adding missing pieces
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fpcp2019_proceeding_unfinished/.gitignore
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fpcp2019_proceeding_unfinished/.gitignore
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*.bak
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*.sav
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fpcp2019_proceeding_unfinished/Makefile
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fpcp2019_proceeding_unfinished/Makefile
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DOC=fpcp2019
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INPUT=$(DOC).tex
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TARGET=$(DOC).pdf
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TEX=pdflatex -shell-escape
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default: $(TARGET)
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$(TARGET): $(INPUT) Makefile
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$(TEX) $< && $(TEX) $<
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clean:
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rm -f $(DOC).{pdf,out,aux,log}
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rm -f *.{out,aux,log,bbl,blg}
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fpcp2019_proceeding_unfinished/fpcp2019.tex
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fpcp2019_proceeding_unfinished/fpcp2019.tex
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\documentclass[twocolumn,twoside]{revtex4}
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\usepackage{graphicx}
|
||||
\usepackage{fancyhdr}
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\pagestyle{fancy}
|
||||
\fancyhead{} % clear all fields
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\fancyhead[C]{\it {
|
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Flavor Physics and CP Violation Conference, Victoria BC, 2019
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||||
}} \fancyhead[RO,LE]{\thepage}
|
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\fancyfoot{} % clear all fields
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||||
\fancyfoot[LE,LO]{}
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||||
\usepackage{amsmath}
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||||
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\renewcommand{\headrulewidth}{0pt}
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\renewcommand{\footrulewidth}{0pt}
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\renewcommand{\sfdefault}{phv}
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||||
|
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\setlength{\textheight}{235mm}
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||||
\setlength{\textwidth}{170mm}
|
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\setlength{\topmargin}{-20mm}
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\usepackage{hyperref}
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\usepackage[noabbrev, capitalize]{cleveref} % hyperref must be loaded first
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\usepackage[
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detect-weight=true,
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per=slash,
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detect-family=true,
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separate-uncertainty=true]{siunitx}
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\bibliographystyle{apsrev}
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% ************* Make changes after here ***************
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\fancyfoot[LE,LO]{\bf MonB1010}
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\begin{document}
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%Title of paper
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\title{Measurements of the muon anomalous magnetic moment}
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\author{Nam H. Tran\\
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on behalf of the Muon $g-2$ Experiment at Fermilab}
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\affiliation{Boston University, Boston, MA, US 02215}
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%
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\begin{abstract}
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The over 3-sigma discrepancy between the latest experimental and theoretical
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values of the anomalous magnetic of the muon has been one of the best
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hints of new physics beyond the Standard Model. Ongoing efforts
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to settle the issue from the experimental side are happening at Fermilab and
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J-PARC. The E989 at Fermilab is using the same key technologies as the last
|
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experiment at BNL (E821), but with great improvement in accuracy. The first
|
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physics data has been taken, and data analysis is going to be finalized soon.
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The E34 at J-PARC adopts a novel approach, is
|
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well advanced in R\&D, and recently received Stage-2 Approval. The
|
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experimental principles, techniques, and prospects of these measurements are
|
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presented.
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\end{abstract}
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|
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%\maketitle must follow title, authors, abstract
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\maketitle
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|
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\thispagestyle{fancy}
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||||
|
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% body of paper here - Use proper section commands
|
||||
% References should be done using the \cite, \ref, and \label commands
|
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% Put \label in argument of \section for cross-referencing
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%\section{\label{}}
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\section{Introduction}
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The magnetic dipole moment, $\vec{\mu}$, of an elementary particle can be
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expressed in terms of its spin, $\vec{S}$, as:
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\begin{equation}
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\vec{\mu} = g\frac{q}{2m}\vec{S},
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\end{equation}
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where $q$ and $m$ are charge and mass of the particle respectively. The
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dimensionless gyromagnetic ratio $g$ for a spin 1/2, structureless particle can
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be calculated from Dirac equation to be exactly 2. Measured values of $g$ is
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slightly different from 2, this anomaly $a$ is defined as:
|
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\begin{equation}
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a = \frac{g - 2}{2}.
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\end{equation}
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The Standard Model (SM) provides very precise predictions of the anomaly of the
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muon, $a_\mu$, at sub-part-per-million level. Experimentally,
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there has been a series of measurements with increasing accuracy at CERN and
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Brookhaven National Laboratory (BNL). The last measurement, the E821 at BNL,
|
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was done with an uncertainty of 540 part-per-billion (ppb)~\cite{BNL2006}, and
|
||||
showed a 3.7 standard deviation from the SM
|
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prediction by Keshavarzi and colleagues~\cite{Alex2018}. This discrepancy
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motivates new and better measurements of $a_\mu$, two of such experiments are:
|
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\begin{itemize}
|
||||
\item E989 at Fermilab: this is the successor of the E821 experiment,
|
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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
|
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comparable accuracy compares to that of the BNL experiment. It will be an
|
||||
important cross check of results from E821 and E989.
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\end{itemize}
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|
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Principle of measurements}
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When a muon is injected perpendicularly into a uniform dipole magnetic field,
|
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$\vec{B}$, it will move in a circle with the cyclotron frequency:
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\begin{equation}
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\vec{\omega}_c = -\frac{e}{\gamma m_\mu}\vec{B},
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\label{eq:omega}_c
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\end{equation}
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where $\gamma$ is the Lorentz factor.
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|
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Assuming spin of the muon is also perpendicular to the magnetic field, the spin
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will precess with a fixed frequency:
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\begin{equation}
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\vec{\omega}_s = -g_\mu \frac{e}{2m_\mu}\vec{B} -
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(1-\gamma)\frac{e}{\gamma m_\mu}\vec{B}.
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\label{eq:omega_s}
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\end{equation}
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|
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The difference between $\vec{\omega}_c$ and $\vec{\omega}_s$:
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% \begin{align}
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% \vec{\omega}_a &= \vec{\omega}_s - \vec{\omega}_c \\
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% &= -\frac{g-2}{2}\frac{e}{m_\mu} \vec{B} \\
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% &= -a_\mu \frac{e}{m_\mu}\vec{B}.
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% \end{align}
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\begin{equation}
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\vec{\omega}_a = \vec{\omega}_s - \vec{\omega}_c = -a_\mu \frac{e}{m_\mu}\vec{B}.
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\label{eq:omega_a0}
|
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\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
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\begin{acknowledgments}
|
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This work was supported in part by the US DOE, Fermilab.
|
||||
\end{acknowledgments}
|
||||
|
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\bigskip % extra skip inserted
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% 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 ******
|
||||
372
fpcp2019_proceeding_unfinished/fpcp2019template.tex
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fpcp2019_proceeding_unfinished/fpcp2019template.tex
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|
||||
% ************* 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 ******
|
||||
Reference in New Issue
Block a user