Trinities
Referring to the triple of exceptional Galois groups
and its connection to the Platonic solids I
wrote : “It sure seems that surprises often come in triples…”. Briefly I considered replacing triples by trinities, but then, I didnt want to sound too mystic…
David Corfield of the n-category cafe and a dialogue on infinity (and perhaps other blogs I’m unaware of) pointed me to the paper Symplectization, complexification and mathematical trinities by Vladimir I. Arnold. (Update : here is a PDF-conversion of the paper)
The paper is a write-up of the second in a series of three lectures Arnold gave in june 1997 at the meeting in the Fields Institute dedicated to his 60th birthday. The goal of that lecture was to explain some mathematical dreams he had.
The next dream I want to present is an even more fantastic set of theorems and conjectures. Here I also have no theory and actually the ideas form a kind of religion rather than mathematics.
The key observation is that in mathematics one encounters many trinities. I shall present a list of examples. The main dream (or conjecture) is that all these trinities are united by some rectangular “commutative diagrams”.
I mean the existence of some “functorial” constructions connecting different trinities. The knowledge of the existence of these diagrams provides some new conjectures which might turn to be true theorems.
Follows a list of 12 trinities, many taken from Arnold’s field of expertise being differential geometry. I’ll restrict to the more algebraically inclined ones.
1 : “The first trinity everyone knows is”
but I would like to alter it into
where
are the Hamiltonian
quaternions. The trinity on the left may be natural to differential geometers who see real and complex and hyper-Kaehler manifolds as distinct but related beasts, but I’m willing to bet that most algebraists would settle for the trinity on the right where
are the
octonians.
2 : The next trinity is that of the exceptional Lie algebras E6, E7 and E8.
![\xymatrix{& E_7 \ar@{-}[rd] & \\ E_6 \ar@{-}[ru] \ar@{-}[rr] & & E_8} \xymatrix{& E_7 \ar@{-}[rd] & \\ E_6 \ar@{-}[ru] \ar@{-}[rr] & & E_8}](/latexrender/pictures/8203b658c346645061ddcdc313f3f9c6.gif)
with corresponding Dynkin-Coxeter diagrams


Arnold has this to say about the apparent ubiquity of Dynkin diagrams in mathematics.
Manin told me once that the reason why we always encounter this list in many different mathematical classifications is its presence in the hardware of our brain (which is thus unable to discover a more complicated scheme).
I still hope there exists a better reason that once should be discovered.
Amen to that. I’m quite hopeful human evolution will overcome the limitations of Manin’s brain…
3 : Next comes the Platonic trinity of the tetrahedron, cube and dodecahedron
![\xymatrix{& Cube \ar@{-}[rd] & \\ Tetra \ar@{-}[ru] \ar@{-}[rr] & & Dode} \xymatrix{& Cube \ar@{-}[rd] & \\ Tetra \ar@{-}[ru] \ar@{-}[rr] & & Dode}](/latexrender/pictures/02d8facd8be9e61d323d5305bcb0e0b2.gif)
Clearly one can argue against this trinity as follows : a tetrahedron is a bunch of triangles such that there are exactly 3 of them meeting in each vertex, a cube is a bunch of squares, again 3 meeting in every vertex, a dodecahedron is a bunch of pentagons 3 meeting in every vertex… and we can continue the pattern. What should be a bunch a hexagons such that in each vertex exactly 3 of them meet? Well, only one possibility : it must be the hexagonal tiling (on the left below). And in normal Euclidian space we cannot have a bunch of septagons such that three of them meet in every vertex, but in hyperbolic geometry this is still possible and leads to the Klein quartic (on the right). Check out this wonderful post by John Baez for more on this.
4 : The trinity of the rotation symmetry groups of the three Platonics
![\xymatrix{& S_4 \ar@{-}[rd] & \\ A_4 \ar@{-}[ru] \ar@{-}[rr] & & A_5} \xymatrix{& S_4 \ar@{-}[rd] & \\ A_4 \ar@{-}[ru] \ar@{-}[rr] & & A_5}](/latexrender/pictures/35097927ee7dc758a6c1ff47c60b0080.gif)
where
is the
alternating group on n letters and
is the
symmetric group.
