\documentclass[12pt,color=dvipsnames]{beamer}

%
% This is the tex file of the presentation that I actually gave.  Some
% of the stuff in here is only here because it was in the sample that
% I copied from; some other stuff is a basic hack that I put in to do
% something complicated and which I couldn't see a simple way to do
% otherwise.  I didn't have overmuch time to learn the ins and outs of
% beamer so had to take the 'quick and dirty' route a few times.  Now
% that I've had time to read the whole manual, I've figured out what I
% would do differently.  That's in a different file - as this is an
% example I thought it best to put up what I actually did as well as
% what I would have done.
% 

%
% Options to beamer: the default font size is 11pt; I chose to
% increase this to 12pt to make everything that bit bigger and clearer
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% names such as 'WildStrawberry'.  I didn't, in the end, but it's nice
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\mode<presentation>
{
%
% Sets up the look of the thing.  I chose Pittsburgh as it seemed a
% fairly sparse theme.  I also used the sidebar outer theme to give me
% more control over the size of the frame titles (as I was using
% simple one-line titles I didn't need all the space usually
% allocated).  The 0pt on the width effectively turns off the sidebar
% itself.  That seemed to muck around with the colours a bit so the
% colour theme 'lily' restores things to normal again.  As I was using
% a larger font size, I figured that I could get away with serif
% lettering but made sure that any small font was in the more legible
% sans-serif (see the beamer user manual section on fonts).
%

  \usetheme{Pittsburgh}

  \useoutertheme[width=0pt,height=25pt]{sidebar}
  \usecolortheme{lily}
  \usefonttheme[stillsansserifsmall]{serif}
}

%
% Despite using the colour theme 'lily', the frametitle colour wasn't
% what it originally was.
%

\setbeamercolor{frametitle}{fg=blue}

%
% Apart from the pxfonts line, the next block was all in the original
% template that I copied from.  I prefer pxfonts to Computer Modern;
% they're in the standard teTeX distribution so should be on most TeX
% installations.  If LaTeX complains about fonts when compiling this
% document, try commenting out the pxfonts line.  Then go and get
% yourself some decent TeX fonts.
%

\usepackage[english]{babel}
\usepackage[latin1]{inputenc}
\usepackage{pxfonts}
\usepackage[T1]{fontenc}

%
% Standard stuff now; amsthm is loaded by default with beamer.
%

\usepackage{amsmath}
\usepackage[arrow,matrix,curve]{xy}

%
% The argument of a 'mode' command is only active in the specified
% mode.  I was thinking of producing a handout based on the slides,
% but didn't in the end.  If I had done so, this would have made it
% clear what was a slide and what wasn't (say, if I'd done them 2-up)
% by making the background slightly grey.
%

\mode<handout>{\beamertemplatesolidbackgroundcolor{black!5}}

%
% More standard stuff
%

\DeclareMathOperator{\Topcat}{Top}
\DeclareMathOperator{\gab}{GAb}
\DeclareMathOperator{\Sq}{Sq}
\newcommand{\Z}{\mathbb{Z}}
\newcommand{\Q}{\mathbb{Q}}
\newcommand{\F}{\mathbb{F}}

\newtheorem{proposition}[theorem]{Proposition}

%
% Sometimes - and only sometimes - math text in normal text can get a
% little lost; generally in situations like: ``Let n be an integer.''
% So I defined a new colour to make this stand out a little.  I
% implemented this manually rather than changing all math text (to do
% that, see the beamer user guide) as I only wanted to change the
% colour where I thought it really necessary.
%

\definecolor{math}{named}{violet}

%
% I wanted a visual clue that I was on the last slide of a frame.  I
% chose to change the colour of the frame title.  This colour is the
% colour to change to.
%

\definecolor{last}{named}{purple}

\bibliographystyle{halpha}

\title{Delooping Moravian Maps}

\subtitle{Stable and Unstable Operations in the Morava K--theories\\
%
arXiv: math.AT/0605471\\[20pt]
21st British Topology Meeting
}

