%Paper: 
%From: MRENNA@CITHE1.CITHEP.CALTECH.EDU
%Date: Fri, 17 Jun 1994 16:34:30 -0800 (PST)

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%
% The following file is written in the REVTEX 3.0 format.
% After \end{document}, 3 postscript files are included (simply
% concatenated).  Extract the portion of this file from \end{document} to the
% end and put it into another file, then separate out the figures.
%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\documentstyle[preprint,aps]{revtex}
%
%  \slashchar puts a slash through a character to represent contraction
%  with Dirac matrices. Use \not instead for negation of relations, and use
%  \hbar for hbar.
%
\def\slashchar#1{\setbox0=\hbox{$#1$}           % set a box for #1
   \dimen0=\wd0                                 % and get its size
   \setbox1=\hbox{/} \dimen1=\wd1               % get size of /
   \ifdim\dimen0>\dimen1                        % #1 is bigger
      \rlap{\hbox to \dimen0{\hfil/\hfil}}      % so center / in box
      #1                                        % and print #1
   \else                                        % / is bigger
      \rlap{\hbox to \dimen1{\hfil$#1$\hfil}}   % so center #1
      /                                         % and print /
   \fi}                                         %
%
%
\begin{document}
% \draft command makes pacs numbers print
\draft
\title{Possible Detection of a Higgs Boson at Higher Luminosity Hadron
Colliders}
% repeat the \author\address pair as needed
\author{Stephen Mrenna}
\address{California Institute of Technology \\
        Pasadena, CA}
\author{G.L. Kane}
\address{Randall Physics Laboratory, Univ. of Michigan \\
        Ann Arbor, MI }
\date{12 June 1994}
\maketitle
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% ABSTRACT
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{abstract}
%
   We have examined how a Standard Model or Supersymmetric Higgs boson
$h$ might be detected at possible hadron colliders.
The channels $W(\rightarrow\ell\nu)h(\rightarrow b\bar{b})$,
$Z(\rightarrow\ell\bar{\ell})h(\rightarrow b\bar{b})$ and
$W,Z(\rightarrow q\bar{q})h(\rightarrow\tau^{+}\tau^{-})$ are most useful.  The
results imply that $h$
with mass $M_h$
can be detected or excluded for 80~GeV$~{\stackrel{\scriptstyle <}{\scriptstyle
\sim}}~ M_h ~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~$130~GeV
at any hadron collider
with energy $\sqrt{\rm s~}$ $~{\stackrel{\scriptscriptstyle
>}{\scriptscriptstyle \sim}}~$2~TeV and an integrated luminosity
${\cal L} ~{\stackrel{\scriptscriptstyle >}{\scriptscriptstyle \sim}}~ 10$
fb$^{-1}$; high luminosity is the essential requirement.
For ${\cal L} ~{\stackrel{\scriptscriptstyle >}{\scriptscriptstyle \sim}}~ 30$
fb$^{-1}$, the $M_h$ reach is expanded beyond 130 GeV.
A \mbox{p--$\overline{\rm p}$~} collider is slightly better than a p--p
collider of
equal $\sqrt{\rm s~}$ and ${\cal L}$ for Higgs
detection.
We comment on measuring $h$ couplings and branching
ratios.
\end{abstract}
% insert suggested PACS numbers in braces on next line
\pacs{}
%
% body of paper here
%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%  BEGIN HERE                   %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% introduction
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{\rm Introduction}
Understanding the physics of the Higgs sector is the central task of
particle physics today.  This is necessary to complete the Standard Model
(SM), and the result will help point the way to extending the SM and
strengthening its foundations.  Probably it will be necessary to detect
or exclude a Higgs boson to make progress.

Discussing a Higgs boson in the SM is subtle, because no way is known
to maintain a light Higgs boson if any high scale exists.
If the
apparent perturbative unification of the SM gauge couplings \cite{langacker}
at a scale of the order $10^{16}$~GeV is not dismissed as a meaningless
accident, then there is an upper limit of about 200~GeV on the mass of the
SM Higgs boson
$h_{SM}$ \cite{cabi}.  In any supersymmetric theory, this upper limit
drops to about 150~GeV \cite{espinosa}.  These arguments are general.
While such indirect reasoning may not satisfy everyone, they surely imply
that the highest priority should be to search for the Higgs boson in the
mass range below about 200~GeV.  Its discovery will indicate that
supersymmetry (SUSY)
is probably realized in Nature, while its exclusion will be the final chapter
of low energy SUSY.

To put it succinctly, the best arguments known
today imply that the region $M_h =$~60--200~GeV
is the most important one,
and we have focussed on the most
difficult part: 80~GeV$~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~ M_h
{}~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~$130~GeV.
The region below 80~GeV will be covered at
LEP2, while the region above 145~GeV is rather easily studied at a hadron
collider with enough energy and luminosity in any case.  For
130--145~GeV, the situation needs to be analyzed in detail for a given
collider; we think this region can also be covered.
The remaining mass region, covering the gap from LEP2 up to about 125
GeV, is generally thought to be coverable by the rare two photon decay
of $h$ at the CERN LHC.  This requires an LHC electromagnetic calorimeter
with excellent energy resolution and pointing capabilities that is,
additionally, radiation hard.

We find that the inclusive production p + p$(\bar{\rm p})\rightarrow h + X$ is
not helpful to detect or exclude $h$, because of
a combination of small cross sections and large QCD backgrounds,
for hadron colliders with $\sqrt{\rm s~}$ $~{\stackrel{\scriptstyle
<}{\scriptstyle \sim}}~$14~TeV and
instantaneous luminosity $L < 10^{34}$cm$^{-2}$s$^{-1}$.
However, the
associated production processes $W+h$ and $Z+h$ can provide a signal for $h$
in several decay channels: $W(\rightarrow\ell\nu)h(\rightarrow b\bar{b}),
Z(\rightarrow\ell\bar{\ell})h(\rightarrow b\bar{b})$ and
$W,Z(\rightarrow q\bar{q})h(\rightarrow\tau^{+}\tau^{-})$.  The channels with
$W,Z\rightarrow $quark jets and
$h\rightarrow\tau^{+}\tau^{-}$ have not been considered elsewhere to our
knowledge.

We have examined many backgrounds to these processes, and present most of
our
results in terms of the number of signal events $S$ divided by the square
root of the number of background events $B$, $S/\sqrt{B}$.  We think it
is appropriate to combine channels, so the final results are the combined
significance for the four channels listed above.  Somewhat surprisingly,
we find that the behavior of signal and background with collider energy are
such that there is little or no gain in going to higher energies.  Rather,
luminosity is the key variable for $M_h ~{\stackrel{\scriptstyle
<}{\scriptstyle \sim}}~ 130$ GeV.

We find that,
with an instantaneous luminosity $L$
of order $10^{33} {\rm cm}^{-2}{\rm s}^{-1}$,
it is possible to detect or exclude $h_{SM}$ in the
region 80~GeV$~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~ M_{h_{SM}}
{}~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~ 130$~GeV at a hadron
collider
with $\sqrt{\rm s~}$ $~{\stackrel{\scriptscriptstyle >}{\scriptscriptstyle
\sim}}~$2~TeV.
Studies of supersymmetric theories \cite{kane2} have shown that if the
combined constraints of unification of the couplings, electroweak symmetry
breaking and consistency with data are imposed, then the lightest
SUSY Higgs boson
behaves essentially identically to a light
SM Higgs in all ways, so our results
apply equally as well to the lightest SUSY Higgs boson of the constrained
models.  In this paper, we show results for a 2 TeV \mbox{p--$\overline{\rm
p}$~}, 4 TeV p--p, and
a 14 TeV p--p collider with $L ~{\stackrel{\scriptscriptstyle
>}{\scriptscriptstyle \sim}}~ 10^{33}{\rm cm}^{-2}{\rm s}^{-1}$.

We assume a typical SSC or LHC detector is available to detect $h$.  The
detailed properties used in the analysis are described in Section 2.  The
most difficult requirement is that the detector must operate efficiently
at luminosities of order $10^{33}{\rm cm}^{-2}{\rm s}^{-1}$.
Sections 3--5 present the results for different channels, section 6 the
combined results, section 7 comments on measuring
$h$ properties, and section 8  some concluding remarks.

While we were preparing this paper, two other papers \cite{marciano,gunion}
appeared on
the same topic.  Where we overlap, the cross sections and
results are consistent.  We have considered
in addition the $W,Z(\rightarrow q\bar{q})h(\rightarrow\tau^{+}\tau^{-})$
channels,
so our conclusions are more favorable for Higgs detection.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% event simulation
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{\rm Event Simulation}

   Calculations are parton level, unless a full simulation is needed for
a given signal or background, based
on the PAPAGENO \cite{papageno} and PYTHIA \cite{pythia} generators.
We use $m_t = 150$~GeV, 2nd order
running of $\alpha_s$ and CTEQ-1M structure functions.
The signal and backgrounds to $\tau^{+}\tau^{-}$ + jets
(such as $W^\pm\rightarrow\tau^{\pm}\nu_\tau +$ jets, with
a real $\tau$ and a jet that fakes the hadronic decay of
a $\tau$ in the final state)
were estimated using PYTHIA with initial and final state showering and
fragmentation.
We use no ``K-factors'' for the signals or backgrounds in the
individual channels considered, so our results will
improve when radiative corrections are included.  However, when presenting
the combined significance of all channels in Figure 2,
the effect of varying K over the
region $1 ~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~ {\rm K}
{}~{\stackrel{\scriptstyle <}{\scriptstyle \sim}}~ 1.2$ is illustrated by a
light shaded band.

   The following detector properties are implicit to this analysis:
\begin{itemize}
\item   Hadron calorimetry resolution $60\%/\sqrt{\rm E }\oplus 4\%$ covering
$|\eta| \le$ 2.5.
\item   Electromagnetic calorimetry resolution $7\%/\sqrt{\rm E}\oplus .5\%$
covering $|\eta| \le$ 2.5.
\item   Muon acceptance and momentum resolution comparable to electrons.
\item   Forward calorimetry covering to $|\eta|=$ 5 and
   $\slashchar{E}_{t}$
   resolution 40\%/$\sqrt{\slashchar{E}_t}$.
\item   A central tracker with good impact resolution and a high reconstruction
   efficiency to allow the tagging of $b$--jets and $\tau$ decays.
\end{itemize}

The choice of hadronic calorimetry is slightly worse than that
available presently at the ${\bf D0}$ detector at FNAL, but is
slightly better than that at  ${\bf CDF}$.
The excellent electromagnetic energy resolution was chosen for optimizing
the $h\rightarrow\gamma\gamma$ and $h\rightarrow Z^{(*)}Z^{(*)}$ detection
studies.
Since these channels were found not to be significant with the Higgs mass
range and integrated luminosity considered, such electromagnetic
resolution is not essential to the remainder of this study.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Z + h
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{$Z(\rightarrow\ell\bar{\ell})h(\rightarrow {b\bar{b}})$}

The signal considered is $Z + h, Z\rightarrow \nu\bar{\nu}, e^+e^-,$ or
$\mu^+\mu^-$,
and $h\rightarrow b\bar{b}$.  In the SM, $BR(h\rightarrow b\bar{b})$ = .83
(.65) for $M_h$ =
80 (120) GeV.   The $Z$ boson decays to the lepton final states
$\nu\bar{\nu},e^+e^-,$ and $\mu^+\mu^-$
with a branching ratio $\approx 27\%$.

The kinematic cuts requested for the leptons are:
\begin{itemize}
\item $p_{t}^{\ell} >$ 20~GeV, $|\eta^{\ell}| <$ 2.5,
 and~ $ |M_{\ell\bar{\ell}}-M_Z | <$ 5 GeV, for
$Z\rightarrow\ell\bar{\ell}, \ell=e,\mu,$ and
\item $\slashchar{E}_{t} >$ 20~GeV, for $Z\rightarrow\nu\overline{\nu}$.
\end{itemize}


We also require the reconstruction of 2 jets $j$,
where $j$ is defined in the standard manner
with R~=~.6 as the jet cone size, such that:

\begin{itemize}
\item $E_{t}^{j} >$ 20~GeV and $|\eta^{j}| <$ 2.5.
\end{itemize}

In addition, one can demand a $|\cos\theta^*|$ distribution for the
jets, where
$\theta^*$ is the decay angle of the jets in the jet--jet rest frame,
that is consistent with higgs decay.  We find that, after the previous cuts,
such an additional cut is not effective and only reduces the significance
of the signal.

Each jet $j$ is required to pass a single or double heavy flavor tag, where
the efficiencies for tagging $b$--jets, $c$--jets, and $g,u,d,s$--jets as
$b$--jets
are (${\epsilon}_{b}^{b},{\epsilon}^{b}_{c},{\epsilon}^{b}_{j}$).
We considered several sets of tagging efficiencies for both tagging
scenarios.
In this paper, we only report results for one scenario, (40\%,5\%,1\%).
We think this number is quite reasonable, since the
optimal tagging efficiency will result from a combination of
impact parameter, soft lepton, multivariate regression analysis,
and other techniques.
Recently, CDF estimated their b-tagging efficiency to be ${\epsilon}_{b}^{b}
\approx$ .22
\cite{CDFTop}.

The backgrounds considered are:

\begin{itemize}
\item $Z(\rightarrow\ell\bar{\ell}) j_1 j_2$, where $j_1$,$j_2$ are any
combination of $g,u,d,s,c,$ or $b$ (and their anti-particles),
\item $Z(\rightarrow\ell\bar{\ell})Z(\rightarrow b\bar{b})$, and
\item $t\bar{t}\rightarrow bW^+ \bar{b}W^-$.
\end{itemize}
The $W$-bosons produced in $t$--decay are allowed to decay to leptons or jets.

