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Diffstat (limited to 'Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex')
-rw-r--r-- | Master/texmf-dist/doc/latex/hepthesis/example/chap1.tex | 21 |
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} |