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                XVI International Workshop on Deep-Inelastic Scattering, DIS2008},
                 April 7-11,~2008,~London} \\
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                  Parallel Session & {\bf Electroweak and Searches}   & & \\ \hline
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  \Large
  {\bf Search for Lepton Flavour Violation in {\boldmath{$e^-p$}} Collisions at HERA~II}

  \vspace*{1cm}
    {\Large H1 Collaboration} 
\end{center}

\begin{abstract}
\noindent
A search for scalar and vector leptoquarks coupling to first and second generation fermions and thus mediating lepton flavour violation is presented. This search uses all HERA~II $e^-p$ data collected by the H1 experiment, which corresponds to a total integrated luminosity of $158$\,pb$^{-1}$. Especially the sensitivity to leptoquarks with fermion number $F=2$ is increased with respect to the previous H1 results. No evidence for the direct or indirect production of such particles is found in data samples with a large transverse momentum final state muon. The results of the present analysis are used to set new constraints on lepton flavour violating leptoquark couplings, assuming $\lambda_{eq} = \lambda_{\mu q} = \lambda$ and $\lambda_{\tau q} = 0$. For a coupling of $\lambda = 0.3$, $F=2$ leptoquarks with masses up to $ 433\,{\rm GeV}$ are ruled out.

\noindent
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\section{Introduction}

The $ep$ collider HERA offers the unique possibility to search for the 
resonant production of new particles which couple directly to a lepton and a parton. Leptoquarks (LQs), colour triplet bosons, which appear naturally in various unifying theories beyond the Standard Model (SM) 
are such an example. At HERA, leptoquarks could be singly produced by the fusion of the initial state lepton of energy $27.6 \GeV$ with a quark from the incoming proton of energy up to $920 \GeV$.

The phenomenology of LFV at HERA is discussed in detail in~\cite{H1LFV07}. The effective Lagrangian considered there conserves lepton and baryon number, obeys the symmetries of the SM gauge groups $U(1)_Y$, $SU(2)_L$ and $SU(3)_C$ and includes both scalar and vector LQs. Dimensionless couplings $\lambda_{eq}$, $\lambda_{\mu q}$ and  $\lambda_{\tau q}$ define the coupling at the $e$-$q$-LQ, $\mu$-$q$-LQ and $\tau$-$q$-LQ vertex, respectively. At HERA, LQs can be resonantly produced in the $s$-channel or exchanged in the $u$-channel between the incoming lepton and a quark coming from the proton. In both cases, the production requires a non-zero $\lambda_{eq}$. The leptoquark can then decay either lepton flavour conserving via the same coupling, or via one of the lepton flavour violating couplings $\lambda_{\mu q}$ or  $\lambda_{\tau q}$ into final states with a jet and a muon or $\tau$-lepton with high transverse momentum.

Although particle interactions in the SM conserve lepton flavour, experimental evidence for lepton flavour violation (LFV)  has been obtained in neutrino physics~\cite{SUPK, SNO}. While experimental upper bounds on neutrino masses imply very small LFV in the charged lepton sector, an observation of such effects would clearly indicate new phenomena beyond the SM.  

This note presents a search for LQs coupling to first and second generation 
fermions with fermion number\footnote{The fermion number $F$ is given by $F=|3B+L|$, with $B$ and $L$ being the baryon and lepton number respectively.} $F=2$ in scattering of longitudinally 
polarised electrons on protons at a center-of-mass energy of 
$\sqrt{s_{ep}} \approx 320 \GeV$. For the
lefthanded\footnote{The names `lefthanded' and `righthanded' refer to the
  longitudinal polarisation of the electrons in the beam} running phase with an 
average polarisation of  $-26~\%$, the integrated luminosity amounts to 
$105 \picob^{-1}$, whereas for the righthanded running phase with an 
average polarisation of  $32~\%$,  $54 \picob^{-1}$ of data are analysed. 
The results of this search are combined with the HERA~I results~\cite{H1LFV07},
 which correspond to an integrated luminosity of 14~pb$^{-1}$ for $e^-p$ and 67~pb$^{-1}$ for $e^+p$ running.

