinate of crossing point of selected track with the
     scintillator plane , given in the local scintillator coordinate
     system \\  \hline
    \end{tabular}
  \end{center}
  
    \label{tab:var3b}
\end{table}
}

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  \begin{center}
    \begin{tabular}{ccp{8.0cm}}
    \hline
     \multicolumn{2}{c}{{\sc hpch} value} & Description \\ 
     dec & bin & \\ 
     \hline
       1 & 00000001 & valid hit \\ 
       2 & 00000010 & nohit \\ 
       4 & 00000100 & number of wires hit $\leq$ 2 \\ 
       8 & 00001000 & number of wires hit $\geq$ 16 \\ 
      16 & 00010000 & correct number of wires identified, but not
                    consecutive. \\ 
      32 & 00100000 & The first or last wire had the shortest drift
                     time (smallest time is external) \\ 
      64 & 01000000 & {\sc tdc} value out-of-range \\ 
     128 & 10000000 & wire number out of range \\ 
    \hline
    \end{tabular}
  \end{center}
  
    \label{tab:Hitp}
\end{table}
}

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\hline
Variable & Comments \\ 
\hline
\verb+spec_e.th_tg/spec_e.ph_tg+ & Reconstructed theta and phi target
coordinates of the electron spectrometer. These angles can only be optimized
for a measurement with a {\it sieve} collimator. Both of them are
optimized at the same time, see \cite{vertex} \\ 
\verb+spec_h.th_tg/spec_h.ph_tg+ & The same for the hadron
spectrometer. \\  \hline
\verb+spec_e.y_tg+ & Reconstructed y target coordinate of the
the electron spectrometer. The non-dispersive position can be optimized after
a series of measurements have been performed in which the beam spot has been
put at different positions. \\  \hline
\verb+spec_h.y_tg+ & The same for the hadron spectrometer. \\  \hline
\verb+tc_cor+ & Coincidence time between e and h spectrometer after
correction for path length differences wrt the central rays and time
offsets between the scintillators. \\  \hline
\verb+e_miss+ & Missing energy for (e,e'x) \\  \hline
\verb+e_miss/p_miss+ & Missing energy and momentum for H(e,e'p) \\  \hline
\end{tabular}
}

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{\tt hbook} & C & ``hbook'' {\tt  D='off'} \\ 

\end{tabular}
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{\tt ntuple} & C & ``NTUPLE format'' {\tt  D='off'} \\ 

\end{tabular}
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{\tt trig\_cor} & C & ``vdc com. stop corr.'' {\tt  D='on'} \\ 

\end{tabular}
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{\tt cosmic\_rays} & C & ``cosmic corr.'' {\tt  D='off'} \\ 

\end{tabular}
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{\tt iterate\_vdc} & I & ``iterate VDC'' {\tt  D=1 R=1:4} \\ 

\end{tabular}
}

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{\tt output\_file} & C & ``output file'' {\tt  D='espace.hbook'} \\ 

\end{tabular}
}

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{\tt plane} & C & ``scintillator plane'' {\tt  D='s1'} \\ 


{\tt side} & C & ``paddle side'' {\tt  D='left'} \\ 

\end{tabular}
}

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{\tt plane} & C & ``scintillator plane'' {\tt  D='s1'} \\ 


{\tt side} & C & ``paddle side'' {\tt  D='left'} \\ 

\end{tabular}
}

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{\tt type} & I & ``e-spec type'' {\tt  D=1 R=1:16} \\ 

\end{tabular}
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{\tt type} & I & ``h-spec type'' {\tt  D=2 R=1:16} \\ 

\end{tabular}
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{\tt type} & I & ``coin type'' {\tt  D=4 R=1:16} \\ 

\end{tabular}
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{\tt type} & I & ``scaler type'' {\tt  D=15 R=1:16} \\ 

\end{tabular}
}

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{\tt list} & C & ``list of spectra'' {\tt  D='1-100'} \\ 

\end{tabular}
}

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  \begin{center}
    \begin{tabular}{|l|l|l|p{10.0cm}|}
    \hline
    item & & units & Description \\ 
    \hline\hline
    \verb+database+ & & & path and name of database file (see appendix
                       \ref{sec:Database}) \\  \hline
    \verb+e0+ & & MeV & electron energy of {\sc mami} \\  \hline
    \verb+spece+ & & & parameters of the electron spectrometer \\ 
     & \verb+field+ & kG & magnetic induction of the dipole \\ 
     & \verb+angle+ & deg & angular position of spectrometer in-plane\\ 
     &              & deg & angular position of spectrometer out-of-plane\\ 
     & \verb+solid+ & & spectrometer collimator acceptances\\ 
                  & & mrad & half horizontal acceptance\\ 
                  & & mrad & half vertical acceptance \\  \hline
    \verb+spech+ & & & parameters of the hadron spectrometer \\ 
     & \verb+field+ & kG & magnetic induction of the dipole \\ 
     & \verb+angle+ & deg & angular position of spectrometer in-plane\\ 
     &              & deg & angular position of spectrometer out-of-plane\\ 
     & \verb+solid+ & & spectrometer collimator acceptances\\ 
                  & & mrad & half horizontal acceptance\\ 
                  & & mrad & half vertical acceptance \\  \hline
     \verb+target+ & & & target parameters \\ 
                  & & mg/cm$^2$ ; cm & target thickness; target radius \\ 
                  & &  g/cm$^3$ & target density \\ 
                  & & & number of isotopes \\ 
                  & & & isotope being investigated \\ 
                  & & & target model (1:flat; 2:circular;3:cylindrical) \\ 
                                                                          \hline
     \verb+tar_angle+ & & deg & target angle \\  \hline
     \verb+isotope1_name+ & & & name of isotope 1 \\  \hline
     \verb+isotope1+ & & & \\ 
                  & f & & abundancy $\leq$ 1.0 \\ 
                  & A & amu & atomic mass \\ 
                  & Z & & isotope number \\  \hline
     \verb+isotope2_name+ & & & name of isotope 2 \\  \hline
     \verb+isotope2+ & & & \\ 
                  & f & & abundancy $\leq$ 1.0 \\ 
                  & A & amu & atomic mass \\ 
                  & Z & & isotope number \\  \hline
     \verb+reconstruct+ & & & parameter controling extended target
			      corrections \\ 
                  & 0 & & It is assumed that the reaction happened in the
			  center of the target\\ 
                  & 1 & & The position information of the beam and the vertex
			  reconstructed with the spectrometers are used to 
			  calculate the reaction point in the target. \\ 
                  & 2 & & In addition to option 1 the vertices of all
			  spectrometers are corrected for the fact that the
			  particle did not emerge from the optical point. \\ 
    \hline
    \end{tabular}
  \end{center}
  
    \label{tab:Header}
\end{table}
}

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\samepage \begin{tabular}{cp{8.0cm}}
line & Description \\ 
\hline
1 & Detector type for each of the four wire planes. Vertical Drift
Chamber=1. \\ 
2 & Number of wires for each plane. \\ 
3 & Distance of each wire plane from the first plane (m). \\ 
4 & Wire angle in each plane (deg). \\ 
5 & Wire spacing in each plane (m). \\ 
6 & Estimate of drift time resolution (chan). \\ 
7 & Electron drift velocity (m/s). \\ 
8 & coefficients of a polynomial for drift length correction in the {\sc vdc}
    (m) \\ 
\hline
\end{tabular}
}

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\end{document}