We emphasize that the $Zj_1 j_2$ background includes $Zbj$ and
$Zcj$ (where $j$ is specifically $g,u,d,s$ and their anti-particles)
final states which are single tagged with efficiency $\simeq
{\epsilon}_{b}^{b}$ and
${\epsilon}^{b}_{c}$ and double tagged with an efficiency
${\epsilon}_{b}^{b}\times{\epsilon}^{b}_{j}$ and
${\epsilon}^{b}_{c}\times{\epsilon}^{b}_{j}$, respectively.
In Table 1(a) we list the signal and background for various hadron colliders,
using a single $b$--tag at a 2 TeV \mbox{p--$\overline{\rm p}$~} collider and a
double $b$--tag for
a 4 TeV and 14 TeV p--p collider, assuming 30 fb$^{-1}$ of integrated
luminosity.  The cross sections listed are those after all
cuts and $b$--tag requirements.  We also show the Gaussian width of the
reconstructed signal and the significance.

Once a candidate bump is detected in the invariant mass spectrum of
the reconstructed $b\bar{b}$ pair,
the ``signal'' is the number of excess events over a smooth --
relatively flat -- background
within $\pm 2~ \sigma_M$ of the central value of the bump, where $\sigma_M$ is
the Gaussian width of the observed signal.
%
For $M_h =$ 80 (120) GeV, $\sigma_M$
$\simeq$ 5.5 (7.2) GeV.

As pointed out by Gunion and Han \cite{gunion},
the semi--leptonic decays of the $b$-- and
$c$--quarks affect the reconstructed invariant mass of the $b$-quark pair
from $h$ decay.  In addition, final state showering will have an affect.
{}From a full analysis of the fragmentation and decays of $h\rightarrow
b\bar{b}$ using
JETSET 7.4 \cite{jetset}, we find that the peak of the invariant mass
distribution is nearly the
same as for $h\rightarrow{q}\bar{q}$, where $q$ is a light quark,
but the shape is skewed to lower values.
The average of the distribution is typically \mbox{3--4~GeV} below the peak.
We feel that a $b$--jet reconstruction algorithm can be developed based on
our knowledge of the $B$--meson mass and lifetime, the $b$--quark fragmentation
function, the kinematics of semi--leptonic decays and a measurement of
the $\slashchar{E_t}$.  If uncorrected, we find that tighter cuts on the
non--Gaussian invariant mass distribution retain a signal with a significance
reduced by 8--10\%.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% W + h
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{$W(\rightarrow\ell\nu)h(\rightarrow {b\bar{b}})$}

The signal considered is $W + h, W\rightarrow e\nu_e$ or $\mu\nu_\mu$,
and $h\rightarrow b\bar{b}$.
The $W$ boson decays to $e\nu_e$ and $\mu\nu_{\mu}$
with a branching ratio $\approx 2/9$ = .22\%.

The kinematic cuts requested for the leptons are:
\begin{itemize}
\item $p_{t}^{\ell} >$ 20~GeV and $|\eta^{\ell}| <$ 2.5, $\ell = e,\mu$, and
\item $\slashchar{E}_{t} >$ 20~GeV.
\end{itemize}

The same jet and tagging requirements are used as previously stated.
The backgrounds considered are:
\begin{itemize}
\item $W^{\pm}(\rightarrow\ell^{\pm}\nu)j_1 j_2$,
where $j_1 j_2$ are any combination of $g,u,d,s,c,$ or $b$ (and their
anti--particles),
\item $W^{\pm}(\rightarrow\ell^{\pm}\nu)Z(\rightarrow b\bar{b})$,
\item $t\bar{t}\rightarrow bW^+\bar{b}W^-$, and
\item
$q\overline{q}^{'}\rightarrow W^{*}\rightarrow t\bar{b}\rightarrow
b\bar{b}W^{\pm}(\rightarrow\ell^{\pm}\nu)$.
\end{itemize}

The $W$--bosons from $t$--decay are allowed to decay to leptons or jets.

In Table 1(b), we summarize the results for various hadron colliders in the
same manner as for the $Z(\rightarrow\ell\bar{\ell})h(\rightarrow b\bar{b})$
channel.
In Figure 1(a), we show a simulation of the signal and the
background, with the background subtracted, in this channel for
$M_h \simeq M_Z$ at a 2 TeV \mbox{p--$\overline{\rm p}$~} collider with an
integrated luminosity
of 30 fb$^{-1}$.  In this figure, we have applied a single $b$-tag to
all events.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% tau signal
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{$W/Z(\rightarrow jj)h(\rightarrow\tau^{+}\tau^{-})$}

The final signal considered here is $W/Z + h, W/Z\rightarrow$ jets,
$h\rightarrow\tau^{+}\tau^{-}$.
In the SM, the $BR(h\rightarrow\tau^{+}\tau^{-}$) is
.080 (.067) for $M_h$ = 80 (120) GeV.
For this channel, we do not use the leptonic decays of the
heavy gauge bosons to reduce backgrounds, but, rather, the fact that
$\tau$ decays have a low multiplicity of secondaries and can
produce a large $\slashchar{E_t}$.  The dominant $\tau$
decay modes are:
\begin{itemize}
   \item $BR(\tau^{\pm}\rightarrow\ell^{\pm}\nu_\ell\nu_\tau) \simeq 35\%, \ell
= e,\mu$, and
   \item $BR(\tau^{\pm}{\rightarrow}h^{\pm} + \ge 0$~ neutrals $)\simeq 50\%$,
\end{itemize}
where $h^{\pm}$ includes $\pi^{\pm}, \rho^{\pm}$, and $K^{\pm}$.
The remaining significant decay modes contain 3 charged pions and zero or more
neutral particles.

Since the $\tau$ pairs produced from $h$ decay are extremely energetic
compared to $m_\tau$ and have low multiplicities,
the decay products of each $\tau$ travel nearly in the same
direction as the parent $\tau$.
Therefore,
the measurement of the momentum of the secondary charged track determines,
to high accuracy, the
primary $\tau$'s direction of motion.  The measured
$\slashchar{E_t}$ vector, projected onto the charged track's direction,
determines the full $p_t$ of the $\tau$.
Given the $p_t$ of the $\tau$ and assuming all the decay products point
in the direction of the observed charged track (which is also, by assumption,
the moving direction of the $\tau$), we fully reconstruct the $\tau$
momentum.  The reconstruction works much better if the $\tau$ pair system
is boosted, thereby removing the possibility that the $\slashchar{E_t}$ of
the neutrinos totally destructively interfere.

Once the momentum of the
$\tau$'s has been reconstructed in this method, the validity of the
approximation can be tested.  Taking, for example,
the case $\tau^{\pm}\rightarrow\pi^{\pm}\nu_\tau$,
the goodness of the reconstruction is tested by evaluating
$\cos\delta = 1-\frac{m_\tau^2}{E_{\pi}E_{\nu}}$ for each $\tau$, where
$E_\nu$ and $E_\pi$ are the energies of the reconstructed
neutrino and measured charged track,
respectively.  The $\tau$ with the smallest value of $\cos\delta$ has been
reconstructed more poorly than the other.  For this $\tau$, the
$\slashchar{E_t}$ should not be projected onto the charged track's
direction of motion, but, rather, onto a vector lying on a cone with
opening angle $\delta$ with respect to the charged track.  By proceeding
in this manner and choosing the neutrino direction of motion on this
cone that minimizes
the invariant mass of the $\tau$ pair, a better estimate is made of the
invariant mass.  This method is just a crude attempt at obtaining a
better measurement of $m_{\tau^{+}\tau^{-}}$, and a more detailed algorithm
will do better.

Since a good measurement of $\slashchar{E_t}$ is needed, we do not consider the
leptonic decays of the $W$ or the neutrino channels of the $Z$, but, instead,
reconstruct the $W$ or $Z$ in jets.  Fortunately, this still leads to a
detectable signal.
Concentrating on the one-prong final states of the $\tau$, there are
$\tau^{+}\tau^{-}$ final states $\ell^{+}\ell^{-}$, $\ell^{+}\pi^{-}$,
$\pi^{+}\ell^{-}$, and $\pi^{+}\pi^{-}$.  Here, and in the
following discussion, $\ell$ refers to $e$ or $\mu$, while $\pi$ includes
$\rho$ and $K$ mesons.
The previously discussed channels all contained a high $p_t$
charged lepton, $\slashchar{E_t}$, or combination of these to use as a
trigger.  It is reasonable that a combination of $\slashchar{E_t}$ and
the isolation of the $\pi$ from neighboring hadronic activity can be used to
trigger on the $\pi^+\pi^-$ final states.  We considered two cases, without and
with an isolated $\pi$ trigger.  The $\ell^+\ell^-$, $\ell^+\pi^-$,
and $\pi^+\ell^-$ final states
have a combined branching ratio of .47, while including the $\pi^+\pi^-$
final states increases this to .72.


Each event must contain at least 2 jets $j$,
defined with R = .6, and 2 reconstructed
$\tau$'s
satisfying the
following requirements:
\begin{itemize}
\item $E^j_t >$ 15 GeV, $|\eta^j| <$ 2.5,
\item $M_{W}  - 15$ GeV $< M_{jj} < M_{Z} + 15$ GeV,
\item $p_{t}^{\tau} >$ 20~GeV and $|\eta^{\tau}| <$ 2.5,
\item $\slashchar{E}_{t} >$ 20~GeV, and
\item  $m^{(lo)}_T>$ 20~GeV, $m^{(hi)}_T>$ 40~GeV,
where $m_T$ is the transverse
mass of the leptons or hadrons from the $\tau$ decays and $\slashchar{E_t}$,
and $(lo)$ and $(hi)$ refer to the smaller and larger values of $m_T$.
\end{itemize}

The one-prong decays of the $\tau$ are reconstructed
by finding a
charged track $(t)$,
with $p^{(t)}_t >$ 5 GeV, $|\eta^{(t)}|<$ 2.5,
pointing to the center of a narrow calorimeter
bump, so that
$\Delta R_{(t)j} \le $ .15.
$m_{\tau^{+}\tau^{-}}$ is reconstructed by projecting
the measured $\slashchar{E}_{t}$
onto the two charged tracks, as explained previously,
keeping only those events
that give a positive magnitude for the reconstructed $p^{\tau}_t$.

The backgrounds are events with
two leptons or one lepton and a jet that fakes the hadronic decay of a $\tau$,
a large $\slashchar{E}_{t}$, and a combination of jets that give an invariant
mass near the $W$ or $Z$ mass.
The jet that fakes the hadronic decay of a $\tau$
must not only have a single charged
track pointing to the core of its calorimetric cluster, but also
a $\slashchar{E}_{t}$ component pointing in its direction.
We ignore the possibility of a large fake $\slashchar{E}_{t}$
measurement because this is kinematically limited by the beam
energy and $|\eta|$ coverage of the forward calorimeter.  Even if a jet
with the
beam energy were lost ``down the beam--pipe'',
the maximal $\slashchar{E_t} =
E_{\rm beam}\sin\theta \simeq \frac{1}{2}E_{\rm beam}\exp^{-|\eta|}$, for
small $\theta$ measured from the beam--pipe.  All the backgrounds considered,
then, have at least one neutrino from the decays of $W$'s or $Z$'s.

The backgrounds considered are:
\begin{itemize}
\item $W^{\pm}(\rightarrow jj)Z(\rightarrow\tau^{+}\tau^{-})$,
\item $Z(\rightarrow jj)Z(\rightarrow\tau^{+}\tau^{-})$,
\item $t\bar{t}\rightarrow\ell$ + jets or $\ell\ell^{'}$ + jets, where
$\ell,\ell^{'} =
e,\mu,\tau$,
\item $W^{\pm}(\rightarrow\ell^{\pm}\nu)$+jets, where $\ell=e,\mu,\tau$, and
\item $Z(\rightarrow\tau^{+}\tau^{-})jj$.
\end{itemize}

The probability that a jet is tagged as a $\tau$ is estimated,
very conservatively, at 5\%,
based on a particle--level
simulation including fragmentation.  This estimate relies only on
the charged track multiplicity, not on a shower--shape analysis, which
could significantly reduce this number \cite{atlas}.
The $t\bar{t}$ and $W^{\pm}$ + jets
backgrounds are estimated by first finding a candidate jet that can fake
the hadronic decay of the $\tau$, then multiplying the final event rate by
this probability.
The decay $b\rightarrow c\tau\nu_\tau$ is
included in the JETSET  decay tables, which were used in
estimating the jet misidentification probability for $b$--,$c$-- and
light quarks and gluons.


We considered the scenario where only the leptonic $\tau$ decays can be
used as a trigger ($\ell$ trigger) and where the single-charged track decays
can be used as well ($\pi$ trigger).  The results presented assume
an isolated $\pi$ trigger.  The loss of significance of the signal
in using only the
$\ell$ trigger is typically 35\%.
Because of the importance of the resonant background
$Z(\rightarrow\tau^{+}\tau^{-})jj$,
the significance of the signal is calculated using MINUIT \cite{minuit}, which
accounts for the shape of the signal and background.
We stress that this background will be
normalized to high accuracy by observed $e^+e^- jj$ and $\mu^+\mu^- jj$ events
and assuming lepton universality.
In Table 1(c), we summarize our significance results for various
hadron colliders
by presenting the number of signal events for 30 fb$^{-1}$ of data
and the error on this number as determined by a functional fit to
the signal and background.
The significance is the ratio of these numbers, which
correspond to
$S$ and $\sqrt{B}$ in the previous discussion of significance.
We do not present results
for $M_h \simeq M_Z$ or for a collider with $\sqrt{\rm s~}$ = 14 TeV, since,
for those cases, a significant signal could not be found in this
channel.
In Figure 1(b), we show a simulation of the signal and the
background, with the background subtracted, in this channel for
$M_h$ = 120~GeV at a 2 TeV \mbox{p--$\overline{\rm p}$~} collider with an
integrated luminosity
of 30 fb$^{-1}$.