Due to the more favourable quark-densities of quarks with respect to
anti-quarks at high $x$, the $e^{-}p$ data sets are mostly sensitive to LQs with fermion number $F=2$. The search reported here considers only decays into  ${\rm{LQ}} \rightarrow \mu q$
% with $q$ standing for both quarks and anti-quarks. 
. These LQ decays lead to unique final states with a jet and a muon with  high transverse momenta. 

\section{Experimental Conditions}

The H1 detector components most relevant to this analysis are the
liquid argon calorimeter, which measures the positions and energies of
charged and neutral particles over the polar angle\footnote{The polar
  angle $\theta$ is defined with respect to the incident proton
  momentum vector (the positive $z$ axis).} range of $4^\circ<\theta<154^\circ$, the inner tracking detectors which measure the angles and momenta of charged particles over the range $7^\circ<\theta<165^\circ$ and the instrumented iron return yoke which allows muon identification in the polar angle range of $5^\circ<\theta<175^\circ$. A full description of the H1 detector can be found in~\cite{h1det}. 

The leptoquark signal is generated with the LEGO~\cite{LEGO} event generator using the CTEQ5D~\cite{CTEQ5D} parametrisation of the parton distributions. 
The main characteristic of the signal events is an isolated muon with large transverse momentum which is back-to-back in the transverse plane with the hadronic final state. To avoid the simulation of signal events for each leptoquark mass and coupling, the LEGO sample is generated with a flat mass distribution and the same reweighting technique as used in~\cite{H1LFV07} is applied to calculate the selection efficiencies for arbitrary masses and couplings. This procedure provides an exact leading order prediction over the full range of LQ parameters.

The LQ kinematics are reconstructed using  the double angle method~\cite{DAmeth}. The direction of the detected lepton
and jet are used to reconstruct the Bj{\o}rken scaling variable $x$ and therefore the LQ mass $m_{\rm LQ}^{\rm rec}=\sqrt{xs}$.

The SM background to this search includes the following processes: The most important background to the final selection is lepton pair production, which has been generated with GRAPE~\cite{GRAPE}. It can mimic the signal topology either if one of the muons is lost into the beam pipe or if one of the muons happens to be close to the hadronic final state. Additional muons in jets are not  rejected because in a LFV leptoquark decay semileptonically decaying heavy quarks should not be excluded. Further backgrounds are real $W$ boson production generated with EPVEC~\cite{EPVEC}, photoproduction generated with PYTHIA~\cite{PYTHIA} and neutral current (NC) and charged current (CC) deep-inelastic scattering (DIS) generated by RAPGAP~\cite{RAPGAP} and DJANGO~\cite{DJANGO}, respectively.

All signal and SM samples are passed through a detailed simulation
of the H1 detector \linebreak response based on the GEANT program \cite{GEANT} and the 
same reconstruction and analysis algorithms as used for the data. 	


