\batchmode
\documentstyle[html,psfig,harvard,preprint,aps,Times]{revtex}
\makeatletter



\makeatother
\newenvironment{tex2html_wrap}{}{}
\begin{document}
\pagestyle{empty}
\newpage

{\samepage \clearpage $G$
}


\newpage

{\samepage \clearpage $L=5, 10, 30$
}


\newpage

{\samepage \clearpage $200$
}


\newpage

{\samepage \clearpage $\delimiter "426830A w\delimiter "526930B =10$
}


\newpage

{\samepage \clearpage $W=20$
}


\newpage

{\samepage \clearpage $w=10$
}


\newpage

{\samepage \clearpage $L=5$
}


\newpage

{\samepage \clearpage $W=10$
}


\newpage

{\samepage \clearpage $L=10$
}


\newpage

{\samepage \clearpage $L=20$
}


\newpage

{\samepage \clearpage $L=50$
}


\newpage

{\samepage \clearpage $L=100$
}


\newpage

{\samepage \clearpage $N=1000, 1000, 3000, 4000$
}


\newpage

{\samepage \clearpage $L=10,20,50,100$
}


\newpage

{\samepage \clearpage $L=200$
}


\newpage

{\samepage \clearpage $\lambda \rightarrow \lambda /100$
}


\newpage

{\samepage \clearpage ${\string\prm\space DOS}\rightarrow {\string\prm\space DOS}*5$
}


\newpage

{\samepage \clearpage $E=-2$
}


\newpage

{\samepage \clearpage $E=-3.73$
}


\newpage

{\samepage \clearpage $E=-0.5$
}


\newpage

{\samepage \clearpage $E=-3.8$
}


\newpage

{\samepage \clearpage $N=4000$
}


\newpage

{\samepage \clearpage $L=4$
}


\newpage

{\samepage \clearpage $L=300$
}


\newpage

{\samepage \clearpage $p=5\%$
}


\newpage

{\samepage \clearpage $L=4,10,20,50,100,200$
}


\newpage

{\samepage \clearpage $\delimiter "426830A G(E)\delimiter "526930B $
}


\newpage

{\samepage \clearpage ${\string\prm\space rms} (G(E))$
}


\newpage

{\samepage \clearpage $p=1\%$
}


\newpage

{\samepage \clearpage $\delimiter "426830A G\delimiter "526930B $
}


\newpage

{\samepage \clearpage $E=-0.5,-2$
}


\newpage

{\samepage \clearpage $-3.73$
}


\newpage

{\samepage \clearpage $\mathop {\mathgroup \z@ exp}\nolimits (\delimiter "426830A \mathop {\mathgroup \z@ ln}\nolimits G\delimiter "526930B )$
}


\newpage

{\samepage \clearpage $N=1000$
}


\newpage

{\samepage \clearpage $(L=10)$
}


\newpage

{\samepage \clearpage $N=3000$
}


\newpage

{\samepage \clearpage $(L=50)$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $2e^2/h$
}


\newpage

{\samepage \clearpage $l$
}


\newpage

{\samepage \clearpage $w$
}


\newpage

{\samepage \clearpage $\lambda_F$
}


\newpage

{\samepage \clearpage $L$
}


\newpage

{\samepage \clearpage $\lambda$
}


\stepcounter{section}
\newpage

{\samepage \clearpage \begin{figure}[h]\relax\end{figure}
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_1.ps,width=7in}

\label{wire}
\end{figure}
}


\newpage

{\samepage \clearpage $10$
}


\newpage

{\samepage \clearpage $\sim 100$
}


\newpage

{\samepage \clearpage \begin{equation}{\bf H}= \sum_{i} |i\rangle \varepsilon_i \langle i| +
\sum_{i,j \atop (i \ne j)} |i\rangle V_{ij} \langle j|
\label{eq:hamilt}
\end{equation}
}