Since $\tau$ signatures at hadron colliders have not been well-studied,
we suggest several improvements
which will increase the significance of
this channel once they are included:
\begin{itemize}
  \item A better estimate of jet rejection will eliminate
backgrounds to the hadronic $\tau$ decay modes.
  \item Incorporating the correct polarization for $\tau$ decays
      may be useful, since $\tau$'s from $h$ decay
      lead to a {\it soft-soft} and {\it hard-hard}
      momentum correlation between the
      two charged hadrons.
  \item An impact parameter cut would reduce drastically all but
      the real $\tau$ and
      heavy quark backgrounds.
  \item Inclusion of the 3-prong decays of the $\tau$ will increase the
      signal event rate by 28\%.  Jet backgrounds can be reduced by
      using the kinematic constraint $m_{\pi\pi\pi} < m_\tau$ for the
      three charged tracks $\pi$.
  \item Better mass resolution, based on a more sophisticated $\tau$
      reconstruction algorithm,  will reduce the contribution of
$Z(\rightarrow\tau^{+}\tau^{-})jj$.
  \item If all or some of the above improvements can be realized, the
      direct production process p + p$(\bar{\rm p})\rightarrow
h(\rightarrow\tau^{+}\tau^{-})+X$
\cite{hinchliffe}, which has
      a larger cross section but potentially more backgrounds, may be
      accessible.
\end{itemize}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% combined significance
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{\rm Combined Significance}

The significance of a signal $S$ above a background $B$, $S/\sqrt{B}$ in
the case of large statistics for a signal bump on a flat background, is
a measure of the probability that the background has fluctuated up to
fake the signal.  The probability is the same as exceeding $S/\sqrt{B}$
standard deviations
of a Gaussian probability function.   When combining two signals, where the
probability that the background has fluctuated up to the signal is
$p_1$ and $p_2$, respectively, one has
several options:  (1) use $p_1{\times}p_2$ as the combined probability,
(2) use $\alpha(1-\ln\alpha)$, where $\alpha=p_1{\times}p_2$, as a statistic,
and determine the probability that a second measurement
\mbox{$\alpha^{'}=p_1^{'}\times{p_2^{'}} < \alpha$},
or (3) combine the two signals and backgrounds
as though coming from the same experiment.  Method (1) will reject the
hypothesis that the signal is consistent with background if $p_1$ is very
small, even if $p_2 \simeq 1$.  Method (2) compensates for this by sampling
all combinations of $p_1$ and $p_2$ that could lead to a given
$\alpha=p_1\times{p_2}$.  Method (3) treats the two measurements as
independent data sets which are used to test the hypothesis that the
signal is consistent with background in exactly the same way.
Methods (1) and (2) will differ significantly only in extreme cases, which
are not present in this analysis.
%
For the cases when all channels
yield a significance $\sim$ 5, we simply use method (3); otherwise,
we use method (1), since we desire a high
significance in only one channel.

Figure 2 shows the combined significance of all channels considered in this
study as a function of $M_h$.  Figure 2 contains three
graphs, one for each hadron collider option, and each graph contains two
separated bands, which are further divided by different shadings.
The upper bands show the significance for an integrated luminosity of
30~fb$^{-1}$, the lower bands for 10~fb$^{-1}$.
The dark shading shows the range of significance
from varying the $Q^2$ scale of the
Electroweak-QCD background processes from $\bar{m}_T^2$ to $\hat{s}/2$.
$\bar{m}_T^2$ is the square of the average transverse mass ${m_T}_j$
of the outgoing
partons $j$ of mass $m_j$,
${m_T}_j = \sqrt{{p_T}_j^2 + {m}_j^2}$, and $\hat{s}$ is the
invariant mass of the hard-scattering parton process.  The lower bound of
the dark band corresponds to $Q^2 = \bar{m}_T^2$, the upper bound to
$Q^2 = \hat{s}/2$.  For example, at a $\sqrt{\rm s~}$ = 2~TeV hadron collider
with
and integrated luminosity ${\cal L} = 30~$fb$^{-1}$, the significance of
the signal for $M_h = 100$~GeV varies from 7.3 to 8.3 by choosing
$Q^2 = \bar{m}_T^2$ or $\hat{s}/2$.
Also, when radiative corrections are applied, typically the shape of
kinematic distributions of a given process are
only slightly changed, but the
magnitude of the distribution is scaled by a ``K--factor''.
The light shading shows the range of significance
from multiplying the signal by a
``K-factor'' of 1 to 1.2.  Therefore, the absolute lower bound for
each band in Figure 2 corresponds to $Q^2 = \bar{m}_T^2$ and K=1,
the absolute upper bound to $Q^2 = \hat{s}/2$ and K=1.2.

Several comments concerning the results presented in
Figure 2 are in order.  First, the $Q^2$ dependence
of the $W/Zjj$ backgrounds, which arises in evaluating the structure functions
$f_i(x,Q^2)$
and $\alpha_s(Q^2)$, is more important at a lower energy collider \cite{han}.
Since the
kinematic cuts have been chosen to accept the signal efficiently, it is
expected that the background which passes these same cuts has a topology
similar to the signal with the Higgs resonance replaced by an off-shell gluon.
In this case, a choice of $Q^2 = \hat{s}/2$ is better motivated than
$\bar{m}_T^2$.  Secondly, the $W,Z(\rightarrow
q\bar{q})h(\rightarrow\tau^{+}\tau^{-})$ channel increases
the reach of the lower energy colliders.  The increase of the $Zjj$,
$t\bar{t}$,
and $W$ + jet backgrounds and the decrease in importance of the
p + p $\rightarrow W/Z + h$ processes make a signal in this channel
untenable at \mbox{$\sqrt{\rm s~}$ = 14 TeV}.
Of course, higher luminosity and consideration of p + p $\rightarrow
h(\rightarrow\tau^{+}\tau^{-}) + X$
might change this conclusion.
Finally, though for brevity not presented here,
we also
considered a 4 TeV \mbox{p--$\overline{\rm p}$~} hadron collider.
For the same integrated luminosity,
a 4 TeV \mbox{p--$\overline{\rm p}$~} collider has a significance $\sim$
20--30\% higher than
a 4 TeV p--p collider.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% studying the Higgs properties
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{\rm Studying Higgs Properties}

Ideally, it would be possible not only to detect a Higgs boson, but also to
study its properties, establish that it interacted like a Higgs boson, and
even distinguish $h_{SM}$ from $h_{SUSY}$.
%\cite{kane3}.
Showing that the spin of a
detected $h$ is zero will not be hard.
%
The important observables at a hadron collider are of the form
$\sigma\times BR$.  The full width $\Gamma_h$, for example, is
probably too narrow
to overcome experimental resolution.  Using the decay modes
discussed in this paper,
the following set of equations can be written:

\[
\begin{array}{ccc}
{\cal{L}}\times\sigma_{Wh}\times BR_b      & = & N_b \\
{\cal{L}}\times\sigma_{Wh}\times BR_{\tau} & = & N_{\tau} \\
BR_b + BR_{\tau}            & \approx & 1, \\
\end{array}
\]
where $\sigma_{Wh}$ is the cross section for the associated production
of $h$ with $W$ or $Z$, $BR_b$, $BR_\tau$ are the branching ratios for
$h(\rightarrow b\bar{b})$ and $h(\rightarrow\tau^{+}\tau^{-})$, respectively,
and
${\cal{L}}$ is the integrated luminosity of the collider in units of
inverse cross section.
Solving these equations allows us to write ${\cal{L}}\times
\sigma_{Wh} = N_b + N_\tau$.
$N_i$ is the number of $i$ type events corrected for reconstruction
efficiencies, tagging efficiencies, etc.
%
{}From the number of observed events
at a hadron collider, it will be possible to measure $g^2_{WWh}\times{BR_b},
g^2_{ZZh}\times{BR_b}, g^2_{WWh}\times{BR_\tau}$,
and $g^2_{ZZh}\times{BR_\tau}$.
The ratio $BR_\tau/BR_b$ is predicted to be $\frac{m^2_\tau}{3 m^2_b(M_h)}
\simeq \frac{1}{9}$ for any gauge theory, since $b$ and $\tau$ are in the
same position in any doublet; thus its measurement could establish that a
detected
boson was indeed coupling proportional to mass, but could never distinguish
among theories.  Similarly, since
$BR_\mu/BR_\tau = m^2_\mu/m^2_\tau \simeq\frac{1}{300}$, no excess of
events should be seen in $\mu^+\mu^-$ final states.  Given $BR_b/BR_\tau$,
the equality of the $WWh$ and $ZZh$ couplings could be checked at a 2 TeV
hadron collider.

We have not found a way to measure the $t\bar{t}h$ or $c\bar{c}h$
coupling at a low energy hadron
collider; the first of them can be measured at LHC,
which
corresponds to the $\sqrt{\rm s~}$ = 14 TeV collider considered here but with
an instantaneous luminosity of $L = 10^{34}$cm$^{-2}$s$^{-1}$,
and NLC.  Measuring the
$t\bar{t}h$ or $c\bar{c}h$ coupling could, in principle, distinguish among
theories, since the relative coupling of $T_3 = \pm\frac{1}{2}$ states
{\it does} depend on the theory, though in constrained SUSY theories these
couplings are expected to be very close to their SM values.
The important $\gamma\gamma$ coupling, with $BR \simeq 10^{-3}$, can only be
measured at LHC, where the cross section and luminosity are both large,
or at a photon collider.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%   conclusions
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section{\rm Conclusions}

Developing the ability to do $\tau$ physics at a hadron collider is a
natural extenstion of the present ability to do heavy quark physics, and
can have a significant impact on the ability to do Higgs physics at a
hadron collider.

We see from Tables 1(a)--(c) and Figure 2 that
the detection or exclusion of $h$ for $M_h ~{\stackrel{\scriptstyle
<}{\scriptstyle \sim}}~ 130$~GeV is not only
possible at a 2 TeV high luminosity \mbox{p--$\overline{\rm p}$~} collider
(10--30 fb$^{-1}$),
it is competitive with -- if not better than --
hadron colliders at a higher $\sqrt{\rm s~}$,
because of the relative behavior of signal and
backgrounds.
%
%
The $W,Z(\rightarrow{jj})h(\rightarrow\tau^{+}\tau^{-})$ channel is the
strongest far enough above
$M_h \simeq M_Z$; near $M_Z$, the $W(\rightarrow\ell\nu)h(\rightarrow
b\bar{b})$ and
$Z(\rightarrow\ell\ell)h(\rightarrow b\bar{b})$ channels are adequate.  It is
probably possible to
detect $h$ above 130~GeV, but more analysis is needed to establish that.
%
The ratio of $\tau^{+}\tau^{-}$ and $b\bar{b}$ branching ratios and the ratio
of the couplings
of $h$ to $WW$ and $ZZ$ can be measured at a 2 or 4 TeV hadron collider.
The $t\bar{t}h$ coupling and the $\gamma\gamma$ branching ratio will probably
only be accessible at LHC or NLC.

Our analysis shows that a \mbox{p--$\overline{\rm p}$~} collider with
$\sqrt{\rm s~}$ = 2~TeV and integrated
luminosity ${\cal L} ~{\stackrel{\scriptscriptstyle >}{\scriptscriptstyle
\sim}}~$ 10 fb$^{-1}$ can detect or exclude a Higgs boson
with a mass ranging from the present upper limit up to about 130 GeV (and
perhaps higher), thus covering the region of greatest interest.  This is
a remarkable physics opportunity.


