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author | Karl Berry <karl@freefriends.org> | 2017-11-11 23:15:55 +0000 |
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committer | Karl Berry <karl@freefriends.org> | 2017-11-11 23:15:55 +0000 |
commit | cddb15c8413b400589d6b4fb6587ad9d06b39024 (patch) | |
tree | 8a15c612ce6e0bc03fd687f00782a4e0f8d56b66 /Master/texmf-dist/doc/latex/gridslides/example.tex | |
parent | 6b4ac9ddeb57d6ddf1115869635ba7eefbbd8f61 (diff) |
gridslides (11nov17)
git-svn-id: svn://tug.org/texlive/trunk@45752 c570f23f-e606-0410-a88d-b1316a301751
Diffstat (limited to 'Master/texmf-dist/doc/latex/gridslides/example.tex')
-rw-r--r-- | Master/texmf-dist/doc/latex/gridslides/example.tex | 111 |
1 files changed, 111 insertions, 0 deletions
diff --git a/Master/texmf-dist/doc/latex/gridslides/example.tex b/Master/texmf-dist/doc/latex/gridslides/example.tex new file mode 100644 index 00000000000..624c73d4bb7 --- /dev/null +++ b/Master/texmf-dist/doc/latex/gridslides/example.tex @@ -0,0 +1,111 @@ +% Package: gridslides +% Description: LaTeX package to create free form slides with blocks placed on a grid +% File: example.tex +% Author: Daniel Mendler <mail@daniel-mendler.de> +% Version: 0.1 +% Date: 2017/11/11 +% License: GPL2 or LPPL1.3 at your option +% Homepage: https://github.com/minad/gridslides +\documentclass{gridslides} + +\usepackage{cmbright} + +\newcommand{\hcterm}{\text{H.c.}} +\newcommand{\nodag}{{\phantom{\dag}}} +\newcommand{\hc}{^\dag} +\newcommand{\trans}{^\intercal} +\newcommand{\nohc}{^\nodag} +\newcommand{\OpH}{\ensuremath{\mathcal{H}}\xspace} +\newcommand{\HH}{\ensuremath{\widehat{\OpH}}\xspace} +\renewcommand{\vec}[1]{\ensuremath{\boldsymbol{#1}}\xspace} + +\newcommand{\border}{ + \block(0,0,32){\tikz\fill[blue!40!black] (0,0) rectangle (128mm,2mm);} + \block(0,0.5,32){\tikz\fill[blue!40!black] (0,0) rectangle (2mm,86mm);} + \block(31.5,0.5,1){\tikz\fill[blue!40!black] (0,0) rectangle (2mm,86mm);} + \block(0,22,32){\tikz\fill[blue!40!black] (0,0) rectangle (128mm,8mm);} +} + +\author{Author} +\title{Presentation Title} +\date{\today} +\institute{Institute~$\cdot$~University} + +\begin{style} + \border + \txt(26.5,1.5){\Large\textbf{\color{blue!50!black}LOGO}} + \block(1.5,2,26){\LARGE\theheadline} + \txt(1,22.8){\color{white}\theslide} + \txt(4,22.9){\color{white}\scriptsize\theauthor~$\cdot$~\thetitle} +\end{style} + +\begin{document} + +\begin{rawslide} + \border + \txt(26.5,1.5){\Large\textbf{\color{blue!50!black}LOGO}} + \block(2,5,28){\LARGE\thetitle} + \txt(2,9.5){\theauthor~$\cdot$~\thedate} + \txt(2,11.7){\footnotesize\theinstitute} +\end{rawslide} + +\begin{slide}{Overview} + \block(1.5,5,29){ + \begin{enumerate}[1.] + \item Topological phases + \item 1D p-wave superconductor + \end{enumerate} + } +\end{slide} + +\begin{slide}{Topological Phases} + \fig(3,4,12){qahe} + \fig(17,4,12){qshe} + \txt(6,11){Conducting edge channels $\longleftrightarrow$ Non-trivial bandstructure} + + \txt<2->(1.5,12.5){QAHE bulk Hamiltonian $\HH(\vec{k}) = \vec{g}(\vec{k})\cdot\vec{\sigma}$} + \eq<2->(13,14.2){\vec{g}(k_x,k_y) = \left(\sin k_x, \sin k_y, \cos k_x + \cos k_y - M \right)\trans} + + \only<3>{ + \fig(0.5,15,16){skyrmion} + \eq(4,20){M=1} + \block(4,15,5){\tikz \node[fill=white,text=red!90!black,inner sep=0.5mm] + {non-trivial};} + + \fig(15,16,16){trivial} + \eq(18,21){M=3} + \block(20,17.5,2.2){\tikz \node[fill=white,inner sep=0.5mm,text=blue!90!black] + {trivial};} + } +\end{slide} + +\begin{slide}{1D p-wave-SC} + \txt(1.5,11){Lattice} + \eq(6.5,10){\OpH = \sum_{i=1}^{n-1} \left [ t c_i\hc c_{i+1}\nohc + \Delta c\nohc_i c\nohc_{i+1} + \hcterm \right] - \mu \sum_{i=1}^n c_i\hc c_i\nohc} + + \fig(2,4,12){chain_trivial} + \fig(18,5.5,12){chain_nontrivial} + + \block<2->(26,10.5,4){% + \tikz \node[draw=red,inner sep=1mm] { + \scriptsize Majorana operators + $\begin{aligned} + \gamma_j\nohc &= \frac{c_j\nohc + c_j\hc}{2}\\ + \gamma_j' &= \frac{c_j\nohc - c_j\hc}{2 \imath} + \end{aligned}$ + }; + } + + \only<3>{ + \fig(3,13.5,9){kitaev_band02} + \txt(5,13.5){t=0.2} + + \fig(16,13.5,9){kitaev_band08} + \txt(18,13.5){t=0.8} + + \txt(4,20.5){Bulk} + \eq(9,20.3){\HH(k) = (2t \cos k - \mu)\tau_z - 2\Delta\sin k\, \tau_y\qquad\vec{c}_k\hc = \left( c_k\hc,\, c_{-k}\nohc\right)} + } +\end{slide} + +\end{document} |