\newpage

{\samepage \clearpage $|i\rangle$
}


\newpage

{\samepage \clearpage $i$
}


\newpage

{\samepage \clearpage $ \varepsilon_i $
}


\newpage

{\samepage \clearpage $V_{ij}$
}


\newpage

{\samepage \clearpage $j$
}


\newpage

{\samepage \clearpage $V_{ij} \equiv V$
}


\newpage

{\samepage \clearpage $V$
}


\newpage

{\samepage \clearpage $x$
}


\newpage

{\samepage \clearpage $M$
}


\newpage

{\samepage \clearpage $T_{mn}=|t_{mn}|^2$
}


\newpage

{\samepage \clearpage $n$
}


\newpage

{\samepage \clearpage $m$
}


\newpage

{\samepage \clearpage $t_{mn}$
}


\newpage

{\samepage \clearpage \begin{equation}t_{mn} = \sqrt{\frac{v_m}{v_n}} \left[ {\bf U}^{-1}(+)V{\bf G}_{0,L+1}
         [{\bf F}^{-1}(+) - {\bf F}^{-1}(-)] {\bf U}(+) \right]_{mn}
\label{eq:ando}
\end{equation}
}


\newpage

{\samepage \clearpage \begin{equation}{\bf F}(\pm)  =  {\bf U}(\pm){\Lambda}(\pm){\bf U}^{-1}(\pm),
\label{eq:f}
\end{equation}
}


\newpage

{\samepage \clearpage $v_n$
}


\newpage

{\samepage \clearpage ${\bf G}_{0,L+1}$
}


\newpage

{\samepage \clearpage $0$
}


\newpage

{\samepage \clearpage $(L+1)$
}


\newpage

{\samepage \clearpage \begin{equation}{\bf U}(\pm)=\left[{\bf u}_1(\pm) \cdots {\bf u}_M(\pm) \right]~,
\label{eq:Upm}
\end{equation}
}


\newpage

{\samepage \clearpage \begin{displaymath} \Lambda (\pm) = \left( \begin{array}{cccc}
 \zeta_1(\pm) &   &   &  \\ 
   & \zeta_2(\pm) &   &  \\ 
   &  &        \cdots   &  \\ 
   &  &  &  \zeta_M(\pm)
\end{array} \right)~.\end{displaymath}
}


\newpage

{\samepage \clearpage \begin{eqnarray}\zeta  \left( \begin{array}{l}
   {\bf C}_{J}   \\ 
   {\bf C}_{J-1}
\end{array} \right) = \left( \begin{array}{cr}
    V^{-1}\left( E{\bf I}-{\bf H}_0^{(1)} \right)  &  -{\bf I}     \\ 
          {\bf I}                                 &   {\bf 0}
 \end{array} \right)  \left( \begin{array}{l}
   {\bf C}_{J}   \\ 
   {\bf C}_{J-1}
\end{array} \right)
\label{eq:eigenproblem}
\end{eqnarray}
}


\newpage

{\samepage \clearpage $-\infty$
}


\newpage

{\samepage \clearpage $+\infty$
}


\newpage

{\samepage \clearpage \begin{equation}(E{\bf I} - {\bf H}_J^{(1)}){\bf C}_J-{\bf V}{\bf C}_{J-1}-
{\bf V}{\bf C}_{J+1}=0
\label{eq:discr_schr}
\end{equation}
}


\newpage

{\samepage \clearpage ${\bf H}_J^{(1)}$
}


\newpage

{\samepage \clearpage ${\bf H}_0^{(1)}$
}


\newpage

{\samepage \clearpage ${\bf C}_J$
}


\newpage

{\samepage \clearpage $J$
}


\newpage

{\samepage \clearpage ${\bf V}$
}


\newpage

{\samepage \clearpage \begin{equation}\zeta {\bf C}_{J-1}={\bf C}_J~,
\label{eq:c2}
\end{equation}
}


\newpage

{\samepage \clearpage $\zeta=\exp({\rm i}ka)$
}


\newpage

{\samepage \clearpage $a$
}


\newpage

{\samepage \clearpage $\zeta$
}


\newpage

{\samepage \clearpage ${\bf u}$
}


\newpage

{\samepage \clearpage $\zeta(-)$
}


\newpage

{\samepage \clearpage ${\bf u}(-)$
}


\newpage

{\samepage \clearpage $\zeta(+)$
}


\newpage

{\samepage \clearpage ${\bf u}(+)$
}


\newpage

{\samepage \clearpage $\zeta < 1$
}


\newpage

{\samepage \clearpage $\zeta > 1$
}


\newpage

{\samepage \clearpage \begin{eqnarray}j & = & \frac{e}{2{\rm i}\hbar}\left[
{\bf C}_J^{\dag}{\bf C}_{J+1} - {\bf C}_J{\bf C}_{J+1}^{\dag} +
{\bf C}_{J-1}^{\dag}{\bf C}_{J} - {\bf C}_{J-1}{\bf C}_{J}^{\dag} \right]
\nonumber \\ 
 & = & \frac{2e}{\hbar} |{\bf C}_J|^2~\mathop{\rm Im}\nolimits\zeta
\label{eq:j}
\end{eqnarray}
}