Clearly, any rotation of a Platonic solid takes vertices to vertices, edges to edges and faces to faces. For the tetrahedron we can easily see the 4 of the group
, say the 4 vertices. But what is the 4 of
in the case of a cube? Well, a cube has 4 body-diagonals and they are permuted under the rotational symmetries. The most difficult case is to see the
of
in the dodecahedron. Well, here’s the solution to this riddle
there are exactly 5 inscribed cubes in a dodecahedron and they are permuted by the rotations in the same way as
.
7 : The seventh trinity involves complex polynomials in one variable
![\xymatrix{& \mathbb{C}[z,z^{-1}] \ar@{-}[rd] & \\ \mathbb{C}[z] \ar@{-}[ru] \ar@{-}[rr] & & \mathbb{C}[z,z^{-1},(z-1)^{-1}] } \xymatrix{& \mathbb{C}[z,z^{-1}] \ar@{-}[rd] & \\ \mathbb{C}[z] \ar@{-}[ru] \ar@{-}[rr] & & \mathbb{C}[z,z^{-1},(z-1)^{-1}] }](/latexrender/pictures/493df8095af71084722dcb0f1c6d8ac7.gif)
the Laurant polynomials and the modular polynomials (that is, rational functions with three poles at 0,1 and
.
8 : The eight one is another beauty
![\xymatrix{& TrigonoNumbers \ar@{-}[rd] & \\ Numbers \ar@{-}[ru] \ar@{-}[rr] & & EllipticNumbers } \xymatrix{& TrigonoNumbers \ar@{-}[rd] & \\ Numbers \ar@{-}[ru] \ar@{-}[rr] & & EllipticNumbers }](/latexrender/pictures/8842a61479e294fd3c7ab07a9bb52ba3.gif)
Here ‘numbers’ are the ordinary complex numbers
, the ‘trigonometric numbers’ are the quantum version of those (aka q-numbers) which is a one-parameter deformation and finally, the ‘elliptic numbers’ are a two-dimensional deformation. If you ever encountered a Sklyanin algebra this will sound familiar.
This trinity is based on a paper of Turaev and Frenkel and I must come back to it some time…
The paper has some other nice trinities (such as those among Whitney, Chern and Pontryagin classes) but as I cannot add anything sensible to it, let us include a few more algebraic trinities. The first one attributed by Arnold to John McKay
13 : A trinity parallel to the exceptional Lie algebra one is
![\xymatrix{& 28-biTangents \ar@{-}[rd] & \\ 27-Lines \ar@{-}[ru] \ar@{-}[rr] & & 120-Tritangents } \xymatrix{& 28-biTangents \ar@{-}[rd] & \\ 27-Lines \ar@{-}[ru] \ar@{-}[rr] & & 120-Tritangents }](/latexrender/pictures/33c6c61b377082891907d711d4666713.gif)
between the 27 straight lines on a cubic surface, the 28 bitangents on a quartic plane curve and the 120 tritangent planes of a canonic sextic curve of genus 4.
14 : The exceptional Galois groups
![\xymatrix{& L_2(7) \ar@{-}[rd] & \\ L_2(5) \ar@{-}[ru] \ar@{-}[rr] & & L_2(11) } \xymatrix{& L_2(7) \ar@{-}[rd] & \\ L_2(5) \ar@{-}[ru] \ar@{-}[rr] & & L_2(11) }](/latexrender/pictures/ea8f1bffb973e1ae957c3e967efb8a47.gif)
explained last time.
