Report tex added

2 files changed, 72 insertions, 16 deletions

diff --git a/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/Makefile b/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/Makefile
index a2cc642..a1d036c 100644
--- a/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/Makefile
+++ b/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/Makefile
@@ -1,6 +1,6 @@
 # -*- make -*-
 # FILE: "/home/evmik/src/my_src/Nresonances/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/Makefile"
-# LAST MODIFICATION: "Wed, 28 Sep 2011 17:14:37 -0400 (evmik)"
+# LAST MODIFICATION: "Wed, 28 Sep 2011 17:35:55 -0400 (evmik)"
 # (C) 2007 by Eugeniy Mikhailov, <evgmik@gmail.com>
 # $Id:$
 
@@ -19,7 +19,7 @@ all:  pdf
 pdf:  $(pdf_targets) 
 
 $(pdf_targets): %.pdf : %.tex $(includes)
-	pdflatex  $< 
+	rubber --pdf  $< 
 
 
 clean_latex_tmp:
diff --git a/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/report.tex b/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/report.tex
index ec8dd19..8f50a7c 100644
--- a/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/report.tex
+++ b/xmds2/Nlevels_no_dopler_with_z_fast_and_slow_light/report/report.tex
@@ -1,12 +1,11 @@
-\documentclass{article}
+\documentclass[aps,pra,twocolumn,groupedaddress,amsmath,amssymb]{revtex4}
 \usepackage{graphicx}
 \usepackage[normalem]{ulem} % needed by strike
 \usepackage[urlcolor=blue,colorlinks=true]{hyperref}
-\usepackage{fullpage}  % user defined
 
+\begin{document}
 \title{N-level system: slow and fast light}
 \author{E. E. Mikhailov}
-\begin{document}
 \date{2011/09/27}
 \maketitle
 %\clearpage
@@ -33,28 +32,85 @@ fast (field 3 is on and strong) light, and situations in between.
 Below the examples of fast and slow propagation for the following set of parameters:
 
 \begin{verbatim}
-G3=3.4e7         // decay rate of level |3> in 1/s
-G4=3.8e7         // decay rate of level |4> in 1/s 
-gt=3.1416e+04    // repopulation rate in 1/s
-z=1.5e-2         // cell length in m
-N=1e10*(1e6);    // number of particles per cubic m i.e. density
-delta1=0;        // field 1 one photon detuning 
-delta2=0;        // field 2 --------//---------
-delta3=0;        // field 3 --------//---------
+G3=3.4e7       // decay rate of level |3> in 1/s
+G4=3.8e7       // decay rate of level |4> in 1/s 
+gt=3.1416e+04  // repopulation rate in 1/s
+z=1.5e-2       // cell length in m
+N=1e10*(1e6);  // number of particles per cubic m 
+delta1=0;      // field 1 one photon detuning 
+delta2=0;      // field 2 --------//---------
+delta3=0;      // field 3 --------//---------
 \end{verbatim}
 
+\begin{figure}[h]
+	\begin{center}
+			\includegraphics[width=1.00\columnwidth]{slow_light/fields_propagation.pdf}
+	\end{center}
+	\caption{Propagation of the fields under slow light condition}
+	\label{fig:3fields_slow}
+\end{figure}
+
 Slow light behavior is observed for the 1 $\backslash$mu S long Gaussian pulse and
 the following fields parameters
-
 \begin{verbatim}
 E1=7.5e7;  // field  1 Rabi frequency  in 1/s
 E2=1;      // field  2 --------//----------- 
 E3=0;      // field  3 --------//-----------
 \end{verbatim}
 fields 1 and 3 have no time dependence at the input of the cell.
-light propagation 
-\includegraphics{slow_light/fields_propagation.png} 
 
+Propagation of all 3 fields is depicted at Fig.\ref{fig:3fields_slow}
+and output beam fields profiles in comparison with input are shown at
+Fig.\ref{fig:3fields_in_out_slow}
+where it easy to see delayed pulse for the field 2 in the middle.
+
+\begin{figure}[h]
+	\begin{center}
+			\includegraphics[width=1.00\columnwidth]{slow_light/fields_before_after_cell.pdf}
+	\end{center}
+	\caption{Propagation of the fields under slow light condition}
+	\label{fig:3fields_in_out_slow}
+\end{figure}
+
+
+Fast light or negative group delay is observed for the similar conditions
+but with field 3 switched on
+\begin{verbatim}
+E1=7.5e7;  // field  1 Rabi frequency  in 1/s
+E2=1;      // field  2 --------//----------- 
+E3=1.5e8;  // field  3 --------//-----------
+\end{verbatim}
+
+Propagation of all 3 fields is depicted at Fig.\ref{fig:3fields_fast}
+and output beam fields profiles in comparison with input are shown at
+Fig.\ref{fig:3fields_in_out_fast}.
+
+\begin{figure}[h]
+	\begin{center}
+			\includegraphics[width=1.00\columnwidth]{fast_light/fields_propagation.pdf}
+	\end{center}
+	\caption{Propagation of the fields under fast light condition}
+	\label{fig:3fields_fast}
+\end{figure}
+
+\begin{figure}[h]
+	\begin{center}
+			\includegraphics[width=1.00\columnwidth]{fast_light/fields_before_after_cell.pdf}
+	\end{center}
+	\caption{Propagation of the fields under fast light condition}
+	\label{fig:3fields_in_out_fast}
+\end{figure}
+
+The advancement of the pulse is very small but it could be seen on zoomed
+in Fig.\ref{fig:field2_in_out_fast}.
+
+\begin{figure}[h]
+	\begin{center}
+		\includegraphics[width=1.00\columnwidth]{fast_light/probe_before_after_cell.pdf}
+	\end{center}
+	\caption{Propagation of the fields under fast light condition}
+	\label{fig:field2_in_out_fast}
+\end{figure}
 
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