\newpage

{\samepage \clearpage $|\zeta|=1$
}


\newpage

{\samepage \clearpage $\mathop{\rm Im}\nolimits\zeta > 0$
}


\newpage

{\samepage \clearpage $j>0$
}


\newpage

{\samepage \clearpage $\mathop{\rm Im}\nolimits\zeta < 0$
}


\newpage

{\samepage \clearpage \begin{eqnarray}{\bf G}_{1,N+1}^{(N+1)} &=& {\bf G}_{1,N}^{(N)}{\bf V}_{N,N+1}
{\bf G}_{N+1,N+1}^{(N+1)}, \label{eq:G1L} \\ 
{\bf G}_{N+1,N+1}^{(N+1)} &=& \left[ E{\bf I} - {\bf H}_{N+1}^{(1)} -
{\bf V}_{N,N+1}^{\dag}{\bf G}_{N,N}^{(N)}{\bf V}_{N,N+1} \right]^{-1}\;.
 \label{eq:GLL}
\end{eqnarray}
}


\newpage

{\samepage \clearpage ${\bf G}_{NN}$
}


\newpage

{\samepage \clearpage ${\bf G}_d^{(\infty/2)}$
}


\newpage

{\samepage \clearpage \begin{equation}{\bf G}_{00} =
{\bf G}_d^{(\infty/2)}(\mbox{L--lead}) =
  {\bf U}(+)\Lambda (+){\bf U}^{-1}(+)V^{-1}
\label{eq:G00}
\end{equation}
}


\newpage

{\samepage \clearpage \begin{equation}{\bf G}_d^{(\infty/2)}(\mbox{R--lead}) =
  {\bf U}(+)\Lambda (-){\bf U}^{-1}(+)V^{-1} = {\bf S}_{\infty}^{-1}
\label{eq:S}
\end{equation}
}


\newpage

{\samepage \clearpage ${\bf S}_{\infty}^{-1}$
}


\newpage

{\samepage \clearpage \begin{displaymath} \tilde{\bf H}={\bf H}_0+{\bf S}_{\infty}~\end{displaymath}
}


\newpage

{\samepage \clearpage ${\bf G}_{1N}$
}


\newpage

{\samepage \clearpage ${\bf F}(\pm)$
}


\newpage

{\samepage \clearpage \begin{equation}t_{mn} = \sqrt{\frac{v_m}{v_n}}~\left[~{\bf U}^{-1}(+)V{\bf G}_{0,L+1}
 {\bf U}(+) [\Lambda (-) - \Lambda (+)]~\right]_{mn}~~.
\label{eq:my}
\end{equation}
}


\newpage

{\samepage \clearpage ${\bf U}(\pm)$
}


\newpage

{\samepage \clearpage \begin{equation}T_{mn} = |t_{mn}|^{2} = |\zeta_{m}(+)|^{2L} \delta_{mn}
\label{eq:Tperf}
\end{equation}
}


\newpage

{\samepage \clearpage \begin{equation}G= 2\frac{e^2}{h} \sum_{n=1}^{N_L} \sum_{m=1}^{N_R}|t_{mn}|^2~~.
\label{eq:conductance}
\end{equation}
}


\newpage

{\samepage \clearpage $N_L$
}


\newpage

{\samepage \clearpage $N_R$
}


\newpage

{\samepage \clearpage \begin{equation} {\rm rms} (G) = \left( \langle G^2\rangle - \langle G\rangle^2 \right)^{1/2}
\label{eq:fluctuation}
\end{equation}
}


\newpage

{\samepage \clearpage $\langle\rangle$
}


\newpage

{\samepage \clearpage $\epsilon_{\mbox{\scriptsize{isl}}}\rightarrow \infty$
}


\newpage

{\samepage \clearpage $T=0K$
}


\stepcounter{section}
\newpage

{\samepage \clearpage $\langle w \rangle =10$
}


\newpage

{\samepage \clearpage $E$
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_2.ps}

