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writeup/EDIT2013poster/contents.tex

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%--the poster is one beamer frame, so we have to start with:
\begin{frame}[t]
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%--abstract block--------------------------------------------------------
\begin{alertblock}{Introduction}
Charged lepton flavor violation (CLFV) has attracted much attention
from experimentalists and theorists in particle physics. The CLFV rates
are predicted to be in the order of of O($10^{-54}$) in the Standard
Model.
Therefore, any observation of CLFV processes would be an
unambiguous signal for physics beyond the Standard Model. The COMET is
an experiment that aims to search for a CLFV process of
muon-to-electron conversion in the presence of a nucleus, \muec. Using
the J-PARC proton beam and the pion capture by a solenoidal
field, COMET expects to have a sensitivity a factor of 10,000 times
that of the current limit. The COMET experiment has taken a phased
approach in which the COMET Phase-I (first phase) will start its
construction in 2013 and initial data taking in around 2016. Some more
details of COMET Phase-I and its related issues will be presented.
\end{alertblock}
\begin{alertblock}{Staging approach of the COMET}
The proposed J-PARC mid-term plan includes the construction of the
COMET beamline. This will provide the proton beamline for COMET and
part of the muon beamline in the south area of the J-PARC Hadron
Experimental Hall. We consider a staged approach for COMET: “COMET
Phase-I” and “COMET Phase-II”.
For the COMET Phase-I, we will construct the first 90 degrees of the
muon beamline so that a muon beam can be extracted to the experimental
area. Then, we will:
1) make a direct measurement of the proton beam extinction and other
potential back- ground sources for the COMET Phase-II ex- periment,
using the actual COMET beamline, and
2) carry out a search for e conversion with a singe-event
sensitivity (S.E.S.) of 3 1015, which is better than achieved
by SINDRUM-II.
After these measurements, the muon transport will be extended up
to 180 degrees for the COMET Phase-II. We will start the e
conversion search with S.E.S. of 3 1017 sensitivity with an
electron spectrometer and detectors
\begin{figure}[h!]
\begin{center}
\includegraphics[width=0.95\onecolwid]{figs/cometfull}
\end{center}
\caption{Schematic lay out of the COMET Phase I and COMET
Phase II}
\label{fig:cometscheme}
\end{figure}
\begin{figure}[h!]
\begin{center}
\includegraphics[width=0.95\onecolwid]{figs/cometphase1}
\end{center}
\caption{Schematic lay out of the COMET Phase I and COMET
Phase II}
\label{fig:cometp1}
\end{figure}
\end{alertblock}
\end{column}
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\begin{block}{The new measurement of charged particles emission
from muon capture}
\begin{itemize}
\item A joint collaboration between COMET and Mu2e
\item Goals of the experiment:
\begin{itemize}
\item[$\bullet$] measure \textcolor{red}{rate and energy
spectra} of the charged
particles (p, d, $\alpha$) emitted after muon capture on
some targets:
\begin{itemize}
\item [-] Al: default target of COMET and Mu2e
\item [-] Ti: possible target for future $\mu-e$
conversion experiments
\item [-] Si: active target, for cross-checking against
previous experiment, and studying the energy loss of
charged particles inside the targets
\end{itemize}
\item[$\bullet$] required precision: \textcolor{red}{5\%}
for both the rate and the
energy spectra in the range from 2.5 $-$ 12 MeV
\end{itemize}
\item Will be conducted at TRIUMF (Canada) and PSI
(Switzerland).
\end{itemize}
\end{block}
\vskip1ex
% Methods
\begin{block}{Methods}
\begin{figure}[]
\includegraphics[width=0.95\twocolwid]{figs/setupa}
\caption{Experimental setup: schematic view (left) and image (right)}
\label{fig:setup}
\end{figure}
\begin{minipage}[t]{\onecolwid}
\begin{itemize}
\item Low momentum muon beam: to ensure a high rate of stopped
muons, and a well determined range of muons in the targets. A
cloud muon of 30 $-$ 34 MeV/c from a surface muon channel is
optimal.
