adding missing pieces

2019-11-12 16:11:31 -06:00
parent 2e3caf4d63
commit 238119d740
29 changed files with 2559 additions and 0 deletions
--- a/CINANP2015_abstract/abstract.tex
+++ b/CINANP2015_abstract/abstract.tex
@@ -0,0 +1,30 @@
+\documentclass{article}
+\begin{document}
+The AlCap is an experiment which precisely measures products of
+nuclear muon capture on aluminum. It is a joint project between COMET and Mu2e
+collaborations since both experiments intend to search for lepton flavor
+violating conversion $\mu^-+A\rightarrow e^-+A$ where the capture products
+would cause significant issues on detector hit rates, radiation damage, and
+backgrounds.
+
+The first run of AlCap has been carried out at PSI in December 2013 for
+protons measurement. Initial analysis showed that emission rate of protons from
+4 to 8 MeV is $(1.7 \pm 0.1)$ per nuclear muon capture. The proton spectrum
+peaks at 3.7 MeV and decreases exponentially with a decay constant of 2.6 MeV.
+Two more runs are scheduled in June (for neutrons and photons), and October
+(for protons) 2015.
+
+
+%The AlCap experiment is a joint project between the COMET and Mu2e
+%collaborations. Both experiments intend to look for the lepton-flavour
+%violating conversion $\mu^-+A\rightarrow e^-+A$, using tertiary muons from high-power pulsed
+%proton beams. In these experiments the products of ordinary muon capture in the
+%muon stopping target are an important concern, both in terms of hit rates in
+%tracking detectors and radiation damage to equipment. The goal of the AlCap
+%experiment is to provide precision measurements of the products of nuclear
+%capture on Aluminium, which is the favoured target material for both COMET and
+%Mu2e. The results will be used for optimising the design of both conversion
+%experiments, and as input to their simulations. Data was taken in December 2013
+%and is currently being analysed. 
+  
+\end{document}
--- a/cv/pd_application/Makefile
+++ b/cv/pd_application/Makefile
@@ -0,0 +1,20 @@
+DOC=cv
+INPUT=$(DOC).tex
+TARGET=$(DOC).pdf
+TEX=pdflatex
+
+default: $(TARGET)
+
+$(TARGET): $(INPUT) Makefile *.bib
+	# $(TEX) $< && $(TEX) $<
+	$(TEX) $< 
+	bibtex jrnl.aux
+	bibtex thes.aux
+	bibtex proc.aux
+	$(TEX) $<
+	$(TEX) $<
+	$(TEX) soi.tex
+
+clean:
+	rm -f $(DOC).{pdf,out,aux,log}
+	rm -f *.{pdf,out,aux,log,bbl,blg}
--- a/cv/pd_application/cv.tex
+++ b/cv/pd_application/cv.tex
@@ -0,0 +1,250 @@
+\documentclass[11pt,a4paper,sans]{moderncv}      
+\moderncvstyle{classic}
+\moderncvcolor{orange}
+
+\usepackage[utf8]{inputenc}
+\usepackage[scale=0.75]{geometry}
+% \setlength{\hintscolumnwidth}{3cm}
+
+% personal data
+\name{Nam}{Tran}
+\title{Curriculum Vit\ae}
+\address{Department of Physics, Osaka University}{1-1 Machikaneyama, Toyonaka, Osaka}{Japan 560-0043}
+\phone[fixed]{+81~06~6850~6739}
+\phone[fax]{+81~06~6850~6739}
+\email{nam@kuno-g.phys.sci.osaka-u.ac.jp}
+%\photo[64pt][0.4pt]{picture}                       
+
+% bibliography with mutiple entries
+\usepackage{multibib}
+\newcites{thes,jrnl,proc}{{Theses},{Journals}, {Conferences and Proceedings}}
+
+\usepackage{float}
+
+% Define \cvdoublecolumn, which sets its arguments in two columns without any labels
+
+\newcommand{\cvdoublecolumn}[2]{%
+  \cvitem[0.75em]{}{%
+    \begin{minipage}[t]{\listdoubleitemmaincolumnwidth}#1\end{minipage}%
+    \hfill%
+    \begin{minipage}[t]{\listdoubleitemmaincolumnwidth}#2\end{minipage}%
+    }%
+}
+
+% usage: \cvreference{name}{address line 1}{address line 2}{address line 3}{address line 4}{e-mail address}{phone number}
+% Everything but the name is optional
+% If \addresssymbol, \emailsymbol or \phonesymbol are specified, they will be used.
+% (Per default, \addresssymbol isn't specified, the other two are specified.)
+% If you don't like the symbols, remove them from the following code, including the tilde ~ (space).
+\usepackage{float}
+
+\newcommand{\cvreference}[9]{%
+    \textbf{#1}\newline% Name
+    \ifthenelse{\equal{#2}{}}{}{\addresssymbol~#2\newline}% Department
+    \ifthenelse{\equal{#3}{}}{}{#3\newline}% Company
+    \ifthenelse{\equal{#4}{}}{}{#4\newline}% Position
+    \ifthenelse{\equal{#5}{}}{}{#5\newline}% Adress 1
+    \ifthenelse{\equal{#6}{}}{}{#6\newline}% Adress 2
+    \ifthenelse{\equal{#7}{}}{}{\emailsymbol~\texttt{#7}\newline}% % E-mail
+    \ifthenelse{\equal{#8}{}}{}{\phonesymbol~#8\newline} % Telephone
+    \ifthenelse{\equal{#9}{}}{}{\mobilephonesymbol~#9}} % CellPhone
+
+%----------------------------------------------------------------------------------
+%            content
+%----------------------------------------------------------------------------------
+\begin{document}
+%\begin{CJK*}{UTF8}{gbsn}                          % to typeset your resume in Chinese using CJK
+%-----       resume       ---------------------------------------------------------
+\makecvtitle
+
+\section{Appointments}
+
+\vspace{6pt}
+\cventry
+{2015--today} % time period
+{Postdoctoral researcher} % job title
+{Department of Physics, Osaka University} % affiliation
+{} % location
+{} % optional: grade ..., should be left blank
+{\vspace{3pt}Experimental search for muon to electron
+    conversion in aluminum, the COMET or J-PARC E21 experiment: 
+    \begin{itemize}
+      \item Measure the number of muons that stop in the muon stopping target
+      \item Monte Carlo simulation of cosmic ray background in COMET Phase-I
+      \item Magnetic field map calculation
+    \end{itemize}
+  }
+
+\vspace{6pt}
+\cventry
+{2012--2014} % time period
+{JSPS Fellowship for Young Researcher} % job title
+{Department of Physics, Osaka University} % affiliation
+{} % location
+{} % optional: grade ..., should be left blank
+{\vspace{3pt}Development of a prototype TPC for a $\mu\rightarrow 3e$ search at
+  Osaka University}
+
+\vspace{6pt}
+\cventry
+{2008--2010}
+{Lecturer}
+{School of Nuclear Engineering and Environmental Physics,\newline Hanoi University of Science and Technology}
+{}
+{}
+{\vspace{3pt}
+  \begin{itemize}
+    \item Measurements of photonuclear reaction cross-section,
+      neutron activation method in non-destructive testing
+    \item Teach a course on Radiation Dose Measurements and Protection
+    \item Mentor senior students on basic nuclear experiments
+  \end{itemize}
+}
+
+\section{Education}
+\vspace{6pt}
+\cventry
+{2010-2014}
+{PhD, Physics}
+{Osaka University}
+{}
+{}
+{
+  \begin{itemize}
+    \item \textbf{Thesis:} \href{http://hdl.handle.net/11094/52295}{\emph{A study of proton emission following nuclear
+        muon capture for the COMET experiment}}
+    % \item \textbf{Advisor:} Yoshitaka Kuno
+  \end{itemize}
+}
+
+\vspace{6pt}
+\cventry
+{2007-2010}
+{Master, Engineering Physics}
+{Hanoi University of Science and Technology}
+{}
+{}
+{
+  \begin{itemize}
+    \item \textbf{Thesis:} \emph{Measurements of isomeric yield ratios for the
+      \textsuperscript{45}Sc($\gamma$, n)\textsuperscript{44m,g}Sc reaction at
+      50, 60, 70 MeV bremsstrahlung}
+  \end{itemize}
+}
+
+\vspace{6pt}
+\cventry
+{2002-2007}
+{Engineer, Engineering Physics}
+{Hanoi University of Technology}
+{}
+{}
+{
+  \begin{itemize}
+    \item \textbf{Thesis:} \emph{Design and production of an ionization chamber
+        for neutron detection via the \textsuperscript{6}Li(n,
+        $\alpha$)\textsuperscript{3}H reaction }
+  \end{itemize}
+}
+
+
+\section{Short-term schools and courses}
+\cventry {Jun. 2014}{International school on real-time systems}{
