Trinities
- Galois’ last letter
- Arnold’s trinities
- Arnold’s trinities version 2.0
- the buckyball symmetries
- Klein’s dessins d’enfant and the buckyball
- the buckyball curve
Arnold has written a follow-up to the paper mentioned last time called “Polymathematics : is mathematics a single science or a set of arts?” (or here for a (huge) PDF-conversion).
On page 8 of that paper is a nice summary of his 25 trinities :
I learned of this newer paper from a comment by Frederic Chapoton who maintains a nice webpage dedicated to trinities.
In his list there is one trinity on sporadic groups :
![\xymatrix{& BabyMonster \ar@{-}[rd] & \\ F_{24} \ar@{-}[ru] \ar@{-}[rr] & & Monster} \xymatrix{& BabyMonster \ar@{-}[rd] & \\ F_{24} \ar@{-}[ru] \ar@{-}[rr] & & Monster}](/latexrender/pictures/bf79de845c99e568c85bc82e3644e26d.gif)
where
is the
Fischer simple group of order
, which is the third largest sporadic group (the two larger ones being the
Baby Monster and the
Monster itself).
I don’t know what the rationale is behind this trinity. But I’d like to recall the (Baby)Monster history as a warning against the trinity-reflex. Sometimes, there is just no way to extend a would be trinity.
The story comes from Mark Ronan’s book Symmetry and the Monster on page 178.
Let’s remind ourselves how we got here. A few years earlier, Fischer has created his ‘transposition’ groups Fi22, Fi23, and Fi24. He had called them M(22), M(23), and M(24), because they were related to Mathieu’s groups M22,M23, and M24, and since he used Fi22 to create his new group of mirror symmetries, he tentatively called it.
It seemed to appear as a cross-section in something even bigger, and as this larger group was clearly associated with Fi24, he labeled it. Was there something in between that could be called
?
Fischer visited Cambridge to talk on his new work, and Conway named these three potential groups the Baby Monster, the Middle Monster, and the Super Monster. When it became clear that the Middle Monster didn’t exist, Conway settled on the names Baby Monster and Monster, and this became the standard terminology.
Marcus du Sautoy’s account in Finding Moonshine is slightly different. He tells on page 322 that the Super Monster didn’t exist. Anyone knowing the factual story?
Some mathematical trickery later revealed that the Super Monster was going to be impossible to build: there were certain features that contradicted each other. It was just a mirage, which vanished under closer scrutiny. But the other two were still looking robust. The Middle Monster was rechristened simply the Monster.
And, the inclusion diagram of the sporadic simples tells yet another story.
Anyhow, this inclusion diagram is helpful in seeing the three generations of the Happy Family (as well as the Pariahs) of the sporadic groups, terminology invented by Robert Griess in his 100+p Inventiones paper on the construction of the Monster (which he liked to call, for obvious reasons, the Friendly Giant denoted by FG). The happy family appears in Table 1.1. of the introduction.
It was this picture that made me propose the trinity on the left below in the previous post. I now like to add another trinity on the right, and, the connection between the two is clear.
constructed using ![\xymatrix{& Leech \ar@{-}[rd] & \\ Golay \ar@{-}[ru] \ar@{-}[rr] & & Griess} \xymatrix{& Leech \ar@{-}[rd] & \\ Golay \ar@{-}[ru] \ar@{-}[rr] & & Griess}](/latexrender/pictures/48407ede6b47b80b9bb8489ce8e96cc8.gif)
Here
denotes the extended binary
Golay code of which the Mathieu group
is the automorphism group.
is of course the 24-dimensional
Leech lattice of which the automorphism group is a double cover of the Conway group
.
is the
Griess algebra which is a nonassociative 196884-dimensional algebra of which the automorphism group is the Monster.
I am aware of a construction of the Leech lattice involving the quaternions (the icosian construction of chapter 8, section 2.2 of SPLAG). Does anyone know of a construction of the Griess algebra involving octonions???
.
. Was there something in between that could be called
?
Referring to the triple of exceptional Galois groups
and its connection to the Platonic solids I
but I would like to alter it into
are the Hamiltonian
are the
![\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)


![\xymatrix{& Cube \ar@{-}[rd] & \\ Tetra \ar@{-}[ru] \ar@{-}[rr] & & Dode} \xymatrix{& Cube \ar@{-}[rd] & \\ Tetra \ar@{-}[ru] \ar@{-}[rr] & & Dode}](/latexrender/pictures/02d8facd8be9e61d323d5305bcb0e0b2.gif)
![\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)
is the
is the
, 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
![\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)
. ![\xymatrix{& TrigonoNumbers \ar@{-}[rd] & \\ Numbers \ar@{-}[ru] \ar@{-}[rr] & & EllipticNumbers } \xymatrix{& TrigonoNumbers \ar@{-}[rd] & \\ Numbers \ar@{-}[ru] \ar@{-}[rr] & & EllipticNumbers }](/latexrender/pictures/8842a61479e294fd3c7ab07a9bb52ba3.gif)
, 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.![\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)
![\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)
![\xymatrix{& KleinQuartic \ar@{-}[rd] & \\ Dodecahedron \ar@{-}[ru] \ar@{-}[rr] & & ? } \xymatrix{& KleinQuartic \ar@{-}[rd] & \\ Dodecahedron \ar@{-}[ru] \ar@{-}[rr] & & ? }](/latexrender/pictures/59f157a92e8434c8efbfc21c488a4a12.gif)
![\xymatrix{& Conway \ar@{-}[rd] & \\ Mathieu \ar@{-}[ru] \ar@{-}[rr] & & Monster } \xymatrix{& Conway \ar@{-}[rd] & \\ Mathieu \ar@{-}[ru] \ar@{-}[rr] & & Monster }](/latexrender/pictures/b024a43c1715cbda7492d383019a7705.gif)
and 
and hence are hiding in a special polygonal region of the

, via its
an odd edge. Fortunately, kfarey also allows us to draw the special polygonal region determined by a Farey-symbol. So, here it is (without the pairing data) :

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
.