% alun määritelmät sallivat latex-kaavojen suoran siirron tähän % plain-tex documenttiin: % - yksirivinen latex kaava: suoraan muuttumattomana, edellyttäen % että label on mukana, juuri ennen \end{equation} lausetta % - useampiriviset kaavat: lisää ennen varsinaista kaavaa \eqalign{ % ja perään }, sekä poista toiset &. %\magnification=1200 \input epsf.def %needed only for post script figures \hsize=16.5truecm \vsize=25truecm \def\tensor#1{\bar{\bar{#1}}} \def\begin#1{$$} \def\label#1#2#3{$$} \def\section#1{{\bf #1}} \def\ref#1{} \def\cite#1{} \def\nonumber{} \def\mbox{} \def\\{\cr} \parindent=0pt Matalien l\"amp\"otilojen fysiikan teoria (Kyl-0.104)\hfil Autumn 2000\break Electronic transport in mesoscopic systems\hfil Exercise set 11\break \parindent=20pt \bigskip 1. Continue the exercise 1 in set 10 by going through those parts in the derivation of 2D weak localization correction to conductivity and its magnetic-field dependence, that were not properly discussed in the lectures. \bigskip 2. Exercises E.6.1 - E.6.4 from Datta's book. \bigskip This is the last exercise. Make sure that you come to the examination soon. The longer you wait, the more you will forget. \bigskip \end