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various fixes

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nam
2014-11-27 15:46:58 +09:00
parent befa19706a
commit b99a626448
7 changed files with 42 additions and 41 deletions
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38
thesis/chapters/chap4_alcap_phys.tex
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@@ -548,8 +548,8 @@ The classical Coulomb barrier $V$ they used are given by:
\label{eqn:classical_coulomb_barrier} \label{eqn:classical_coulomb_barrier}
\end{equation} \end{equation}
where $z$ and $Z$ are the charges of the outgoing particle and of the residual where $z$ and $Z$ are the charges of the outgoing particle and of the residual
nucleus respectively, $e^2 = 1.44 \si{\MeV}$, $r_0 = 1.35 \textrm{ fm}$, and nucleus respectively, $e^2 = 1.44 \si{\MeV}\cdot\textrm{fm}$, $r_0 = 1.35
$\rho = 0 \textrm{ fm}$ for protons were taken. \textrm{ fm}$, and $\rho = 0 \textrm{ fm}$ for protons were taken.
\begin{figure}[htb] \begin{figure}[htb]
\centering \centering
\includegraphics[width=0.48\textwidth]{figs/wyttenbach_rate_1p} \includegraphics[width=0.48\textwidth]{figs/wyttenbach_rate_1p}
@@ -684,25 +684,25 @@ al.~\cite{VilgelmovaEvseev.etal.1971} observed.
%nucleus & calculation & experiment & calculation & experiment \\ %nucleus & calculation & experiment & calculation & experiment \\
%\textbf{Col1}\\ %\textbf{Col1}\\
\midrule \midrule
$^{27}_{13}$Al & 9.7 & {(4.7)} & 40 & {$> 28 \pm 4$} &(70)\\ $^{27}_{13}$Al & 9.7 & {(4.7)} & 40 & {$> 28 $} &(70)\\
$^{28}_{14}$Si & 32 & 53 \pm 10 & 144 & 150 \pm 30 & \\ $^{28}_{14}$Si & 32 & 53 \pm 10 & 144 & 150 \pm 30 & \\
$^{31}_{15}$P & 6.7 & {(6.3)} & 35 & {$> 61 \pm 6$}&(91) \\ $^{31}_{15}$P & 6.7 & {(6.3)} & 35 & {$> 61$}&(91) \\
$^{39}_{19}$K & 19 & 32 \pm 6 & 67 & {} \\ $^{39}_{19}$K & 19 & 32 \pm 6 & 67 & {} \\
$^{41}_{19}$K & 5.1 & {(4.7)} & 30 & {$> 28 \pm 4$} &(70)\\ $^{41}_{19}$K & 5.1 & {(4.7)} & 30 & {$> 28$} &(70)\\
$^{51 }_{23}$V &3.7 &2.9 \pm 0.4 &25 &{$>20 \pm 1.8$}& (32)\\ %$^{51 }_{23}$V &3.7 &2.9 \pm 0.4 &25 &{$>20 \pm 1.8$}& (32)\\
$^{55 }_{25}$Mn &2.4 &2.8 \pm 0.4 &16 &{$>26 \pm 2.5$}& (35)\\ %$^{55 }_{25}$Mn &2.4 &2.8 \pm 0.4 &16 &{$>26 \pm 2.5$}& (35)\\
$^{59 }_{27}$Co &3.3 &1.9 \pm 0.2 &21 &{$>37 \pm 3.4$}& (50)\\ %$^{59 }_{27}$Co &3.3 &1.9 \pm 0.2 &21 &{$>37 \pm 3.4$}& (50)\\
$^{60 }_{28}$Ni &8.9 &21.4 \pm 2.3 &49 &40 \pm 5&\\ %$^{60 }_{28}$Ni &8.9 &21.4 \pm 2.3 &49 &40 \pm 5&\\
$^{63 }_{29}$Cu &4.0 &2.9 \pm 0.6 &25 &{$>17 \pm 3 $}& (36)\\ %$^{63 }_{29}$Cu &4.0 &2.9 \pm 0.6 &25 &{$>17 \pm 3 $}& (36)\\
$^{65 }_{29}$Cu &1.2 &{(2.3)} &11 &{$>35 \pm 4.5$}& (36)\\ %$^{65 }_{29}$Cu &1.2 &{(2.3)} &11 &{$>35 \pm 4.5$}& (36)\\
$^{75 }_{33}$As &1.5 &1.4 \pm 0.2 &14 &{$>14 \pm 1.3$}& (19)\\ %$^{75 }_{33}$As &1.5 &1.4 \pm 0.2 &14 &{$>14 \pm 1.3$}& (19)\\
$^{79 }_{35}$Br &2.7 &{} &22 & &\\ %$^{79 }_{35}$Br &2.7 &{} &22 & &\\
$^{107}_{47}$Ag &2.3 &{} &18 & &\\ %$^{107}_{47}$Ag &2.3 &{} &18 & &\\
$^{115}_{49}$In &0.63 &{(0.77)} &7.2 &{$>11 \pm 1$} &(12)\\ %$^{115}_{49}$In &0.63 &{(0.77)} &7.2 &{$>11 \pm 1$} &(12)\\
$^{133}_{55}$Cs &0.75 &0.48 \pm 0.07 &8.7 &{$>4.9 \pm 0.5$} &(6.7)\\ %$^{133}_{55}$Cs &0.75 &0.48 \pm 0.07 &8.7 &{$>4.9 \pm 0.5$} &(6.7)\\
$^{165}_{67}$Ho &0.26 &0.30 \pm 0.04 &4.1 &{$>3.4 \pm 0.3$} &(4.6)\\ %$^{165}_{67}$Ho &0.26 &0.30 \pm 0.04 &4.1 &{$>3.4 \pm 0.3$} &(4.6)\\
$^{181}_{73}$Ta &0.15 &0.26 \pm 0.04 &2.8 &{$>0.7 \pm 0.1$} &(3.0)\\ %$^{181}_{73}$Ta &0.15 &0.26 \pm 0.04 &2.8 &{$>0.7 \pm 0.1$} &(3.0)\\
$^{208}_{82}$Pb &0.14 &0.13 \pm 0.02 &1.1 &{$>3.0 \pm 0.8$} &(4.1)\\ %$^{208}_{82}$Pb &0.14 &0.13 \pm 0.02 &1.1 &{$>3.0 \pm 0.8$} &(4.1)\\
\bottomrule \bottomrule
\end{tabular} \end{tabular}
\end{center} \end{center}