\author[Stacey \and Whitehouse]
{Andrew Stacey\inst{1} \and Sarah Whitehouse\inst{2}}

\institute[Sheffield]{
  University of Sheffield \\
\inst{2}Partially and \inst{1}fully supported by the EPSRC, grant no.:
  GR/S76823/01%
}

\date{12th September 2006}

\begin{document}

\begin{frame}
\label{title}
  \titlepage
\end{frame}

%
% This is the most complicated frame.  Slides of this frame appear at
% two later places.  Here we get slides 1 and 2, the second time we
% get slide 3, then last of all we get 4 to 7.  In actual fact, slides
% 2, 3, and 4 are identical but making them actually the same makes
% LaTeX complain about multiple references and makes the labelling go
% wrong.  Thus the best way is to ensure that at least the first slide
% of any new appearance has not been seen before, even if it is
% identical to another.
%

%
% This also shows the recolouring of the frame title.  This occurs on
% frames 2,3, and 7 (which are the last slides of each occurrence).
% I also put labels on the last slides of each occurrence.  This was
% so that at the end of the talk I could jump back to any given frame
% and be sure of landing on the last slide of that frame (i.e. with
% all the junk displayed).  This worked as one would hope: the
% 'qnsorig' jumped back to this occurrence of the frame, 'qnsreprise'
% to the second, and 'qnsconclude' to the third.
%

\begin{frame}<1-2>[label=qns]
\frametitle{{\only<2,3,7>{\color{last}}Questions}}
\label<2>{qnsorig}
\label<3>{qnsreprise}
\label<7>{qnsconclude}

\uncover<5->{
{\color{blue}For the Morava K--theories:}
}

\vfill
  \begin{enumerate}
  \item When is an unstable cohomology operation a component of a
stable one?

\vfill
\uncover<6->{
{\color{blue} If it can be delooped once.}
}
\vfill
\pause
  \item If we have a component of a stable operation, can we construct
the other components?

\vfill
\uncover<7->{
{\color{blue} Yes;  easily, using the periodicity.}
}

  \end{enumerate}

\vfill

\end{frame}

\begin{frame}
  \frametitle{{\only<3>{\color{last}}Preliminaries}}

\label<3>{prelim}

Let \(E^*(-)\) be a \alert{graded, generalised cohomology
  theory}. \pause

\vspace{20pt}

Contravariant functor \(E^*(-) : \Topcat \to \gab\)

\begin{itemize}
\item \(X\) topological space \(\xymatrix@1{{} \ar@{~>}[r] & {}}\)
\(E^*(X)\), graded abelian group.

\item \(f : X \to Y\) continuous \(\xymatrix@1{{} \ar@{~>}[r] & {}}\)
\(f^* : E^*(Y) \to E^*(X)\) of graded abelian groups (degree zero), with
 \((f g)^* = g^* f^*\).

\pause

\item \(E^*(-)\) \alert{intertwines suspensions}: \\
\(E^k(\Sigma X) \cong (\Sigma E^*(X))^k = E^{k-1}(X)\), natural in \(X\).
\end{itemize}

\vfill

\end{frame}


\begin{frame}
\frametitle{{\only<4>{\color{last}}Forgetfulness}}
\label<4>{forget}

Three views of \(E^*(-)\):

\pause
\vfill

\begin{itemize}
\item One functor, \(E^*(-)\), into graded abelian groups. \pause
\vfill
\item A family of functors, \(\{E^k(-)\}\), into abelian
groups. \pause
\vfill
\item A family of functors, \(\{E^k(-)\}\), into sets.
\end{itemize}
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<2>{\color{last}}Operations}}
\label<2>{nat}

An \alert{operation} is a natural transformation between
functors. \pause

\vfill
\(F, G : \mathcal{C} \to \mathcal{D}\) contravariant.