\section{The $e^-p \rightarrow \mu X$ Selection}

The event selection requires an isolated muon and at least one jet. The muon should have a transverse momentum $p_t > 8$~GeV and a polar angle in the range $10^{\circ} < \theta < 140^{\circ}$ and has to be identified in the instrumented return yoke. The isolation criterion requires that the minimal angular distance of the muon candidate to any other track $D=\sqrt{(\Delta\eta)^2+(\Delta\phi)^2}$ has to be larger than 0.5. Only exactly one muon fulfilling this isolation criterion is allowed in order to reject di-muon events.
The fact that a high energetic muon only leaves a minimal energy deposit 
in the calorimeter leads to a high net transverse momentum reconstructed 
from all clusters recorded in the LAr calorimeter, $p_T^{\rm calo}$, which 
is required to be larger than 25~GeV. Two cuts are employed to further 
exploit the event topology in the transverse plane. The azimuthal angle 
between the jet and the muon has to be larger than $170^{\circ}$ and 
$V_{ap}/V_p<0.2$ is required, where $V_{ap}/V_p$ is defined as the 
ratio of the anti-parallel to parallel projections of all energy 
deposits in the calorimeter with respect to the direction of 
$\vec{p}_{T}^{\rm calo}$ \cite{H12001}. In order to reject any remaining NC 
background events with an isolated electron candidate are vetoed. 
With these cuts, a high signal efficiency of 45\% to 70\% is obtained 
over a broad range of masses for all LQ types starting at about 75~GeV up to 
the contact interaction limit. Two candidate events are found in the data, 
compared to a total SM background expectation of $2.2\pm 0.6$ events, dominated by lepton pair production, which contributes $1.4\pm 0.4$ events.

The following experimental systematic uncertainties are applied to the SM background expectation as well as to the signal: The reconstructed polar angle of the jet is varied by 10~mrad in the central region of the detector and by 5~mrad in the forward region, where as the polar angle of the muon is assumed to be measured with a precision of 3~mrad. The azimuthal angle of both the muon and the jet are varied within 1~mrad each. The muon identification efficiency is assumed to be known to 15\% in the forward region and to 5\% in the central part of the detector and the reconstructed transverse momentum of the muon is varied by 5\%. 

Further uncertainties of 4\% for the luminosity measurement, 3\% for the 
polarisation measurement and a 30\% theoretical uncertainty on the modelling of lepton pair production as the main background source and 50\% on the photoproduction background are taken into account. The uncertainties originating from the parton densities, which are the main uncertainty on the signal expectation have been treated in the same way as in~\cite{H1LFV07}.  

The leptoquark mass spectra obtained after the final selection are shown in figure~\ref{fig:mass}. Two candidate events are observed in the data. Both events are consistent with lepton pair production, where one muon is too close to the hadronic final state to be recognized as a second isolated muon, which would lead to a rejection of the event. 

Since no evidence for LQ production is observed, the data are used to set constraints on LQs coupling to first and second generation fermions. The results of this analysis are combined with the results of the HERA~I data published in~\cite{H1LFV07}. 

 The majority of the background has a $p_T^{\rm calo}$ of less than 45~GeV, whereas a large fraction of the leptoquark signal is expected to have $p_T^{\rm calo}>45$~GeV. Thus signal and background expectation as well as the data are divided into two bins in $p_T^{\rm calo}$, one with between 25 and 45~GeV and one bin above 45~GeV. Both are combined with a procedure designed to fully exploit the sensitivity to the signal. The statistical method has been described in detail in~\cite{H1LQ05}.

\section{Limit Results}

In the following we will show limits derived within the phenomenological model proposed by Buchm\"uller, R\"uckl and Wyler (BRW)~\cite{BRW}.

The BRW model describes 7 LQs with $F=0$ and 7 LQs with $F=2$ coupling to $eq$. We use here the nomenclature of~\cite{LQNAME} to label the various scalar $S_{I,L}$ ($\tilde{S}^{\mbox{\tiny \hspace{-3mm}\raisebox{1.5mm}{(}\hspace{2mm}\raisebox{1.5mm}{)}}}_{I,R}$) or vector $\tilde{V}^{\mbox{\tiny
\hspace{-3mm}\raisebox{1.5mm}{(}\hspace{2mm}\raisebox{1.5mm}{)}}}_{I,L}$ ($V_{I,R}$) LQ types of weak isospin $I$, which couple to a left-handed (right-handed) electron. The tilde is used to distinguish LQs which differ only by their hypercharge.  Table~\ref{tab:lqbrw} lists the 7 LQ types with fermion number $F=2$ described by the BRW model. 

Since here only leptoquarks coupling to first and second generation fermions are under consideration, the number of free parameters is reduced by choosing $\lambda_{eq} = \lambda_{\mu q} = \lambda$ and $\lambda_{\tau q} = 0$. All results in this sections are obtained with this choice of the couplings.

