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Mathematicians often tell her this; hence the book.
If I had to summarise her views in one sentence, it would be:
Everything is an adjunction.
I also like the division these mathematicians are making to her: essentially, a theorem is anything that solves Feynman’s challenge: by a series of clear, unsurprising steps, one arrives at an unexpected conclusion.
surprising rep-theory consequences of Young diagrams, Ferrers sequences, and so on (you could say the strangeness of integer partitions is really to blame here…)
59 icosahedra
8 geometric layouts
Books which are bristling with mathematical ideas of this kind include Montesinos on tessellations, Geometry and the Imagination (the original one), and Coxeter’s book on polyhedra (start with Baez on A-D-E if you want to follow my path). Moonshine and anything by Thurston or his students, I’ve found similarly flush with shockng content—quite different to what I thought mathematics would be like. (I had pictured something more like a formal logic book: row by row of symbols. But instead, the deeper I got into mathematics, the fewer the symbols and the more the surnames thanking the person who came up with some good idea.)
Note that a theorem is different here to some geometry — as in The Geometry of Schemes. The word geometry used in that sense, I feel, is to have a comprehensive enough vision of a subject to say how it “looks” — but the word theorem means the result is surprising or unintuitive.
This definition of a theorem, to me, presents a useful challenge to annoying pop-psychology that today lurks under the headings of Bayesianism, cognitive _______, behavioural econ/finance, and so on.
Following Buliga and Thurston to understand the nature of mathematical progress, within mathematics at least (where it’s clearer than elsewhere whether you understand something or not—compare to economic theory for example), there is a clear delination of what’s obvious and what’s not.
What is definitely not the case in mathematics, is that every logical or computable consequence of a set of definitions is computed and known immediately when the definitions are stated! You can look at a (particularly a good) mathematical exposition as walking you through the steps of which shifts in perspective you need to take to understand a conclusion. For example start with some group, then consider it as a topological object with a cohomology to get the centraliser. Or in Fourier analysis: re-present line-elements on a series of widening circles. Use hyperbolic geometry to learn about integers. Use stable commutator length (geometry) to learn about groups. Or read about Teichmüller stuff and mapping class groups because it’s the confluence of three rivers.
Sometimes mathematical explanations require fortitude (Gromov’s "energy") and sometimes a shift in perspective (Gromov’s (neg)"entropy").
This view of theorems should be contrasted to the disease of generalisation in mathematical culture. Citing two real-life grad students and a tenured professor in logic (one philosophical, one mathematical, the professor in computer science):
I like your distinction between hemi-toposes, demi-toposes, and semi-toposes
I care about hyper-reals, sur-reals, para-consistency, and so on
Abstract thought — like mathematicians do — is the best kind of thought.
(twitter.com/replicakill, the author of twitter.com/logicians, ragged on David Lewis by saying “What do mathematicians like?” “What do mathematicians think?” —— And Corey Mohler has done a wonderful job of mocking Platonism, which is how I guess the thirst for over-generalisation reaches non-mathematicians.)
Paul Halmos knew that cool examples beat generalisations for generalisation’s sake, as did V. I. Arnol’d. And it seems that the people a Harvard mathematician spends her time with make reasonable demands of a mathematical idea as well. It shouldn’t just contain previous theories; it should surprise. In Buliga’s Blake/Reynolds dispute, Blake wins hands down.
Hopf algebras are vector spaces but also rings (so they have dilation-by-scalars, “plus”, and “times”)
associativity is x⊗x⊗x ↦ 1⊗x⊗x → x⊗x ↦ 1⊗x → x and x⊗x⊗x ↦ x⊗x⊗1 → x⊗x ↦ x⊗1 → x
multiplication takes number ⊗ number → number, so comultiplication should take number → number ⊗ number
Hopf algebra is a vector space with multiplication, comultiplication, and antipodes.
Direct product
⊕ (=direct sum) is like two levers pulling on two things. They are sort-of-fake-ly wrapped together, but really the two levers are moving separate parts.
Tensor product
⊗ is really two levers moving one thing. The way to make it as un-complicated as possible is to think about moving only one of the levers at a time—and stipulating that, if they do move together, that should also be as decomposable as possible.
For example:
11 × 19 = (10 + 1) × (20 − 1)
is the standard technique we’re suppose to teach children for thinking through hard multiplications. (Rather than make them commit a large lookup table to memory.) The reason the splitting above works is because of bilinearity—and with any other bilinear operator on other kinds of objects (like ⊗ with vectors, instead of multiplication with numbers), you can do something similar.
At minute 33, Federico Ardila shows how you can make up a “multiplication” even combining two different types of things. I think of sound as an ∞-dimensional wave (an infinite Fourier series looking, algebraically, roughly like a polynomial: it pairs a constant to each of 1 Hz, 2 Hz, 4 Hz, 8 Hz, … ad infinitum) — so what might a sound “times” a matrix be? Since the axiomatisation of ⊗ is pretty general, he can make this work. (You do end up with a hybrid object looking like color⊗matrix at the end, but the sounds and the matrices can intermix somewhat.
Polynomials over one letter, tensored with itself, gives a ring of polynomials over two letters
If you can tensor matrices, then you can tensor graphs, which in the Facebook era is easy to relate to real life. So 7⌫ + 2Δ + 3Γ (as graph-shapes) can now be meaningful.
permutations can be tensored
together. The coproduct looks pretty weird, like a Δ (abc) ≝ ∅⊗abc + a⊗bc + ab⊗c + abc⊗∅ style, and the product looks like shuffling.
In video 3 you’ll see a “pure algebraic” construction of the tensor of two vector spaces: it’s the free vector space (just an extremely dumb way to construct a big, generic object which is the highest-dimensionality vector-space you can get from a set), then quotient by the ideal generated by (a+b,c) − (a,c) − (b,c) & (a,b+c) − (a,b) − (a,c), and (λa,b) − λ(a,b) & (a,λb) − λ(a,b). In other words you take the biggest thing you can think of and divide out some stuff, in this case getting rid of FOIL leftovers.
The previous descriptions of tensors I’d seen were:
a 3-D matrix
something about stress on the faces of a cube
nasty index juggling (Christoffel symbol Γ)
Jacob Lurie
something about a braided monoidal category
There’s a big difference between setting up a system where ƒ(λa,λb) = λ ƒ(a,b) and one where ƒ(λa,b) = λ ƒ(a,b) = ƒ(a, λb), or ƒ(λa,a) = ƒ(a,λa) only when left matches right.
Added: See michiexile’s addenda/corrections. The fact that free objects are universal covers makes the setup of free /~ rules = my thing work.
Both direct sum and tensor product are standard ways of putting together little Hilbert spaces to form big ones. They are used for different purposes. Suppose we have two physical systems.... Roughly speaking, if ... a physical system's ... states are either of A OR of B, its Hilbert space will be [a] direct sum.... If we have a system whose states are states of A AND states of B, its Hilbert space will be [a] tensor product....
MEASURE SPACE disjoint union Cartesian product
HILBERT SPACE direct sum tensor product
John Baez
@isomorphisms We use direct sums and products of small covariance matrices to generate full-size covariance structures in mixed models.