4
thesis/chapters/chap6_analysis.tex
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@@ -178,7 +178,7 @@ which is consistent with the number of X-rays counted using the active target.
\toprule \toprule
\textbf{Efficiency and intensity} & \textbf{Value} & \textbf{Absolute error} & \textbf{Relative error} \\ \textbf{Efficiency and intensity} & \textbf{Value} & \textbf{Absolute error} & \textbf{Relative error} \\
\midrule \midrule
Detector efficiency & \num{4.40E-4} & \num{0.978E-5} & 0.02 \\ Detector efficiency & \num{4.40E-4} & \num{0.10E-4} & 0.02 \\
X-ray intensity & 0.803 & 0.008 & 0.009 \\ X-ray intensity & 0.803 & 0.008 & 0.009 \\
\vspace{0.03em}\\ \vspace{0.03em}\\
\toprule \toprule
@@ -336,7 +336,7 @@ With the aid from MC study (\cref{fig:pid_sim}), the banding on
The band of protons is then extracted by cut on likelihood probability The band of protons is then extracted by cut on likelihood probability
calculated as: calculated as:
\begin{equation} \begin{equation}
p_{i} = \dfrac{1}{\sqrt{2\pi}\sigma_{\Delta E}} P_{i} = \dfrac{1}{\sqrt{2\pi}\sigma_{\Delta E}}
\exp{\left[\dfrac{(\Delta E_{meas.} - \Delta E_i)^2} {2\sigma^2_{\Delta \exp{\left[\dfrac{(\Delta E_{meas.} - \Delta E_i)^2} {2\sigma^2_{\Delta
E}}\right]} E}}\right]}
\end{equation} \end{equation}

18
thesis/chapters/chap7_results.tex
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@@ -57,20 +57,20 @@ layer due to these protons with
different absorber thickness are shown in \cref{tab:proton_cdc_hitrate}. different absorber thickness are shown in \cref{tab:proton_cdc_hitrate}.
\begin{table}[htb] \begin{table}[htb]
\begin{center} \begin{center}
\begin{tabular}{S S S S S} \begin{tabular}{S S S S S S}
\toprule \toprule
{\textbf{Absorber}} &{\textbf{Inner wall}} & {\textbf{Total CFRP}}& {\textbf{Absorber}} &{\textbf{Inner wall}} & {\textbf{Total CFRP}}&
{\textbf{Proton}} & {\textbf{Momentum}}\\ {\textbf{Proton}} & {\textbf{Momentum}} & {\textbf{Integrated charge}}\\
{\textbf{thickness}} &{\textbf{thickness}} & {\textbf{thickness}}& {\textbf{thickness}} &{\textbf{thickness}} & {\textbf{thickness}}&
{\textbf{hit rate}} &{\textbf{spread $\Delta p$}}\\ {\textbf{hit rate}} &{\textbf{spread $\Delta p$}} &{\textbf{300 days}}\\
{(\si{\mm})} & {(\si{\mm})} & {(\si{\mm})} & {(\si{\Hz})} {(\si{\mm})} & {(\si{\mm})} & {(\si{\mm})} & {(\si{\Hz})}
& {(\si{\keV\per\cc)}}\\ & {(\si{\keV\per\cc)}} &{(mC/cm)}\\
\midrule \midrule
1 &0.5&1.5 & 2 & 195\\ 1 &0.5&1.5 & 2 & 195 & 25\\
0.5 &0.5&1.0 & 126 & 167\\ 0.5 &0.5&1.0 & 126 & 167 & 60\\
0 &0.5&0.5 & 1436 & 133\\ 0 &0.5&0.5 & 1436 & 133 & 160\\
0 &0.3&0.3 & 8281 & {-}\\ %0 &0.3&0.3 & 8281 & {-} & {-}\\
0 &0.1&0.1 & 15011& {-}\\ %0 &0.1&0.1 & 15011& {-} & {-}\\
\bottomrule \bottomrule
\end{tabular} \end{tabular}
\end{center} \end{center}