% % ------------------ TABLE : Scalar Leptoquarks  -------------------------
% \begin{table*}[htb]
%   \renewcommand{\doublerulesep}{0.4pt}
%   \renewcommand{\arraystretch}{1.2}
%  \vspace{-0.1cm}
% 
% \begin{center}
%     \begin{tabular}{|c|r|c||c|r|c|}
%       \hline
%        $F=2$ & Prod./Decay & $\beta_e$
%               & $F=0$ & Prod./Decay & $\beta_e$  \\
% 
%       \hline
% %
% % -> Scalar LQ :
%      \multicolumn{6}{|c|}{Scalar Leptoquarks} \\ \hline
%     $S_{0,L}$     & $e^-_L u_L \rightarrow e^- u$ & $1/2$
%   & $S_{1/2,L}$   & $e^+_R u_R \rightarrow e^+ u$ & $1$  \\
%                   &           $\rightarrow \nu d$ & $1/2$ & & & \\ \hline
%     $S_{0,R}$     & $e^-_R u_R \rightarrow e^- u$ & $1$
%   & $S_{1/2,R}$   & $e^+_L u_L \rightarrow e^+ u$ & $1$ \\
%       \cline{1-3}
%     $\tilde{S}_{0,R}$
%                   & $e^-_R d_R \rightarrow e^- d$ & $1$
%   &               & $e^+_L d_L \rightarrow e^+ d$ & $1$ \\
%       \hline
%     $S_{1,L}$     & $e^-_L d_L \rightarrow e^- d$ & $1$
%   & $\tilde{S}_{1/2,L}$ 
%                   & $e^+_R d_R \rightarrow e^+ d$ & $1$ \\
%                   & $e^-_L u_L \rightarrow e^- u$ & $1/2$ & & &  \\
%                   &           $\rightarrow \nu d$ & $1/2$ & & & \\
%       \hline
% %
% % -> Vector LQ :
%      \multicolumn{6}{|c|}{Vector Leptoquarks} \\ \hline
%     $V_{1/2,R}$   & $e^-_R d_L \rightarrow e^- d$ & $1$
%   & $V_{0,R}$     & $e^+_L d_R \rightarrow e^+ d$ & $1$ \\
%       \cline{4-6}
%                   & $e^-_R u_L \rightarrow e^- u$ & $1$
%   & $V_{0,L}$     & $e^+_R d_L \rightarrow e^+ d$ & $1/2$ \\
%             & & & &           $\rightarrow \overline{\nu}u$ & $1/2$ \\ \hline
%     $V_{1/2,L}$   & $e^-_L d_R \rightarrow e^- d$ & $1$
%   & $\tilde{V}_{0,R}$
%                   & $e^+_L u_R \rightarrow e^+ u$ & $1$ \\
%       \hline
%     $\tilde{V}_{1/2,L}$
%                   & $e^-_L u_R \rightarrow e^- u$ & $1$
%   & $V_{1,L}$     & $e^+_R u_L \rightarrow e^+ u$ & $1$ \\
%                           &                                            &
%   &               & $e^+_R d_L \rightarrow e^+ d$ & $1/2$ \\
%             & & & &           $\rightarrow \overline{\nu}u$ & $1/2$ \\
%       \hline
%       \hline
%     \end{tabular}
%     \caption {\small \label{tab:lqbrw}
%                Leptoquark isospin families in the Buchm\"uller-R\"uckl-Wyler
%                model.
%                For each leptoquark, the subscript denotes its weak isospin
%                and the chirality of the incoming {\it{electron}} which
%                could mediate their production in $e^-p$ collisions.
%                Charge conjugate processes are not shown.
%                }
% \end{center}
% \end{table*}
% % ------------------------------------------------------------------------
% ------------------ TABLE : Scalar Leptoquarks  -------------------------
\begin{table*}[htb]
  \renewcommand{\doublerulesep}{0.4pt}
  \renewcommand{\arraystretch}{1.2}
 \vspace{-0.1cm}

\begin{center}
    \begin{tabular}{|c|r|c|}
      \hline
       $F=2$ & Prod./Decay & $\beta_{e,\nu}$\\

