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-rw-r--r--Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex21
1 files changed, 12 insertions, 9 deletions
diff --git a/Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex b/Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex
index f531623f3fa..a2b6b2d2087 100644
--- a/Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex
+++ b/Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex
@@ -1,11 +1,14 @@
\chapter{\CP violation in the \Bmeson system}
\label{chap:SomeStuff}
-%% Note that the citations in this chapter use the journal and
-%% arXiv keys: I used the SLAC-SPIRES online BibTeX retriever
+%% Restart the numbering to make sure that this is definitely page #1!
+\pagenumbering{arabic}
+
+%% Note that the citations in this chapter use the journal and
+%% arXiv keys: I used the SLAC-SPIRES online BibTeX retriever
%% to build my bibliography. There are also quite a few non-standard
%% macros, which come from my personal collection. You can have them
-%% if you want, or I might get round to properly releasing them at
+%% if you want, or I might get round to properly releasing them at
%% some point myself.
\chapterquote{Laws were made to be broken.}%
@@ -13,16 +16,16 @@
Symmetries, either intact or broken, have proved to be at the heart
of how matter interacts. The Standard Model of fundamental interactions
-(SM) is composed of three independent continuous symmetry groups denoted
-$\SUgroup{3} \times \SUgroup{2} \times \Ugroup{1}$, representing the
-strong force, weak isospin and hypercharge
+(SM) is composed of three independent continuous symmetry groups denoted
+$\SUgroup{3} \times \SUgroup{2} \times \Ugroup{1}$, representing the
+strong force, weak isospin and hypercharge
respectively~\cite{Phys.Rev.Lett.19.1264, Phys.Rev.D2.1285,hep-ph/0410370}.
\section{Neutral meson mixing}
\label{sec:neutralmixing}
We can go a long way with an effective Hamiltonian approach in
canonical single-particle quantum mechanics. To do this we construct
-a wavefunction from a combination of a generic neutral meson state
+a wavefunction from a combination of a generic neutral meson state
$\ket{\Xzero}$ and its anti-state $\ket{\Xzerobar}$:
%
\begin{equation}
@@ -35,9 +38,9 @@ which is governed by a time-dependent matrix differential equation,
\I \pdByd{}{t} \colvector{a \\ b}
=
\underbrace{%
- \twomatrix{ M_{11}-\frac{\I}{2}\Gamma_{11}
+ \twomatrix{ M_{11}-\frac{\I}{2}\Gamma_{11}
& M_{12}-\frac{\I}{2}\Gamma_{12} }
- { M_{12}^\ast-\frac{\I}{2}\Gamma_{12}^\ast
+ { M_{12}^\ast-\frac{\I}{2}\Gamma_{12}^\ast
& M_{22}-\frac{\I}{2}\Gamma_{22} }
}_{\boldmatrix{H}}
\colvector{a \\ b}