Universal Kernel

Première partie · Le langage des suturesChapitre 3

La table des sutures du groupe d’ordre 168

The seam table of the group of order 168

Read from the draft of 3 October 2026

168184C256C324C742C41G28S314A4b7S4b7S4a14A4a21D842V4b42V4a87:3
Plate 3.1The fifteen objects of the group of order 168, one for each conjugacy class of subgroups, by size and stabilizer: the aa-classes above the line of sizes, the bb-classes below, and the classes the outer automorphism fixes on it.
  1. 3.1
  2. 3.2
  3. 3.3
  4. 3.4
  5. 3.5
  6. 3.6
  7. 3.7

What are the objects of the group of order 168, and where does each of them appear?

By the stabilizer principle the objects of a finite group correspond to the conjugacy classes of its subgroups, and the automorphisms of the object G/HG/H form the group NG(H)/HN_G(H)/H. For G=PSL⁡(2,7)G=\PSL(2,7) this chapter makes the correspondence concrete. It lists the fifteen classes, proves Burnside’s theorem that the numbers of fixed points determine a GG-set and prints the table of those numbers, and then sets out the seam table itself: for each of the fifteen objects, its incarnations in five theories (the Fano plane, the projective line over F7\F_7, the group itself, the Klein quartic, and two graphs), with the cells that are empty by necessity.

Throughout, GG acts by the Möbius maps of P1(F7)\Proj^1(\F_7), generated by g ⁣:z↦z+1g\colon z\mapsto z+1, h ⁣:z↦4zh\colon z\mapsto4z and s ⁣:z↦−1/zs\colon z\mapsto-1/z, and one marking μA ⁣:G→GL⁡(3,2)\mu_A\colon G\to\GL(3,2) is fixed once and for all. Three later chapters complete the table: Chapter 4 follows the seams of the nine objects that are not rigid around their cycles, Chapter 10 adds the theories that meet the objects at the primes 2 and 7 and at the complex place, and Chapter 11 adds the double cover and closes the table.

The central result · The first block

Every entry of the seam table’s first block, in the Fano plane, the projective line, the group, the Klein quartic and the two graphs, is a transitive GG-set whose stabilizers form the class of its row. In particular the Fano plane, the projective line and the Klein quartic each carry an incarnation of every one of the fifteen objects.

Proof

By machine: each set of figures was built, split into orbits under GG acting through the marking of its theory, and the stabilizer of a representative of each orbit was computed and identified among the 179 subgroups. The Klein quartic is handled in exact arithmetic in Q(ζ7)\Q(\zeta_7); the points of contact of the bitangents need Q(ζ21)\Q(\zeta_{21}) and the eigenvectors for ii need Q(ζ28)\Q(\zeta_{28}). Many entries also have short proofs: an ordered pair of points (p,q)(p,q) of the Fano plane determines the line L=pqL=pq, and its stabilizer is the group of elations with axis LL, a member of V4bV_4^b.

Status

Every table and every statement here was checked by machine in exact arithmetic: the 179 subgroups and their fifteen classes, normalizers and quotients, in agreement with Dickson’s classification; the table of marks; and each entry of the seam table. Burnside’s theorem, the Gassmann pairs, the rigid objects and the forced gaps are also proved by hand, the last with Elkies’s description of the orbits on the quartic.

Every entry of the table has status built: two orbits with the same class are joined by the explicit seam gx↦gygx\mapsto gy for points with equal stabilizers. The two families taken from the literature, Klein’s map on the quartic and the cusps of the modular curve X(7)X(7), are built too, since their stabilizers are proved there. The labels aa and bb are fixed by the marking and exchanged by the outer automorphism; no rule invariant under Aut⁡(G)\Aut(G) chooses them.

Les quinze classesThe fifteen classes

168184C256C324C742C41G28S314A4b7S4b7S4a14A4a21D842V4b42V4a87:3
Plate 3.1The fifteen objects of the group of order 168, one for each conjugacy class of subgroups, by size and stabilizer: the aa-classes above the line of sizes, the bb-classes below, and the classes the outer automorphism fixes on it.

