Universal Kernel

Dictionnaire des sutures

A dictionary of seams: each concept with its definition, its theorems and a worked example

The dictionary holds what the Esquisse tells as a story, entry by entry. Its concepts stand on seven floors, each answering one question, from what the classical theories supply to the continua, under a roof that names the subject. Each entry says which chapter introduces it and which chapters of Something Lawfully Occurs read it physically.

the study of seams
6Les continus
5Les complétions
4Les doubles vies
3Ce qui est su
Negative space
2Les sutures
1L’incarnation
0Le fonds classique

G-sets and G-maps · stabilizers and normalizers · orbitals · permutation isomorphism · Gassmann equivalence · the table of marks

seam

Floor 2, Les sutures

How are two incarnations of one object matched?

An equivariant bijection between two incarnations of one object; the seams between two incarnations form a torsor under the object’s automorphisms.

In the volume
IV, VII, X, XII, XVIII

The entry for seam

Plate 1The tower of named concepts, from the classical floor to the roof. Choose a concept: what it is built from is set in blue and traced down the floors, and what is built on it is dotted.

0Le fonds classiqueThe classical stock

What does each theory supply before anything is compared?

Groups acting on sets, stabilizers, characters, and the classical groups with their geometries. The objects of the book are classical, and so is the group theory it uses: orbits and stabilizers, normalizers, automorphisms of permutation groups.

Several classical tools are adopted as they are: orbital graphs, which carry structure across seams; permutation isomorphisms; Gassmann equivalence; Burnside’s marks; power maps; the Frobenius–Schur indicator; equivariant bundles over a finite GG-set; Hurwitz groups; the Bruhat–Tits building; and the triangle presentations of Cartwright, Mantero, Steger and Zappa. What the book isolates is the matchings themselves.

1L’incarnationIncarnation

When do two theories name one object?

An object of a group GG is a transitive GG-set. A theory supplies a set and a group acting on it, both defined without reference to GG; a marking identifies GG with a subgroup of that group, and the marked set is an incarnation of an object when it is GG-isomorphic to it.

The floor rests on the stabilizer principle: an object is determined by its stabilizer class, so an entry of an atlas of objects is a conjugacy class of subgroups. The group of order 168 has exactly fifteen objects, and the Fano plane, the projective line over F7\F_7 and the Klein quartic each carry an incarnation of every one of them.

Its double cover SL⁡(2,7)\SL(2,7) adds objects on which −I-I acts without fixed points, sets that come from no set of the group of order 168. There are exactly four of these new objects, one over each class of subgroups of odd order.

2Les suturesSeams

In how many ways are two incarnations one, and do the ways agree?

A seam is a GG-isomorphism between two incarnations of one object. The seams between two incarnations form a torsor under the automorphism group NG(H)/HN_G(H)/H of the object, so they are unique, and consistent around every cycle, exactly when the stabilizer is self-normalizing. Six of the fifteen objects of the group of order 168 are rigid in this sense.

The other nine carry freedom. When theories supply their seams by their own constructions, a cycle of natural seams can return a nontrivial automorphism, its monodromy. On the object of size 24 the flex-tangent map of the Klein quartic closes a cycle of length two with monodromy of order 3, and the power of an automorphism makes such monodromies comparable across theories.

Read in a choice of alignments, a family of seams over a graph is a lattice gauge connection with gauge group NG(H)/HN_G(H)/H, and monodromy is its holonomy. A seam over an automorphism of GG, a seam after twisting the action by it, joins incarnations that a fixed marking keeps apart, as the polarity joins the lines of the Fano plane to its points.

3Ce qui est suWhat is known

What has been proved about a bridge, and what is proved not to exist?

A bridge asserts that two sets, given in two theories, are incarnations of one object, and its status records what is known: built, type, name or refuted. Only built bridges are theorems. For two marked sets of one group the stabilizer principle decides every type bridge, which is either built or refuted. Type recurrence is not identification.

Beside the statuses stands the negative space: absences, theorems that something is not there, with their windows, the parameter values where the excluded thing can still happen, and their imprints, the structures an absence forces to exist. The absences reduce to one another in three clusters: the group of order 168, the octonions and Hilbert space.

A map between theories that is not a seam is a description: it goes one way and forgets something, and what it forgets at a point is its kernel, a stabilizer. Read so, each concept of the floor is a statement about a description and what it forgets: a built bridge is a description that forgets nothing, an absence is an empty fibre, a carrier imprint is induced from what an orbit description forgets, and monodromy is what remains of the loops once the kernel of the holonomy is divided out.

4Les doubles viesDouble lives

When does one group carry the geometries of two families?

A life of a group is an isomorphism onto a member of the families PSL⁡(n,q)\PSL(n,q), acting on its projective space, or AmA_m, acting on mm letters. Isomorphisms between members of different families are rare: by Artin’s absence exactly four groups have a double life, A5A_5, PSL⁡(2,7)\PSL(2,7), A6A_6 and A8A_8. The floor consists of those survivors, read as seams.

Each double life comes with a dictionary of which natural sets of the two lives are one object, computed by matching stabilizers. For the group of order 168 the dictionary is the seam table itself. In three of the four double lives an outer automorphism exchanges two dual objects of one life and is unremarkable in the other.

5Les complétionsCompletions

Where do the finite geometries sit inside buildings over local fields?

