Mentioned “incompatibility” with linear distributivity and compact closure, in the sense that combining them forces the category to be thin.

]]>Explicitly relate to coproduct preservation, remark that all biCCC are distributive

]]>Added to related concepts, completely distributive category and totally distributive category.

]]>Recorded facts about free distributive categories from Cockett 1993, following Heindel’s question on CT Zulip.

]]>Add redirect for distributive coproduct

]]>Added a missing assumption. In order for an extensive category to be distributed it needs to have finite products.

Tomas Jakl

]]>Re #22, oh, I see I didn’t put the link in properly in #19 to Sam Staton’s comment.

]]>If I recall correctly, when $E=2$ then the algebras are precisely the rectangular bands.

There should probably also be some disambiguation to the band of a gerbe.

]]>Thanks, Yemon. As per the other thread (here), now both *band* and *rectangular band* point to the same entry, containing essentially the material you provided. Any further disambiguation can be written there. Or if the entries should be split, in two (or more) please do (or let me know if I should do it).

Okay, so I made *rectangular band* a hyperlink. Will create an annoyingly empty stub for it now, hoping to prompt you to add some content…

They are definitely worth an entry. A look at the old catlist-dicussion shows that they pop up as example for a lot of different things like affine theories, collapsed toposes, in Barr’s “point of the empty set”-paper, they also share the associativity-for-free-property with graphic monoids. For the terminology I don’t know, I used the name suggested by Peter Johnstone there and apparently taken from semigroup theory.

]]>rectangular bands

They cropped up before as algebras for some version of the reader monad.

]]>Thanks!!

Should we make a page for your example of “rectangular bands”? I had never heard of these before.

Just on formatting: Where you had

```
$xx= x$ for all $x\in X$ and $xyx=x$
```

I have inserted whitespace

```
$x x = x$ for all $x\in X$ and $x y x=x$
```

because otherwise Instiki renders the products as variable names typeset in mathrm

]]>Added further examples and non-examples.

]]>I have added (here) the (small) list of examples as grabbed form *rig category*.

But really some counter-examples should be mentioned…

]]>It seems somewhat strange that Heyting algebra and co-Heyting algebra don’t mention

infinite distributionor give formulas for the exponentials.

Actually, Heyting algebra does both. Look carefully here.

]]>Re #12: it looks fine, except that if it were me, I’d be more inclined to put this mostly at frame, with a quick mention and link from distributive lattice. Definitely the calculation of the exponential would improve the article frame, which at present contents itself with a quick glossing mention of adjoint functor theorem.

However, it doesn’t make sense to say those two exponentials agree, not even in the Boolean case. For example $u \backslash 0 = u$, whereas $u \Rightarrow 0$ is the negation of $u$. The variance is also off: $u \Rightarrow v$ is contravariant in $u$ and covariant in $v$; it’s the other way around for $u \backslash v$. In the Boolean case, we actually have $u \Rightarrow 0 = 1 \backslash u$.

]]>For future reference, there is no need to copy on the forum the text added – anyone can follow the link and see it for themselves.

]]>i added to distributive lattice the following section and modified the finite distributive section to note that such lattices are bi-Heyting. I probably made some minor errors or may be even wronger.

I haven’t modified or cross linked any of the related pages: Heyting algebra, co-Heyting algebra, frame, locale, completely distributive lattice.

It seems somewhat strange that Heyting algebra and co-Heyting algebra don’t mention **infinite distribution** or give formulas for the exponentials.

A distributive lattice that is complete (not necessarily completely distributive) may be **infinitely distributive** or said to satisfiy the **infinite distributive law** :

This property is sufficient to give the lattice Heyting algebra stucture where the implication $a\Rightarrow b$ (or exponential object $b^a$) is:

$(u \Rightarrow v) = \bigvee_{x \wedge u \leq v} x$Note that this property does not imply the dual **co-infinitely distributive** property:

Instead this dual gives the lattice co-Heyting structure where the co-implication or “subtraction” ($\backslash$) is

$(u \backslash v) = \bigwedge_{u \leq v \vee x} x$If a lattice has both properties, as in a completely distributive lattice, then it has bi-Heyting structure (both Heyting and co-Heyting) and the two exponentials are equal.

$(u \Rightarrow v) = \bigvee_{x \wedge u \leq v} x \qquad = \qquad (u \backslash v) = \bigwedge_{u \leq v \vee x} x$]]>

Thanks for the pointer. I wonder whether the forbidden sublattices and pinwheels can be seen as cases of the forbidden minor theorem?

]]>I don’t know that we have such a page; it’s certainly worth considering. There is however a major theorem in graph theory, the graph minor theorem of Robertson and Seymour, that says that for any class $C$ of finite graphs that is closed under taking graph minors, there is a finite collection of “forbidden graphs” that cannot appear as a minor of any element of $C$. The best known special case might be Kruskal’s theorem, on the class of finite forests, where the triangle $K_3$ is the forbidden graph. We have a smidgen about this in the nLab, here.

]]>Do we have a page about “forbidden subobjects”? In addition to Birkhoff’s sublattices blocking distributivity, and the classical $K_{5}$ and $K_{3,3}$ blocking planarity of a graph, there is the “pinwheel configuration” that blocks composability of a brick diagram in a double category; and what others?

]]>Neat; thanks!

]]>