Chapter 17 - It’s All About Morphisms

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\begin{quote}
This is part 17 of Categories for Programmers. Previously:
\href{https://bartoszmilewski.com/2015/10/28/yoneda-embedding/}{Yoneda
Embedding}. See the
\href{https://bartoszmilewski.com/2014/10/28/category-theory-for-programmers-the-preface/}{Table
of Contents}.
\end{quote}
If I haven't convinced you yet that category theory is all about
\lettrine[lhang=0.17]{I}{f I haven't} convinced you yet that category theory is all about
morphisms then I haven't done my job properly. Since the next topic is
adjunctions, which are defined in terms of isomorphisms of hom-sets, it
makes sense to review our intuitions about the building blocks of
@ -38,13 +30,16 @@ constructions (with the notable exceptions of the initial and terminal
objects). We've seen this in the definitions of products, coproducts,
various other (co-)limits, exponential objects, free monoids, etc.
\begin{wrapfigure}[9]{R}{0pt}
\raisebox{0pt}[\dimexpr\height-0.75\baselineskip\relax]{
\fbox{\includegraphics[width=1.78125in]{images/productranking.jpg}}}%
\end{wrapfigure}
The product is a simple example of a universal construction. We pick two
objects \code{a} and \code{b} and see if there exists an object
\code{c}, together with a pair of morphisms \code{p} and \code{q},
that has the universal property of being their product.
\includegraphics[width=1.78125in]{images/productranking.jpg}
A product is a special case of a limit. A limit is defined in terms of
cones. A general cone is built from commuting diagrams. Commutativity of
those diagrams may be replaced with a suitable naturality condition for
@ -60,8 +55,12 @@ naturality square are the mappings of some morphism \code{f} under two
functors \code{F} and \code{G}. The other sides are the components
of the natural transformation (which are also morphisms).
\begin{figure}[H]
\centering
\includegraphics[width=2.25000in]{images/3_naturality.jpg}
\end{figure}
\noindent
Naturality means that when you move to the ``neighboring'' component (by
neighboring I mean connected by a morphism), you're not going against
the structure of either the category or the functors. It doesn't matter
@ -74,8 +73,12 @@ you up and down or back and forth --- so to speak. You can visualize the
transformation maps one such sheet corresponding to F, to another,
corresponding to G.
\includegraphics{images/sheets.png}
\begin{wrapfigure}[10]{R}{0pt}
\raisebox{0pt}[\dimexpr\height-0.75\baselineskip\relax]{
\includegraphics[width=60mm]{images/sheets.png}}%
\end{wrapfigure}
\noindent
We've seen examples of this orthogonality in Haskell. There the action
of a functor modifies the content of a container without changing its
shape, while a natural transformation repackages the untouched contents
@ -89,21 +92,19 @@ cones. These mappings must also satisfy commutativity conditions. (For
instance, the triangles in the definition of the product must commute.)
These conditions, too, may be replaced by naturality. You may recall
that the \newterm{universal} cone, or the limit, is defined as a natural
that the \emph{universal} cone, or the limit, is defined as a natural
transformation between the (contravariant) hom-functor:
\begin{verbatim}
F :: c -> C(c, Lim D)
\end{verbatim}
and the (also contravariant) functor that maps objects in \emph{C} to
cones, which themselves are natural transformations:
\begin{verbatim}
G :: c -> Nat(Δc, D)
\end{verbatim}
Here, \code{Δc} is the constant functor, and \code{D} is the functor
\begin{Verbatim}[commandchars=\\\{\}]
G :: c -> Nat(\ensuremath{\Delta}\textsubscript{c}, D)
\end{Verbatim}
Here, \code{\ensuremath{\Delta}\textsubscript{c}} is the constant functor, and \code{D} is the functor
that defines the diagram in \emph{C}. Both functors \code{F} and
\code{G} have well defined actions on morphisms in \emph{C}. It so
happens that this particular natural transformation between \code{F}
@ -133,9 +134,8 @@ there is a morphism \code{h} whose composition (either pre- or post-)
with \code{f} is different than that with \code{g}, for instance:
\begin{verbatim}
h ∘ f ≠ h ∘ g
h ◦ f ≠ h ◦ g
\end{verbatim}
then we can directly ``observe'' the difference between \code{f} and
\code{g}. But even if the difference is not directly observable, we
might use functors to zoom in on the hom-set. A functor \code{F} may
@ -144,15 +144,13 @@ map the two morphisms to distinct morphisms:
\begin{verbatim}
F f ≠ F g
\end{verbatim}
in a richer category, where the abutting hom-sets provide more
resolution, e.g.,
\begin{verbatim}
h' ∘ F f ≠ h' ∘ F g
h' ◦ F f ≠ h' ◦ F g
\end{verbatim}
where \code{h\'} is not in the image of \code{F}.
where \code{h'} is not in the image of \code{F}.
