Talk:PlanetPhysics/Alternative Definition of Category

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%%% This file is part of PlanetPhysics snapshot of 2011-09-01 %%% Primary Title: alternative definition of category %%% Primary Category Code: 00. %%% Filename: AlternativeDefinitionOfCategory.tex %%% Version: 2 %%% Owner: rspuzio %%% Author(s): bci1, rspuzio %%% PlanetPhysics is released under the GNU Free Documentation License. %%% You should have received a file called fdl.txt along with this file. %%% If not, please write to gnu@gnu.org. \documentclass[12pt]{article} \pagestyle{empty} \setlength{\paperwidth}{8.5in} \setlength{\paperheight}{11in}

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The notion of \htmladdnormallink{category}{http://planetphysics.us/encyclopedia/Cod.html} may be defined in a form which only

involves \htmladdnormallink{morphisms}{http://planetphysics.us/encyclopedia/TrivialGroupoid.html} and does not mention \htmladdnormallink{objects}{http://planetphysics.us/encyclopedia/TrivialGroupoid.html}. This definition shows that categories are a generalization of \htmladdnormallink{semigroups}{http://planetphysics.us/encyclopedia/TrivialGroupoid.html} in which the closure axiom has been weakened; rather than requiring that the product of two arbitrary elements of the \htmladdnormallink{system}{http://planetphysics.us/encyclopedia/SimilarityAndAnalogousSystemsDynamicAdjointnessAndTopologicalEquivalence.html} be defined as an element of the system, we only require the product to be defined in certain cases.

We define a \emph{category} to be a set \footnote{ For simplicity, we will only consider \htmladdnormallink{small categories}{http://planetphysics.us/encyclopedia/Cod.html} here, avoiding logical complications related to proper classes.} $M$ (whose elements we shall term \emph{morphisms}) and a \htmladdnormallink{function}{http://planetphysics.us/encyclopedia/Bijective.html} $\circ$ (which we shall term \emph{\htmladdnormallink{composition}{http://planetphysics.us/encyclopedia/Cod.html}}) from a subset $D$ of $M \times M$ to $M$ which satisfies the following properties: \begin{itemize} \item{\bf 1.} If $a,b,c,d$ are elements of $M$ such that $(a,c) \in D$ and $(a,d) \in D$ and $(b,c) \in D$, then $(b,d) \in D$. \item{\bf 2} If $a,b,c$ are elements of $M$ such that $(a,b) \in D$ and $(b,c) \in D$, then $(a \circ b, c) \in D$ and $(a, b \circ c) \in D$ and $(a \circ b) \circ c = a \circ (b \circ c)$ \item{\bf 3a} For every $a \in M$, there exists an element $e \in M$ such that \begin{enumerate} \item $(e,e) \in D$ and $e \circ e = e$ \item $(a,e) \in D$ and $a \circ e = a$ \item For all $x \in M$ such that $(x,e) \in D$, we have $x \circ e = x$. \end{enumerate} \item{\bf 3a} For every $a \in M$, there exists an element $e \in M$ such that \begin{enumerate} \item $(e,e) \in D$ and $e \circ e = e$ \item $(e,a) \in D$ and $e \circ a = a$ \item For all $x \in M$ such that $(x,e) \in D$, we have $e \circ a = x$. \end{enumerate} \end{itemize} This definition may also be stated in terms of \htmladdnormallink{predicate}{http://planetphysics.us/encyclopedia/Predicate.html} calculus. Defining the three place predicate $P$ by $P(a,b,c)$ if and only if $(a,b) \in D$ and $a \circ b = c$, our axioms look as follows: \begin{itemize} \item{\bf 0.} $(\forall a,b,c,d) ~ P(a,b,c) \land P(a,b,d) \Rightarrow c = d$. \item{\bf 1.} $(\forall a,b,c,d) ~ ((\exists e)~P(a,c,e)) \land ((\exists e)~P(a,d,e)) \land ((\exists e)~P(b,c,e))z \Rightarrow ((\exists e)~P(b,d,e))$ \item{\bf 2.} $(\forall a,b,c,d,e) ~ P(a,b,d) \land P(b,c,e) \Rightarrow (\exists f) ~ P(d,c,f) \land P(a,e,f)$ \item{\bf 3a.} $(\forall a) (\exists b) ~ P(b,b,b) \land P(b,a,a) \land ((\forall c,d) ~ P(b,c,d) \Rightarrow c = d)$ \item{\bf 3b.} $(\forall a) (\exists b) ~ P(b,b,b) \land P(a,b,a) \land ((\forall c,d) ~ P(c,b,d) \Rightarrow c = d)$ \end{itemize}