+  Osaka University, Japan} {} {}{
+  Hand-on lessons on modern DAQ system using waveform digitizers, FPGA-based
+  front-ends, and data collection and distribution over network.}
+
+\vspace{6pt}
+\cventry{Mar. 2013}{
+  Excellence in detectors and instrumentation technologies 2013 (EDIT2013)}{
+  KEK, Japan}{}{}{
+  Lectures and hand-on exercises on wire chambers and silicon detectors}
+
+\vspace{6pt}
+\cventry{Oct. 2012}{Asia Europe Pacific school of high energy physics 2012
+  (AEPSHEP2012)}{Fukuoka, Japan}{}{}{
+  Lectures on high energy physics from an experimental and phenomenological
+  perspective, focused on accelerator-based programmes}
+
+%%%%%%%%%%%%%%%%%%%%%%
+\section{References}
+% \begin{cvcolumns}
+  % \cvcolumn{}{
+    % \begin{itemize}
+      % \item \textbf{Yoshitaka Kuno}, Professor, Department of Physics, Osaka University
+      % \item Person 2
+      % \item Person 3
+    % \end{itemize}}
+% \end{cvcolumns}
+
+\cvdoublecolumn{
+    \cvreference{Yoshitaka Kuno}
+        {Professor}% Position
+        {Department of Physics}% Department
+        {Osaka University}% Company
+        {Toyonaka, Osaka, Japan 560-0043}% Adress 1
+        {}% Adress 2
+        {kuno@phys.sci.osaka-u.ac.jp}% E-mail
+        {+81-06-6850-5565}% Telephone
+        {}% CellPhone
+        {}
+    }
+    {
+    \cvreference{Peter Kammel}% Name
+        {Professor}% Position
+        {Department of Physics}% Department
+        {University of Washington}% Company
+        {Seattle, WA 98195-1560}% Adress 1
+        {}% Adress 2
+        {pkammel@uw.edu}% E-mail
+        {206-685-2401}% Telephone
+        {}% CellPhone
+        {}
+    }
+\cvdoublecolumn{
+    \cvreference{James Miller}
+        {Professor}% Position
+        {Department of Physics}% Department
+        {Boston University}% Company
+        {Boston, MA 02215}% Adress 1
+        {}% Adress 2
+        {miller@bu.edu}% E-mail
+        {617-353-2659}% Telephone
+        {}% CellPhone
+        {}
+    }
+    {
+      }
+%%%%%%%%%%%%%%%%%%%%%%
+\section{Publications}
+\nocitethes{*}
+\bibliographystylethes{ieeetr}
+\bibliographythes{theses}
+
+\nocitejrnl{*}
+\bibliographystylejrnl{ieeetr}
+\bibliographyjrnl{journals}
+
+\nociteproc{*}
+\bibliographystyleproc{ieeetr}
+\bibliographyproc{proceedings}
+
+
+%-----       letter       ---------------------------------------------------------
+% recipient data
+% \newpage
+% \recipient{Lee Roberts}{Department of Physics, Boston University\\590 Commonwealth Avenue\\Boston, MA 02215}
+% \date{\today}
+% \opening{Dear Professor Roberts,}
+% \closing{Yours faithfully,}
+% \enclosure[Attached]{curriculum vit\ae{}}          % use an optional argument to use a string other than "Enclosure", or redefine \enclname
+% \makelettertitle
+% Body text
+% \makeletterclosing
+%-----       letter       -----------------------------------------------
+
+\end{document}
+
+
+%% end of file `template.tex'.
+
--- a/cv/pd_application/cv2.tex
+++ b/cv/pd_application/cv2.tex
@@ -0,0 +1,149 @@
+\documentclass[11pt,a4paper,sans]{moderncv}      
+\moderncvstyle{classic}
+\moderncvcolor{orange}
+
+\usepackage[utf8]{inputenc}
+\usepackage[scale=0.75]{geometry}
+% \setlength{\hintscolumnwidth}{3cm}
+
+% personal data
+\name{Nam}{Tran}
+\title{Curriculum Vitae}
+\address{Department of Physics, Osaka University}{1-1 Machikaneyama, Toyonaka, Osaka}{Japan 560-0043}
+\phone[fixed]{+81~06~6850~6739}
+\phone[fax]{+81~06~6850~6739}
+\email{nam@kuno-g.phys.sci.osaka-u.ac.jp}
+%\photo[64pt][0.4pt]{picture}                       
+
+% bibliography with mutiple entries
+\usepackage{multibib}
+\newcites{thes,jrnl,proc}{{Theses},{Journals}, {Conferences and Proceedings}}
+%----------------------------------------------------------------------------------
+%            content
+%----------------------------------------------------------------------------------
+\begin{document}
+%\begin{CJK*}{UTF8}{gbsn}                          % to typeset your resume in Chinese using CJK
+%-----       resume       ---------------------------------------------------------
+\makecvtitle
+
+\section{Appointments}
+
+\vspace{6pt}
+\cventry
+{2015--today} % time period
+{Postdoctoral researcher} % job title
+{Department of Physics, Osaka University} % affiliation
+{} % location
+{} % optional: grade ..., should be left blank
+{\vspace{3pt}Experimental search for muon to electron
+    conversion in aluminum, the COMET or J-PARC E21 experiment: 
+    \begin{itemize}
+      \item Normalisation of number of stopped muons in the stopping target
+      \item Monte Carlo simulation of cosmic background in COMET Phase-I
+      \item Magnetic field calculation
+    \end{itemize}
+  }
+
+\vspace{6pt}
+\cventry
+{2012--2014} % time period
+{JSPS Fellowship for Young Researcher} % job title
+{Department of Physics, Osaka University} % affiliation
+{} % location
+{} % optional: grade ..., should be left blank
+{\vspace{3pt}Development of a prototype TPC for a $\mu\rightarrow 3e$ search at
+  Osaka University}
+
+\vspace{6pt}
+\cventry
+{2008--2010}
+{Lecturer}
+{School of Nuclear Engineering and Environmental Physics,\newline Hanoi University of Science and Technology}
+{}
+{}
+{\vspace{3pt}
+  \begin{itemize}
+    \item Research on measurements of photonuclear reaction cross-section,
+      neutron activation method in non-destructive testing
+    \item Teach a course on Radiation Dose Measurements and Protection
+    \item Mentor for basic nuclear experiments for senior students
+  \end{itemize}
+}
+
+\section{Education}
+\vspace{6pt}
+\cventry
+{2010-2014}
+{PhD, Physics}
+{Osaka University}
+{}
+{}
+{
+  \begin{itemize}
+    \item \textbf{Thesis:} \href{http://hdl.handle.net/11094/52295}{\emph{A study of proton emission following nuclear
+        muon capture for the COMET experiment}}
+    % \item \textbf{Advisor:} Yoshitaka Kuno
+  \end{itemize}
+}
+
+\vspace{6pt}
+\cventry
+{2007-2010}
+{Master, Engineering Physics}
+{Hanoi University of Science and Technology}
+{}
+{}
+{
+  \begin{itemize}
+    \item \textbf{Thesis:} \emph{Measurements of isomeric yield ratios for the
+      \textsuperscript{45}Sc($\gamma$, n)\textsuperscript{44m,g}Sc reaction at
+      50, 60, 70 MeV bremsstrahlung}
+  \end{itemize}
+}
+
+\vspace{6pt}
+\cventry
+{2002-2007}
+{Engineer, Engineering Physics}
+{Hanoi University of Technology}
+{}
+{}
+{
+  \begin{itemize}
+    \item \textbf{Thesis:} \emph{Design and production of an ionization chamber
+        for neutron detection via the \textsuperscript{6}Li(n,
+        $\alpha$)\textsuperscript{3}H reaction }
+  \end{itemize}
+}
+
+%%%%%%%%%%%%%%%%%%%%%%
+\section{Publications}
+\nocitethes{*}
+\bibliographystylethes{ieeetr}
+\bibliographythes{theses}
+
+\nocitejrnl{*}
+\bibliographystylejrnl{ieeetr}
+\bibliographyjrnl{journals}
+
+\nociteproc{*}
+\bibliographystyleproc{ieeetr}
+\bibliographyproc{proceedings}
+
+%-----       letter       ---------------------------------------------------------
+% recipient data
+\recipient{Dr. Lee Roberts}{Department of Physics\\Boston University\\590 Commonwealth Avenue\\ Boston, MA 02215}
+\date{April 26, 2016}
+\opening{Dear Sir or Madam,}
+\closing{Yours faithfully,}
+% \enclosure[Attached]{curriculum vit\ae{}}          % use an optional argument to use a string other than "Enclosure", or redefine \enclname
+\makelettertitle
+
+
+\makeletterclosing
+
+\end{document}
+
+
+%% end of file `template.tex'.