GG has exactly 179 subgroups, in fifteen conjugacy classes. With the number of conjugates and the quotient NG(H)/HN_G(H)/H they are: the trivial group (1; GG), C2C_2 (21; C2×C2C_2\times C_2), C3C_3 (28; C2C_2), C4C_4 (21; C2C_2), two classes of Klein four-groups V4aV_4^a and V4bV_4^b (7 each; S3S_3), S3S_3 (28; 1), C7C_7 (8; C3C_3), D8D_8 (21; 1), two classes A4aA_4^a and A4bA_4^b (7 each; C2C_2), the Frobenius group 7:37{:}3 (8; 1), two classes S4aS_4^a and S4bS_4^b (7 each; 1), and GG. So the fifteen objects have sizes 168, 84, 56, 42, 42, 42, 28, 24, 21, 14, 14, 8, 7, 7 and 1.

The labels aa and bb are fixed by the marking: S4aS_4^a is the class of the stabilizers of the points of the Fano plane and S4bS_4^b that of its lines, and V4aV_4^a, A4aA_4^a (respectively V4bV_4^b, A4bA_4^b) are the normal Klein four-group and the alternating group of a member of S4aS_4^a (respectively S4bS_4^b). In GL⁡(3,2)\GL(3,2) a member of V4aV_4^a is the group of elations with a common centre and a member of V4bV_4^b the group of elations with a common axis; a member of S4aS_4^a contains its normal V4aV_4^a and three members of V4bV_4^b, and dually.

The outer automorphism group has order 2, induced by conjugation by any element of PGL⁡(2,7)\PGL(2,7) outside GG, such as z↦3zz\mapsto3z. It fixes nine classes and exchanges the three pairs (V4a,V4b)(V_4^a,V_4^b), (A4a,A4b)(A_4^a,A_4^b) and (S4a,S4b)(S_4^a,S_4^b), so which member of a pair carries the label aa is a matter of marking: changing μA\mu_A by an outer automorphism exchanges the labels.

Theorem(The subgroups of PSL(2,7)PSL(2,7)) computed

The group GG has exactly 179 subgroups. They fall into fifteen conjugacy classes, with the orders, numbers of conjugates, normalizers and quotients NG(H)/HN_G(H)/H listed above.

Proof

By machine. The enumeration starts from the trivial subgroup and adjoins one element at a time; every subgroup is reached from the trivial one by adjoining its elements in turn, and each intermediate group is a subgroup, so the enumeration is complete. Classes, normalizers and quotients are then computed directly. The list agrees with Dickson’s classification of the subgroups of PSL⁡(2,p)\PSL(2,p).

Objets rigides et non rigidesRigid and non-rigid objects

1681G84C2C2 × C256C3C224C7C342C4C21G28S314A4bC27S4b7S4a14A4aC221D842V4bS342V4aS387:3in blue: NG(H)/H
Plate 3.2The six rigid objects of the group of order 168, in gold; beside each of the other nine, its automorphism group NG(H)/HN_G(H)/H.

By the rigidity criterion an object is rigid exactly when its stabilizer is self-normalizing. Six of the fifteen are: those with stabilizers S3S_3, D8D_8, 7:37{:}3, S4aS_4^a, S4bS_4^b and GG, of sizes 28, 21, 8, 7, 7 and 1. For each of them all seams between incarnations are unique and consistent: once the markings are fixed, the antiflags, the flags, the points of the projective line, the points and the lines of the Fano plane, and the plane itself are matched across theories in exactly one way.

The other nine, of sizes 168, 84, 56, 42, 42, 42, 24, 14 and 14, have automorphism groups GG, C2×C2C_2\times C_2, C2C_2, C2C_2, S3S_3, S3S_3, C3C_3, C2C_2 and C2C_2. Between two incarnations of one of them there is more than one seam, and the seams that theories supply naturally need not agree.

Corollary(Rigid and non-rigid objects) proved

Exactly six of the fifteen objects of GG are rigid: those with stabilizers in S3S_3, D8D_8, 7:37{:}3, S4aS_4^a, S4bS_4^b and GG, of sizes 28, 21, 8, 7, 7 and 1. For each of them all seams between incarnations are unique and consistent. The other nine objects, of sizes 168, 84, 56, 42, 42, 42, 24, 14 and 14, have automorphism groups GG, C2×C2C_2\times C_2, C2C_2, C2C_2, S3S_3, S3S_3, C3C_3, C2C_2, C2C_2.