%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%  bibliography
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\begin{references}
%%%%
\bibitem{langacker} P. Langacker and Ming--Xing Luo, Phys. Rev. {\bf D44}
(1991) 2433, and U. Amaldi, W. de Boer, and H. Furstenav, Phys. Letts.
{\bf B260} (1991) 447.
%%%%
\bibitem{cabi} N. Cabibbo, L. Maiani, G. Parisi and R. Petronzio,
Nuc. Phys. {\bf B158} (1979) 447.
%%%%%%
\bibitem{espinosa} J.R. Espinosa and M. Quiros, Phys. Lett. {\bf B302} (1993)
51, and
G.L. Kane, C. Kolda, and J.D. Wells, Phys. Rev. Letts.
{\bf 70},
No. 18 (1993) 2686.
%%%%%
\bibitem{kane2} G.L. Kane, C. Kolda, L. Roszkowski, and J.D. Wells,
UM--TH--93--24 (1993), Phys. Rev. {\bf D} in press; see also J.L. Lopez et al,
Phys. Lett. {\bf B 306} (1993) 73, and references within.
%%%%%
\bibitem{marciano} A. Stange, W. Marciano,
and S. Willenbrock, ILL--(TH)--94--8.
%%%%%
\bibitem{gunion} J.F. Gunion and T. Han, UCD--94--10.
%%%%%%
%\bibitem{LEPI} The L3 Collaboration, Phys. Letts. {\bf B 303} (1993) 391.
%
%\bibitem{LEPII}  B. Zhou, $\cdots$, CERN-PPE/93--28.
%\bibitem{snowmass} Snowmass 86
%%%%%
\bibitem{papageno} I. Hinchliffe, LBL--34372, June 1993.
%%%%
\bibitem{pythia} H.--U. Bengtsson and T. Sj\"{o}strand,
Computer Physics Commun. {\bf 46} (1987) 43.
%%%%%%
\bibitem{CDF} The CDF Collaboration, Phys. Rev. Letts. {\bf 71}, No. 15
(1993) 2396, and Phys. Rev. Letts. {\bf 71}, No. 21 (1993) 3421.
%%%%%
\bibitem{jetset} T. Sj\"{o}strand and M. Bengtsson,
Computer Physics Commun.
{\bf 43} (1987) 367.
%%%%%
\bibitem{CDFTop} The CDF Collaboration, FERMILAB--PUB--94/097--E, May 1994.
%%%%%
%\bibitem{dawson} S. Dawson, Producing the Intermediate Mass Higgs Boson --
%this is from the book you edited.
%\bibitem{kane3} G.L. Kane, Perspectives in Higgs Physics, ed. G.L. Kane,
%World Scientific Publishing (1992).
%%%%%%
\bibitem{atlas} D. Cavalli, L. Cozzi, L. Perini, and P. Pronesti,
{\it ATLAS Internal Note}, PHYS--NO--025, 30 April 1993.
\bibitem{minuit} F. James and M. Roos, {\it MINUIT--Users Guide},
CERN Program Library entry D506. CERN, 1981.
%%%%
\bibitem{hinchliffe} R.K. Ellis, I. Hinchliffe, M. Soldate, and J.J. van der
Bij, Nucl. Phys. {\bf B297} (1988) 221--243.
%%%
\bibitem{han} V. Barger, T. Han, J. Ohnemus, and D. Zeppenfeld,
Phys. Rev. {\bf D40}, No. 9 (1989) 2888.
\end{references}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% the tables
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\newpage
%
%  Begin table 1
%
\setcounter{table}{0}
\begin{table}[htb]
\caption{(a) Sensitivity for the
$Z(\rightarrow\ell\bar{\ell})h(\rightarrow b\bar{b})$ channel}
\begin{center}
\begin{tabular}{||l|c|c|c|c|c|c||}
\tableline\tableline
 & Mass (GeV) &  80 &  90 & 100 & 110 & 120 \\
%
   &   $\sigma_M$ (GeV)           & 5.5 & 6.0 & 6.5 & 7.0 & 7.4 \\ \tableline
%
Cross Section (fb) &
SM Higgs     &    23. &    18. &    14. &    11. &  7. \\
%
$\sqrt{\rm s~}$ = 2 TeV, \mbox{p--$\overline{\rm p}$~} &
Backgrounds   &   242. &   246. &   212. &   176. &   152.   \\ \cline{1-7}
%
S/$\sqrt{\rm B}$ for 30 fb$^{-1}$   &
      1 Tag  &   8.0 &   6.2 &   5.0 &   4.2  &  3.0   \\
\tableline\tableline
%
%  Continue table 1
%
Cross Section (fb) &
SM Higgs     &    9.1 &    7.0 &    5.2 &    3.8 &   2.6  \\
$\sqrt{\rm s~}$ = 4 TeV, p--p  &
Backgrounds     &  56. &  62. &   52. &  43. &   40.  \\ \cline{1-7}
S/$\sqrt{\rm B}$ for 30 fb$^{-1}$
&     2 Tags  &   6.7 &   4.8 &   4.0 &   3.1 &   2.3       \\
\tableline\tableline
%
%  NOW LHC
%
Cross Section (fb) &
SM Higgs     &   40.0 &   32.0 &   25.4 &  19.4 &  13.4  \\
$\sqrt{\rm s~}$ = 14 TeV, p--p & Backgrounds    & 494. &  552. &  508. &  459.
&  449. \\
\tableline
S/$\sqrt{\rm B}$ for 30 fb$^{-1}$ &
     2 Tags  &   9.7 &   7.4 &   6.2 &  5.0 &  3.5  \\
\tableline\tableline
\end{tabular}
\end{center}
\end{table}
%
%  Begin table 2
%
\setcounter{table}{0}
\begin{table}[htb]
\caption{(b) Sensitivity for the
$W(\rightarrow\ell\nu)h(\rightarrow b\bar{b})$ channel}
\begin{center}
\begin{tabular}{||l|c|c|c|c|c|c||}
\tableline\tableline
 & Mass (GeV) &  80 &  90 & 100 & 110 & 120 \\
%\cline{2-7}
   &   $\sigma_M$ (GeV)           & 5.5 & 6.0 & 6.5 & 7.0 & 7.4 \\ \cline{1-7}
Cross Section (fb) &
SM Higgs     &    26. &    20. &    15. &    11. &     7.   \\
$\sqrt{\rm s~}$ = 2 TeV, \mbox{p--$\overline{\rm p}$~} &
Backgrounds     &   303. &   303. &   272. &   240. &  207.   \\ \tableline
S/$\sqrt{\rm B}$ for 30 fb$^{-1}$
 &   1 Tag  &   8.1 &   6.1 &   4.8 &   3.8 &   2.7   \\
\tableline\tableline
Cross Section (fb) &
SM Higgs     &    10.5 &  7.9 &  6.0 &  4.4 &  2.9   \\
$\sqrt{\rm s~}$ = 4 TeV, p--p &
Backgrounds     &   42. &   48. &   41. &   36. &   34.   \\ \tableline
S/$\sqrt{\rm B}$ for 30 fb$^{-1}$
 &     2 Tags  &   8.8 &   6.2 &   5.2 &   4.0 &   2.8        \\
\tableline\tableline
%
Cross Section (fb) &
SM Higgs     &   41.3 &   32.2 &   26.1 &    20.0 &   13.8  \\
$\sqrt{\rm s~}$ = 14 TeV, p--p  &
Backgrounds   &  458. &  518. &  511. &  520. &  540.  \\   \tableline
S/$\sqrt{\rm B}$ for 10 fb$^{-1}$  &
    2 Tags  &  10.5 &   7.8 &   6.4 &  4.9 &   3.3   \\
\tableline\tableline
\end{tabular}
\end{center}
\end{table}
%
% Begin Table 3
%
\setcounter{table}{0}
\begin{table}[htb]
\caption{(c) Sensitivity for the
$Z/W(\rightarrow{jj})h(\rightarrow\tau^{+}\tau^{-})$ channel}
\begin{center}
\begin{tabular}{||l|l|c|c||}
\tableline\tableline
                  & Mass (GeV)  &  110 & 120 \\
\tableline\tableline
$\sqrt{\rm s~}$ = 2 TeV   & Signal Events                & 83.8 & 47.3 \\
%\cline{2-4}
\mbox{p--$\overline{\rm p}$~}           & Error on Signal              & 14.5 &
 9.1 \\
%\cline{2-4}
\tableline
${\cal L} = 30$ fb$^{-1}$     & Significance                 &  5.8 & 5.2  \\
\tableline\tableline
$\sqrt{\rm s~}$ = 4 TeV   & Signal Events                &  127.5&  72.1   \\
%\cline{2-4}
p--p             & Error on Signal              &   30.2&  23.7   \\
%\cline{2-4}
\tableline
${\cal L} = 30$ fb$^{-1}$     & Significance                 &  4.2 &   3.0
\\
\tableline\tableline
\end{tabular}
\end{center}
\end{table}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%  the figures
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\setcounter{figure}{0}
\begin{figure}[htb]
   \hspace*{1.2in}
%
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
%%\psfig{file=mbb.ps,height=3.3in,width=3.5in,bbllx=0bp,bblly=114bp,bburx=571bp,bbury=716bp,clip=}
   \caption{(a) $W(\rightarrow\ell\nu)h(\rightarrow b\bar{b})$ signal.  We show
the case
$M_h \simeq M_Z$ to illustrate the ability to discriminate $h$ from $Z$.}
\end{figure}
%
\setcounter{figure}{0}
\begin{figure}[htb]
   \hspace*{1.2in}
%
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
%%\psfig{file=tau2.ps,height=3.3in,width=3.5in,bbllx=0bp,bblly=114bp,bburx=571bp,bbury=716bp,clip=}
   \caption{(b) $W/Z(\rightarrow jj)h(\rightarrow\tau^{+}\tau^{-}$) signal.
$M_h = 120$ GeV.}
\end{figure}
%
%
\setcounter{figure}{1}
\begin{figure}[htb]
   \hspace*{1.2in}
%
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
%%\psfig{file=significance.ps,height=3.3in,width=3.5in,bbllx=0bp,bblly=114bp,bburx=571bp,bbury=716bp,clip=}
   \caption{Combined significance.  See the text for details.}
\end{figure}
%
%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% acknowledgements
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\acknowledgements

S.M. thanks N. Longley, X. Shi, and J. Urheim for informative discussions.
This research is supported by the U.S. DOE.