+
--- a/cv/pd_application/journals.bib
+++ b/cv/pd_application/journals.bib
@@ -0,0 +1,34 @@
+@article{doi:10.7566/JPSJ.82.044202, 
+  author = { Hiroyasu Ejiri and Izyan H.  Hashim and Yuko Hino and Yoshitaka
+    Kuno and Yuki Matsumoto and Kazuhiko Ninomiya and Hideyuki Sakamoto and
+      Akira Sato and Tatsushi Shima and Atsushi Shinohara and Keiji Takahisa
+      and Nam H. Tran}, 
+  title = {Nuclear $\gamma$ Rays from Stopped Muon Capture Reactions for
+    Nuclear Isotope Detection}, 
+  journal = {Journal of the Physical Society of Japan},
+  volume = {82}, 
+  number = {4}, 
+  pages = {044202}, 
+  year = {2013}, 
+  doi = {10.7566/JPSJ.82.044202}, 
+  URL = { http://dx.doi.org/10.7566/JPSJ.82.044202 },
+  eprint = { http://dx.doi.org/10.7566/JPSJ.82.044202 } 
+}
+
+@Article{Do2010, 
+  author="Do, Nguyen Van and Khue, Pham Duc and Thanh, Kim Tien and Nam, Tran
+    Hoai and Rahman, Md. Shakilur and Kim, Kyung-Sook and Lee, Manwoo and Kim,
+  Guinyun and Lee, Hee-Seock and Cho, Moo-Hyun and Ko, In Soo and Namkung,
+  Won",
+  title="Measurement of isomeric yield ratios for the $^{44m,g}${S}c isomeric pairs
+    produced from $^{45}${S}c and $^{nat}${T}i targets at 50-, 60-, and 70-{MeV}
+    bremsstrahlung",
+  journal="Journal of Radioanalytical and Nuclear Chemistry",
+  year="2010",
+  volume="287",
+  number="3",
+  pages="813--820",
+  issn="1588-2780",
+  doi="10.1007/s10967-010-0831-y",
+  url="http://dx.doi.org/10.1007/s10967-010-0831-y" 
+}
--- a/cv/pd_application/proceedings.bib
+++ b/cv/pd_application/proceedings.bib
@@ -0,0 +1,37 @@
+@conference{cipanp15,
+  author       = {Nam Hoai Tran and the AlCap collaboration}, 
+  title        = {Measurements of the emission products of nuclear muon capture
+    on aluminum},
+  booktitle = {The 12th Conference on the Intersections of Particle and Nuclear
+    Physics (CIPANP 2015)},
+  year         = 2015,
+  month        = 5,
+}
+
+@article{doi:10.7566/JPSCP.1.013006,
+  Author = {Nam Hoai Tran and the COMET Collaboration},
+  journal = {Proceedings of the 12th Asia Pacific Physics Conference (APPC12)},
+  Chapter = {147},
+  year = 2013,
+  month = 7,
+  Doi = {10.7566/JPSCP.1.013006},
+  Eprint = {http://journals.jps.jp/doi/pdf/10.7566/JPSCP.1.013006},
+  Title = {Status of the COMET Experiment at J-PARC},
+  Url = {http://journals.jps.jp/doi/abs/10.7566/JPSCP.1.013006},
+  Bdsk-Url-1 = {http://journals.jps.jp/doi/abs/10.7566/JPSCP.1.013006},
+  Bdsk-Url-2 = {http://dx.doi.org/10.7566/JPSCP.1.013006}}
+
+
+  @article{panic11,
+    author = "Tran, Nam Hoai and the MuSIC Collaboration",
+    title = "The first muon beam from a new highly-intense {DC} muon source,
+    {MuSIC}",
+    journal = "AIP Conference Proceedings",
+    year = "2012",
+    volume = "1441",
+    number = "1", 
+    pages = "652-654",
+    url = "http://scitation.aip.org/content/aip/proceeding/aipcp/10.1063/1.3700644",
+    doi = "http://dx.doi.org/10.1063/1.3700644" 
+  }
+
--- a/cv/pd_application/soi.tex
+++ b/cv/pd_application/soi.tex
@@ -0,0 +1,113 @@
+\documentclass[11pt,a4paper]{article}
+\usepackage[utf8]{inputenc}
+\usepackage[]{lmodern}
+\renewcommand{\familydefault}{\sfdefault}
+
+\date{\today}
+
+\setlength{\topmargin}{-10mm}
+\setlength{\textwidth}{7in}
+\setlength{\oddsidemargin}{-8mm}
+\setlength{\textheight}{9in}
+\setlength{\footskip}{1in}
+
+\begin{document}
+\pagenumbering{gobble}% Remove page numbers (and reset to 1)
+
+\begin{center}
+  \LARGE
+  Statement of Research Interests\\
+  % \large
+  % Nam Tran
+\end{center}
+
+\bigskip
+
+My work centers in an experimental search for charged lepton flavor violation
+(CLFV) with muons, namely the COMET experiment at J-PARC. COMET is a new
+experiment that aims to find the neutrinoless decay of muon to electron in
+a nuclear field, or
+muon to electron conversion, at a single event sensitivity of $10^{-17}$. The
+experiment has high impact as a positive result would provide an unambiguous
+evidence of new physics beyond the Standard Model (BSM); and a negative result
+will place stringent limits on theoretical models. The search is part of the
+Intensity Frontier in particle physics, which will provide a window to probe
+physics at energy scales far beyond the reach of the most powerful accelerator
+currently exists. I was inspired to join the COMET experiment because of its
+elegance: 
+\begin{itemize}
+  \itemsep-0.5em
+  \item the overall idea is simple;
+  \item the signal is clean and distinctive; 
+  \item and many novel technologies and solutions are needed to realize its goal.
+\end{itemize}
+
+% One issue had arisen in the preparation for COMET experiment is our knowledge
+% on the products of the nuclear muon capture process on aluminum target was not
+% sufficient. 
+One issue that arose during the preparation for COMET is that our knowledge of
+the products of the nuclear capture process on aluminum was not sufficient.
+Protons are expected to be a significant source of hits in the tracking
+detector of COMET, but there was no direct measurement of the proton rate and
+spectrum in the relevant energy range. Neutrons could cause serious problem for
+the front-end electronics. Therefore, COMET and its counterpart, Mu2e at
+Fermilab, jointly carried out a series of measurements, in the so-called AlCap
+experiment, of the products emitted after nuclear muon capture on aluminum and
+titanium at Paul Scherer Institute (PSI), Switzerland. I did a Monte Carlo
+study that showed the feasibility of the experiment, and contributed to DAQ
+developement, and hardware and electronics works on silicon and germanium
+detectors.
+
+My initial analysis of proton data in 2013 showed that the proton emission rate
+is low enough for the tracking detector of COMET to operate normally. The
+smallness of proton emission rate was later confirmed by another independent
+analysis on a larger dataset. However, there are still discrepancies between
+the two analyses. Therefore we have had another run for the  proton measurement
+in 2015. The data analysis for this run is ongoing.
+
+Since November 2014, I have been assigned as a subproject leader of COMET,
+responsible for monitoring the number of muons that stop in the muon stopping
+target. The number is evidently necessary for calculation of branching ratio
+and single event sensitivity of the experiment. There have been several
+ideas on how to achieve the goal: online measurement of muonic X-rays and
+delayed gamma rays from activated $^{27}$Mg; measurement of the spectrum of
+decay-in-orbit electrons, and the rate of protons emitted after nuclear muon
+capture. I have proposed another activation measurement: measure population of
+a long-lived activation product, namely $^{24}$Na ($T_{1/2} = 14.96$~h). The
+measuring scheme will be:
+\begin{itemize}
+  \itemsep-0.5em
+  \item irradiation with muon beam for 2 days,
+  \item beam off,
+  \item measure delayed gammas from $^{24}$Na (1368 and 2574 keV) for 2 hours,
+  \item continue irradiating, then repeat the cycle.
+\end{itemize}
+All these methods could be used simultaneously for cross-checking and
+reducing systematic uncertainties.
+
+% I also involve in other works, such as Monte Carlo simulation of cosmic ray
+% background in COMET Phase-I, and magnetic field map calculation for both COMET
+% Phase-I and Phase-II. 
+
+Having been working in COMET for 5 years, I have been able to work together
+with great collaborators, and have gained a wide range of skills
+needed for an experimental physicist, including simulation, detector
+development, data acquisition, and data analysis.  Now I would like to broaden
+my perspective and earn more experience by joining the Muon $g-2$ experiment.
+I am attracted by the ambitious goal of measuring the muon anomalous magnetic
+moment at an unprecedented precision, its impact of the measurement in
+establishing a signal for new physics beyond the Standard Model, as well as the
+synergy between $g-2$ and $\mu-e$ conversion experiments. My areas of
+contribution could be Monte Carlo simulation, detector and DAQ development.
+Besides, I am eager to learn new skills including accelerator-related
+techniques, FPGA development, and data analysis using machine learning.  
+
+% moving to another position.
+% The
+% transition to Mu2e would be smooth since the two
+% experiments have many things in common. 
+% Personally, I would like to strengthen
+% my data analysis skill with a new technique: machine learning. I believe
+% machine learning will be used extensively as I continue working in the
+% Intensity Frontier.