      \hline
%
% -> Scalar LQ :
     \multicolumn{3}{|c|}{Scalar Leptoquarks} \\ \hline
    $S_{0,L}$     & $e^-_L u_L \rightarrow e^- u$ & $1/2$\\
                  &           $\rightarrow \nu d$ & $1/2$ \\ \hline
    $S_{0,R}$     & $e^-_R u_R \rightarrow e^- u$ & $1$\\
      \cline{1-3}
    $\tilde{S}_{0,R}$
                  & $e^-_R d_R \rightarrow e^- d$ & $1$\\
      \hline
    $S_{1,L}$     & $e^-_L d_L \rightarrow e^- d$ & $1$\\
                  & $e^-_L u_L \rightarrow e^- u$ & $1/2$ \\
                  &           $\rightarrow \nu d$ & $1/2$ \\
      \hline
%
% -> Vector LQ :
     \multicolumn{3}{|c|}{Vector Leptoquarks} \\ \hline
    $V_{1/2,R}$   & $e^-_R d_L \rightarrow e^- d$ & $1$\\
                  & $e^-_R u_L \rightarrow e^- u$ & $1$ \\
\hline
    $V_{1/2,L}$   & $e^-_L d_R \rightarrow e^- d$ & $1$ \\
      \hline
    $\tilde{V}_{1/2,L}$
                  & $e^-_L u_R \rightarrow e^- u$ & $1$\\
      \hline
      \hline
    \end{tabular}
    \caption {\small \label{tab:lqbrw}
Leptoquark isospin families with $F=2$ in the Buchm\"uller-R\"uckl-Wyler model. For each leptoquark, the subscript denotes its weak isospin and the chirality of the incoming electron which could mediate their production in $e^-p$ collisions. $\beta_{e,\nu}$ indicates the assumed branching fraction into electrons or neutrinos if both channels are allowed.
               }
\end{center}
\end{table*}
% ------------------------------------------------------------------------
%
The resulting constraints are shown in figure~\ref{fig:brw}a for the four scalar and in figure~\ref{fig:brw}b for the three vector LQs with $F=2$. The areas above the curves are excluded at $95\%
$
confidence level. The strongest constraints on the coupling $\lambda$ can be set for LQ masses below the kinematic limit of the $s$-channel. At higher masses the production is not resonant anymore but contact interaction--like and the cross--sections scale approximately with $(\lambda/M_{LQ})^4$. For a coupling of electromagnetic strength $\alpha_{\rm em}$ ($\lambda = \sqrt{4\pi\alpha_{\rm em}}=0.3$) this analysis rules out LQ masses below $291$ to $433$~GeV, depending on the LQ type.

Figure~\ref{fig:brwcompar} summarises the constraints on the $S_{0,L}$ leptoquark obtained by H1 and by the D0 experiment at the Tevatron~\cite{d0}.  The limits from the Tevatron are independent of the coupling $\lambda$ as they were derived from the dominant pair production processes. However they assume leptoquarks coupling to only one generation, whereas at HERA the first generation coupling is needed for production even if the decay into second generation fermions is searched for. Therefore the most stringent mass constraints from the Tevatron experiments corresponding to the HERA scenario can be derived from the $e\nu qq$ channel. The published H1 results~\cite{H1LFV07} from the HERA~I phase (mainly $e^+ p$ running) are shown for comparison. 
%Above the kinematic limit, the improvement with respect to the HERA~I results is smaller than at lower masses, because the production is no longer resonant and thus the sensitivities of the $e^+p$ and the $e^-p$ datasets (which have approximately the same integrated luminosity) to $F=2$ LQs are very similar. 