%
\end{document}
%!PS-Adobe-2.0
%%Title: paw.pst (Portrait A 4)
%%Pages: atend
%%Creator: HIGZ Version 1.20/11
%%CreationDate: 94/06/01   16.45
%%EndComments
/s {stroke} def /l {lineto} def /m {moveto} def /t { translate} def
/sw {stringwidth} def /r {rotate} def /rl {roll} def
/d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def
/c {setrgbcolor} def /lw {setlinewidth} def /sd {setdash} def
/cl {closepath} def /sf {scalefont setfont} def
/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def
/bl {box s} def /bf {box f} def
/mp {newpath /y exch def /x exch def} def
/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def
/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def
/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def
/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def
/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26 {mt s} def
/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def
 /m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def
 /m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d
 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def
 /m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
 4 {side} repeat cl fill gr} def
 /m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
 5 {side} repeat s gr} def /m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d
 x w2 sub y w2 add m w w neg d x w2 sub y w2
 sub m w w d s} def
/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def
/m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def
/reencdict 24 dict def /ReEncode {reencdict begin /nco&na exch def
/nfnam exch def /basefontname exch def /basefontdict basefontname findfont def
/newfont basefontdict maxlength dict def basefontdict {exch dup /FID ne
{dup /Encoding eq {exch dup length array copy newfont 3 1 roll put} {exch
newfont 3 1 roll put} ifelse} {pop pop} ifelse } forall newfont
/FontName nfnam put nco&na aload pop nco&na length 2 idiv {newfont
/Encoding get 3 1 roll put} repeat nfnam newfont definefont pop end } def
/accvec [ 176 /agrave 181 /Agrave 190 /acircumflex 192 /Acircumflex
201 /adieresis 204 /Adieresis 209 /ccedilla 210 /Ccedilla 211 /eacute
212 /Eacute 213 /egrave 214 /Egrave 215 /ecircumflex 216 /Ecircumflex
217 /edieresis 218 /Edieresis 219 /icircumflex 220 /Icircumflex
221 /idieresis 222 /Idieresis 223 /ntilde 224 /Ntilde 226 /ocircumflex
228 /Ocircumflex 229 /odieresis 230 /Odieresis 231 /ucircumflex 236
/Ucircumflex
237 /udieresis 238 /Udieresis 239 /aring 242 /Aring 243 /ydieresis
244 /Ydieresis 246 /aacute 247 /Aacute 252 /ugrave 253 /Ugrave] def
/Times-Roman /Times-Roman accvec ReEncode
/Times-Italic /Times-Italic accvec ReEncode
/Times-Bold /Times-Bold accvec ReEncode
/Times-BoldItalic /Times-BoldItalic accvec ReEncode
/Helvetica /Helvetica accvec ReEncode
/Helvetica-Oblique /Helvetica-Oblique accvec ReEncode
/Helvetica-Bold /Helvetica-Bold accvec ReEncode
/Helvetica-BoldOblique /Helvetica-BoldOblique  accvec ReEncode
/Courier /Courier accvec ReEncode
/Courier-Oblique /Courier-Oblique accvec ReEncode
/Courier-Bold /Courier-Bold accvec ReEncode
/Courier-BoldOblique /Courier-BoldOblique accvec ReEncode
/oshow {gsave [] 0 sd true charpath stroke gr} def
/stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf
 text sw pop xs add /xs exch def} def
/stwb { /fs exch def /fn exch def /nbas exch def /textf exch def
textf length /tlen exch def nbas tlen gt {/nbas tlen def} if
fn findfont fs sf textf dup length nbas sub nbas getinterval sw
pop neg xs add /xs exch def} def
/accspe [ 65 /plusminus 66 /bar 67 /existential 68 /universal
69 /exclam 70 /numbersign 71 /greater 72 /question 73 /integral
74 /colon 75 /semicolon 76 /less 77 /bracketleft 78 /bracketright
79 /greaterequal 80 /braceleft 81 /braceright 82 /radical
83 /spade 84 /heart 85 /diamond 86 /club 87 /lessequal
88 /multiply 89 /percent 90 /infinity 48 /circlemultiply 49 /circleplus
50 /emptyset 51 /lozenge 52 /bullet 53 /arrowright 54 /arrowup
55 /arrowleft 56 /arrowdown 57 /arrowboth 48 /degree 44 /comma 43 /plus
 45 /angle 42 /angleleft 47 /divide 61 /notequal 40 /equivalence 41 /second
 97 /approxequal 98 /congruent 99 /perpendicular 100 /partialdiff 101 /florin
 102 /intersection 103 /union 104 /propersuperset 105 /reflexsuperset
 106 /notsubset 107 /propersubset 108 /reflexsubset 109 /element 110
/notelement
 111 /gradient 112 /logicaland 113 /logicalor 114 /arrowdblboth
 115 /arrowdblleft 116 /arrowdblup 117 /arrowdblright 118 /arrowdbldown
 119 /ampersand 120 /omega1 121 /similar 122 /aleph ] def
/Symbol /Special accspe ReEncode
/Zone {/iy exch def /ix exch def gsave ix 1 sub 2224 mul 1 iy sub 3144
 mul t} def
gsave 20 28 t .25 .25 scale gsave
%%EndProlog
%%Page: number 1
 1 1 Zone
 gsave 0 0 t 0 setgray [] 0 sd 1 lw
 /xs 0 def
(b)
 /Times-Roman   84 stwn
(-)
 /Symbol   84 stwn
(b)
 /Times-Roman   84 stwn
( Mass \(GeV\))
 /Times-Roman   84 stwn
 gsave 1112 507
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   84 sf 0    0 m
(b)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(b)
 show
 currentpoint pop 0 t
 gsave /Times-Roman findfont   84 sf
(b)
 dup length 1 sub 1 getinterval
 stringwidth pop 2 div neg    0 rm
 /Times-Roman findfont   59 sf 0   59 rm
(\261)
 stringwidth pop 2 div neg 0 rm
(\261)
 show gr
 /Times-Roman findfont   84 sf 0    0 m
( Mass \(GeV\))
 show
 gr
 /xs 0 def
(R)
 /Special   84 stwn
(s = 2 TeV, p)
 /Times-Roman   84 stwn
(-)
 /Symbol   84 stwn
(p)
 /Times-Roman   84 stwn
 gsave 1112 2508
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Special findfont   84 sf 0    0 m
(R)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(s = 2 TeV, p)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(p)
 show
 currentpoint pop 0 t
 gsave /Times-Roman findfont   84 sf
(p)
 dup length 1 sub 1 getinterval
 stringwidth pop 2 div neg    0 rm
 /Times-Roman findfont   59 sf 0   59 rm
(\261)
 stringwidth pop 2 div neg 0 rm
(\261)
 show gr
 gr
 /xs 0 def
(Background Subtracted)
 /Times-Roman   68 stwn
 gsave 1112 2365
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(Background Subtracted)
 show
 gr
 /xs 0 def
(Number of Events for 30 fb)
 /Times-Roman   84 stwn
(-1)
 /Times-Roman   59 stwn
 gsave 72 1572
 t  90 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   84 sf 0    0 m
(Number of Events for 30 fb)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   59 sf 0   42 m
(-1)
 show
 gr
 1779 1778 222 683 bl 222 979 m 222 683 l 258 683 l 258 954 l 293 954 l 293
1397
 l 329 1397 l 329 1438 l 365 1438 l 365 683 l 400 683 l 436 683 l 471 683 l 471
 1152 l 507 1152 l 507 1402 l 542 1402 l 542 1003 l 578 1003 l 578 880 l 614
880
 l 614 1426 l 649 1426 l 649 1241 l 685 1241 l 685 683 l 720 683 l 720 935 l
756
 935 l 756 1401 l 791 1401 l 791 2078 l 827 2078 l 827 1420 l 863 1420 l 863
 2126 l 898 2126 l 898 2151 l 934 2151 l 934 2342 l 969 2342 l 969 2013 l 1005
 2013 l 1005 1437 l 1040 1437 l 1040 1321 l 1076 1321 l 1076 1578 l 1112 1578 l
 1112 1588 l 1147 1588 l 1147 717 l 1183 717 l 1183 1713 l 1218 1713 l 1218 924
 l 1254 924 l 1254 683 l 1289 683 l 1289 1024 l 1325 1024 l 1325 1048 l 1360
 1048 l 1360 727 l 1396 727 l 1396 1197 l 1432 1197 l 1432 871 l 1467 871 l
1467
 1097 l 1503 1097 l 1503 958 l 1538 958 l 1538 683 l 1574 683 l 1574 1401 l
1609
 1401 l 1609 683 l 1645 683 l 1645 1022 l 1681 1022 l 1681 889 l 1716 889 l
1716
 1079 l 1752 1079 l 1752 944 l 1787 944 l 1787 829 l 1823 829 l 1823 1106 l
1858
 1106 l 1858 1083 l 1894 1083 l 1894 929 l 1930 929 l 1930 1030 l 1965 1030 l
 1965 979 l 2001 979 l 2001 979 l s 222 979 m 222 979 l 231 979 l 240 979 l 249
 979 l 258 979 l 267 979 l 276 979 l 285 979 l 294 979 l 303 979 l 312 979 l
321
 979 l 330 979 l 339 979 l 348 979 l 357 979 l 366 979 l 375 979 l 384 979 l
393
 979 l 402 979 l 411 979 l 420 979 l 429 979 l 438 979 l 447 979 l 456 979 l
465
 979 l 474 979 l 483 979 l 492 979 l 501 979 l 510 979 l 519 980 l 528 980 l
537
 980 l 546 980 l 555 981 l 564 981 l 573 982 l 582 983 l 591 985 l 600 986 l
609
 988 l 618 991 l 626 995 l 635 999 l 644 1005 l 653 1012 l 662 1020 l 671 1030
l
 680 1043 l 689 1057 l 698 1075 l 707 1095 l 716 1118 l 725 1145 l 734 1175 l
 743 1209 l 752 1248 l 761 1290 l 770 1336 l 779 1386 l 788 1439 l 797 1496 l
 806 1555 l 815 1616 l 824 1678 l 833 1741 l 842 1802 l 851 1863 l 860 1920 l
 869 1973 l 878 2022 l 887 2065 l 896 2101 l 905 2129 l 914 2150 l 923 2162 l
 932 2164 l 941 2158 l 950 2144 l 959 2120 l 968 2089 l 977 2050 l 986 2005 l
 995 1955 l 1004 1900 l 1013 1841 l 1022 1780 l 1031 1718 l 1040 1656 l 1049
 1594 l 1058 1534 l 1067 1475 l 1076 1420 l 1085 1368 l 1094 1319 l 1103 1274 l
 1112 1234 l 1120 1197 l 1129 1164 l 1138 1135 l 1147 1109 l 1156 1087 l 1165
 1068 l 1174 1052 l 1183 1038 l 1192 1027 l 1201 1017 l 1210 1009 l 1219 1003 l
 1228 998 l 1237 994 l 1246 990 l 1255 988 l 1264 986 l 1273 984 l 1282 983 l
 1291 982 l 1300 981 l 1309 981 l 1318 980 l 1327 980 l 1336 980 l 1345 980 l
 1354 979 l 1363 979 l 1372 979 l 1381 979 l 1390 979 l 1399 979 l 1408 979 l
 1417 979 l 1426 979 l 1435 979 l 1444 979 l 1453 979 l 1462 979 l 1471 979 l
 1480 979 l 1489 979 l 1498 979 l 1507 979 l 1516 979 l 1525 979 l 1534 979 l
 1543 979 l 1552 979 l 1561 979 l 1570 979 l 1579 979 l 1588 979 l 1597 979 l
 1606 979 l 1614 979 l 1623 979 l 1632 979 l 1641 979 l 1650 979 l 1659 979 l
 1668 979 l 1677 979 l 1686 979 l 1695 979 l 1704 979 l 1713 979 l 1722 979 l
 1731 979 l 1740 979 l 1749 979 l 1758 979 l 1767 979 l 1776 979 l 1785 979 l
 1794 979 l 1803 979 l 1812 979 l 1821 979 l 1830 979 l 1839 979 l 1848 979 l
 1857 979 l 1866 979 l 1875 979 l 1884 979 l 1893 979 l 1902 979 l 1911 979 l
 1920 979 l 1929 979 l 1938 979 l 1947 979 l 1956 979 l 1965 979 l 1974 979 l
 1983 979 l 1992 979 l 2001 979 l s 222 683 m 222 2461 l s 256 683 m 222 683 l
s
 239 757 m 222 757 l s 239 831 m 222 831 l s 239 905 m 222 905 l s 256 979 m
222
 979 l s 239 1053 m 222 1053 l s 239 1127 m 222 1127 l s 239 1201 m 222 1201 l
s
 256 1276 m 222 1276 l s 239 1350 m 222 1350 l s 239 1424 m 222 1424 l s 239
 1498 m 222 1498 l s 256 1572 m 222 1572 l s 239 1646 m 222 1646 l s 239 1720 m
 222 1720 l s 239 1794 m 222 1794 l s 256 1868 m 222 1868 l s 239 1943 m 222
 1943 l s 239 2017 m 222 2017 l s 239 2091 m 222 2091 l s 256 2165 m 222 2165 l
 s 239 2239 m 222 2239 l s 239 2313 m 222 2313 l s 239 2387 m 222 2387 l s 256
 2461 m 222 2461 l s
 /xs 0 def
(-20)
 /Times-Roman   47 stwn
 gsave 178 667
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(-20)
 show
 gr
 /xs 0 def
(0)
 /Times-Roman   47 stwn
 gsave 178 964
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(0)
 show
 gr
 /xs 0 def
(20)
 /Times-Roman   47 stwn
 gsave 178 1260
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(20)
 show
 gr
 /xs 0 def
(40)
 /Times-Roman   47 stwn
 gsave 178 1556
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(40)
 show
 gr
 /xs 0 def
(60)
 /Times-Roman   47 stwn
 gsave 178 1853
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(60)
 show
 gr
 /xs 0 def
(80)
 /Times-Roman   47 stwn
 gsave 178 2149
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(80)
 show
 gr
 /xs 0 def
(100)
 /Times-Roman   47 stwn
 gsave 178 2446
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(100)
 show
 gr
 222 683 m 2001 683 l s 222 716 m 222 683 l s 258 699 m 258 683 l s 293 699 m
 293 683 l s 329 699 m 329 683 l s 365 699 m 365 683 l s 400 716 m 400 683 l s