\section{Hom-Set Isomorphisms}\label{hom-set-isomorphisms}
@ -184,10 +182,9 @@ between hom-sets.
The definition of a limit is also a natural isomorphism between hom-sets
(the second one, again, in the functor category):
\begin{verbatim}
C(c, Lim D) ≃ Nat(Δc, D)
\end{verbatim}
\begin{Verbatim}[commandchars=\\\{\}]
C(c, Lim D) \ensuremath{\simeq} Nat(\ensuremath{\Delta}\textsubscript{c}, D)
\end{Verbatim}
It turns out that our construction of an exponential object, or that of
a free monoid, can also be rewritten as a natural isomorphism between
hom-sets.
@ -199,16 +196,16 @@ hom-sets.
\section{Asymmetry of Hom-Sets}\label{asymmetry-of-hom-sets}
There is one more observation that will help us understand adjunctions.
Hom-sets are, in general, not symmetric. A hom-set \code{C(a,\ b)} is
often very different from the hom-set \code{C(b,\ a)}. The ultimate
Hom-sets are, in general, not symmetric. A hom-set \code{C(a, b)} is
often very different from the hom-set \code{C(b, a)}. The ultimate
demonstration of this asymmetry is a partial order viewed as a category.
In a partial order, a morphism from \code{a} to \code{b} exists if
and only if \code{a} is less than or equal to \code{b}. If
\code{a} and \code{b} are different, then there can be no morphism
going the other way, from \code{b} to \code{a}. So if the hom-set
\code{C(a,\ b)} is non-empty, which in this case means it's a
singleton set, then \code{C(b,\ a)} must be empty, unless
\code{a\ =\ b}. The arrows in this category have a definite flow in
\code{C(a, b)} is non-empty, which in this case means it's a
singleton set, then \code{C(b, a)} must be empty, unless
\code{a = b}. The arrows in this category have a definite flow in
one direction.
A preorder, which is based on a relation that's not necessarily
@ -227,20 +224,10 @@ empty. We can visualize a general category as a ``thick'' preorder.
Consider some degenerate cases of a naturality condition and draw the
appropriate diagrams. For instance, what happens if either functor
\code{F} or \code{G} map both objects \code{a} and \code{b}
(the ends of \code{f\ ::\ a\ ->\ b}) to the same
object, e.g., \code{F\ a\ =\ F\ b} or \code{G\ a\ =\ G\ b}?
(the ends of\\ \code{f :: a -> b}) to the same
object, e.g., \code{F a = F b} or \code{G a = G b}?
(Notice that you get a cone or a co-cone this way.) Then consider
cases where either \code{F\ a\ =\ G\ a} or \code{F\ b\ =\ G\ b}.
cases where either \code{F a = G a} or \code{F b = G b}.
Finally, what if you start with a morphism that loops on itself ---
\code{f\ ::\ a\ ->\ a}?
\code{f :: a -> a}?
\end{enumerate}
Next:
\href{https://bartoszmilewski.com/2016/04/18/adjunctions/}{Adjunctions}.
\section{Acknowledgments}\label{acknowledgments}
I'd like to thank Gershom Bazerman for checking my math and logic, and
André van Meulebrouck, who has been volunteering his editing help
throughout this series of posts.\\
\href{https://twitter.com/BartoszMilewski}{Follow @BartoszMilewski}

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@ -117,6 +117,13 @@ PDF compiled by @url{https://github.com/hmemcpy/milewski-ctfp-pdf, Igal Tabachni
\chapter{Natural Transformations}
\subfile{content/1.10/Natural Transformations}
\part{Part Two}
\part{Part Three}
\chapter{It's All About Morphisms}
\subfile{content/3.1/It's All About Morphisms}
\backmatter
@unnumbered Acknowledgments