+\end{document}
--- a/cv/pd_application/theses.bib
+++ b/cv/pd_application/theses.bib
@@ -0,0 +1,9 @@
+@phdthesis{phdthesis,
+  author       = {Nam Hoai Tran}, 
+  title        = {A study of proton emission following nuclear muon capture for
+  the COMET experiment},
+  school       = {Osaka University},
+  year         = 2014,
+  month        = 12,
+  note         = {\url{http://hdl.handle.net/11094/52295}}
+}
--- a/fpcp2019_proceeding_unfinished/.gitignore
+++ b/fpcp2019_proceeding_unfinished/.gitignore
@@ -0,0 +1,2 @@
+*.bak
+*.sav
--- a/fpcp2019_proceeding_unfinished/Makefile
+++ b/fpcp2019_proceeding_unfinished/Makefile
@@ -0,0 +1,13 @@
+DOC=fpcp2019
+INPUT=$(DOC).tex
+TARGET=$(DOC).pdf
+TEX=pdflatex -shell-escape
+
+default: $(TARGET)
+
+$(TARGET): $(INPUT) Makefile 
+	$(TEX) $< && $(TEX) $<
+
+clean:
+	rm -f $(DOC).{pdf,out,aux,log}
+	rm -f *.{out,aux,log,bbl,blg}
--- a/fpcp2019_proceeding_unfinished/fpcp2019.tex
+++ b/fpcp2019_proceeding_unfinished/fpcp2019.tex
@@ -0,0 +1,194 @@
+\documentclass[twocolumn,twoside]{revtex4}
+\usepackage{graphicx}
+\usepackage{fancyhdr}
+\pagestyle{fancy}
+\fancyhead{} % clear all fields
+\fancyhead[C]{\it {
+Flavor Physics and CP Violation Conference, Victoria BC, 2019
+}} \fancyhead[RO,LE]{\thepage}
+\fancyfoot{} % clear all fields
+\fancyfoot[LE,LO]{}
+\usepackage{amsmath}
+
+\renewcommand{\headrulewidth}{0pt}
+\renewcommand{\footrulewidth}{0pt}
+\renewcommand{\sfdefault}{phv}
+
+\setlength{\textheight}{235mm}
+\setlength{\textwidth}{170mm}
+\setlength{\topmargin}{-20mm}
+\usepackage{hyperref}
+\usepackage[noabbrev, capitalize]{cleveref} % hyperref must be loaded first
+\usepackage[
+  detect-weight=true,
+  per=slash,
+  detect-family=true,
+  separate-uncertainty=true]{siunitx}
+
+\bibliographystyle{apsrev}
+
+% ************* Make changes after here  ***************
+
+\fancyfoot[LE,LO]{\bf MonB1010}
+
+\begin{document}
+
+%Title of paper
+\title{Measurements of the muon anomalous magnetic moment}
+\author{Nam H. Tran\\
+  on behalf of the Muon $g-2$ Experiment at Fermilab}
+\affiliation{Boston University, Boston, MA, US 02215}
+%
+
+\begin{abstract}
+  The over 3-sigma discrepancy between the latest experimental and theoretical
+  values of the anomalous magnetic of the muon has been one of the best
+  hints of new physics beyond the Standard Model. Ongoing efforts
+  to settle the issue from the experimental side are happening at Fermilab and
+  J-PARC. The E989 at Fermilab is using the same key technologies as the last
+  experiment at BNL (E821), but with great improvement in accuracy. The first
+  physics data has been taken, and data analysis is going to be finalized soon.
+  The E34 at J-PARC adopts a novel approach, is
+  well advanced in R\&D, and recently received Stage-2 Approval. The
+  experimental principles, techniques, and prospects of these measurements are
+  presented.
+\end{abstract}
+
+%\maketitle must follow title, authors, abstract
+\maketitle
+
+\thispagestyle{fancy}
+
+% body of paper here - Use proper section commands
+% References should be done using the \cite, \ref, and \label commands
+% Put \label in argument of \section for cross-referencing
+%\section{\label{}}
+
+\section{Introduction}
+The magnetic dipole moment, $\vec{\mu}$, of an elementary particle can be
+expressed in terms of its spin, $\vec{S}$, as:
+\begin{equation}
+  \vec{\mu} = g\frac{q}{2m}\vec{S},
+\end{equation}
+where $q$ and $m$ are charge and mass of the particle respectively. The
+dimensionless gyromagnetic ratio $g$ for a spin 1/2, structureless particle can
+be calculated from Dirac equation to be exactly 2. Measured values of $g$ is
+slightly different from 2, this anomaly $a$ is defined as:
+\begin{equation}
+  a = \frac{g - 2}{2}.
+\end{equation}
+
+The Standard Model (SM) provides very precise predictions of the anomaly of the
+muon, $a_\mu$, at sub-part-per-million level. Experimentally,
+there has been a series of measurements with increasing accuracy at CERN and
+Brookhaven National Laboratory (BNL). The last measurement, the E821 at BNL,
+was done with an uncertainty of 540 part-per-billion (ppb)~\cite{BNL2006}, and
+showed a 3.7 standard deviation from the SM
+prediction by Keshavarzi and colleagues~\cite{Alex2018}. This discrepancy
+motivates new and better measurements of $a_\mu$, two of such experiments are:
+\begin{itemize}
+  \item E989 at Fermilab: this is the successor of the E821 experiment, 
+    inheriting the muon storage ring, general experimental techniques, as well
+    as analysis methods. The E989 will improve the precision by four times
+    by collecting 20 times more data, and reducing systematic uncertainties.
+  \item E34 at Japan Proton Accelerator Research Complex (J-PARC): a completely
+    new experiments with novel approaches, aiming for a measurement with
+    comparable accuracy compares to that of the BNL experiment. It will be an
+    important cross check of results from E821 and E989.
+\end{itemize}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Principle of measurements}
+When a muon is injected perpendicularly into a uniform dipole magnetic field,
+$\vec{B}$, it will move in a circle with the cyclotron frequency:
+\begin{equation}
+  \vec{\omega}_c = -\frac{e}{\gamma m_\mu}\vec{B},
+  \label{eq:omega}_c
+\end{equation}
+where $\gamma$ is the Lorentz factor.
+
+Assuming spin of the muon is also perpendicular to the magnetic field, the spin
+will precess with a fixed frequency:
+\begin{equation}
+  \vec{\omega}_s = -g_\mu \frac{e}{2m_\mu}\vec{B} -
+  (1-\gamma)\frac{e}{\gamma m_\mu}\vec{B}.
+  \label{eq:omega_s}
+\end{equation}
+
+The difference between $\vec{\omega}_c$ and $\vec{\omega}_s$:
+% \begin{align}
+  % \vec{\omega}_a &= \vec{\omega}_s - \vec{\omega}_c \\
+  % &= -\frac{g-2}{2}\frac{e}{m_\mu} \vec{B} \\
+  % &= -a_\mu \frac{e}{m_\mu}\vec{B}.
+% \end{align}
+\begin{equation}
+  \vec{\omega}_a = \vec{\omega}_s - \vec{\omega}_c = -a_\mu \frac{e}{m_\mu}\vec{B}.
+  \label{eq:omega_a0}
+\end{equation}
+
+The magnetic field strength in~\cref{eq:omega_a0} can be measured most
+precisely using NMR technique using a sample with high hydrogen content.
+Introducing the Larmor precession frequency of the proton in the magnetic
+field, $\omega_p$, the proton magnetic moment, $\mu_p$, the electron
+$g$-factor, $g_e$, the electron mass, $m_e$, and the electron magnetic moment,
+$\mu_e$, the~\cref{eq:omega_a0} can be rearranged into the form:
+\begin{equation}
+  a_\mu = \frac{g_e}{2} \frac{\omega_a}{\omega_p} \frac{m_\mu}{m_e} \frac{\mu_p}{\mu_e}.
+  \label{eq:omega_a1}
+\end{equation}
+
+The ratio $\omega_a/\omega_p$ is experimentally measured in the muon $g$-2
+experiments, while other quantities $g_e/2$, $m_\mu/m_e$, and $\mu_p/\mu_e$ are
+known to 0.26 part-per-trillion, 22 ppb, and 3 ppb,
+respectively~\cite{codata}.
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{The E989 experiment at Fermilab}
+%% TODO: this paragraph is from James Tau 2016, need paraphrasing
+The Muon $g − 2$ experiment at Fermilab aims to measure the anomalous magnetic
+moment of the muon to a precision of 140 ppb, reducing the experimental
+uncertainty by a factor of 4 compared to the previous measurement at E821
+The measurement technique adopts the storage ring concept used for
+E821, with magic-momentum muons stored in a highly uniform 1.45 T magnetic
+dipole field. The spin precession frequency is extracted from an analysis of
+the modulation of the rate of higher-energy positrons from muon decays,
+detected by 24 calorimeters and 3 straw tracking detectors. Compared to the
+E821 experiment, muon beam preparation, storage ring internal hardware, field
+measuring equipment, and detector and electronics systems are all new or
+significantly upgraded.