 436 699 m 436 683 l s 471 699 m 471 683 l s 507 699 m 507 683 l s 542 699 m
542
 683 l s 578 716 m 578 683 l s 614 699 m 614 683 l s 649 699 m 649 683 l s 685
 699 m 685 683 l s 720 699 m 720 683 l s 756 716 m 756 683 l s 791 699 m 791
683
 l s 827 699 m 827 683 l s 863 699 m 863 683 l s 898 699 m 898 683 l s 934 716
m
 934 683 l s 969 699 m 969 683 l s 1005 699 m 1005 683 l s 1040 699 m 1040 683
l
 s 1076 699 m 1076 683 l s 1112 716 m 1112 683 l s 1147 699 m 1147 683 l s 1183
 699 m 1183 683 l s 1218 699 m 1218 683 l s 1254 699 m 1254 683 l s 1289 716 m
 1289 683 l s 1325 699 m 1325 683 l s 1360 699 m 1360 683 l s 1396 699 m 1396
 683 l s 1432 699 m 1432 683 l s 1467 716 m 1467 683 l s 1503 699 m 1503 683 l
s
 1538 699 m 1538 683 l s 1574 699 m 1574 683 l s 1609 699 m 1609 683 l s 1645
 716 m 1645 683 l s 1681 699 m 1681 683 l s 1716 699 m 1716 683 l s 1752 699 m
 1752 683 l s 1787 699 m 1787 683 l s 1823 716 m 1823 683 l s 1858 699 m 1858
 683 l s 1894 699 m 1894 683 l s 1930 699 m 1930 683 l s 1965 699 m 1965 683 l
s
 2001 716 m 2001 683 l s
 /xs 0 def
(50)
 /Times-Roman   47 stwn
 gsave 222 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(50)
 show
 gr
 /xs 0 def
(60)
 /Times-Roman   47 stwn
 gsave 400 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(60)
 show
 gr
 /xs 0 def
(70)
 /Times-Roman   47 stwn
 gsave 578 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(70)
 show
 gr
 /xs 0 def
(80)
 /Times-Roman   47 stwn
 gsave 756 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(80)
 show
 gr
 /xs 0 def
(90)
 /Times-Roman   47 stwn
 gsave 934 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(90)
 show
 gr
 /xs 0 def
(100)
 /Times-Roman   47 stwn
 gsave 1112 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(100)
 show
 gr
 /xs 0 def
(110)
 /Times-Roman   47 stwn
 gsave 1289 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(110)
 show
 gr
 /xs 0 def
(120)
 /Times-Roman   47 stwn
 gsave 1467 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(120)
 show
 gr
 /xs 0 def
(130)
 /Times-Roman   47 stwn
 gsave 1645 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(130)
 show
 gr
 /xs 0 def
(140)
 /Times-Roman   47 stwn
 gsave 1823 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(140)
 show
 gr
 /xs 0 def
(150)
 /Times-Roman   47 stwn
 gsave 2001 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(150)
 show
 gr
 gr
showpage gr
%%Trailer
%%Pages: 1
gr gr
%%EOF
%!PS-Adobe-2.0
%%Title: tau2.ps (Portrait A 4)
%%Pages: atend
%%Creator: HIGZ Version 1.20/11
%%CreationDate: 94/06/03   10.07
%%EndComments
/s {stroke} def /l {lineto} def /m {moveto} def /t { translate} def
/sw {stringwidth} def /r {rotate} def /rl {roll} def
/d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def
/c {setrgbcolor} def /lw {setlinewidth} def /sd {setdash} def
/cl {closepath} def /sf {scalefont setfont} def
/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def
/bl {box s} def /bf {box f} def
/mp {newpath /y exch def /x exch def} def
/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def
/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def
/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def
/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def
/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26 {mt s} def
/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def
 /m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def
 /m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d
 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def
 /m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
 4 {side} repeat cl fill gr} def
 /m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
 5 {side} repeat s gr} def /m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d
 x w2 sub y w2 add m w w neg d x w2 sub y w2
 sub m w w d s} def
/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def
/m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def
/reencdict 24 dict def /ReEncode {reencdict begin /nco&na exch def
/nfnam exch def /basefontname exch def /basefontdict basefontname findfont def
/newfont basefontdict maxlength dict def basefontdict {exch dup /FID ne
{dup /Encoding eq {exch dup length array copy newfont 3 1 roll put} {exch
newfont 3 1 roll put} ifelse} {pop pop} ifelse } forall newfont
/FontName nfnam put nco&na aload pop nco&na length 2 idiv {newfont
/Encoding get 3 1 roll put} repeat nfnam newfont definefont pop end } def
/accvec [ 176 /agrave 181 /Agrave 190 /acircumflex 192 /Acircumflex
201 /adieresis 204 /Adieresis 209 /ccedilla 210 /Ccedilla 211 /eacute
212 /Eacute 213 /egrave 214 /Egrave 215 /ecircumflex 216 /Ecircumflex
217 /edieresis 218 /Edieresis 219 /icircumflex 220 /Icircumflex
221 /idieresis 222 /Idieresis 223 /ntilde 224 /Ntilde 226 /ocircumflex
228 /Ocircumflex 229 /odieresis 230 /Odieresis 231 /ucircumflex 236
/Ucircumflex
237 /udieresis 238 /Udieresis 239 /aring 242 /Aring 243 /ydieresis
244 /Ydieresis 246 /aacute 247 /Aacute 252 /ugrave 253 /Ugrave] def
/Times-Roman /Times-Roman accvec ReEncode
/Times-Italic /Times-Italic accvec ReEncode
/Times-Bold /Times-Bold accvec ReEncode
/Times-BoldItalic /Times-BoldItalic accvec ReEncode
/Helvetica /Helvetica accvec ReEncode
/Helvetica-Oblique /Helvetica-Oblique accvec ReEncode
/Helvetica-Bold /Helvetica-Bold accvec ReEncode
/Helvetica-BoldOblique /Helvetica-BoldOblique  accvec ReEncode
/Courier /Courier accvec ReEncode
/Courier-Oblique /Courier-Oblique accvec ReEncode
/Courier-Bold /Courier-Bold accvec ReEncode
/Courier-BoldOblique /Courier-BoldOblique accvec ReEncode
/oshow {gsave [] 0 sd true charpath stroke gr} def
/stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf
 text sw pop xs add /xs exch def} def
/stwb { /fs exch def /fn exch def /nbas exch def /textf exch def
textf length /tlen exch def nbas tlen gt {/nbas tlen def} if
fn findfont fs sf textf dup length nbas sub nbas getinterval sw
pop neg xs add /xs exch def} def
/accspe [ 65 /plusminus 66 /bar 67 /existential 68 /universal
69 /exclam 70 /numbersign 71 /greater 72 /question 73 /integral
74 /colon 75 /semicolon 76 /less 77 /bracketleft 78 /bracketright
79 /greaterequal 80 /braceleft 81 /braceright 82 /radical
83 /spade 84 /heart 85 /diamond 86 /club 87 /lessequal
88 /multiply 89 /percent 90 /infinity 48 /circlemultiply 49 /circleplus
50 /emptyset 51 /lozenge 52 /bullet 53 /arrowright 54 /arrowup
55 /arrowleft 56 /arrowdown 57 /arrowboth 48 /degree 44 /comma 43 /plus
 45 /angle 42 /angleleft 47 /divide 61 /notequal 40 /equivalence 41 /second
 97 /approxequal 98 /congruent 99 /perpendicular 100 /partialdiff 101 /florin
 102 /intersection 103 /union 104 /propersuperset 105 /reflexsuperset
 106 /notsubset 107 /propersubset 108 /reflexsubset 109 /element 110
/notelement
 111 /gradient 112 /logicaland 113 /logicalor 114 /arrowdblboth
 115 /arrowdblleft 116 /arrowdblup 117 /arrowdblright 118 /arrowdbldown
 119 /ampersand 120 /omega1 121 /similar 122 /aleph ] def
/Symbol /Special accspe ReEncode
/Zone {/iy exch def /ix exch def gsave ix 1 sub 2224 mul 1 iy sub 3144
 mul t} def
gsave 20 28 t .25 .25 scale gsave
%%EndProlog
%%Page: number 1
 1 1 Zone
 gsave 0 0 t 0 setgray [] 0 sd 1 lw
 /xs 0 def
(t)
 /Symbol   84 stwn
(+)
 /Symbol   59 stwn
(t)
 /Symbol   84 stwn
(-)
 /Symbol   59 stwn
( Mass \(GeV\))
 /Times-Roman   84 stwn
 gsave 1112 507
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Symbol findfont   84 sf 0    0 m
(t)
 show
 currentpoint pop 0 t
 /Symbol findfont   59 sf 0   42 m
(+)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(t)
 show
 currentpoint pop 0 t
 /Symbol findfont   59 sf 0   42 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
( Mass \(GeV\))
 show
 gr
 /xs 0 def
(R)
 /Special   84 stwn
(s = 2 TeV, p)
 /Times-Roman   84 stwn
(-)
 /Symbol   84 stwn
(p)
 /Times-Roman   84 stwn
 gsave 1112 2522
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Special findfont   84 sf 0    0 m
(R)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(s = 2 TeV, p)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(p)
 show
 currentpoint pop 0 t
 gsave /Times-Roman findfont   84 sf
(p)
 dup length 1 sub 1 getinterval
 stringwidth pop 2 div neg    0 rm
 /Times-Roman findfont   59 sf 0   59 rm
(\261)
 stringwidth pop 2 div neg 0 rm
(\261)
 show gr
 gr
 /xs 0 def
(Background Subtracted)
 /Times-Roman   68 stwn
 gsave 1112 2320
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(Background Subtracted)
 show
 gr
 /xs 0 def
(Number of Events for 30 fb)
 /Times-Roman   84 stwn
(-1)
 /Times-Roman   59 stwn
 gsave 94 1572
 t  90 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   84 sf 0    0 m
(Number of Events for 30 fb)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   59 sf 0   42 m
(-1)
 show
 gr
 1779 1778 222 683 bl 222 979 m 222 1870 l 267 1870 l 267 683 l 311 683 l 356
 683 l 356 1341 l 400 1341 l 400 683 l 445 683 l 445 1236 l 489 1236 l 489 683
l
 534 683 l 534 1599 l 578 1599 l 578 1260 l 622 1260 l 622 1702 l 667 1702 l
667
 1432 l 711 1432 l 711 1643 l 756 1643 l 756 2014 l 800 2014 l 800 1909 l 845
 1909 l 845 1067 l 889 1067 l 889 1910 l 934 1910 l 934 1799 l 978 1799 l 978
 1739 l 1023 1739 l 1023 1271 l 1067 1271 l 1067 1971 l 1112 1971 l 1112 2131 l
 1156 2131 l 1156 804 l 1200 804 l 1200 1236 l 1245 1236 l 1245 1878 l 1289
1878
 l 1289 1125 l 1334 1125 l 1334 1610 l 1378 1610 l 1378 976 l 1423 976 l 1423
 783 l 1467 783 l 1467 1290 l 1512 1290 l 1512 897 l 1556 897 l 1556 1332 l
1601
 1332 l 1601 683 l 1645 683 l 1645 1048 l 1689 1048 l 1689 1043 l 1734 1043 l
 1734 683 l 1778 683 l 1778 1140 l 1823 1140 l 1823 968 l 1867 968 l 1867 937 l
 1912 937 l 1912 1048 l 1956 1048 l 1956 979 l 2001 979 l s 245 1052 m 289 1067
 l 333 1084 l 370 1101 l 378 1105 l 412 1123 l 422 1129 l 455 1149 l 467 1158 l
 498 1180 l 511 1191 l 541 1216 l 556 1229 l 584 1257 l 600 1273 l 629 1305 l
 645 1323 l 674 1360 l 689 1378 l 722 1423 l 734 1439 l 778 1503 l 823 1568 l
 861 1624 l 867 1632 l 895 1669 l 911 1689 l 935 1715 l 951 1730 l 956 1734 l
 971 1746 l 984 1754 l 997 1760 l 1000 1761 l 1015 1765 l 1027 1766 l 1039 1765
 l 1045 1764 l 1059 1758 l 1071 1751 l 1083 1742 l 1089 1736 l 1101 1723 l 1113
 1707 l 1126 1688 l 1134 1675 l 1145 1654 l 1159 1626 l 1175 1591 l 1178 1583 l
 1191 1552 l 1209 1504 l 1223 1469 l 1267 1344 l 1300 1255 l 1312 1225 l 1330
 1182 l 1342 1154 l 1354 1130 l 1356 1125 l 1371 1099 l 1383 1079 l 1396 1060 l
 1401 1054 l 1413 1040 l 1427 1026 l 1442 1013 l 1445 1011 l 1458 1003 l 1477
 995 l 1489 990 l 1507 986 l 1534 982 l 1558 980 l 1578 980 l 1623 979 l 1667
 979 l 1712 979 l 1756 979 l 1801 979 l 1845 979 l 1890 979 l 1934 979 l 1978
 979 l s 222 683 m 222 2461 l s 256 683 m 222 683 l s 239 742 m 222 742 l s 239
 801 m 222 801 l s 239 861 m 222 861 l s 239 920 m 222 920 l s 256 979 m 222
979
 l s 239 1038 m 222 1038 l s 239 1098 m 222 1098 l s 239 1157 m 222 1157 l s
239
 1216 m 222 1216 l s 256 1276 m 222 1276 l s 239 1335 m 222 1335 l s 239 1394 m
 222 1394 l s 239 1453 m 222 1453 l s 239 1513 m 222 1513 l s 256 1572 m 222
 1572 l s 239 1631 m 222 1631 l s 239 1691 m 222 1691 l s 239 1750 m 222 1750 l
 s 239 1809 m 222 1809 l s 256 1868 m 222 1868 l s 239 1928 m 222 1928 l s 239
 1987 m 222 1987 l s 239 2046 m 222 2046 l s 239 2106 m 222 2106 l s 256 2165 m
 222 2165 l s 239 2224 m 222 2224 l s 239 2283 m 222 2283 l s 239 2343 m 222