\label{rEone}
 \end{figure}
}


\newpage

{\samepage \clearpage $l<L<\lambda$
}


\newpage

{\samepage \clearpage $e^2/h$
}


\newpage

{\samepage \clearpage $L=30$
}


\newpage

{\samepage \clearpage $E_c\sim 1/L$
}


\newpage

{\samepage \clearpage $E_c\sim 1/L^2$
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_3.ps}
 
\label{G_rEaverage}
\end{figure}
}


\newpage

{\samepage \clearpage $\langle
G\rangle$
}


\newpage

{\samepage \clearpage $\exp(\langle \ln~G\rangle)$
}


\newpage

{\samepage \clearpage \begin{equation}G(E,L)\sim\exp(-2L/\lambda(E))~.
\label{eq:Gexp}
\end{equation}
}


\newpage

{\samepage \clearpage ${\rm DOS}\rightarrow {\rm DOS}*5$
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_4.ps}
 
\label{G_rEflc}
\end{figure}
}


\newpage

{\samepage \clearpage $L\simeq l$
}


\newpage

{\samepage \clearpage $L>\lambda$
}


\newpage

{\samepage \clearpage $L<<\lambda$
}


\newpage

{\samepage \clearpage ${\rm rms} (G)=0.729
e^2/h$
}


\newpage

{\samepage \clearpage ${\rm rms}
(G(E))$
}


\newpage

{\samepage \clearpage $\lambda(E)$
}


\newpage

{\samepage \clearpage ${\rm rms} (G)$
}


\newpage

{\samepage \clearpage $P(\tau)$
}


\newpage

{\samepage \clearpage $\tau$
}


\newpage

{\samepage \clearpage $0\le\tau\le 1$
}


\newpage

{\samepage \clearpage ${\bf t}{\bf t}^{\dag}$
}


\newpage

{\samepage \clearpage ${\bf
t}$
}


\newpage

{\samepage \clearpage $\tau=0$
}


\newpage

{\samepage \clearpage $\tau=1$
}


\newpage

{\samepage \clearpage ${\bf
t}_L{\bf t}_L^{\dag}$
}


\newpage

{\samepage \clearpage $(2)e^2/h$
}


\newpage

{\samepage \clearpage $0.1<\tau\le 1$
}


\newpage

{\samepage \clearpage $\langle(\mathop{\rm Tr}\nolimits {\bf t}{\bf t}^{\dag})^n\rangle$
}


\newpage

{\samepage \clearpage $\mathop{\rm Tr}\nolimits\langle ({\bf t}{\bf
t}^{\dag})^n\rangle$
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_5.ps}

\label{G_rLaverage}
\end{figure}
}


\newpage

{\samepage \clearpage $\exp(\langle\ln G\rangle)$
}


\newpage

{\samepage \clearpage $\langle\ln G\rangle$
}


\newpage

{\samepage \clearpage \begin{equation}\lambda = - \frac{\partial \langle\ln G\rangle}{2\partial L} .
\label{eq:lag}
\end{equation}
}


\newpage

{\samepage \clearpage $L>>\lambda$
}


\newpage

{\samepage \clearpage $L<10$
}


\stepcounter{section}
\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_6.ps}

\label{iEone}
\end{figure}
}


\newpage

{\samepage \clearpage $50$
}


\newpage

{\samepage \clearpage $E_c$
}


\newpage

{\samepage \clearpage $2\pi$
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_7.ps}

\label{G_iEaverage}
\end{figure}
}


\newpage

{\samepage \clearpage $\langle G(E)\rangle$
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_8.ps}

\label{i1Eaverage}
\end{figure}
}


\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_9.ps}

\label{G_iLaverage}
\end{figure}
}


\newpage

{\samepage \clearpage $\exp(\langle \ln (G)\rangle)$
}


\newpage

{\samepage \clearpage ${\rm rms} (G) \approx 0.73$
}


\stepcounter{section}
\newpage

{\samepage \clearpage \begin{figure}\psfig{file=fig94_10.ps}

\label{VI_L10a}
\end{figure}
}


\stepcounter{section}
\newpage

{\samepage \clearpage $0.729e^2/h$
}


\newpage

{\samepage \clearpage $W\sim w$
}


\newpage

{\samepage \clearpage $W$
}


\newpage

{\samepage \clearpage $W>>w$
}



\end{document}