That a category defined in the usual way satisfies these properties is easily enough established. Given two morphisms $f$ and $g$, the composition $f \circ g$ is only defined if $f \in {\rm Hom} (B,C)$ and $g \in {\rm Hom} (A,B)$ for suitable objects $A,B,C$, i.e if the final object of $f$ equals the initial object of $g$. The three hypotheses of axiom 1 state that the initial object of $a$ equals the final objects of $c$ and $d$ and that the initial object of $b$ also equals the final object of $c$; hence the initial object of $b$ equals the final object of $d$ so we may compose $b$ with $d$. Axiom 2 states associativity of composition whilst axioms 3a and 3b follow from existence of \htmladdnormallink{identity}{http://planetphysics.us/encyclopedia/Cod.html} elements.

To show that the new definition implies the old one is not so easy because we must first recover the objects of the category somehow. The observation which makes this possible is that to each object $A$ we may associate two sets: the set ${\bf L}$ of morphisms which have $A$ as initial object, ${\bf L} = \cup_{B \in {\rm Ob}} {\rm Hom} (A,B)$, and the set ${\bf R}$ of morphisms which have $A$ as final object, ${\bf R} = \cup_{B \in {\rm Ob}} {\rm Hom} (B,A)$. Moreover, this pair of sets $({\bf L},{\bf R})$ determines $A$ uniquely. In order for this observation to be useful for our purposes, we must somehow characterize these pairs of sets without reference to objects, which may be done by the further observation that, if we have two sets ${\bf L}$ and ${\bf R}$ of morphisms such that $x \in {\bf L}$ if and only if $x \circ y$ is defined for all $y \in {\bf R}$ and $x \in {\bf R}$ if and only if $y \circ x$ is defined for all $y \in {\bf L}$, then there exists an object $A$ which gives rise to ${\bf L}$ and ${\bf R}$ as above. This fact may be demonstrated easily enough from the usual definition of category. We will now reverse the procedure, using our axioms to show that such pairs behave as objects should, justifying defining objects as such pairs.

Returning to our new definition, let us now define $\ell \colon M \to {\cal P} (M)$, $r \colon m \to {\cal P} (M)$, ${\cal L} \subseteq {\cal P} (M)$, and ${\cal R} \subseteq {\cal P} (M)$ as follows: \begin{align*} \ell (a) &= \{ b \in M \mid (b,a) \in D \} \\ r (a) &= \{ b \in M \mid (a,b) \in D \} \\ {\cal L} &= \{ \ell (a) \mid a \in M \} \\ {\cal R} &= \{ r (a) \mid a \in M \} \end{align*}

We now show that, if $U,V \in {\cal L}$ then either $U \cap V = \emptyset$ or $U = V$. Suppose that $U,V \in {\cal L}$ and $U \cap V \neq \emptyset$. Then there exists a morphism $a$ such that $a \in U$ and $a \in V$. By the definition of ${\cal L}$, there exist morphisms $b$ and $c$ such that $U = \ell (b)$ and $V = \ell (c)$. By definition of $\ell$, we have $(a,b) \in D$ and $(a,c) \in D$. If $d \in U$, then $(d,b) \in D$ so, by axiom 1, $(d,c) \in D$, i.e. $d \in \ell (c) = V$. Likewise, switching the roles of $U$ and $V$ we conclude that, if $d \in V$, then $d \in U$. Hence $U = V$.