\(\nu : F \to G\) is:

 for every \(\mathcal{C}\)--object \(X\),
\(\nu_X : F(X) \to G(X)\) such that:
%
\[
  \xymatrix{
    F(X) \ar[r]^{\nu_X} \ar@{}[rd]|{\circlearrowleft} & 
%
    G(X) \\
%
    F(Y) \ar[r]^{\nu_Y} \ar[u]^{F(f)} &
%
    G(Y) \ar[u]_{G(f)}
}
\]
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<5>{\color{last}}Operations}}
\label<5>{ops}

There are \alert{three} types of operation: \pause

\begin{itemize}
\item {\color{blue}Stable:} \(r : E^*(-) \to E^*(-)\) of graded
abelian groups, respecting suspension.
\hfill
\(\mathcal{S}^h\)\pause

\vspace{20pt}

\item {\color{blue} Additive:} \(r : E^k(-) \to E^l(-)\) of abelian
groups.
\hfill
\(\mathcal{A}_k^l\) \pause

\vspace{20pt}

\item {\color{blue} Unstable:} \(r : E^k(-) \to E^l(-)\) of sets.
\hfill
\(\mathcal{U}_k^l\)
\end{itemize}

\pause

\[
\mathcal{S}^h \to \mathcal{A}_k^{k+h} \subseteq \mathcal{U}_k^{k+h}
\]
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<5>{\color{last}}Examples}}
\label<5>{exop}

\begin{itemize}
\item Coefficient operations on \(E^*(-)\): \(n (x) = n
x\); \pause

\item Multiplication operations on \(H^*(-)\): \(x \mapsto x^k\) \pause

\item Steenrod squares on \(H^*(-;\F_2)\). \pause

\item Bott periodicity in K--theory: \(\beta : K^{k+2}(X)
\xrightarrow{\cong} K^k(X)\); \pause

\item Adams operations in K--theory: for \(k \in \Z\), \(\Psi^k :
K^0(X) \to K^0(X)\).

\(\Psi^k(L) = L^{\otimes k}\), \(\Psi^k(V \oplus W) = \Psi^k(V) \oplus
\Psi^k(W)\).
\end{itemize}
\vfill
\end{frame}

\againframe<3>{qns}

\begin{frame}
\frametitle{{\only<2>{\color{last}}Looping}}
\label<2>{loop}

Consider an unstable operation:
%
\[
  r : E^k(-) \to E^l(-)
\]

\pause

Define a new operation:
%
\[
  \Omega r : E^{k-1}(-) \to E^{l-1}(-)
\]
%
by:
%
\[
  (\Omega r)_X : E^{k-1}(X) \cong E^k(\Sigma X) \xrightarrow{r_{\Sigma
      X}} E^l(\Sigma X) \cong E^{l-1}(X)
\]
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<6>{\color{last}}Looping}}
\label<6>{loopprop}

\begin{proposition}
\begin{enumerate}
\item {\color{math}\(\Omega r\)} is an unstable (additive) operation;

\pause

\item If {\color{math}\(r\)} is the \(k\)th component of a stable operation, \\
{\color{math}\((-1)^{l-k} \Omega r\)} is the \((k-1)\)th component.
\end{enumerate}
\end{proposition}

\pause

\alert<3>{Lower} components are easy.

\pause

\alert<4>{Higher} components are the hard part.

\pause

That is, to \alert<5>{deloop} the operation \(r\).

\pause

Mild help: often have a uniqueness theorem.
\vfill
\end{frame}

%
% This is one of the more complicated slides.  This has an xypic
% diagram with elements revealed piece-by-piece.  Unfortunately, an xy
% diagram doesn't work well with the \uncover command so one has to use
% the \only version.  This means that the diagram jumps around as more
% bits are revealed.  The solution that I found was to use pitprops
% and their horizontal versions to ensure that the diagram remained
% where it was put.  Essentially, the pitprops were just big enough
% that any new bits did not require any reformating of the diagram.
% Try making all the '0pt's to '1pt's in the arguments of the \rule
% commands in the diagram.
%


\begin{frame}
\frametitle{{\only<7>{\color{last}}Example: K--theory}}
\label<7>{exk}