+
+\subsection{Magnetic field}
+\subsection{Muon beam line}
+\subsection{Detector systems}
+\subsection{Status}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{The E34 experiment at J-PARC}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Summary}
+
+% If you have acknowledgments, this puts in the proper section head.
+%\bigskip % extra skip inserted
+\begin{acknowledgments}
+This work was supported in part by the US DOE, Fermilab.
+\end{acknowledgments}
+
+\bigskip % extra skip inserted
+% Create the reference section using BibTeX:
+%\bibliography{basename of .bib file}
+\begin{thebibliography}{9}   % Use for  1-9  references
+%\begin{thebibliography}{99} % Use for 10-99 references
+\bibitem{Alex2018} A. Keshavarzi{\em et al.}, Phys.~Rev.~D 97, 114025 (2018).
+\bibitem{BNL2006} G.W. Bennet{\em et al.}, Phys.~Rev.~D 73, 072003 (2006).
+\bibitem{codata} Mohr, Peter J. and Newell, David B. and Taylor, Barry N., Rev.~Mod.~Phys.~88, 035009 (2016).
+
+
+\end{thebibliography}
+
+
+\end{document}
+%
+% ****** End of file template.aps ******
--- a/fpcp2019_proceeding_unfinished/fpcp2019template.tex
+++ b/fpcp2019_proceeding_unfinished/fpcp2019template.tex
@@ -0,0 +1,372 @@
+% ************* Make changes after \begin{document} ***************
+%
+%  02 May 2019: original template is from 
+%  http://www.slac.stanford.edu/econf/editors/eprint-template/instructions.html
+%             Modified for FPCP 2006 by Asoka de Silva (TRIUMF)
+%             Further modified for FPCP 2019 by Bob Kowalewski (U. Victoria)
+%
+%% ****** Start of file slactemplate.tex ****** %
+%%
+%%
+%%   This file is part of the APS files in the REVTeX 4 distribution.
+%%   Version 4.0 of REVTeX, August 2001
+%%
+%%
+%%   Copyright (c) 2001 The American Physical Society.
+%%
+%%   See the REVTeX 4 README file for restrictions and more information.
+%%
+%
+% This is a template for producing manuscripts for use with REVTEX 4.0
+% Copy this file to another name and then work on that file.
+% That way, you always have this original template file to use.
+%
+\documentclass[twocolumn,twoside]{revtex4}
+\usepackage{graphicx}
+\usepackage{fancyhdr}
+\pagestyle{fancy}
+\fancyhead{} % clear all fields
+\fancyhead[C]{\it {
+Flavor Physics and CP Violation Conference, Victoria BC, 2019
+}} \fancyhead[RO,LE]{\thepage}
+\fancyfoot{} % clear all fields
+\fancyfoot[LE,LO]{}
+
+\renewcommand{\headrulewidth}{0pt}
+\renewcommand{\footrulewidth}{0pt}
+\renewcommand{\sfdefault}{phv}
+
+\setlength{\textheight}{235mm}
+\setlength{\textwidth}{170mm}
+\setlength{\topmargin}{-20mm}
+
+\bibliographystyle{apsrev}
+
+% ************* Make changes after here  ***************
+
+\fancyfoot[LE,LO]{\bf Insert PSN Here, eg. MonB0900}
+
+\begin{document}
+
+%Title of paper
+\title{LaTeX Template for FPCP 2019 Conference Proceedings}
+
+% Repeat the \author .. \affiliation  etc. as needed
+%
+% \affiliation command applies to all authors since the last
+% \affiliation command. The \affiliation command should follow the
+% other information
+
+\author{R. V. Kowalewski\\
+on behalf of the LOC}
+\affiliation{University of Victoria, BC, Canada, V8N2X3}
+%
+
+\begin{abstract}
+This document serves as a template for the proceedings of the FPCP~2019 
+conference.  
+Authors should prepare their papers using a copy and follow the
+guidelines described here.
+For optimum use, do not modify the page layout or styles. 
+\end{abstract}
+
+%\maketitle must follow title, authors, abstract
+\maketitle
+
+\thispagestyle{fancy}
+
+% body of paper here - Use proper section commands
+% References should be done using the \cite, \ref, and \label commands
+% Put \label in argument of \section for cross-referencing
+%\section{\label{}}
+
+\section{Introduction}
+Proceedings of the Flavor Physics and CP Violation Conference 2019 (FPCP~2019)
+will be made available at the Electronic Conference Proceedings 
+Archive~\cite{slaceconf}.  
+The purpose of this document is to guide the author and to provide a template 
+that maintains a uniform style for the proceedings; the next sections
+will describe this in detail.
+
+\section{Using this Template}
+The first step to preparing the paper is to copy the %slac\_two.rtx file, 
+tar file available at the 
+FPCP~2019 web site~\cite{fpcpsiteproc} 
+for download as a template package into a new directory.
+Next copy this template (fpcp2019template.tex) and rename it as you wish.
+Edit the file to make the necessary modifications and save when finished. 
+
+Because this template has been set up to meet
+requirements for conference proceedings papers, it is important to maintain
+these established styles.  Other editorial guidelines are described in the next section.
+
+\section{Manuscript}
+
+\subsection{Footers}
+A PSN is a sequential number that incorporates meaningful information 
+about individual proceedings papers and makes it easier for authors 
+and editors to track papers.  This unique PSN is constructed from the
+timetable available in indico~\cite{fpcpindico}.
+The PSN format is DDDRTTTT,
+where DDD is the day (Mon, Tue, Wed, Thu, Fri, 
+R is the room (B for Bob Wright B150, E for Elliott 162) and
+TTTT is the start time of the talk with the colon removed.
+For example, Dr. Chris Hearty's talk in parallel session 2 on Thursday, May 9 has
+PSN = ThuE1700.
+The PSN should be placed in the footer of the paper. 
+
+\subsection{Text Layout}
+There is no page limit for papers but conciseness is appreciated.  
+Avoid nestling more than three sub-levels in sections; also 
+the first character of section title key words should be
+uppercase.
+
+\subsection{Acronyms and Abbreviations}
+Acronyms should be defined the first time they appear.  
+Abbreviations may be used for figures (Fig.), equations (Eq.) 
+or if they are commonly used in language (etc., e.g., i.e., v.s.).
+However, when starting a sentence, abbreviations should not be used.
+
+\subsection{Tables}
+Tables may be one (e.g.~Table~\ref{example_table})
+or two columns (e.g.~Table~\ref{example_table_2col})
+in width with single border lines.
+The caption should appear above the table and, 
+in the tex file, labels should be used to refer to tables.
+
+% tables should appear as floats within the text
+%
+% Here is an example of the general form of a table:
+% Fill in the caption in the braces of the \caption{} command. Put the label
+% that you will use with \ref{} command in the braces of the \label{} command.
+% Insert the column specifiers (l, r, c, d, etc.) in the empty braces of the
+% \begin{tabular}{} command.
+% The ruledtabular environment adds doubled rules to table and sets a
+% reasonable default table settings.
+% Use the table* environment to get a full-width table in two-column
+% Add \usepackage{longtable} and the longtable (or longtable*}
+% environment for nicely formatted long tables. Or use the the [H]
+% placement option to break a long table (with less control than
+% in longtable).
+% \begin{table}%[H] add [H] placement to break table across pages
+% \caption{\label{}}
+% \begin{ruledtabular}
+% \begin{tabular}{}
+% Lines of table here ending with \\
+% \end{tabular}
+% \end{ruledtabular}
+% \end{table}
+% Surround table environment with turnpage environment for landscape
+% table
+% \begin{turnpage}
+% \begin{table}
+% \caption{\label{}}
+% \begin{ruledtabular}
+% \begin{tabular}{}
+% \end{tabular}
+% \end{ruledtabular}
+% \end{table}
+% \end{turnpage}
+
+\begin{table}[h]
+\begin{center}
+\caption{Example of a Table.}
+\begin{tabular}{|l|c|c|c|}
+\hline \textbf{Margin} & \textbf{Dual} & \textbf{A4 Paper} &
+\textbf{US Letter Paper}
+\\
+\hline Top & 7.6 mm & 37 mm & 19 mm \\
+ & (0.3 in) & (1.45 in) & (0.75 in) \\
+\hline Bottom & 20 mm & 19 mm & 19 mm \\
+ & (0.79 in) & (0.75 in)& (0.75 in) \\
+\hline Left & 20 mm & 20 mm & 20 mm \\
+ & (0.79 in) & (0.79 in) & (0.79 in) \\
+\hline Right & 20 mm & 20 mm & 26 mm \\
+ & (0.79 in) & (0.79 in) & (1.0 in) \\
+\hline
+\end{tabular}
+\label{example_table}
+\end{center}
+\end{table}
+
+\begin{table*}[t]
+\begin{center}
+\caption{Example of a Full Width Table.}
+\begin{tabular}{|l|c|c|c|c|c|c||l|c|c|c|c|c|c|}
+\hline \textbf{H-Margin} & \multicolumn{2}{c|}{\textbf{Dual}} & 
+\multicolumn{2}{c|}{\textbf{A4}} &
+\multicolumn{2}{c||}{\textbf{US Letter}} &
+\textbf{V-Margins} & \multicolumn{2}{c|}{\textbf{Dual}} &
+\multicolumn{2}{c|}{\textbf{A4}} &
+\multicolumn{2}{c|}{\textbf{US Letter}} \\
+\hline 
+Left & 20 mm & 0.79 in & 20 mm & 0.79 in & 20 mm & 0.79 in &
+Top & 7.6 mm & 0.3 in & 37 mm & 1.45 in & 19 mm & 0.75 in \\
+\hline 
+Right & 20 mm & 0.79 in & 20 mm & 0.79 in & 26 mm & 1.0 in &
+Bottom & 20 mm & 0.79 in  & 19 mm & 0.75 in & 19 mm & 0.75 in \\
+\hline
+\end{tabular}
+\label{example_table_2col}
+\end{center}
+\end{table*}
+
+\subsection{Figures}
+
+% figures should be put into the text as floats.
