2.2.1 - Definition and first examples
Definition 2.2: A symmetric monoidal structure on a preoirder $(X, \leq)$ consists of
- (i) a monoidal unit, $I \in X$
- (ii) a monoidal product $\otimes: X \times X \rightarrow X$
And the monoidal product $\otimes(x_1,x_2) = x_1 \otimes x_2$ must also satisfy the following properties (assume all elements are in $X$)
- (a) $x_1 \leq y_1$ and $x_2 \leq y_2 \implies x_1 \otimes x_2 \leq y_1 \otimes y_2$
- (b) $I \otimes x = x \otimes I = x$
- (c) associativity
- (d) commutivity/symmetry
(a) is called monotnoicity and (b) is unitality
Remark 2.3: replacing $=$ with $\cong$ in definition 2.2 will give us a weak monoidal structure.
Exercise 2.5: The preorder structure $(\mathbb{R}, \leq)$ and the multiplication operation $\times$ will not give us a symmetric monoidal order because of the simple counter example of $-2 \times -2 \nleq 1 \times 1$.
Example 2.6: A monid is similar to a symmetric monoidal preorder in that it consists of a set $M$, a function $*: M\times M \rightarrow M$, and an elment $e \in M$ called the monid unit, such that for every $m,n,p \in M$,
- $m * e = m$
- $e * m = m$
- associativity holds
Further, if commutivity holds (which isn’t not generally true), then it is also called commutative
2.2.2 - Introducing wiring diagrams
⚠️ I am seeing the wiring diagrams, but I fail to understand why they are any different from the Hasse diagrams we’ve seen previously.
Essentially, wiring diagrams seem to be a way to encode information about symmetric monoidal structures. The basic rules built up so far are as follows:
- A wire without a label, or with the label of the monoidal unit, is equivalent to nothing
- Otherwise, a wire labeled with an element represents that element (⚠️ this could be wrong)
- Two parallel wires represent the monoidal product of those elements
- Placing a $\leq$ block between two $x,y$ wires indicates that $x \leq y$
Thinking back to the conditions for a symmetric monoidal structure, we find that
Transitivity allows us to combine wiring diagrams left to right
Monotonicity is represented as being able to combine wiring diagrams top to bottom
A monoidal product with a monoidal unit and another element gives us the element again, because the monoidal unit is equivalent to nothing (reflexivity)
Associativity means we can “wiggle” around parallel wires
Commutivity means we can cross wires
It is intuitive to see how these wiring diagrams can be used to prove statements. In fact, the above images are trivial proofs. Take a look at the following exercise
Exercise 2.20: Prove–given $t \leq v+w$, $w+u \leq x+z$, and $v+x \leq y$–that $t+u \leq y+z$.
ALgebraically, we proceed like so:
$$\begin{align} t + u &\leq (v+w) + u \\ &\leq v + (w+u) \\ &\leq v + (x+z) \\ &\leq (v + x) + z \\ &\leq y + z \\ \end{align}$$and the wiring diagram would look like
2.2.3 - Applied examples
While this section did solidify some concepts. It wasn’t too important. Although, it did carry two useful examples: discarding and splitting.
With discarding, if a symmetric monoidal structure also satisfies $x \leq I$ for every $x \in X$, then it is possible to terminate any wire:
And if instead have a property like $x \leq x + x$, then we can split any wire:
2.2.4 - Abstract examples
Again, after a skim through, this section did not seem critical.
2.2.5 - Monoidal montone maps
We begin with recalling that for any preorder $(X,\leq)$ we have an induced equivalence relation $\cong$ on $X$ where two elements $x \cong x' \iff x \leq x$ and $x' \leq x$
Definition 2.41: $\mathcal{P} = (P, \leq_P, I_P, \otimes_P)$ and $\mathcal{Q} = (Q, \leq_Q, I_Q, \otimes_Q)$ be monoidal preorders. A monoidal monotone from $\mathcal{P}$ to $\mathcal{Q}$ is a monotone map $f: (P, \leq_P) \rightarrow (Q, \leq_Q)$ which satisfies
- (a) $I_Q \leq_Q f(I_P)$
- (b) $f(p_1) \otimes_Q f(p_1 \otimes_P p_2)$ for all $p_1,p_2 \in P$.
Additionally, $f$ is a strong monoidal monotone if it satisfies
- (a’) $I_Q \cong f(I_P)$
- (b’) $f(p_1) \otimes_Q f(p_1 \otimes_P p_2) \cong f(p_1) \otimes_Q f(p_2)$ And it is called a strict monoidal monotone if it satisfies
- (a’’) $I_Q = f(I_P)$
- (b’’) $f(p_1) \otimes_Q f(p_1 \otimes_P p_2) = f(p_1) \otimes_Q f(p_2)$
Monoidal monotones are said to be examples of monoidal functors in category theory.
The exercises for this section seem a little easy, so I will be skipping them for now, returning to them if I get confused on the defnitions of monoidal monotones.