K--theory: \uncover<4->{\(2\)--periodic.}

\pause

\[
  \xymatrix{
    K^{-2}(X) \only<3->{\ar[d]^{\Omega^2 r}} &
%
    K^{-1}(X) \only<3->{\ar[d]^{\Omega r}} &
%
    K^0(X) \ar[d]^{r} &
%
    K^1(X) \only<6->{\ar[d]^{\Omega (\beta^{-1} r \beta)}} &
%
    K^2(X)
    \ar@{}[d]^{\rule{25pt}{0pt}}
    \ar@{}[ll]_{\rule{0pt}{30pt}}
    \only<5->{\ar[d]^{\beta^{-1} r \beta}}
    \only<4->{\ar@(ul,ur)[ll]_{\beta}} \\
%
    K^{-2}(X) &
%
    K^{-1}(X) &
%
    K^0(X)
    \ar@{}[rr]_{\rule{0pt}{30pt}}
    \only<4->{\ar@(dr,dl)[rr]_{\beta^{-1}}} &
%
    K^1(X) &
%
    K^2(X)
%
}
\]

\uncover<7->{
\[
\text{Question: }  r = \Omega^2(\beta^{-1} r \beta) ?
\]
}

\vfill
\end{frame}



\begin{frame}
\frametitle{{\only<5>{\color{last}}Adams Operations}}
\label<5>{exadam}

\[
  \Omega^2(\beta^{-1} \Psi^k \beta) = k \Psi^k
\]

\pause

\[
  \xymatrix{
    K^{-2}(X) \only<3->{\ar[d]^{k \Psi^k}} &
%
    K^0(X) \ar[d]^{\Psi^k} &
%
    K^2(X)
    \ar@{}[d]^{\rule{18pt}{0pt}}
    \only<4->{\ar[d]^{\frac1k \Psi^k}} \\
%
    K^{-2}(X) &
%
    K^0(X) &
%
    K^2(X)
%
}
\]

\uncover<5->{
\(\frac1k \Psi^k\) not an operation on \(K^0(-)\) \\
%
(unless \(k = 1\) or \(k = -1\))
}

\vfill

\end{frame}

\begin{frame}
\frametitle{{\only<4>{\color{last}}Coefficients}}
\label<4>{coeff}

How to divide by \(k\): introduce coefficients.

\(R\) a commutative, unital ring\\
%
\(K(-;R)\) K--theory with coefficients in \(R\).

\pause

\begin{examples}
\begin{enumerate}
\item \(R = \Q\)\pause, but \(K^*(-;\Q) \cong H^\pm(-; \Q)\)
\pause

\item \(R = \Z_{(p)}\) retains \(p\)--typical information

\(\Psi^k\) is stable if \(p \not\mid k\)\\
 (see work of Clarke, Crossley, and Whitehouse)

\end{enumerate}
\end{examples}
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<6>{\color{last}}Mod \(p\)}}
\label<6>{modp}

\alert{Warning:} \(K(X; \F_p) \ne K(X)/(p)\).

\pause

\[
p = 3, \; k = 11
\]

\[
  \xymatrix{
    K^0(X;\F_p) \ar[d]^{\Psi^{11}} &
%
    K^2(X;\F_p) \only<3->{\ar[d]^{\frac1{11} \Psi^{11} \only<4->{=2
          \Psi^{11}}}} &
%
    K^4(X;\F_p) \ar@{}[d]^{\rule{45pt}{0pt}}
    \only<5->{\ar[d]^{\frac2{11} \Psi^{11}
        \only<6->{=\Psi^{11}}}} \\
%
    K^0(X;\F_p) &
%
    K^2(X;\F_p) &
%
    K^4(X;\F_p)
  }
\]
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<5>{\color{last}}Answers}}
\label<5>{ans}