+% Use the graphics or graphicx packages (distributed with LaTeX2e)
+% and the \includegraphics macro defined in those packages.
+% See the LaTeX Graphics Companion by Michel Goosens, Sebastian Rahtz,
+% and Frank Mittelbach for instance.
+%
+% Here is an example of the general form of a figure:
+% Fill in the caption in the braces of the \caption{} command. Put the label
+% that you will use with \ref{} command in the braces of the \label{} command.
+% Use the figure* environment if the figure should span across the
+% entire page. There is no need to do explicit centering.
+
+% \begin{figure}
+% \includegraphics{}%
+% \caption{\label{}}
+% \end{figure}
+
+% Surround figure environment with turnpage environment for landscape
+% figure
+% \begin{turnpage}
+% \begin{figure}
+% \includegraphics{}%
+% \caption{\label{}}
+% \end{figure}
+% \end{turnpage}
+
+\begin{figure}[h]
+\centering
+\includegraphics[width=80mm]{figure1.pdf}
+\caption{Example of a One-column Figure.} \label{example_figure}
+\end{figure}
+
+\begin{figure*}[t]
+\centering
+\includegraphics[width=135mm]{figure2.pdf}
+\caption{Example of a Full Width Figure.} \label{example_figure_col2}
+\end{figure*}
+
+Figures may be one column (e.g.~Figure~\ref{example_figure}) 
+or span the paper width (e.g.~Figure~\ref{example_figure_col2}).
+Labels should be used to refer to the figures in the tex file.
+The figure caption should appear below the figure.  
+Color figures are encouraged; however note that some colors, such as 
+pale yellow, will not be visible when printed.  
+Lettering in figures should be large enough to be visible.
+Filenames of figures in the tex file should be numbered
+consecutively, e.g. figure1.ps, figure2a.ps, figure2b.ps, figure3.ps, etc.
+
+\subsection{Equations}
+Equations may be displayed in several ways, as in Eq.~\ref{eq-xy} 
+
+\begin{equation}
+x = y.
+\label{eq-xy}
+\end{equation}
+
+The {\em eqnarray} environment may be used to
+split equations into several lines or to align several equations, 
+for example in Eq.~\ref{eq-sp}
+
+\begin{eqnarray}
+T & = & Im[V_{11} {V_{12}}^* {V_{21}}^* V_{22}]  \nonumber \\
+&  & + Im[V_{12} {V_{13}}^* {V_{22}}^* V_{23}]   \nonumber \\
+&  & - Im[V_{33} {V_{31}}^* {V_{13}}^* V_{11}].
+\label{eq-sp}
+\end{eqnarray}
+
+An alternative method is shown in Eq.~\ref{eq-spa} for long sets of
+equations where only one referencing equation number is required.  
+Again, references should be to labels and not hard-coded equation numbers.
+
+\begin{equation}
+\begin{array}{rcl}
+\bf{K} & = &  Im[V_{j, \alpha} {V_{j,\alpha + 1}}^*
+{V_{j + 1,\alpha }}^* V_{j + 1, \alpha + 1} ] \\
+       &   & + Im[V_{k, \alpha + 2} {V_{k,\alpha + 3}}^*
+{V_{k + 1,\alpha + 2 }}^* V_{k + 1, \alpha + 3} ]  \\
+       &   & + Im[V_{j + 2, \beta} {V_{j + 2,\beta + 1}}^*
+{V_{j + 3,\beta }}^* V_{j + 3, \beta + 1} ]  \\
+       &   & + Im[V_{k + 2, \beta + 2} {V_{k + 2,\beta + 3}}^*
+{V_{k + 3,\beta + 2 }}^* V_{k + 3, \beta + 3}], \\
+& & \\
+\bf{M} & = &  Im[{V_{j, \alpha}}^* V_{j,\alpha + 1}
+V_{j + 1,\alpha } {V_{j + 1, \alpha + 1}}^* ]  \\
+       &   & + Im[V_{k, \alpha + 2} {V_{k,\alpha + 3}}^*
+{V_{k + 1,\alpha + 2 }}^* V_{k + 1, \alpha + 3} ]  \\
+       &   & + Im[{V_{j + 2, \beta}}^* V_{j + 2,\beta + 1}
+V_{j + 3,\beta } {V_{j + 3, \beta + 1}}^* ]  \\
+       &   & + Im[V_{k + 2, \beta + 2} {V_{k + 2,\beta + 3}}^*
+{V_{k + 3,\beta + 2 }}^* V_{k + 3, \beta + 3}].
+\\ & &
+\end{array}\label{eq-spa}
+\end{equation}
+
+\subsection{Bibliography} 
+A frequent citation will perhaps be to the Review of Particle Properties~\cite{PDG2018}.  The bibliography
+is included at the bottom of this input file.
+
+\subsection{Footnotes} 
+Footnotes should only be used in the body of the
+paper and not placed after the list of authors, affiliations, or
+in the abstract. 
+
+\section{Paper Submission}
+
+Authors should submit their papers to the ePrint arXiv 
+server~\cite{arxivserver} 
+after verifying that it is processed correctly by the LaTeX processor.
+Please submit the source code, the style files 
+(revsymb.sty, revtex4.cls) %, slac\_two.rtx) 
+and any figures; 
+these should be self-contained to generate the paper from source.  
+
+It is the author's responsibility to ensure that the papers are 
+generated correctly from the source code at the ePrint server. 
+After the paper is accepted by the ePrint server, please verify that
+the layout in the resulting  PDF file conforms to the guidelines 
+described in this document.
+Finally, contact the local organizers of FPCP~2006 with the 
+ePrint number of the paper; 
+the deadline to do this is 15~May~2006.
+
+% If you have acknowledgments, this puts in the proper section head.
+%\bigskip % extra skip inserted
+\begin{acknowledgments}
+This document is adapted from the ``Instruction for producing FPCP2003
+proceedings'' by P.~Perret 
+and from eConf templates~\cite{templates-ref}.
+\end{acknowledgments}
+
+\bigskip % extra skip inserted
+% Create the reference section using BibTeX:
+%\bibliography{basename of .bib file}
+\begin{thebibliography}{9}   % Use for  1-9  references
+%\begin{thebibliography}{99} % Use for 10-99 references
+
+\bibitem{slaceconf} http://www.slac.stanford.edu/econf/search.html
+
+\bibitem{fpcpsiteproc} https://fpcp2019.triumf.ca/proceedings.html
+
+\bibitem{fpcpindico} https://meetings.triumf.ca/indico/event/48/\\
+timetable/\#all.detailed
+
+\bibitem{PDG2018} M. Tanabashi {\em et al.} (Particle Data Group), Phys.~Rev.~D{\bf 98}, 030001 (2018).