%Beyond the BRW ansatz, generic LQ models can also be considered, where
%other LQ decay modes are allowed such that the branching ratios $\beta_e$
%and $\beta_\nu$ are free parameters.
%Mass dependent constraints on the LQ branching ratios
%can then be set for a given value of $\lambda$.
%For a vector LQ coupling to $e^- u$ (possessing the
%quantum numbers of the $S_{0,L}$) and for $\lambda = 0.06$,
%the domain of the $\beta_e$-$M$ ($\beta_{\nu}$-$M$) plane
%excluded by the NC (CC) analysis is shown in Fig.~\ref{fig:betaeplus}a.
%If the LQ decays into $e q$ or $\nu q$
%only\footnote{It should be noted that $\beta_e + \beta_{\nu} = 1$ does
%   not imply $\beta_e = \beta_{\nu}$ even when
%   invariance under $SU(2)_L$ transformations is required.
%   For example, when LQs belonging to a given isospin multiplet are not
%   mass eigenstates, their mixing usually leads to different branching
%   ratios in both channels for the physical LQ states. },
%the combination of both channels rules out the part of the plane on 
%the left of the second full curve from the left for $\lambda = 0.06$. 
%The resulting combined bound is largely independent of the individual values
%of $\beta_e$ and $\beta_{\nu}$.
%Combined bounds are also shown for $\lambda=0.03$ and $\lambda=0.3$.
%For a coupling $\lambda=0.3$ and high $\beta_{\nu}$ the limit extends to high
% mass values above the kinematic limit of resonant LQ production.
% For this part of the parameter space the coupling
% $\lambda_{\nu}=\lambda\sqrt{\beta_\nu/\beta_e}$ is 
% large\footnote{In the BRW model, 
% $|\lambda_\nu|=|\lambda|$ since $\beta_\nu=\beta_e$. 
% Here, in a generic LQ model, the effective coupling
% $\lambda_\nu$ at the LQ-$\nu$-$q$ vertex can be different from $\lambda$
% at the LQ-$e$-$q$ vertex.},
% but still satisfies
% $\lambda_{\nu}^2/4\pi<1$.
% A smooth transition is observed
% between limits driven by resonant production and limits driven by contact
% interactions.
%The domain excluded by the D$0$ experiment at the Tevatron~\cite{d0} is 
%also shown. For $\lambda$ greater than $\sim 0.06$, 
%the H1 limits on scalar LQs extend considerably beyond the
%region excluded by the D$0$ experiment~\cite{d0}.

%The H1 limit on the $S_{0,L}$-like LQ applies to squark $\tilde{d}_i$ with $R$-parity violating couplings $\lambda^\prime_{11i}$ to $eu$ and subsequent decays $\tilde{d}_i\rightarrow e^-u$ and $\tilde{d}_i\rightarrow \nu d$ (the subscript $i$ is a generation index here).

%Similarly, the limit (unshown) on the $\tilde{S}_{1/2,L}$-like LQ also 
%applies to squark $\tilde{u}_i$ with 
%$R$-parity violating couplings $\lambda^\prime_{1i1}$ to $ed$ and 
%subsequent decay $\tilde{u}_i\rightarrow e^+d$.
%More general limits on squark production taking into account of direct and indirect $R$-parity violating decay modes have been set in~\cite{susylimit}.

\section{Summary}
In summary, a search for leptoquarks with fermion number $F=2$ coupling to first and second generation fermions has been performed using the complete $e^-p$ data set from the HERA~II running phase. No signal has been observed and constraints on leptoquarks have been set in combination with the full HERA~I data published in~\cite{H1LFV07}. The new limits extend beyond the domains excluded previously by H1. For a coupling of electromagnetic strength, leptoquark masses below $291-433$ GeV can be ruled out, depending on the leptoquark type.