\(\Psi^{11}\) repeats with period \(4 \pause = 2(3 - 1)\)

\pause

In \(K^*(-; \F_p)\), for \(p \not\mid k\), \(\Psi^k\)
  repeats with period \(2(p-1)\) (Fermat)

\pause

\begin{proposition}
In \(K^*(-; \F_p)\):
 \begin{enumerate}
\item {\color{math}\(\Psi^k\)} is stable if and only if {\color{math}\(p \not\mid k\)};
\pause
\item If {\color{math}\(\Psi^k\)} is stable the (even) components are blocks of:
%
\[
    (\Psi^k, k^{p-2} \Psi^k, k^{p-3} \Psi^k, k^{p-4} \Psi^k, \dotsc,
    k\Psi^k).
\]
 \end{enumerate}
\end{proposition}
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<2>{\color{last}}All Operations}}
\label<2>{allop}

\begin{theorem}[S -- Whitehouse]
The components of a stable operation on \(K^*(-;\F_p)\) repeat with
periodicity \(2(p-1)\).
\end{theorem}

\pause

\begin{corollary}
If {\color{math}\(\Omega^{2(p-1)}(\beta^{-(p-1)} r \beta^{p-1}) = r\)}
then {\color{math}\(r\)} is a component of a stable operation.
\end{corollary}
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<5>{\color{last}}Reconstruction}}
\label<5>{recon}

Start with a component of a stable operation.


\[
  \xymatrix{
    \only<3->{K^i(X;\F_p)} \only<4->{\ar[d]^{\Omega^j r_k}} &
%
    K^k(X;\F_p) \ar[d]^{r_k} &
%
    \only<2->{K^l(X;\F_p)} \ar@{}[ll]_{\rule{0pt}{30pt}} \only<3->{\ar@(ul,ur)[ll]_{\beta^{m(p-1)}}}
    \only<2->{\ar[d]_{r_l }^{\only<5->{=\beta^{-m(p-1)}(\Omega^j r_k) \beta^{m(p-1)}}}}
    \ar@{}[d]^{\rule{100pt}{0pt}} \\
%
    \only<3->{K^{i+h}(X;\F_p)} \ar@{}[rr]_{\rule{0pt}{30pt}}
    \only<3->{\ar@(dr,dl)[rr]_{\beta^{-m(p-1)}}} &
%
    K^{k+h}(X;\F_p) &
%
    \only<2->{K^{l+h}(X;\F_p)} \\
%
    \rule{70pt}{0pt} &
%
    \rule{70pt}{0pt} &
%
    \rule{70pt}{0pt}
  }
\]
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<3>{\color{last}}Recognition Improvement}}
\label<3>{recog}
\vfill

\begin{corollary}
If {\color{math}\(\Omega^{2(p-1)}(\beta^{-(p-1)} r \beta^{p-1}) = r\)}
then {\color{math}\(r\)} is a component of a stable operation.
\end{corollary}

\pause
\vfill

\begin{theorem}[S -- Whitehouse]
Let {\color{math}\(r\)} be an unstable operation on \(K^*(-;\F_p)\).
Then {\color{math}\(r\)} is a component of a stable operation if (and
only if) there is an unstable operation {\color{math}\(s\)} with
{\color{math}\(r = \Omega s\)}.
\end{theorem}

\pause
\vfill

That is, if \(r\) deloops \alert{once} then it deloops \alert{as many
  times as we like}.

