%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%  This is expt_diff_front.tex%%  Text to be included in the paper "The Shape of the Quantum%    Diffusion Front", to describe the fits to experimental%    quantum kicked rotor data.%%  Created 10/23/00.%  Last modified 11/1/00.%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% Ascii table for electronic transfer troubleshooting%% Upper-case    A B C D E F G H I J K L M N O P Q R S T U V W X Y Z% Lower-case    a b c d e f g h i j k l m n o p q r s t u v w x y z% Digits        0 1 2 3 4 5 6 7 8 9% Exclamation   !           Double quote "          Hash (number) #% Dollar        $           Percent      %          Ampersand     &% Acute accent  '           Left paren   (          Right paren   )% Asterisk      *           Plus         +          Comma         ,% Minus         -           Point        .          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Raizen  (all affiliated with UT-Austin)%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\vspace{0.5in}%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                                                           \textit{  Text to be tacked onto the end of the abstract:                                                                  }These results are also applied to experimental measurementsin the quantum kicked rotor system.%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%  Experimental Figure here%    This link uses the graphicx package.\begin{figure}[h]  \begin{center}  \includegraphics*[trim=0in 0in 0in 0in, scale=0.48]                                     {composite_plot.eps}  \end{center}  \caption{Experimental quantum kicked rotor data (heavy lines)           with best fits (open circles), shown only at the           time of 70 kicks for clarity.  The three regimes shown           are (a) exponential localization, (b) anomalous           diffusion, and (c) noise-induced delocalization, for           which the respective exponents are $\gamma = 1.06$,           1.48, and 2.03.	\label{expt_fig}}\end{figure}%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\vspace{0.5in}%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%  Text to be inserted before the summary in the main body of %    the paper.%We also used Eqs.~(1) and (2) to analyze experimental momentumdistributions of the quantum kicked rotor.  The details of theatom-optics experiment and the measurement conditionsare described in Ref.~\cite{Steck00}.In each case that we study, the distributions after 30, 40, 50,60, and 70 kicks are fit simultaneously to Eq.~(1) while imposingEq.~(2) as a constraint.  To more accurately reflect the experiment,the fundamental distribution in Eq.~(2) is convolved with the initial atomic momentum distribution, and a correction is appliedfor the known response of the detection system.In order to obtain more accurate fits, the center of thedistribution ($|p/2\hbar k_{\mathrm{L}}|<15$, where $\hbar k_{\mathrm{L}}$ is the photon recoil momentum) is excluded from the fit, along with the extreme tails ($|p/2\hbar k_{\mathrm{L}}|>70$), where the signal levels areunreliably small and where ``momentum boundary'' effectsare most significant \cite{Steck00}.We study three distinct cases, beginning with dynamical localization(with a stochasticity parameter $K=11.2$), where we find an exponent $\gamma = 1.06 \pm 0.19$,which is consistent with exponential localization.In the next case, thecorresponding classical dynamics exhibitanomalous diffusion ($K=8.4$), where the fit yields$\gamma = 1.48 \pm 0.16$; this larger exponent is consistent with the curved, nonexponential distribution tails observedin the experiments \cite{Klappauf98}.Finally, we study the kicked rotor with $K=11.2$ driven strongly(200\%) by amplitude noise, where the dynamics mimic classical diffusion; in this case we find$\gamma = 2.03 \pm 0.14$, which is consistent with normal diffusion.The largest contribution to the quoted uncertainties is the sensitivity of the fit to changing the cutoff boundariesdescribed above.The data and fits for all three casesare shown at 70 kicks in Fig.~\ref{expt_fig}, showing excellentagreement in the tails of the distributions.%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\vspace{0.5in}%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                                                           \textit{  Additions to the acknowledgements section                                                                  }NSF grant no.~PHY-9987706.D.A.S. acknowledges support from the Fannie and John Hertz Foundation.%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%  Additional citations%\begin{thebibliography}{99}\bibitem{Steck00}D.~A. Steck, V. Milner, W.~H. Oskay, and M.~G. Raizen,\pre \textbf{62}, 3461 (2000).\bibitem{Klappauf98}B.~G. Klappauf, W.~H. Oskay, D.~A. Steck, and M.~G. Raizen,\prl \textbf{81}, 4044 (1998).\end{thebibliography}%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\end{document}