\section*{Acknowledgements}
%
We are grateful to the HERA machine group whose outstanding
efforts have made this experiment possible.
We thank the engineers and technicians for their work in constructing 
and maintaining the H1 detector, our funding agencies for
financial support, the DESY technical staff for continual assistance
and the DESY directorate for support and for the
hospitality which they extend to the non DESY
members of the collaboration.

\begin{thebibliography}{99}

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  %%CITATION = HEP-EX/0703004;%%

\bibitem{SUPK} Y.~Fukuda {\em et al.} [Super-Kamiokande Collaboration],
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\bibitem{SNO} Q.~R.~Ahmad {\em et al.} [SNO Collaboration],
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\bibitem{h1det}
% H1 Collaboration, I.~Abt {\it et al.}, Nucl.\ Instrum.\ Meth.\ A386 (1997)
% 310 and 348.  -> No, 310 & 397
I.~Abt {\it et al.}  [H1 Collaboration],
%``The H1 detector at HERA,''
Nucl.\ Instrum.\ Meth.\ A {\bf 386} (1997) 310 and 348, \\
%%CITATION = NUIMA,A386,310;%%
%
R.~D.~Appuhn {\it et al.}  [H1 SPACAL Group],
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\end{thebibliography}

% ---------- FIGURE 1: Mass spectrum  ----------------
%
\begin{figure}[p] 
\begin{center}
\begin{picture}(120,120)
\put(0,0){\epsfig{figure=H1prelim-07-167.fig1.eps,width=12cm}}
\end{picture}
\end{center}
  \caption{\label{fig:mass}
Leptoquark mass spectrum after the final selection, together with the corresponding SM expectations (histogram). The shaded bands indicate the $\pm1\sigma$ uncertainty on the SM expectations.}
\end{figure} 
%---------------------------------------------------------------------------

% --------------- FIGURE 2: Limits BRW : H1 Vector & Scalar   --------------
%
\begin{figure}[p] 
\begin{center}
\begin{picture}(80,200)
\put(-30,100){\epsfig{figure=H1prelim-07-167.fig2a.eps,width=12cm}}
\put(0,190){{\bf(a)}}
\put(-30,0){\epsfig{figure=H1prelim-07-167.fig2b.eps,width=12cm}}
\put(0,90){{\bf(b)}}
\end{picture}
\end{center}
  \caption{\label{fig:brw}
  Exclusion limits for the 7 leptoquarks (LQs) with $F=2$ described by the
  Buchm\"uller, R\"uckl and Wyler (BRW) model. The limits are expressed at
  $95\%\,{\rm CL}$ on the coupling $\lambda_{\mu q} = \lambda_{eq}$ as a function of 
  the leptoquark mass for the (a) scalar LQs with $F=2$, 
  (b) vector LQs with $F=2$.
  Domains above the curves are excluded. 
  In the brackets, for each LQ type the pairs of
  Standard Model first generation fermions is indicated to which it couples.}
%  Constraints on LQs with masses above $580$\,GeV,
%  obtained from the H1 contact interaction (CI) analysis~\cite{ci}, 
%  are shown in the rightmost part of the figures.}
  \end{figure} 
%----------------------------------------------------------------------

% --------------- FIGURE 3: Limits BRW : H1  + D0    --------------
%
\begin{figure}[p]
\begin{center}
\begin{picture}(50,90)
\put(-30,0){\epsfig{figure=H1prelim-07-167.fig3.eps,width=10.5cm}}
\end{picture}
\end{center}
  \caption{\label{fig:brwcompar}
  Exclusion limits at $95\%\,{\rm CL}$ on the coupling $\lambda_{\mu q} = \lambda_{eq}$ as a function of the leptoquark (LQ) mass for $S_{0,L}$ in the framework of the BRW model. The  direct D0 limit obtained from leptoquark pair production is shown for comparison. In addition, the published H1 limit on $S_{0,L}$ from HERA~I data is shown.}
\end{figure} 
%----------------------------------------------------------------------

\end{document}