\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<4>{\color{last}}Morava K--theories}}
\label<4>{morava}

For each prime \(p\), a sequence of cohomology theories
\(\{K(n)^*(-)\}\) -- the
{\color{red}chr}{\color{orange}oma}{\color{yellow}tic}{\color{green}\ fi}{\color{blue}ltr}{\color{purple}ati}{\color{violet}on.}

\pause

\begin{itemize}
\item \(K(0)^*(-) = H^*(-;\Q)\) \pause
\item \(K(1)^*(-)\) summand of \(K^*(-;\F_p)\) \pause
\item \(K(n)^*(-)\):
%
\begin{itemize}
\item is periodic, period \(2(p^n-1)\)
\item has coefficients \(\F_p[v_n, {v_n}^{-1}]\), \(\lvert v_n \rvert
= -2(p^n-1)\)
\item has K\"unneth formula and duality
\end{itemize}
\end{itemize}
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<2>{\color{last}}Recognition and Reconstruction}}
\label<2>{recrec}

\begin{theorem}[S -- Whitehouse]
\begin{enumerate}
\item The components of a stable operation in \(K(n)^*(-)\) repeat
with periodicity \(2(p^n-1)\);

\pause

\item If {\color{math}\(r\)} is an unstable operation such that there
is another unstable operation {\color{math}\(s\)} with
{\color{math}\(r = \Omega s\)} then {\color{math}\(r\)} is a component
of a (unique) stable operation.
\end{enumerate}
\end{theorem}
\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<3>{\color{last}}Notes}}
\label<3>{notes}

\vfill

\begin{enumerate}
\item The periodicity has changed to reflect the periodicity of the
cohomology theory. \pause

\vfill

\item The periodicity is always that of the cohomology theory.

(Compare with \(K^*(-;\F_p)\))
 \pause
\vfill

\item The ``delooping'' condition has not changed: if we can deloop
\alert{once} we can deloop as many times as we like.
\end{enumerate}

\vfill
\end{frame}

\begin{frame}
\frametitle{{\only<4>{\color{last}}Remarks}}
\label<4>{remarks}

\begin{enumerate}
\item Projection \(P : \mathcal{U}_k^l \to \mathcal{U}_k^l\) via:
%
\[
  P r = \Omega^{2(p^n-1)} ({v_n}^{-1} r v_n)
\]
%
such that \(r\) is a component of a stable operation if and only if
\(r = P r\).

\pause

\item Closely linked to the Bousfield--Kuhn functor.

\pause

\item Reconstruction is easy using periodicity.

\pause

\item Proof is a straightforward analysis of the \(p\)--series of the
formal group law.
\end{enumerate}
\vfill
\end{frame}


\againframe<4->{qns}

\begin{frame}
\frametitle{Navigation}

\begin{columns}
\begin{column}{6cm}
\hyperlink{title}{\beamergotobutton{Title Page}}\\
\hyperlink{qnsorig}{\beamergotobutton{Questions}}\\
\hyperlink{prelim}{\beamergotobutton{Preliminaries}}\\
\hyperlink{forget}{\beamergotobutton{Forgetfulness}}\\
\hyperlink{nat}{\beamergotobutton{Operations (natural transformations)}}\\
\hyperlink{ops}{\beamergotobutton{Operations}}\\
\hyperlink{exop}{\beamergotobutton{Examples of Operations}}\\
\hyperlink{qnsreprise}{\beamergotobutton{Questions (reprise)}}\\
\hyperlink{loop}{\beamergotobutton{Looping an Operation}}\\
\hyperlink{loopprop}{\beamergotobutton{Properties of Looping}}\\
\hyperlink{exk}{\beamergotobutton{Example: K--theory}}\\
\hyperlink{exadam}{\beamergotobutton{Example: Adams Operations}}
\end{column}
\begin{column}{6cm}
\hyperlink{coeff}{\beamergotobutton{Coefficients}}\\
\hyperlink{modp}{\beamergotobutton{Mod \(p\)}}\\
\hyperlink{ans}{\beamergotobutton{Answers (Adams Operations)}}\\
\hyperlink{allop}{\beamergotobutton{All Operations}}\\
\hyperlink{recon}{\beamergotobutton{Reconstruction}}\\
\hyperlink{recog}{\beamergotobutton{Recognition}}\\
\hyperlink{morava}{\beamergotobutton{Morava K--theories}}\\
\hyperlink{recrec}{\beamergotobutton{Reconstruction and Recognition}}\\
\hyperlink{notes}{\beamergotobutton{Notes}}\\
\hyperlink{remarks}{\beamergotobutton{Remarks}}\\
\hyperlink{qnsconclude}{\beamergotobutton{Questions (conclusion)}}
\end{column}
\end{columns}