+
+\bibitem{arxivserver} http://arxiv.org/help
+
+\bibitem{templates-ref} http://www.slac.stanford.edu/econf/editors/\\
+eprint-template/instructions.html
+
+
+\end{thebibliography}
+
+
+\end{document}
+%
+% ****** End of file template.aps ******
--- a/mu2e_cry/Makefile
+++ b/mu2e_cry/Makefile
@@ -0,0 +1,15 @@
+DOC=cryReport
+INPUT=$(DOC).tex
+TARGET=$(DOC).pdf
+REF=ref.bib
+TEX=pdflatex -shell-escape
+BIB=bibtex
+
+default: $(TARGET)
+
+$(TARGET): $(INPUT) Makefile 
+	$(TEX) $< && $(BIB) $(DOC) && $(TEX) $< && $(TEX) $<
+
+clean:
+	rm -f $(DOC).{pdf,out,aux,log}
+	rm -f *.{pdf,out,aux,log,bbl,blg}
--- a/mu2e_cry/cryReport.tex
+++ b/mu2e_cry/cryReport.tex
@@ -0,0 +1,67 @@
+\documentclass[11pt]{article}
+\usepackage{mhchem}
+\usepackage{booktabs}
+\usepackage{multirow}
+\usepackage{textcomp}
+\usepackage{epsfig}
+\usepackage{hyperref}
+\usepackage[noabbrev, capitalize]{cleveref} % hyperref must be loaded first
+\usepackage[
+  detect-weight=true,
+  per=slash,
+  detect-family=true,
+  separate-uncertainty=true]{siunitx}
+% \usepackage{listings}
+\usepackage[dvipsnames]{xcolor}
+\usepackage{upquote}
+\usepackage{minted}
+\usemintedstyle{perldoc}
+
+\usepackage[framemethod=tikz]{mdframed}
+\usepackage{adjustbox}
+
+% \definecolor{greybg}{rgb}{0.25,0.25,0.25}
+% \definecolor{yellowbg}{rgb}{0.91, 0.84, 0.42}
+% \definecolor{bananamania}{rgb}{0.98, 0.91, 0.71}
+
+\mdfdefinestyle{warning}{%
+  linecolor=red!70,
+  frametitle={Warning},
+  frametitlerule=true,
+  frametitlebackgroundcolor=orange!40,
+  backgroundcolor=orange!30,
+  innertopmargin=\topskip,
+  roundcorner=8pt,
+  linewidth=1pt,
+}
+% \mdtheorem[style=theoremstyle]{warning}{Warning}
+
+\mdfdefinestyle{listing}{%
+  linecolor=Aquamarine!50,
+  linewidth=1pt,
+  backgroundcolor=yellow!40,
+  roundcorner=8pt,
+  % frametitlerule=true,
+  % frametitlebackgroundcolor=yellow!50,
+  innertopmargin=\topskip,
+}
+% \mdtheorem[style=listing]{listing}{Listing}
+
+% \DeclareSIUnit\eVperc{\eV\per\clight}
+% \DeclareSIUnit\clight{\text{\ensuremath{c}}}
+
+\begin{document}
+\title{Cosmic ray simulation with CRY event generator}
+\author{Nam H. Tran \\ Boston University}
+\date{\today}
+\maketitle
+
+\begin{abstract}
+  CRY report
+\end{abstract}
+\section{Overview}
+
+
+\bibliographystyle{h-physrev}
+% \bibliography{stm_study}
+\end{document}
--- a/mu2e_cry/h-physrev.bst
+++ b/mu2e_cry/h-physrev.bst
--- a/r15a_xray/figs/hpge_ecal.png
+++ b/r15a_xray/figs/hpge_ecal.png
--- a/r15a_xray/figs/hpge_higain_acceptance.png
+++ b/r15a_xray/figs/hpge_higain_acceptance.png
--- a/stm_study_201611/figs/ke_time_4vds.png
+++ b/stm_study_201611/figs/ke_time_4vds.png
--- a/stm_study_201611/listings/runall.sh
+++ b/stm_study_201611/listings/runall.sh
@@ -0,0 +1,78 @@
+@mu2egpvm02:step00 namtran $ pwd
+/mu2e/app/users/namtran/STM_study_201611/step00
+
+@mu2egpvm02:step00 namtran $ setup mu2e &&\
+  source /mu2e/app/users/namtran/Offline/setup.sh &&\
+  setup mu2egrid v3_02_00
+Mu2e external products are rooted at:  /cvmfs/mu2e.opensciencegrid.org
+MU2E_DATA_PATH is:  /cvmfs/mu2e.opensciencegrid.org/DataFiles
+Base release directory is:  /mu2e/app/users/namtran/Offline
+MU2E_SEARCH_PATH:    /mu2e/app/users/namtran/Offline/:/cvmfs/mu2e.opensciencegrid.org/DataFiles/
+MU2E_SEARCH_PATH:   /mu2e/app/users/namtran/STM_study_201611/step00/:/mu2e/app/users/namtran/Offline/:/cvmfs/mu2e.opensciencegrid.org/DataFiles/
+
+@mu2egpvm02:step00 namtran $ ./submit.sh
+mu2eart --setup=/mu2e/app/users/namtran/Offline/setup.sh  --fcl=/mu2e/app/users/namtran/STM_study_201611/step00/fcl/step00.fcl --njobs=5098 --inputs=/mu2e/app/users/namtran/STM_study_201611/step00/cd3-beam-g4s2-mubeam.0728a.list --outstage=/pnfs/mu2e/scratch/outstage
+Final set of options:
+$VAR1 = {
+          'priority' => 0,
+          'dry-run' => 0,
+          'verbose' => 1,
+          'disk' => '30GB',
+          'expected-lifetime' => '24h',
+          'mu2e-setup' => '/cvmfs/mu2e.opensciencegrid.org/setupmu2e-art.sh',
+          'jobsub-arg' => [],
+          'group' => 'mu2e',
+          'jobsub-server' => 'https://fifebatch.fnal.gov:8443',
+          'OS' => 'SL6',
+          'fclinput' => [],
+          'help' => 0,
+          'resource-provides' => 'usage_model=OPPORTUNISTIC,DEDICATED',
+          'inputs' => '/mu2e/app/users/namtran/STM_study_201611/step00/cd3-beam-g4s2-mubeam.0728a.list',
+          'outstage' => '/pnfs/mu2e/scratch/outstage',
+          'setup' => '/mu2e/app/users/namtran/Offline/setup.sh',
+          'memory' => '2048MB',
+          'njobs' => 5098,
+          'site' => undef,
+          'fcl' => '/mu2e/app/users/namtran/STM_study_201611/step00/fcl/step00.fcl',
+          'role' => undef,
+          'user-services' => 1
+        };
+
+nlines = 5098 in file /mu2e/app/users/namtran/STM_study_201611/step00/cd3-beam-g4s2-mubeam.0728a.list
+ninputs = 5098
+Adding jobsub_submit option: --disk 30GB
+Adding jobsub_submit option: --resource-provides usage_model=OPPORTUNISTIC,DEDICATED
+Adding jobsub_submit option: --expected-lifetime 24h
+Adding jobsub_submit option: --group mu2e
+Adding jobsub_submit option: --memory 2048MB
+Adding jobsub_submit option: --jobsub-server https://fifebatch.fnal.gov:8443
+Adding jobsub_submit option: --OS SL6
+Will use ifdh version "v1_8_11"
+Using: MU2EGRID_MU2ESETUP => /cvmfs/mu2e.opensciencegrid.org/setupmu2e-art.sh
+Using: MU2EGRID_USERSERVICES => 1
+Using: MU2EGRID_OUTDIRFMT => step00.%d/%05d
+Using: MU2EGRID_NCLUSTERJOBS => 5098
+Using: IFDH_VERSION => "v1_8_11"
+Using: MU2EGRID_OUTSTAGE => /pnfs/mu2e/scratch/outstage
+Using: MU2EGRID_CHUNKSIZE => 1
+Using: MU2EGRID_INPUTLIST => cd3-beam-g4s2-mubeam.0728a.list
+Using: MU2EGRID_MASTERFHICL => step00.fcl
+Using: MU2EGRID_FCLINPUT_NUMENTRIES => 0
+Using: MU2EGRID_DIR => /cvmfs/mu2e.opensciencegrid.org/artexternals/mu2egrid/v3_01_13
+Using: MU2EGRID_USERSETUP => /mu2e/app/users/namtran/Offline/setup.sh
+Using: MU2EGRID_SUBMITTER => namtran
+Command:  jobsub_submit --disk 30GB --resource-provides usage_model=OPPORTUNISTIC,DEDICATED --expected-lifetime 24h --group mu2e --memory 2048MB --jobsub-server https://fifebatch.fnal.gov:8443 --OS SL6 -l priority=0 -e EXPERIMENT -e MU2EGRID_MU2ESETUP -e MU2EGRID_USERSERVICES -e MU2EGRID_OUTDIRFMT -e MU2EGRID_NCLUSTERJOBS -e IFDH_VERSION -e MU2EGRID_OUTSTAGE -e MU2EGRID_CHUNKSIZE -e MU2EGRID_INPUTLIST -e MU2EGRID_MASTERFHICL -e MU2EGRID_FCLINPUT_NUMENTRIES -e MU2EGRID_DIR -e MU2EGRID_USERSETUP -e MU2EGRID_SUBMITTER -f /mu2e/app/users/namtran/STM_study_201611/step00/fcl/step00.fcl -f /mu2e/app/users/namtran/STM_study_201611/step00/cd3-beam-g4s2-mubeam.0728a.list -N 5098 file:///cvmfs/mu2e.opensciencegrid.org/artexternals/mu2egrid/v3_01_13/bin/impl/copyback.sh /cvmfs/mu2e.opensciencegrid.org/artexternals/mu2egrid/v3_01_13/bin/impl/mu2eart.sh
+Submitting....