Each life of a double life is a geometry over a finite field Fp\F_p, the residue field of Qp\Q_p. The geometry is the link of a vertex of the Bruhat–Tits building over Qp\Q_p, and the stabilizer of the vertex acts on it through the finite group. A completion of a finite projective geometry is such a building with such a vertex.

So a double life sits at two vertices: the group of order 168 acts on the Heawood graph, the link of a vertex of the building of PGL⁡(3,Q2)\PGL(3,\Q_2), and on P1(F7)\Proj^1(\F_7), the link of a vertex of the tree of PGL⁡(2,Q7)\PGL(2,\Q_7). The octonion multiplication table glues Fano links into the building of PGL⁡(3)\PGL(3) over F2( ⁣(t) ⁣)\F_2(\!(t)\!), and no subgroup of finite index of its group is isomorphic to one of Mumford’s lattice.

Kato’s hermitian form glues the same links, without symmetry, into the building over Q2\Q_2, as Mumford’s lattice; a gluing that a Frobenius group of order 21 respects is the octonion one, and it lives in characteristic 2. At 7 Mumford’s form has its own tree, whose base link is the sky, and over Z[1/14]\Z[1/14] the group of order 168 is the stabilizer of a vertex, Klein’s lattice, at which it carries both lives.

At Klein’s lattice the finite geometry is found among short vectors and neighbours: the stabilizer of a point acts on the neighbour through it as the rotations of a cube, a flag is a pair of vectors of norm 2 whose reflection is a half-turn of that cube, and an antiflag is one of its diagonals, of norm 3. One step beyond the link the two trees at 7 carry a doublet and its symmetric square; the object of the points of the Fano plane is carried along the one tree in exactly one way and along the other in none; and the two parents carry independent flips, the sign changes of −3\sqrt{-3} and −7\sqrt{-7}, of which only the first is seen by the oriented cells of the link complement.

The two parents are joined only by fiber products: across scales none keeps the finite line attached, and at one scale the attachment is forced. Around the loops of the scale tree a single relabelling carries the signed octonion table without reversals exactly on the Iwahori subgroup, and on seven loops in eight it must reverse two units; carried observer by observer, every loop returns each fiber changed only by colour, consistently with the meetings.

6Les continusContinua

How do the finite objects reappear in real and complex geometry?

A finite object can appear in a continuous geometry in two ways: as a configuration of points fixed in place by a finite group of symmetries, an embedded continuum, or as a set of classes of an arithmetic configuration modulo a congruence subgroup, an arithmetic one. Which kind an object can have is decided by absences.

The archimedean place joins this floor to the completions: the congruence that gives a residue field at a prime gives, over C\C, Thurston’s congruence link complement, whose eight cusps are the points of P1(F7)\Proj^1(\F_7) and whose cells are objects of the group of order 168. The projective line P1(F7)\Proj^1(\F_7) has no embedded continuum in P1(C)\Proj^1(\C) or in Klein’s plane, only this arithmetic one.

Every row of the seam table is a configuration of cells of that manifold, and the Fano incidence among them is the absence of a shared face. In the Cayley plane one point and one imaginary unit carry the intersection of two maximal subgroups of F4F_4 found by Todorov and Dubois-Violette; in its complexification the same point carries the 16\mathbf{16} of so(10)\mathfrak{so}(10).

On the link complement the spinor system, the local system of the defining representation of SL⁡(2,Z[ω])\SL(2,\Z[\omega]), carries the first of the two parents’ flips at the cusps, and the operators that move between pairs of cusps generate a Clifford algebra whose centre is a single sign.

Le sujetThe subject

What is studied?

Seam theory, the study of seams: whether incarnations in different theories can be joined, in how many ways, whether the joins are consistent around a cycle of theories, how they depend on the identification of symmetry groups, what the maps that are not joins forget, and where a join is impossible. The objects are classical; the joins, not the pieces, are at the centre.

The last question gives the subject its shape: a table of objects against theories in which some cells are empty by necessity, a negative space bounded by the seams that do exist.

The fifteen objects

An object of a group is a transitive set of it, determined up to isomorphism by the conjugacy class of its stabilizers. The group of order 168 has fifteen classes of subgroups, so fifteen objects.

168184C256C324C742C41G28S3anchored observers14A4b7S4bvantage lines7S4aclocks14A4a21D842V4b42V4a87:3the sky

The twenty-eight

The object of size 28, stabilizer S3S_3

Seams between two incarnations
One: the object is rigid.
In the program
anchored observers

The entry for the twenty-eight

Fano plane
antiflags
Projective line
2-subsets; perfect matchings in the orbit of {01,23,45,6∞}\{01,23,45,6\infty\}
The group
subgroups of order 3; of order 6
Klein quartic
bitangents; their poles
Graphs
Coxeter vertices; Heawood hexagons
Plate 2The fifteen objects of G=PSL⁡(2,7)G=\PSL(2,7) on the line of their sizes ∣G:H∣|G:H|. The outer automorphism exchanges each class marked aa, above the line, with its class bb below. Each dot is an automorphism of the object, and the dots number the seams between any two of its incarnations; the six rigid objects, with the identity alone, carry none. Dashed brackets join the three pairs with one permutation character. The chosen object’s maps run in ink to the objects it maps onto and in blue from those that map onto it. Names in italic are the program’s.