 2343 l s 239 2402 m 222 2402 l s 256 2461 m 222 2461 l s
 /xs 0 def
(-1)
 /Times-Roman   47 stwn
 gsave 178 667
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(-1)
 show
 gr
 /xs 0 def
(0)
 /Times-Roman   47 stwn
 gsave 178 964
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(0)
 show
 gr
 /xs 0 def
(1)
 /Times-Roman   47 stwn
 gsave 178 1260
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(1)
 show
 gr
 /xs 0 def
(2)
 /Times-Roman   47 stwn
 gsave 178 1556
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(2)
 show
 gr
 /xs 0 def
(3)
 /Times-Roman   47 stwn
 gsave 178 1853
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(3)
 show
 gr
 /xs 0 def
(4)
 /Times-Roman   47 stwn
 gsave 178 2149
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(4)
 show
 gr
 /xs 0 def
(5)
 /Times-Roman   47 stwn
 gsave 178 2446
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(5)
 show
 gr
 222 683 m 2001 683 l s 222 716 m 222 683 l s 267 699 m 267 683 l s 311 699 m
 311 683 l s 356 699 m 356 683 l s 400 699 m 400 683 l s 445 716 m 445 683 l s
 489 699 m 489 683 l s 534 699 m 534 683 l s 578 699 m 578 683 l s 622 699 m
622
 683 l s 667 716 m 667 683 l s 711 699 m 711 683 l s 756 699 m 756 683 l s 800
 699 m 800 683 l s 845 699 m 845 683 l s 889 716 m 889 683 l s 934 699 m 934
683
 l s 978 699 m 978 683 l s 1023 699 m 1023 683 l s 1067 699 m 1067 683 l s 1112
 716 m 1112 683 l s 1156 699 m 1156 683 l s 1200 699 m 1200 683 l s 1245 699 m
 1245 683 l s 1289 699 m 1289 683 l s 1334 716 m 1334 683 l s 1378 699 m 1378
 683 l s 1423 699 m 1423 683 l s 1467 699 m 1467 683 l s 1512 699 m 1512 683 l
s
 1556 716 m 1556 683 l s 1601 699 m 1601 683 l s 1645 699 m 1645 683 l s 1689
 699 m 1689 683 l s 1734 699 m 1734 683 l s 1778 716 m 1778 683 l s 1823 699 m
 1823 683 l s 1867 699 m 1867 683 l s 1912 699 m 1912 683 l s 1956 699 m 1956
 683 l s 2001 716 m 2001 683 l s
 /xs 0 def
(100)
 /Times-Roman   47 stwn
 gsave 222 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(100)
 show
 gr
 /xs 0 def
(105)
 /Times-Roman   47 stwn
 gsave 445 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(105)
 show
 gr
 /xs 0 def
(110)
 /Times-Roman   47 stwn
 gsave 667 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(110)
 show
 gr
 /xs 0 def
(115)
 /Times-Roman   47 stwn
 gsave 889 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(115)
 show
 gr
 /xs 0 def
(120)
 /Times-Roman   47 stwn
 gsave 1112 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(120)
 show
 gr
 /xs 0 def
(125)
 /Times-Roman   47 stwn
 gsave 1334 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(125)
 show
 gr
 /xs 0 def
(130)
 /Times-Roman   47 stwn
 gsave 1556 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(130)
 show
 gr
 /xs 0 def
(135)
 /Times-Roman   47 stwn
 gsave 1778 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(135)
 show
 gr
 /xs 0 def
(140)
 /Times-Roman   47 stwn
 gsave 2001 629
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   47 sf 0    0 m
(140)
 show
 gr
 gr
showpage gr
%%Trailer
%%Pages: 1
gr gr
%%EOF
%!PS-Adobe-2.0
%%Title: significance.ps (Portrait A 4)
%%Pages: atend
%%Creator: HIGZ Version 1.20/11
%%CreationDate: 94/06/07   15.35
%%EndComments
/s {stroke} def /l {lineto} def /m {moveto} def /t { translate} def
/sw {stringwidth} def /r {rotate} def /rl {roll} def
/d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def
/c {setrgbcolor} def /lw {setlinewidth} def /sd {setdash} def
/cl {closepath} def /sf {scalefont setfont} def
/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def
/bl {box s} def /bf {box f} def
/mp {newpath /y exch def /x exch def} def
/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def
/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def
/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def
/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def
/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26 {mt s} def
/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def
 /m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def
 /m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d
 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def
 /m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
 4 {side} repeat cl fill gr} def
 /m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
 5 {side} repeat s gr} def /m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d
 x w2 sub y w2 add m w w neg d x w2 sub y w2
 sub m w w d s} def
/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def
/m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def
/reencdict 24 dict def /ReEncode {reencdict begin /nco&na exch def
/nfnam exch def /basefontname exch def /basefontdict basefontname findfont def
/newfont basefontdict maxlength dict def basefontdict {exch dup /FID ne
{dup /Encoding eq {exch dup length array copy newfont 3 1 roll put} {exch
newfont 3 1 roll put} ifelse} {pop pop} ifelse } forall newfont
/FontName nfnam put nco&na aload pop nco&na length 2 idiv {newfont
/Encoding get 3 1 roll put} repeat nfnam newfont definefont pop end } def
/accvec [ 176 /agrave 181 /Agrave 190 /acircumflex 192 /Acircumflex
201 /adieresis 204 /Adieresis 209 /ccedilla 210 /Ccedilla 211 /eacute
212 /Eacute 213 /egrave 214 /Egrave 215 /ecircumflex 216 /Ecircumflex
217 /edieresis 218 /Edieresis 219 /icircumflex 220 /Icircumflex
221 /idieresis 222 /Idieresis 223 /ntilde 224 /Ntilde 226 /ocircumflex
228 /Ocircumflex 229 /odieresis 230 /Odieresis 231 /ucircumflex 236
/Ucircumflex
237 /udieresis 238 /Udieresis 239 /aring 242 /Aring 243 /ydieresis
244 /Ydieresis 246 /aacute 247 /Aacute 252 /ugrave 253 /Ugrave] def
/Times-Roman /Times-Roman accvec ReEncode
/Times-Italic /Times-Italic accvec ReEncode
/Times-Bold /Times-Bold accvec ReEncode
/Times-BoldItalic /Times-BoldItalic accvec ReEncode
/Helvetica /Helvetica accvec ReEncode
/Helvetica-Oblique /Helvetica-Oblique accvec ReEncode
/Helvetica-Bold /Helvetica-Bold accvec ReEncode
/Helvetica-BoldOblique /Helvetica-BoldOblique  accvec ReEncode
/Courier /Courier accvec ReEncode
/Courier-Oblique /Courier-Oblique accvec ReEncode
/Courier-Bold /Courier-Bold accvec ReEncode
/Courier-BoldOblique /Courier-BoldOblique accvec ReEncode
/oshow {gsave [] 0 sd true charpath stroke gr} def
/stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf
 text sw pop xs add /xs exch def} def
/stwb { /fs exch def /fn exch def /nbas exch def /textf exch def
textf length /tlen exch def nbas tlen gt {/nbas tlen def} if
fn findfont fs sf textf dup length nbas sub nbas getinterval sw
pop neg xs add /xs exch def} def
/accspe [ 65 /plusminus 66 /bar 67 /existential 68 /universal
69 /exclam 70 /numbersign 71 /greater 72 /question 73 /integral
74 /colon 75 /semicolon 76 /less 77 /bracketleft 78 /bracketright
79 /greaterequal 80 /braceleft 81 /braceright 82 /radical
83 /spade 84 /heart 85 /diamond 86 /club 87 /lessequal
88 /multiply 89 /percent 90 /infinity 48 /circlemultiply 49 /circleplus
50 /emptyset 51 /lozenge 52 /bullet 53 /arrowright 54 /arrowup
55 /arrowleft 56 /arrowdown 57 /arrowboth 48 /degree 44 /comma 43 /plus
 45 /angle 42 /angleleft 47 /divide 61 /notequal 40 /equivalence 41 /second
 97 /approxequal 98 /congruent 99 /perpendicular 100 /partialdiff 101 /florin
 102 /intersection 103 /union 104 /propersuperset 105 /reflexsuperset
 106 /notsubset 107 /propersubset 108 /reflexsubset 109 /element 110
/notelement
 111 /gradient 112 /logicaland 113 /logicalor 114 /arrowdblboth
 115 /arrowdblleft 116 /arrowdblup 117 /arrowdblright 118 /arrowdbldown
 119 /ampersand 120 /omega1 121 /similar 122 /aleph ] def
/Symbol /Special accspe ReEncode
/Zone {/iy exch def /ix exch def gsave ix 1 sub 2224 mul 1 iy sub 3144
 mul t} def
gsave 20 28 t .25 .25 scale gsave
%%EndProlog
%%Page: number 1
 1 1 Zone
 gsave 0 0 t 0 setgray [] 0 sd 1 lw
 /xs 0 def
(R)
 /Special   84 stwn
(s = 2 TeV, p)
 /Times-Roman   84 stwn
(-)
 /Symbol   84 stwn
(p)
 /Times-Roman   84 stwn
 gsave 1112 2374
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Special findfont   84 sf 0    0 m
(R)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(s = 2 TeV, p)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(p)
 show
 currentpoint pop 0 t
 gsave /Times-Roman findfont   84 sf
(p)
 dup length 1 sub 1 getinterval
 stringwidth pop 2 div neg    0 rm
 /Times-Roman findfont   59 sf 0   59 rm
(\261)
 stringwidth pop 2 div neg 0 rm
(\261)
 show gr
 gr
 /xs 0 def
(R)
 /Special   84 stwn
(s = 4 TeV, p)
 /Times-Roman   84 stwn
(-)
 /Symbol   84 stwn
(p)
 /Times-Roman   84 stwn
 gsave 1112 1781
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Special findfont   84 sf 0    0 m
(R)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(s = 4 TeV, p)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(p)
 show
 gr
 /xs 0 def
(R)
 /Special   84 stwn
(s = 14 TeV, p)
 /Times-Roman   84 stwn
(-)
 /Symbol   84 stwn
(p)
 /Times-Roman   84 stwn
 gsave 1112 1189
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Special findfont   84 sf 0    0 m
(R)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(s = 14 TeV, p)
 show
 currentpoint pop 0 t
 /Symbol findfont   84 sf 0    0 m
(-)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
(p)
 show
 gr
 /xs 0 def
(M)
 /Times-Roman   84 stwn
(h)
 /Times-Roman   59 stwn
( \(GeV\))
 /Times-Roman   84 stwn
 gsave 1112 507
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   84 sf 0    0 m
(M)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   59 sf 0  -28 m
(h)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   84 sf 0    0 m
( \(GeV\))
 show
 gr
 /xs 0 def
(Significance for 10 and 30 fb)
 /Times-Roman   84 stwn
(-1)
 /Times-Roman   59 stwn
 gsave 87 1572
 t  90 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   84 sf 0    0 m
(Significance for 10 and 30 fb)
 show
 currentpoint pop 0 t
 /Times-Roman findfont   59 sf 0   42 m
(-1)
 show
 gr
 1779 593 222 1868 bl 0 0 1 c 222 2224 m 222 2224 l 519 2206 l 815 2126 l 1112
 2085 l 1408 2117 l 1704 2082 l 2001 2046 l 2001 2070 l 1704 2100 l 1408 2142 l
 1112 2114 l 815 2165 l 519 2266 l 222 2283 l 222 2224 l f 6 lw 0 setgray 222
 2224 m 222 2224 l 519 2206 l 815 2126 l 1112 2085 l 1408 2117 l 1704 2082 l
 2001 2046 l 2001 2070 l 1704 2100 l 1408 2142 l 1112 2114 l 815 2165 l 519
2266
 l 222 2283 l 222 2224 l cl s 0 1 0 c 1 lw 222 2283 m 222 2283 l 519 2266 l 815
 2165 l 1112 2114 l 1408 2142 l 1704 2100 l 2001 2070 l 2001 2091 l 1704 2123 l
 1408 2186 l 1112 2165 l 815 2227 l 519 2346 l 222 2366 l 222 2283 l f 6 lw
 0 setgray 222 2283 m 222 2283 l 519 2266 l 815 2165 l 1112 2114 l 1408 2142 l
 1704 2100 l 2001 2070 l 2001 2091 l 1704 2123 l 1408 2186 l 1112 2165 l 815
 2227 l 519 2346 l 222 2366 l 222 2283 l cl s 0 0 1 c 1 lw 222 2074 m 222 2074
l
 519 2063 l 815 2017 l 1112 1993 l 1408 2012 l 1704 1992 l 2001 1971 l 2001
1985
 l 1704 2002 l 1408 2027 l 1112 2010 l 815 2040 l 519 2098 l 222 2108 l 222
2074
 l f 6 lw 0 setgray 222 2074 m 222 2074 l 519 2063 l 815 2017 l 1112 1993 l
1408
 2012 l 1704 1992 l 2001 1971 l 2001 1985 l 1704 2002 l 1408 2027 l 1112 2010 l
 815 2040 l 519 2098 l 222 2108 l 222 2074 l cl s 0 1 0 c 1 lw 222 2108 m 222
 2108 l 519 2098 l 815 2040 l 1112 2010 l 1408 2027 l 1704 2002 l 2001 1985 l
 2001 1997 l 1704 2016 l 1408 2052 l 1112 2040 l 815 2075 l 519 2144 l 222 2156
 l 222 2108 l f 6 lw 0 setgray 222 2108 m 222 2108 l 519 2098 l 815 2040 l 1112