+/fife/local/scratch/uploads/mu2e/namtran/2016-12-15_214506.238864_1024
+
+/fife/local/scratch/uploads/mu2e/namtran/2016-12-15_214506.238864_1024/copyback.sh_20161215_214507_2410921_0_1_.cmd
+
+submitting....
+
+Submitting job(s)...............................................................................................................................................................................................................
+
+5098 job(s) submitted to cluster 15577455.
+
+JobsubJobId of first job: 15577455.0@fifebatch2.fnal.gov
+
+Use job id 15577455.0@fifebatch2.fnal.gov to retrieve output
--- a/thesis/raw/ge_eff.csv
+++ b/thesis/raw/ge_eff.csv
@@ -0,0 +1,14 @@
+Energy,Efficiency,Uncertainty
+121.78,9.05E-04,1.182E-05
+244.69,6.40E-04,1.888E-05
+344.28,5.00E-04,5.930E-06
+778.90,2.56E-04,7.709E-06
+964.06,2.22E-04,5.726E-06
+1085.84,1.97E-04,8.219E-06
+1112.08,1.88E-04,5.386E-06
+1408.01,1.53E-04,3.392E-06
+
+346.828,4.95E-04,1.216E-05
+399.268,4.41E-04,9.780E-06
+400.177,4.40E-04,9.747E-06
+476.800,3.81E-04,7.680E-06
--- a/thesis/raw/si_cal_effs.csv
+++ b/thesis/raw/si_cal_effs.csv
@@ -0,0 +1,11 @@
+Detector, Slope,Offset
+SiL-2 , 7.86 , 14.10
+SiR-2 , 7.96 , 22.92
+SiL1-1 , 2.61 , -96.54
+SiL1-2 , 2.54 , -36.47
+SiL1-3 , 2.65 , -114.17
+SiL1-4 , 2.54 , -68.10
+SiR1-1 , 2.53 , -71.72
+SiR1-2 , 2.62 , -122.51
+SiR1-3 , 2.49 , -14.81
+SiR1-4 , 2.53 , -87.22
--- a/thesis/raw/xray_eff.csv
+++ b/thesis/raw/xray_eff.csv
@@ -0,0 +1,4 @@
+X-ray, Efficiency, Uncertainty
+346.828 , 5.12E-4, 0.14E-4
+400.177 , 4.54E-4, 0.11E-4
+
--- a/tikz-feynman/.gitignore
+++ b/tikz-feynman/.gitignore
@@ -0,0 +1,2 @@
+*.bak
+*.sav
--- a/tikz-feynman/a.tex
+++ b/tikz-feynman/a.tex
@@ -0,0 +1,23 @@
+
+\documentclass[11pt]{article}
+% \usepackage{amssymb} %maths
+% \usepackage{amsmath} %maths
+% \usepackage[utf8] %useful to type directly diacritic characters
+\usepackage{tikz-feynman} 
+\tikzfeynmanset{compat=1.0.0}
+
+\begin{document}
+
+\feynmandiagram [horizontal=a to b] {
+  i1 -- [fermion] a -- [fermion] i2,
+  a -- [photon] b,
+  f1 -- [fermion] b -- [fermion] f2,
+};
+
+\feynmandiagram [horizontal=a to b] {
+  i1 [particle=\(e^{-}\)] -- [fermion] a -- [fermion] i2 [particle=\(e^{+}\)],
+  a -- [photon, edge label=\(\gamma\), momentum'=\(k\)] b,
+  f1 [particle=\(\mu^{+}\)] -- [fermion] b -- [fermion] f2 [particle=\(\mu^{-}\)],
+};
+  
+\end{document}
--- a/tikz-feynman/b.tex
+++ b/tikz-feynman/b.tex
@@ -0,0 +1,8 @@
+\documentclass{standalone}
+\usepackage{tikz}
+\usepackage{tikz-feynman} 
+\begin{document}
+\begin{tikzpicture}
+  \draw (0,0) rectangle (2,1) node [midway] {Example};
+\end{tikzpicture}
+\end{document}
--- a/tikz-feynman/d.tex
+++ b/tikz-feynman/d.tex
@@ -0,0 +1,23 @@
+\documentclass[11pt]{standalone}
+% \usepackage{amssymb} %maths
+% \usepackage{amsmath} %maths
+% \usepackage[utf8] %useful to type directly diacritic characters
+\usepackage{tikz-feynman} 
+% \tikzfeynmanset{compat=1.0.0}
+
+\begin{document}
+\begin{tikzpicture}[]
+  \begin{feynman}
+    \vertex (a);
+    \vertex [below=of a] (b);
+    \vertex [below left=of b] (c);
+    \vertex [below right=of b] (d);
+
+    \diagram * {
+      (a) -- [photon, edge label=\(\gamma\)] (b);
+      (c) -- [fermion, edge label=\(\mu\)] (b);
+      (b) -- [fermion, edge label=\(\mu\)] (d);
+    };
+  \end{feynman}
+\end{tikzpicture}
+\end{document}
--- a/tikz-feynman/d2.tex
+++ b/tikz-feynman/d2.tex
@@ -0,0 +1,28 @@
+\documentclass[11pt]{standalone}
+% \usepackage{amssymb} %maths
+% \usepackage{amsmath} %maths
+% \usepackage[utf8] %useful to type directly diacritic characters
+\usepackage{tikz-feynman} 
+% \tikzfeynmanset{compat=1.0.0}
+
+\begin{document}
+\begin{tikzpicture}[]
+  \begin{feynman}
+    \vertex (a);
+    \vertex [below=of a] (b);
+    \vertex [below left=of b] (c);
+    \vertex [below left=of c] (e);
+    \vertex [below right=of b] (d);
+    \vertex [below right=of d] (f);
+
+    \diagram * {
+      (a) -- [photon, edge label=\(\gamma\)] (b);
+      (c) -- [fermion, edge label=\(\mu\)] (b);
+      (e) -- [fermion] (c);
+      (b) -- [fermion, edge label=\(\mu\)] (d);
+      (d) -- [fermion] (f);
+      (c) -- [photon] (d);
+    };
+  \end{feynman}
+\end{tikzpicture}
+\end{document}
--- a/tikz-feynman/gm2-dirac.tex
+++ b/tikz-feynman/gm2-dirac.tex
@@ -0,0 +1,23 @@
+\documentclass[11pt]{standalone}
+% \usepackage{amssymb} %maths
+% \usepackage{amsmath} %maths
+% \usepackage[utf8] %useful to type directly diacritic characters
+\usepackage{tikz-feynman} 
+% \tikzfeynmanset{compat=1.0.0}
+
+\begin{document}
+
+\feynmandiagram [vertical=a to b] {
+  % a [crossed dot] -- [photon, thick, edge label=\(\gamma\)] b [dot],
+  a -- [photon, thick, edge label=\(\gamma\)] b,
+  i1 [particle=\(\mu\)] -- [fermion, thick] b -- [fermion, thick] f1 [particle=\(\mu\)],
+  % f1 -- [fermion] b -- [fermion] f2,
+};
+
+% \feynmandiagram [horizontal=a to b] {
+  % i1 [particle=\(e^{-}\)] -- [fermion] a -- [fermion] i2 [particle=\(e^{+}\)],
+  % a -- [photon, edge label=\(\gamma\), momentum'=\(k\)] b,
+  % f1 [particle=\(\mu^{+}\)] -- [fermion] b -- [fermion] f2 [particle=\(\mu^{-}\)],
+% };
+  
+\end{document}
--- a/tikz-feynman/gm2-schwinger.tex
+++ b/tikz-feynman/gm2-schwinger.tex
@@ -0,0 +1,24 @@
+\documentclass[11pt]{standalone}
+% \usepackage{amssymb} %maths
+% \usepackage{amsmath} %maths
+% \usepackage[utf8] %useful to type directly diacritic characters
+\usepackage{tikz-feynman} 
+% \tikzfeynmanset{compat=1.0.0}
+
+\begin{document}
+
+\feynmandiagram [vertical=a to b] {
+  % a [crossed dot] -- [photon, thick, edge label=\(\gamma\)] b [dot],
+  a -- [photon, thick, edge label=\(\gamma\)] b,
+  i1 [particle=\(\mu\)] -- [fermion, thick] iv1 -- [fermion, thick] b 
+  -- [fermion, thick] iv2 -- [fermion, thick] f1 [particle=\(\mu\)],
+  {[same layer] iv1 -- [photon, thick] iv2},
+};
+
+% \feynmandiagram [horizontal=a to b] {
+  % i1 [particle=\(e^{-}\)] -- [fermion] a -- [fermion] i2 [particle=\(e^{+}\)],
+  % a -- [photon, edge label=\(\gamma\), momentum'=\(k\)] b,
+  % f1 [particle=\(\mu^{+}\)] -- [fermion] b -- [fermion] f2 [particle=\(\mu^{-}\)],
+% };
+  
+\end{document}