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author | 2017-09-19 20:55:22 +0000 | |
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committer | 2017-09-19 20:55:22 +0000 | |
commit | 8e9ddc9fce63ef78f438d3c126a4ab9c1597844c (patch) | |
tree | 3b67e89c9266bc3289ffa9909937aecfa9684cc9 /Docs/source/theory/newcommands.tex | |
parent | 74b55dbbdca668d0a64f68a4699c256a96bf8ada (diff) | |
parent | 594de46736791c12b16b431def869addb9a70077 (diff) | |
download | WarpX-8e9ddc9fce63ef78f438d3c126a4ab9c1597844c.tar.gz WarpX-8e9ddc9fce63ef78f438d3c126a4ab9c1597844c.tar.zst WarpX-8e9ddc9fce63ef78f438d3c126a4ab9c1597844c.zip |
Merged in expand_doc (pull request #31)
Refactor the theoretical section of the documentation
Diffstat (limited to 'Docs/source/theory/newcommands.tex')
-rw-r--r-- | Docs/source/theory/newcommands.tex | 73 |
1 files changed, 0 insertions, 73 deletions
diff --git a/Docs/source/theory/newcommands.tex b/Docs/source/theory/newcommands.tex deleted file mode 100644 index fe1fe8c84..000000000 --- a/Docs/source/theory/newcommands.tex +++ /dev/null @@ -1,73 +0,0 @@ - -\usepackage{bm} -\usepackage{amsmath} -\usepackage{amssymb} -\usepackage{graphicx} -\usepackage{url} -\usepackage{hyperref} - -\usepackage[displaymath]{lineno}\usepackage{bm}% bold math - -\newcommand{\fe}{\mathbf{\tilde{E}}} -\newcommand{\fb}{\mathbf{\tilde{B}}} -\newcommand{\fj}{\mathbf{\tilde{J}}} -\newcommand{\ff}{\tilde{F}} -\newcommand{\fg}{\tilde{G}} -\newcommand{\fk}{\mathbf{k}} -\newcommand{\fkhat}{\mathbf{\hat{k}}} - -% Definitions from Remi's paper on Galilean math -\newcommand{\Km}{\vec{K}_{\vec{m}}} -\newcommand{\km}{\vec{k}_{\vec{m}}} -\renewcommand{\vec}[1]{\boldsymbol{#1}} -\newcommand{\vgal}{\vec{v}_{gal}} -\newcommand{\nab}{\vec{\nabla'}} -\newcommand{\Dt}[1]{ \frac{\partial #1}{\partial t}} -\newcommand{\mc}[1]{\hat{\mathcal{#1}}} -\newcommand{\xj}{\vec{x}'_{\vec{j}}} -\newcommand{\Xll}{\vec{X}_{\vec{\ell}}} -\newcommand{\Integ}[1]{\int_{-\infty}^{\infty} \!\!\!\!\!\! - \mathrm{d}#1} -\newcommand{\RInteg}[1]{\int_{0}^{\infty} \!\! \frac{#1\mathrm{d}#1}{(2\pi)^2}} - -% Definitions from Remi's Thesis -\newcommand{\h}{\mathcal{H}} -\newcommand{\hf}{\frac{1}{2}} -\newcommand{\um}{$\mu$m} -\newcommand{\Um}{\mu \mathrm{m}} -\newcommand{\aal}{\langle \vec{a}_l^2 \rangle} -\newcommand{\etad}{ \eta_d } -\newcommand{\etae}{ \eta_\epsilon } -\newcommand{\etag}{ \eta_\gamma } -\newcommand{\tlambda}{ \tilde{\lambda} } -%\newcommand\comment[1]{\textcolor{red}{\textbf{#1}}} -\newcommand{\gsim}{\mathrel{\hbox{\rlap{\lower.55ex -\hbox{$\sim$}} \kern-.3em \raise.4ex \hbox{$>$}}}} -\newcommand{\lsim}{\mathrel{\hbox{\rlap{\lower.55ex -\hbox{$\sim$}} \kern-.3em \raise.4ex \hbox{$<$}}}} -\newcommand{\kfoc}{k_\mathrm{foc}} -\newcommand{\bkfoc}{\bar{k}_\mathrm{foc}} -\newcommand{\xil}{\xi_{\mathrm{laser}}} - -\newcommand{\Ex}[2]{{E_x}^{#1}_{#2}} -\newcommand{\Ey}[2]{{E_y}^{#1}_{#2}} -\newcommand{\Ez}[2]{{E_z}^{#1}_{#2}} -\newcommand{\Bx}[2]{{B_x}^{#1}_{#2}} -\newcommand{\By}[2]{{B_y}^{#1}_{#2}} -\newcommand{\Bz}[2]{{B_z}^{#1}_{#2}} -\newcommand{\Jx}[2]{{J_x}^{#1}_{#2}} -\newcommand{\Jy}[2]{{J_y}^{#1}_{#2}} -\newcommand{\Jz}[2]{{J_z}^{#1}_{#2}} - -\newcommand{\tEr}[2]{\tilde{E_r}^{#1}_{#2}} -\newcommand{\tEt}[2]{\tilde{E_\theta}^{#1}_{#2}} -\newcommand{\tEz}[2]{\tilde{E_z}^{#1}_{#2}} -\newcommand{\tBr}[2]{\tilde{B_r}^{#1}_{#2}} -\newcommand{\tBt}[2]{\tilde{B_\theta}^{#1}_{#2}} -\newcommand{\tBz}[2]{\tilde{B_z}^{#1}_{#2}} -\newcommand{\tJr}[2]{\tilde{J_r}^{#1}_{#2}} -\newcommand{\tJt}[2]{\tilde{J_\theta}^{#1}_{#2}} -\newcommand{\tJz}[2]{\tilde{J_z}^{#1}_{#2}} - -\newcommand{\CCirc}{\textsc{Calder Circ}} -\newcommand{\CCart}{\textsc{Calder 3D}}
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