 2010 l 1408 2027 l 1704 2002 l 2001 1985 l 2001 1997 l 1704 2016 l 1408 2052 l
 1112 2040 l 815 2075 l 519 2144 l 222 2156 l 222 2108 l cl s 1 lw 1779 592 222
 1276 bl 0 0 1 c 222 1631 m 222 1631 l 519 1602 l 815 1516 l 1112 1480 l 1408
 1492 l 1704 1439 l 2001 1394 l 2001 1400 l 1704 1445 l 1408 1504 l 1112 1492 l
 815 1522 l 519 1628 l 222 1661 l 222 1631 l f 6 lw 0 setgray 222 1631 m 222
 1631 l 519 1602 l 815 1516 l 1112 1480 l 1408 1492 l 1704 1439 l 2001 1394 l
 2001 1400 l 1704 1445 l 1408 1504 l 1112 1492 l 815 1522 l 519 1628 l 222 1661
 l 222 1631 l cl s 0 1 0 c 1 lw 222 1661 m 222 1661 l 519 1628 l 815 1522 l
1112
 1492 l 1408 1504 l 1704 1445 l 2001 1400 l 2001 1412 l 1704 1462 l 1408 1531 l
 1112 1522 l 815 1572 l 519 1699 l 222 1738 l 222 1661 l f 6 lw 0 setgray 222
 1661 m 222 1661 l 519 1628 l 815 1522 l 1112 1492 l 1408 1504 l 1704 1445 l
 2001 1400 l 2001 1412 l 1704 1462 l 1408 1531 l 1112 1522 l 815 1572 l 519
1699
 l 222 1738 l 222 1661 l cl s 0 0 1 c 1 lw 222 1481 m 222 1481 l 519 1464 l 815
 1414 l 1112 1394 l 1408 1401 l 1704 1370 l 2001 1344 l 2001 1347 l 1704 1373 l
 1408 1407 l 1112 1401 l 815 1418 l 519 1479 l 222 1498 l 222 1481 l f 6 lw
 0 setgray 222 1481 m 222 1481 l 519 1464 l 815 1414 l 1112 1394 l 1408 1401 l
 1704 1370 l 2001 1344 l 2001 1347 l 1704 1373 l 1408 1407 l 1112 1401 l 815
 1418 l 519 1479 l 222 1498 l 222 1481 l cl s 0 1 0 c 1 lw 222 1498 m 222 1498
l
 519 1479 l 815 1418 l 1112 1401 l 1408 1407 l 1704 1373 l 2001 1347 l 2001
1354
 l 1704 1383 l 1408 1423 l 1112 1418 l 815 1447 l 519 1520 l 222 1543 l 222
1498
 l f 6 lw 0 setgray 222 1498 m 222 1498 l 519 1479 l 815 1418 l 1112 1401 l
1408
 1407 l 1704 1373 l 2001 1347 l 2001 1354 l 1704 1383 l 1408 1423 l 1112 1418 l
 815 1447 l 519 1520 l 222 1543 l 222 1498 l cl s 1 lw 1779 593 222 683 bl 222
 683 m 2001 683 l s 222 712 m 222 683 l s 282 698 m 282 683 l s 341 698 m 341
 683 l s 400 698 m 400 683 l s 459 698 m 459 683 l s 519 712 m 519 683 l s 578
 698 m 578 683 l s 637 698 m 637 683 l s 697 698 m 697 683 l s 756 698 m 756
683
 l s 815 712 m 815 683 l s 874 698 m 874 683 l s 934 698 m 934 683 l s 993 698
m
 993 683 l s 1052 698 m 1052 683 l s 1112 712 m 1112 683 l s 1171 698 m 1171
683
 l s 1230 698 m 1230 683 l s 1289 698 m 1289 683 l s 1349 698 m 1349 683 l s
 1408 712 m 1408 683 l s 1467 698 m 1467 683 l s 1526 698 m 1526 683 l s 1586
 698 m 1586 683 l s 1645 698 m 1645 683 l s 1704 712 m 1704 683 l s 1764 698 m
 1764 683 l s 1823 698 m 1823 683 l s 1882 698 m 1882 683 l s 1941 698 m 1941
 683 l s 2001 712 m 2001 683 l s
 /xs 0 def
(70)
 /Times-Roman   68 stwn
 gsave 222 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(70)
 show
 gr
 /xs 0 def
(80)
 /Times-Roman   68 stwn
 gsave 519 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(80)
 show
 gr
 /xs 0 def
(90)
 /Times-Roman   68 stwn
 gsave 815 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(90)
 show
 gr
 /xs 0 def
(100)
 /Times-Roman   68 stwn
 gsave 1112 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(100)
 show
 gr
 /xs 0 def
(110)
 /Times-Roman   68 stwn
 gsave 1408 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(110)
 show
 gr
 /xs 0 def
(120)
 /Times-Roman   68 stwn
 gsave 1704 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(120)
 show
 gr
 /xs 0 def
(130)
 /Times-Roman   68 stwn
 gsave 2001 609
 t   0 r  xs 2 div neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(130)
 show
 gr
 222 1276 m 2001 1276 l s 222 1305 m 222 1276 l s 282 1290 m 282 1276 l s 341
 1290 m 341 1276 l s 400 1290 m 400 1276 l s 459 1290 m 459 1276 l s 519 1305 m
 519 1276 l s 578 1290 m 578 1276 l s 637 1290 m 637 1276 l s 697 1290 m 697
 1276 l s 756 1290 m 756 1276 l s 815 1305 m 815 1276 l s 874 1290 m 874 1276 l
 s 934 1290 m 934 1276 l s 993 1290 m 993 1276 l s 1052 1290 m 1052 1276 l s
 1112 1305 m 1112 1276 l s 1171 1290 m 1171 1276 l s 1230 1290 m 1230 1276 l s
 1289 1290 m 1289 1276 l s 1349 1290 m 1349 1276 l s 1408 1305 m 1408 1276 l s
 1467 1290 m 1467 1276 l s 1526 1290 m 1526 1276 l s 1586 1290 m 1586 1276 l s
 1645 1290 m 1645 1276 l s 1704 1305 m 1704 1276 l s 1764 1290 m 1764 1276 l s
 1823 1290 m 1823 1276 l s 1882 1290 m 1882 1276 l s 1941 1290 m 1941 1276 l s
 2001 1305 m 2001 1276 l s 222 1868 m 2001 1868 l s 222 1898 m 222 1868 l s 282
 1883 m 282 1868 l s 341 1883 m 341 1868 l s 400 1883 m 400 1868 l s 459 1883 m
 459 1868 l s 519 1898 m 519 1868 l s 578 1883 m 578 1868 l s 637 1883 m 637
 1868 l s 697 1883 m 697 1868 l s 756 1883 m 756 1868 l s 815 1898 m 815 1868 l
 s 874 1883 m 874 1868 l s 934 1883 m 934 1868 l s 993 1883 m 993 1868 l s 1052
 1883 m 1052 1868 l s 1112 1898 m 1112 1868 l s 1171 1883 m 1171 1868 l s 1230
 1883 m 1230 1868 l s 1289 1883 m 1289 1868 l s 1349 1883 m 1349 1868 l s 1408
 1898 m 1408 1868 l s 1467 1883 m 1467 1868 l s 1526 1883 m 1526 1868 l s 1586
 1883 m 1586 1868 l s 1645 1883 m 1645 1868 l s 1704 1898 m 1704 1868 l s 1764
 1883 m 1764 1868 l s 1823 1883 m 1823 1868 l s 1882 1883 m 1882 1868 l s 1941
 1883 m 1941 1868 l s 2001 1898 m 2001 1868 l s 222 683 m 222 1246 l s 252 683
m
 222 683 l s 237 712 m 222 712 l s 237 742 m 222 742 l s 237 772 m 222 772 l s
 237 801 m 222 801 l s 252 831 m 222 831 l s 237 861 m 222 861 l s 237 890 m
222
 890 l s 237 920 m 222 920 l s 237 950 m 222 950 l s 252 979 m 222 979 l s 237
 1009 m 222 1009 l s 237 1038 m 222 1038 l s 237 1068 m 222 1068 l s 237 1098 m
 222 1098 l s 252 1127 m 222 1127 l s 252 1127 m 222 1127 l s 237 1157 m 222
 1157 l s 237 1187 m 222 1187 l s 237 1216 m 222 1216 l s
 /xs 0 def
(0)
 /Times-Roman   68 stwn
 gsave 181 661
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(0)
 show
 gr
 /xs 0 def
(5)
 /Times-Roman   68 stwn
 gsave 181 809
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(5)
 show
 gr
 /xs 0 def
(10)
 /Times-Roman   68 stwn
 gsave 181 957
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(10)
 show
 gr
 /xs 0 def
(15)
 /Times-Roman   68 stwn
 gsave 181 1105
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(15)
 show
 gr
 222 1276 m 222 1839 l s 252 1276 m 222 1276 l s 237 1305 m 222 1305 l s 237
 1335 m 222 1335 l s 237 1365 m 222 1365 l s 237 1394 m 222 1394 l s 252 1424 m
 222 1424 l s 237 1453 m 222 1453 l s 237 1483 m 222 1483 l s 237 1513 m 222
 1513 l s 237 1542 m 222 1542 l s 252 1572 m 222 1572 l s 237 1602 m 222 1602 l
 s 237 1631 m 222 1631 l s 237 1661 m 222 1661 l s 237 1691 m 222 1691 l s 252
 1720 m 222 1720 l s 252 1720 m 222 1720 l s 237 1750 m 222 1750 l s 237 1779 m
 222 1779 l s 237 1809 m 222 1809 l s 237 1839 m 222 1839 l s
 /xs 0 def
(0)
 /Times-Roman   68 stwn
 gsave 181 1253
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(0)
 show
 gr
 /xs 0 def
(5)
 /Times-Roman   68 stwn
 gsave 181 1402
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(5)
 show
 gr
 /xs 0 def
(10)
 /Times-Roman   68 stwn
 gsave 181 1550
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(10)
 show
 gr
 /xs 0 def
(15)
 /Times-Roman   68 stwn
 gsave 181 1698
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(15)
 show
 gr
 222 1868 m 222 2432 l s 252 1868 m 222 1868 l s 237 1898 m 222 1898 l s 237
 1928 m 222 1928 l s 237 1957 m 222 1957 l s 237 1987 m 222 1987 l s 252 2017 m
 222 2017 l s 237 2046 m 222 2046 l s 237 2076 m 222 2076 l s 237 2106 m 222
 2106 l s 237 2135 m 222 2135 l s 252 2165 m 222 2165 l s 237 2194 m 222 2194 l
 s 237 2224 m 222 2224 l s 237 2254 m 222 2254 l s 237 2283 m 222 2283 l s 252
 2313 m 222 2313 l s 252 2313 m 222 2313 l s 237 2343 m 222 2343 l s 237 2372 m
 222 2372 l s 237 2402 m 222 2402 l s 237 2432 m 222 2432 l s
 /xs 0 def
(0)
 /Times-Roman   68 stwn
 gsave 181 1846
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(0)
 show
 gr
 /xs 0 def
(5)
 /Times-Roman   68 stwn
 gsave 181 1994
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(5)
 show
 gr
 /xs 0 def
(10)
 /Times-Roman   68 stwn
 gsave 181 2143
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(10)
 show
 gr
 /xs 0 def
(15)
 /Times-Roman   68 stwn
 gsave 181 2291
 t   0 r  xs neg 0 t 0 0 m
 /Times-Roman findfont   68 sf 0    0 m
(15)
 show
 gr
 2001 683 m 2001 1246 l s 1971 683 m 2001 683 l s 1986 712 m 2001 712 l s 1986
 742 m 2001 742 l s 1986 772 m 2001 772 l s 1986 801 m 2001 801 l s 1971 831 m
 2001 831 l s 1986 861 m 2001 861 l s 1986 890 m 2001 890 l s 1986 920 m 2001
 920 l s 1986 950 m 2001 950 l s 1971 979 m 2001 979 l s 1986 1009 m 2001 1009
l
 s 1986 1038 m 2001 1038 l s 1986 1068 m 2001 1068 l s 1986 1098 m 2001 1098 l
s
 1971 1127 m 2001 1127 l s 1971 1127 m 2001 1127 l s 1986 1157 m 2001 1157 l s
 1986 1187 m 2001 1187 l s 1986 1216 m 2001 1216 l s 2001 1276 m 2001 1839 l s
 1971 1276 m 2001 1276 l s 1986 1305 m 2001 1305 l s 1986 1335 m 2001 1335 l s
 1986 1365 m 2001 1365 l s 1986 1394 m 2001 1394 l s 1971 1424 m 2001 1424 l s
 1986 1453 m 2001 1453 l s 1986 1483 m 2001 1483 l s 1986 1513 m 2001 1513 l s
 1986 1542 m 2001 1542 l s 1971 1572 m 2001 1572 l s 1986 1602 m 2001 1602 l s
 1986 1631 m 2001 1631 l s 1986 1661 m 2001 1661 l s 1986 1691 m 2001 1691 l s
 1971 1720 m 2001 1720 l s 1971 1720 m 2001 1720 l s 1986 1750 m 2001 1750 l s
 1986 1779 m 2001 1779 l s 1986 1809 m 2001 1809 l s 1986 1839 m 2001 1839 l s
 2001 1868 m 2001 2432 l s 1971 1868 m 2001 1868 l s 1986 1898 m 2001 1898 l s
 1986 1928 m 2001 1928 l s 1986 1957 m 2001 1957 l s 1986 1987 m 2001 1987 l s
 1971 2017 m 2001 2017 l s 1986 2046 m 2001 2046 l s 1986 2076 m 2001 2076 l s
 1986 2106 m 2001 2106 l s 1986 2135 m 2001 2135 l s 1971 2165 m 2001 2165 l s
 1986 2194 m 2001 2194 l s 1986 2224 m 2001 2224 l s 1986 2254 m 2001 2254 l s
 1986 2283 m 2001 2283 l s 1971 2313 m 2001 2313 l s 1971 2313 m 2001 2313 l s
 1986 2343 m 2001 2343 l s 1986 2372 m 2001 2372 l s 1986 2402 m 2001 2402 l s
 1986 2432 m 2001 2432 l s 0 0 1 c 222 1136 m 222 1136 l 519 1107 l 815 1000 l
 1112 947 l 1408 902 l 1704 837 l 2001 792 l 2001 795 l 1704 843 l 1408 908 l
 1112 955 l 815 1015 l 519 1124 l 222 1157 l 222 1136 l f 6 lw 0 setgray 222
 1136 m 222 1136 l 519 1107 l 815 1000 l 1112 947 l 1408 902 l 1704 837 l 2001
 792 l 2001 795 l 1704 843 l 1408 908 l 1112 955 l 815 1015 l 519 1124 l 222
 1157 l 222 1136 l cl s 0 1 0 c 1 lw 222 1157 m 222 1157 l 519 1124 l 815 1015
l
 1112 955 l 1408 908 l 1704 843 l 2001 795 l 2001 819 l 1704 870 l 1408 941 l
 1112 1009 l 815 1080 l 519 1213 l 222 1252 l 222 1157 l f 6 lw 0 setgray 222
 1157 m 222 1157 l 519 1124 l 815 1015 l 1112 955 l 1408 908 l 1704 843 l 2001
 795 l 2001 819 l 1704 870 l 1408 941 l 1112 1009 l 815 1080 l 519 1213 l 222
 1252 l 222 1157 l cl s 0 0 1 c 1 lw 222 945 m 222 945 l 519 928 l 815 866 l
 1112 835 l 1408 809 l 1704 772 l 2001 746 l 2001 748 l 1704 775 l 1408 813 l
 1112 840 l 815 874 l 519 938 l 222 957 l 222 945 l f 6 lw 0 setgray 222 945 m
 222 945 l 519 928 l 815 866 l 1112 835 l 1408 809 l 1704 772 l 2001 746 l 2001
 748 l 1704 775 l 1408 813 l 1112 840 l 815 874 l 519 938 l 222 957 l 222 945 l
 cl s 0 1 0 c 1 lw 222 957 m 222 957 l 519 938 l 815 874 l 1112 840 l 1408 813
l
 1704 775 l 2001 748 l 2001 762 l 1704 791 l 1408 832 l 1112 871 l 815 912 l
519
 989 l 222 1011 l 222 957 l f 6 lw 0 setgray 222 957 m 222 957 l 519 938 l 815
 874 l 1112 840 l 1408 813 l 1704 775 l 2001 748 l 2001 762 l 1704 791 l 1408
 832 l 1112 871 l 815 912 l 519 989 l 222 1011 l 222 957 l cl s gr
showpage gr
%%Trailer
%%Pages: 1
gr gr
%%EOF

