Modified some figures
Signed-off-by: Riccardo Finotello <riccardo.finotello@gmail.com>
This commit is contained in:
@@ -81,15 +81,13 @@ We thus choose $X_{(t)}^1$ and $X_{(t)}^2$ to be the coordinates parallel to the
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\centering
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\begin{subfigure}[b]{0.45\linewidth}
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\centering
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\def\svgwidth{\linewidth}
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\import{img}{branesangles.pdf_tex}
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\import{tikz}{branesangles.pgf}
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\caption{D-branes as lines on $\R^2$.}
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\end{subfigure}
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\hfill
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\begin{subfigure}[b]{0.45\linewidth}
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\centering
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\def\svgwidth{\linewidth}
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\import{img}{welladapted.pdf_tex}
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\import{tikz}{welladapted.pgf}
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\caption{Well adapted system of coordinates.}
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\end{subfigure}
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\caption{%
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@@ -233,15 +233,13 @@ In fact a transformation $\xi \mapsto \chi(\xi)$ and $\bxi \mapsto \bchi(\bxi)$
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\centering
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\begin{subfigure}[b]{0.45\linewidth}
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\centering
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\def\svgwidth{\linewidth}
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\import{img}{complex_plane.pdf_tex}
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\import{tikz}{complex_plane.pgf}
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\caption{Radial ordering.}
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\end{subfigure}
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\hfill
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\begin{subfigure}[b]{0.45\linewidth}
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\centering
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\def\svgwidth{\linewidth}
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\import{img}{radial_ordering.pdf_tex}
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\import{tikz}{radial_ordering.pgf}
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\caption{Difference of time ordered contours.}
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\end{subfigure}
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\caption{Map to the complex plane.}
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@@ -1284,16 +1282,14 @@ The field $\cA^a$ forms a vector representation of the group \SO{D-1-p} and from
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\centering
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\begin{subfigure}[b]{0.45\linewidth}
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\centering
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\def\svgwidth{0.8\linewidth}
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\import{img}{chanpaton.pdf_tex}
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\import{tikz}{chanpaton.pgf}
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\caption{Chan-Paton factors labelling strings.}
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\end{subfigure}
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\hfill
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\begin{subfigure}[b]{0.45\linewidth}
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\centering
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\def\svgwidth{0.7\linewidth}
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\import{img}{quark.pdf_tex}
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\caption{Naive model of a left handed massive quark.}
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\import{tikz}{quark.pgf}
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\caption{Naive model of left handed massive quarks.}
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\end{subfigure}
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\caption{Strings attached to different D-branes.}
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\label{fig:dbranes:chanpaton}
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@@ -1346,8 +1342,7 @@ The light spectrum is thus composed of the desired matter content alongside with
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\begin{figure}[tbp]
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\centering
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\def\svgwidth{0.7\linewidth}
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\import{img}{smbranes.pdf_tex}
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\import{tikz}{smbranes.pgf}
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\caption{%
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Example of \sm-like construction using intersecting D-branes with the indications of the hypercharge $Y$.
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Perpendicular angles are only a matter of convenience: they are in principal arbitrary.
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