2
thesis/chapters/chap8_conclusions.tex
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@@ -24,7 +24,7 @@ was made. The main results are:
with a decay constant of \SI{2.6}{\MeV}. The partial emission rate in the with a decay constant of \SI{2.6}{\MeV}. The partial emission rate in the
energy range from \SIrange{4}{8}{\MeV} is $(1.7 \pm 0.1)\%$, and the total energy range from \SIrange{4}{8}{\MeV} is $(1.7 \pm 0.1)\%$, and the total
emission rate assuming the shape holds for the whole spectrum is emission rate assuming the shape holds for the whole spectrum is
$(3.5\pm0.2)$. $(3.5\pm0.2)\%$.
\end{enumerate} \end{enumerate}
The emission rate is consistent with the lower limit of 2.8\% set by The emission rate is consistent with the lower limit of 2.8\% set by
Wyttenbach et al.~\cite{WyttenbachBaertschi.etal.1978}. It is also compatible Wyttenbach et al.~\cite{WyttenbachBaertschi.etal.1978}. It is also compatible

2
thesis/chapters/frontmatter.tex
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@@ -14,7 +14,7 @@ Osaka University}
violation (CLFV) process, the muon-to-electron conversion in the presence of violation (CLFV) process, the muon-to-electron conversion in the presence of
a nucleus, a nucleus,
\muec. The process is forbidden in the Standard Model (SM), however is \muec. The process is forbidden in the Standard Model (SM), however is
predicted to occur in various extensions of SM, such as . Current experimental predicted to occur in various extensions of SM. Current experimental
upper limit of the branching ratio is $BR(\mu^{-} + Au \rightarrow e^{-} + Au) upper limit of the branching ratio is $BR(\mu^{-} + Au \rightarrow e^{-} + Au)
< 7 \times 10^{-13}$, set by the SINDRUM II experiment [2]. < 7 \times 10^{-13}$, set by the SINDRUM II experiment [2].

9
thesis/mythesis.sty
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@@ -12,10 +12,11 @@ inner=1.25in, outer=1in, twoside]{geometry}
%$ Hyper-link .. %$ Hyper-link ..
\RequirePackage[% \RequirePackage[%
colorlinks=false,% color links instead of using boxes %colorlinks=false,% color links instead of using boxes
linkcolor=red,% color for internal (intra-document) links %linkcolor=red,% color for internal (intra-document) links
citecolor=green,% color for bibliographic links %citecolor=green,% color for bibliographic links
urlcolor=blue,% color for URL links %urlcolor=blue,% color for URL links
hidelinks,
hyperfootnotes=false,% disable links to footnotes (because feature broken) hyperfootnotes=false,% disable links to footnotes (because feature broken)
hyperindex,% make page numbers in index into hyperlinks hyperindex,% make page numbers in index into hyperlinks
pdfstartview={FitH},% startup page view: fit width of page to window pdfstartview={FitH},% startup page view: fit width of page to window

10
thesis/thesis.tex
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@@ -30,13 +30,13 @@ for the COMET experiment}
\mainmatter \mainmatter
%%%\input{chapters/chap1_intro} %%%\input{chapters/chap1_intro}
\input{chapters/chap2_mu_e_conv} %\input{chapters/chap2_mu_e_conv}
\input{chapters/chap3_comet} %\input{chapters/chap3_comet}
\input{chapters/chap4_alcap_phys} %\input{chapters/chap4_alcap_phys}
\input{chapters/chap5_alcap_setup} %\input{chapters/chap5_alcap_setup}
\input{chapters/chap6_analysis} \input{chapters/chap6_analysis}
\input{chapters/chap7_results} \input{chapters/chap7_results}
\input{chapters/chap8_conclusions} %\input{chapters/chap8_conclusions}
\begin{backmatter} \begin{backmatter}
\input{chapters/backmatter} \input{chapters/backmatter}