nam/writeup
1
0
Fork 0
Code Issues Pull Requests Projects Releases Wiki Activity

various fixes

Browse Source
This commit is contained in:
nam
2014-11-27 15:46:58 +09:00
parent befa19706a
commit b99a626448
7 changed files with 42 additions and 41 deletions
Download Patch File Download Diff File Expand all files Collapse all files

38
thesis/chapters/chap4_alcap_phys.tex
View File

@@ -548,8 +548,8 @@ The classical Coulomb barrier $V$ they used are given by:
\label{eqn:classical_coulomb_barrier}
\end{equation}
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
$\rho = 0 \textrm{ fm}$ for protons were taken.
nucleus respectively, $e^2 = 1.44 \si{\MeV}\cdot\textrm{fm}$, $r_0 = 1.35
\textrm{ fm}$, and $\rho = 0 \textrm{ fm}$ for protons were taken.
\begin{figure}[htb]
\centering
\includegraphics[width=0.48\textwidth]{figs/wyttenbach_rate_1p}
@@ -684,25 +684,25 @@ al.~\cite{VilgelmovaEvseev.etal.1971} observed.
%nucleus & calculation & experiment & calculation & experiment \\
%\textbf{Col1}\\
\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 & \\
$^{31}_{15}$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 & {} \\
$^{41}_{19}$K & 5.1 & {(4.7)} & 30 & {$> 28 \pm 4$} &(70)\\
$^{51 }_{23}$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)\\
$^{59 }_{27}$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&\\
$^{63 }_{29}$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)\\
$^{75 }_{33}$As &1.5 &1.4 \pm 0.2 &14 &{$>14 \pm 1.3$}& (19)\\
$^{79 }_{35}$Br &2.7 &{} &22 & &\\
$^{107}_{47}$Ag &2.3 &{} &18 & &\\
$^{115}_{49}$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)\\
$^{165}_{67}$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)\\
$^{208}_{82}$Pb &0.14 &0.13 \pm 0.02 &1.1 &{$>3.0 \pm 0.8$} &(4.1)\\
$^{41}_{19}$K & 5.1 & {(4.7)} & 30 & {$> 28$} &(70)\\
%$^{51 }_{23}$V &3.7 &2.9 \pm 0.4 &25 &{$>20 \pm 1.8$}& (32)\\
%$^{55 }_{25}$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)\\
%$^{60 }_{28}$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 $}& (36)\\
%$^{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$}& (19)\\
%$^{79 }_{35}$Br &2.7 &{} &22 & &\\
%$^{107}_{47}$Ag &2.3 &{} &18 & &\\
%$^{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$} &(6.7)\\
%$^{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$} &(3.0)\\
%$^{208}_{82}$Pb &0.14 &0.13 \pm 0.02 &1.1 &{$>3.0 \pm 0.8$} &(4.1)\\
\bottomrule
\end{tabular}
\end{center}

4
thesis/chapters/chap6_analysis.tex
View File

@@ -178,7 +178,7 @@ which is consistent with the number of X-rays counted using the active target.
\toprule
\textbf{Efficiency and intensity} & \textbf{Value} & \textbf{Absolute error} & \textbf{Relative error} \\
\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 \\
\vspace{0.03em}\\
\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
calculated as:
\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
E}}\right]}
\end{equation}

18
thesis/chapters/chap7_results.tex
View File

@@ -57,20 +57,20 @@ layer due to these protons with
different absorber thickness are shown in \cref{tab:proton_cdc_hitrate}.
\begin{table}[htb]
\begin{center}
\begin{tabular}{S S S S S}
\begin{tabular}{S S S S S S}
\toprule
{\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{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{\keV\per\cc)}}\\
& {(\si{\keV\per\cc)}} &{(mC/cm)}\\
\midrule
1 &0.5&1.5 & 2 & 195\\
0.5 &0.5&1.0 & 126 & 167\\
0 &0.5&0.5 & 1436 & 133\\
0 &0.3&0.3 & 8281 & {-}\\
0 &0.1&0.1 & 15011& {-}\\
1 &0.5&1.5 & 2 & 195 & 25\\
0.5 &0.5&1.0 & 126 & 167 & 60\\
0 &0.5&0.5 & 1436 & 133 & 160\\
%0 &0.3&0.3 & 8281 & {-} & {-}\\
%0 &0.1&0.1 & 15011& {-} & {-}\\
\bottomrule
\end{tabular}
\end{center}

2
thesis/chapters/chap8_conclusions.tex
View File

@@ -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
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
$(3.5\pm0.2)$.
$(3.5\pm0.2)\%$.
\end{enumerate}
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

2
thesis/chapters/frontmatter.tex
View File

@@ -14,7 +14,7 @@ Osaka University}
violation (CLFV) process, the muon-to-electron conversion in the presence of
a nucleus,
\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 $BR(\mu^{-} + Au \rightarrow e^{-} + Au)
< 7 \times 10^{-13}$, set by the SINDRUM II experiment [2].

9
thesis/mythesis.sty
View File

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

10
thesis/thesis.tex
View File

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