15 : The associated curves with these groups as symmetry groups (as in the previous post)
![\xymatrix{& KleinQuartic \ar@{-}[rd] & \\ Dodecahedron \ar@{-}[ru] \ar@{-}[rr] & & ? } \xymatrix{& KleinQuartic \ar@{-}[rd] & \\ Dodecahedron \ar@{-}[ru] \ar@{-}[rr] & & ? }](/latexrender/pictures/59f157a92e8434c8efbfc21c488a4a12.gif)
where the ? refers to the mysterious genus 70 curve. I’ll check with one of the authors whether there is still an embargo on the content of this paper and if not come back to it in full detail.
16 : The three generations of sporadic groups
![\xymatrix{& Conway \ar@{-}[rd] & \\ Mathieu \ar@{-}[ru] \ar@{-}[rr] & & Monster } \xymatrix{& Conway \ar@{-}[rd] & \\ Mathieu \ar@{-}[ru] \ar@{-}[rr] & & Monster }](/latexrender/pictures/b024a43c1715cbda7492d383019a7705.gif)
Do you have other trinities you’d like to worship?
the field of one element, have their own collection of semi-secret texts, surrounded by whispers, of which they try to decode every single line in search of enlightenment. Fortunately, you do not have to search the shelves of the Bibliotheque National in Paris, but the depths of the internet to find them as huge, bandwidth-unfriendly, scanned documents.
The first are the lecture notes “Lectures on zeta functions and motives” by
and over
, cast in the language reminiscent of Grothendieck’s motives. We postulate the existence of a category with tensor product
whose objects correspond not only to the divisors of the Hasse-Weil zeta functions of schemes over
, whose zeta function is
, and whose zeroth power is “the absolute point” which is teh base for Kurokawa’s direct products. We add some speculations about the role of
The second one is the unpublished paper “Cohomology determinants and reciprocity laws : number field case” by
limit of linear algebra over the finite field
is the absolute point, but the real problem is to develop non-trivial consequences of this point of view.”
. But first, let us explain how they define linear algebra over these absolute fields.
is the symmetric group
but as
by
. Clearly, linear maps between such ‘extended’ spaces must be maps of pointed sets, that is, sending
.
with
the group of all n-th roots of unity. Note that if we choose a primitive n-th root
, then
is the cyclic group of order n.
determines an n-set of linear dependent vectors
. In other words, any
with
a set of which the group
elements and there are exactly
orbits for the action of
is a basis if (and only if)
.
is a
. In particular, a linear isomorphism of
is a
for a permutation
.
elements. The dimension
and the general linear group
with
, the identification as matrices with exactly one non-zero entry (being an n-th root of unity) in every row and every column.
be a prime power and let
elements. Assume that
. It is well known that the group of units
is cyclic of order
so by the assumption we can identify
is an
. In other words,
becomes (via restriction of scalars) an
.
when
. (to be continued)
equipped with the usual Hermitian inproduct
. An observable
is a choice of orthonormal basis
consisting of eigenvectors of the self-adjoint matrix
(with orthonormal basis
) are said to be mutally unbiased if the norms of all inproducts
are equal to
. This definition extends to a collection of pairwise mutually unbiased observables. In a d-state quantum system there can be at most d+1 mutually unbiased bases and such a collection of observables is then called a MUB of the system. Using properties of finite fields one has shown that MUBs exists whenever d is a prime-power. On the other hand, existence of a MUB for d=6 still seems to be open…
, consists in taking a system of k object qupits (when
one qupit is a spin l particle) which she will give to the King together with k ancilla qupits that she retains in her possession. These 2k qupits are diligently entangled and prepared is a well chosen state. The final step in finding a suitable state is the solution to a pure combinatorial problem :
ordered sets of d+1 numbers each, with repetitions of numbers within a set allowed, such that any two sets have exactly one identical number in the same place in both. Here’s an example of 16 such strings for d=4 :
with the numbers from 1 to d in some fixed way. Then, the
and take as the first 2 numbers the ones corresponding to these field-elements. The remaning d-2 numbers in the string are those corresponding to the field element
(with
) determined from
by the equation
is the field-element corresponding to the integer i (
corresponds to the zero element). It is easy to see that these
and
that
.