\item The charged particles are measured by dE/dx method
by two pairs of silicon detectors. Active area of each silicon
detector is 5$\times$5 cm$^2$, the dE detectors are 65 $\mu m$
thick, and the E detectors are 1500 $\mu m$ thick.
\end{itemize}
\end{minipage} % Do not put another blank line after this line because
%that will mess up the alignment of the two minipages
\begin{minipage}[t]{\onecolwid}
\begin{itemize}
\item Muon normalization: muonic X-ray measurement by a germanium
detector.
\item Correction for energy loss of charged particles in the
targets: using a response function obtained from the use of the
active silicon target, where the energy loss can be measured. A
waveform digitizer will be used to readout signals from the
active target.
\end{itemize}
\end{minipage}
\end{block}
\vskip2ex
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% cols take all the space of the 'mother' column
\begin{columns}[t,totalwidth=0.60\paperwidth]
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%--the Left block-----------------------------------------------------------
\begin{block}{Calculations}
\begin{itemize}
\item Using Geant4, with assumptions:
\begin{itemize}
\item [$\bullet$] Muon momentum 30 MeV/c, momentum spread 5\%.
\item [$\bullet$] Muon intensity: 10$^4$ muons/sec.
\item [$\bullet$] Proton emission rate is 0.15 per muon capture,
the same value as that is being used in COMET designing
calculations
\item [$\bullet$] Energy resolution (FWHM) of silicon detectors
are: 140 keV for the 65 $\mu m$-thick detectors, and 40 keV for
the 140 $\mu m$-thick detectors.
\item [$\bullet$] Thickness of the beam counter scintillator: 0.5 mm
\end{itemize}
\item Simulation results of particle identification and rate
estimation is shown in Figure \ref{fig:dEdx} and Table
\ref{tb:rates}.
\end{itemize}
\vskip2ex
\begin{figure}[]
\includegraphics[width=0.95\onecolwid]{figs/dEdx}
\caption{Particle identification with two silicon detectors}
\label{fig:dEdx}
\end{figure}
\end{block}
\end{column}
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\begin{alertblock}{Proton beam}
\end{alertblock}
\vskip2ex
\begin{block}{Plan}
\begin{itemize}
\item July 2012: submitted the proposal to TRIUMF as experiment
S1371, requested 36 shifts (3 weeks) beam time
\item September 2012: the proposal was accepted with high priority
\item Late November 2012: beam test
\item Early 2013: physics run, 36 shifts
\item A proposal will be submitted to PSI
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{References}
\small{\begin{thebibliography}{99}
%\bibitem{cdr} The COMET Collaboration, ``Conceptual Design Report for
%Experimental Search for Lepton Flavor Violating $\mu^--e^-$
%Conversion at
%Sensitivity of $10^{-16}$ with a Slow-Extracted Bunched Proton Beam
%(COMET)'', KEK-2009-10
\bibitem{loi} The COMET Collaboration, ``Letter of Intent for Phase-I
of the COMET Experiment at J-PARC'', J-PARC-2012-3
\bibitem{sidata} S. E. Sobottka and E. L. Wills, ``Energy Spectrum
of Charged Particles Emitted Following Muon Capture in Si$^{28}$'',
Phys. Rev. Lett. \textbf{20} (1968) 596-598.
\end{thebibliography}}
\end{block}
\end{column}
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%Those pictures where drawn with the TikZ package, which is a perfect tool if
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%manual \cite{pgf}. It is even possible to wonderfull frames around posters.
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%--Conclusion block-------------------------------------------------------------
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% As you can see it is possible to make your poster very colorfull. But in
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% shades of the jacobs blue and some decent green highlights. These colors
% where chosen carefully to keep a consistent look of the poster. The
% \emph{cpbgposter} style is installed our office computers, so you should be
% able to compile this example out of the box with pdflatex. If you want to
% work on your computer make sure that you have a recent TeX distribution
% (TeXlive 2008, Miktex) and download the beamerthemecpbgposter.sty file from
% our teamwork page and put it in your local TeX directory.
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% If you have any questions, critics, ideas or if you just want to praise the
% awesome dude who created this insanely great poster style then don't
% hastitate to write an email to \emph{j.liebers@jacobs-university.de}
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