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\begin{description}
\item[Figure 1:] {\em Simple sketch of the VLQ and the 
    SpaCal projected onto one plane in the $z$-direction where one
    photon is detected in the SpaCal and one in the VLQ (top), and
    where both photons are detected in one identical VLQ-module
    (bottom). The numbers give the relative geometric acceptance for
    the underlying Odderon induced process.}  
\item[Figure 2:] {\em Invariant mass spectrum of the
    two photon candidates for SpaCal-VLQ events, where one photon is
    detected in  the Very-Low-Q$^2$ calorimeter (VLQ) and one in the SpaCal (SpaCal), requiring an electron in the
    electron tagger and a neutron in the forward neutron counter.}
\item[Figure 3] {\em Invariant mass spectrum of the
    two photon candidates for both event signature classes: one photon
    is detected in the VLQ and one in the SpaCal (SpaCal-VLQ) and both photons 
    detected in the identical VLQ-module (VLQ-VLQ). The data points are
    compared to the signal Monte Carlo OPIUM for Odderon exchange and
    the photoproduction 
    Monte Carlos PYTHIA and PYTHIA-mod. PYTHIA-mod is a modified
    version of PYTHIA where, with regard to exclusive events, some
    "unphysical" processes are excluded (following an advice by the
    auther of PYTHIA, Tjorben Sj\"ostrand).\\
    The dashed lines define the 4 $\sigma$ pion mass window (mean
    $=135$ MeV, width = 20 MeV) for simulated events and the dotted
    lines define the 4 $\sigma$ pion mass window (mean
    $=175$ MeV, width = 40 MeV) for data events.}
\item[Figure 4:] {\em Summary of cross section limit
for Odderon production.}
\end{description}


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