\vfill
\end{frame}

\end{document}

%
% This bibilography didn't appear in the final presentation, but I
% would have included it in any handout or online version.  I created
% it by doing a normal bibliography and then including the .bbl file
% and manually formating it to fit in the frames.
%
% The original frame was thus:
%
%\begin{frame}
%\frametitle{Further Reading}
%
%\nocite{math.AT/0605471,jb4,jbdjww,ww,tknspt,drww,nk2,ab2,fcmcsw,fcmcsw2}
%
%
%\bibliography{arxiv,articles,books,misc}
%\end{frame}
%

\begin{frame}
\frametitle{Further Reading}

{\tiny

\begin{thebibliography}{CCW05}

\bibitem[BJW95]{jbdjww}
J.~Michael Boardman, David~Copeland Johnson, and W.~Stephen Wilson.
\newblock Unstable operations in generalized cohomology.
\newblock In {\em Handbook of algebraic topology}, pages 687--828.
  North-Holland, Amsterdam, 1995.

\bibitem[Boa95]{jb4}
J.~Michael Boardman.
\newblock Stable operations in generalized cohomology.
\newblock In {\em Handbook of algebraic topology}, pages 585--686.
  North-Holland, Amsterdam, 1995.

\bibitem[Bou87]{ab2}
A.~K. Bousfield.
\newblock Uniqueness of infinite deloopings for {$K$}-theoretic spaces.
\newblock {\em Pacific J. Math.}, 129(1):1--31, 1987.

\bibitem[CCW01]{fcmcsw2}
Francis Clarke, M.~D. Crossley, and Sarah Whitehouse.
\newblock Bases for cooperations in {$K$}-theory.
\newblock {\em $K$-Theory}, 23(3):237--250, 2001.

\bibitem[CCW05]{fcmcsw}
Francis Clarke, Martin Crossley, and Sarah Whitehouse.
\newblock Algebras of operations in {$K$}-theory.
\newblock {\em Topology}, 44(1):151--174, 2005.
\end{thebibliography}
}
\end{frame}

\begin{frame}
\frametitle{Further Reading}

{\tiny


\begin{thebibliography}{CCW05}

\bibitem[KST96]{tknspt}
Takuji Kashiwabara, Neil Strickland, and Paul Turner.
\newblock The {M}orava {$K$}-theory {H}opf ring for {$BP$}.
\newblock In {\em Algebraic topology: new trends in localization and
  periodicity (Sant Feliu de Gu\'\i xols, 1994)}, volume 136 of {\em Progr.
  Math.}, pages 209--222. Birkh\"auser, Basel, 1996.

\bibitem[Kuh89]{nk2}
Nicholas~J. Kuhn.
\newblock Morava {$K$}-theories and infinite loop spaces.
\newblock In {\em Algebraic topology (Arcata, CA, 1986)}, volume 1370 of {\em
  Lecture Notes in Math.}, pages 243--257. Springer, Berlin, 1989.

\bibitem[RW77]{drww}
Douglas~C. Ravenel and W.~Stephen Wilson.
\newblock The {H}opf ring for complex cobordism.
\newblock {\em J. Pure Appl. Algebra}, 9(3):241--280, 1976/77.

\bibitem[SW]{math.AT/0605471}
Andrew Stacey and Sarah Whitehouse.
\newblock {Stable and Unstable Operations in mod p Cohomology Theories},
  arXiv:math.AT/0605471.

\bibitem[Wil84]{ww}
W.~Stephen Wilson.
\newblock The {H}opf ring for {M}orava {$K$}-theory.
\newblock {\em Publ. Res. Inst. Math. Sci.}, 20(5):1025--1036, 1984.

\end{thebibliography}
}
\end{frame}
\end{document}