Making an argument similar to that of last paragraph, but with $r$ instead of $\ell$ and ${\cal R}$ instead of ${\cal L}$, we also conclude that, if $U,V \in {\cal R}$ then either $U \cap V = \emptyset$ or $U = V$. Because of axiom 3a, we know that, for every $a \in M$, there exists $b \in M$ such that $a \in \ell (b)$ and, by axiom 3b, there exists $c \in M$ such that $a \in r (c)$. Hence, the sets ${\cal L}$ and ${\cal R}$ are each partitions of $M$.

Next, we show that, if $S \in {\cal L}$ and $a,b \in S$, then $r(a) = r(b)$. By definition, there exists a morphism $c$ such that $S = \ell (c)$, so $(a,c) \in D$ and $(b,c) \in D$. Now suppose that $d \in r(a)$. This means that $(a,d) \in D$. By axiom 1, we conclude that $(b,d) \in D$, so $d \in r(b)$. Likewise, switching the roles of $a$ and $b$ in the foregoing argument, we conclude that, if $d \in r(b)$, then $d \in r(a)$. Thus, $r(a) = r(b)$.

By a similar argument to that of the last paragraph, we may also show that, if $S \in {\cal R}$ and $a,b \in S$, then $\ell(a) = \ell(b)$. Taken together, these results tell us that there is a one-to-one correspondence between of ${\cal L}$ and ${\cal R}$ --- to each $S \in {\cal L}$, there exists exactly one $T \in {\cal R}$ such that $S \times T \in D$ and vice-versa. In light of this fact, we shall define and object of our category to be a pair $(P,Q)$ of subsets of $M$ such that $x \in P$ if and only if $(x,y) \in D$ for all $y \in Q$ and $y \in Q$ if and only if $(x,y) \in D$ for all $x \in Q$. Given two objects $A = (P,Q)$ and $B = (R,S)$, we define ${\rm Hom} (A,B) = P \cap S$. We now will verify that, with these definitions, our axioms reproduce the defining properties of the standard definition of category.

Suppose that $A = (P,Q)$ and $B = (R,S)$ and $C = (U,V)$ are objects according to the above definition and that $f \in {\rm Hom} (A,B)$ and $g \in {\rm Hom} (B,C)$. Then $f \in S$ and $g \in R$. By the way we defined our pairs, $(g,f) \in D$, so $g \circ f$ is defined. Let $h$ be any element of $Q$. Since $f \in P$, it follows that $(f,h) \in D$. Since $(g,f) \in D$ as well, it follows from axiom 2 that $(g \cdot f, h) \in D$, so $g \circ f\in P$. Let $k$ be any element of $U$. Since $g \in V$, it follows that $(k,g) \in D$. Since $(g,f) \in D$ as well, it follows from axiom 2 that $(k,g \circ f) \in D$, so $g \circ f \in V$. Hence, $g \circ f \in P \cap V = {\rm Hom} (A,C)$. Thus, $\circ$ is defined as a function from ${\rm Hom} (A,B) \times {\rm Hom} (B,C) \to {\rm Hom} (A,C)$.

Next, suppose that $A = (P,Q)$ and $B = (R,S)$ are distinct objects. By the properties described earlier, $P \cap R = \emptyset$ and $Q \cap S = \emptyset$. Let $E$ and $F$ be two objects. Since ${\rm Hom} (A,E) \subset P$ and ${\rm Hom} (B,F) \subset R$, it follows that ${\rm Hom} (A,E) \cap {\rm Hom} (B,F) = \emptyset$. Likewise, since ${\rm Hom} (E,A) \subset Q$ and ${\rm Hom} (F,B) \subset S$, it follows that ${\rm Hom} (E.A) \cap {\rm Hom} (F,B) = \emptyset$. Hence, it follows that, given four objects $A,B,E,F$, we have ${\rm Hom} (A,E) \cap {\rm Hom} (B,F) = \emptyset$ unless $A = B$ and $E = F$.

[more to come]

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