Proof

Part (c) of the stabilizer principle and the rigidity criterion, with the quotients NG(H)/HN_G(H)/H of the classes.

Les marquesMarks

1C2C3C4V4aV4bS3C7D8A4aA4b7:3S4aS4bGKG/1168G/C2844G/C35602G/C442202G/V4a426006G/V4b4260006G/S328410001G/C7240000003G/D82150133001G/A4a14220200002G/A4b142200200002G/7:3802000010001G/S4a7311131011001G/S4b73113110101001G/G111111111111111
Plate 3.3The table of marks of the group of order 168: the entry in row G/HG/H and column KK is the number of points of G/HG/H fixed by KK. It is lower triangular, with the automorphism counts ∣NG(H):H∣|N_G(H):H| in gold on the diagonal.

For subgroups HH and KK, the mark of KK on the object G/HG/H is the number m(H,K)=∣(G/H)K∣m(H,K)=|(G/H)^K| of cosets that KK fixes; for a finite GG-set XX, its mark at KK is ∣XK∣|X^K|. The term is Burnside’s. A mark depends only on the classes of HH and KK, and marks add over disjoint unions.

The coset gHgH is fixed by KK exactly when K≤gHg−1K\le gHg^{-1}, so a mark counts the conjugates of HH that contain KK, each ∣NG(H):H∣|N_G(H):H| times. Ordered by size, the table is lower triangular with the automorphism counts on the diagonal, and so invertible: the marks of a finite GG-set give its numbers of orbits of each type, and with them the set. For the group of order 168 the row of G/S4aG/S_4^a reads 7,3,1,1,1,3,1,0,1,1,0,0,1,0,0: the seven points of the Fano plane, of which an involution fixes three, an element of order 3 one, and an element of order 7 none.

The permutation character of G/HG/H is its row read at the cyclic subgroups, the columns 1, C2C_2, C3C_3, C4C_4 and C7C_7. Burnside’s marks, read at every subgroup, are a finer invariant, and they determine a finite GG-set up to isomorphism.

Theorem(Burnside) proved

Let H1,…,HrH_1,\dots,H_r represent the conjugacy classes of subgroups of a finite group GG, numbered so that ∣Hi∣≤∣Hj∣|H_i|\le|H_j| for i<ji<j. (a) m(H,K)=∣NG(H):H∣⋅#{H′ conjugate to H:K≤H′}m(H,K)=|N_G(H):H|\cdot\#\{H'\text{ conjugate to }H: K\le H'\}; in particular m(H,K)≠0m(H,K)\neq0 if and only if KK is contained in a conjugate of HH. (b) The matrix (m(Hi,Hj))\bigl(m(H_i,H_j)\bigr) is lower triangular, with diagonal entries ∣NG(Hi):Hi∣|N_G(H_i):H_i|; in particular it is invertible. (c) Two finite GG-sets XX and YY are isomorphic if and only if ∣XK∣=∣YK∣|X^K|=|Y^K| for every subgroup K≤GK\le G.

Proof

(a) gHgH is fixed by KK exactly when K≤gHg−1K\le gHg^{-1}; the map gH↦gHg−1gH\mapsto gHg^{-1} onto the conjugates containing KK has fibres {gnH:n∈NG(H)}\{gnH: n\in N_G(H)\}, of size ∣NG(H):H∣|N_G(H):H|. (b) For j>ij>i, HjH_j lies in a conjugate of HiH_i only if the two have the same order and are conjugate, so only for j=ij=i; and the only conjugate of HiH_i containing HiH_i is HiH_i. (c) By the stabilizer principle XX is the disjoint union of cic_i copies of G/HiG/H_i, so ∣XHj∣=∑ici m(Hi,Hj)|X^{H_j}|=\sum_ic_i\,m(H_i,H_j), and the matrix is invertible, so the marks determine the cic_i.

Les paires de GassmannThe Gassmann pairs

1C2C3C4V4aV4bS3C7D8A4aA4b7:3S4aS4bGKG/1168G/C2844G/C35602G/C442202G/V4a426006G/V4b4260006G/S328410001G/C7240000003G/D82150133001G/A4a14220200002G/A4b142200200002G/7:3802000010001G/S4a7311131011001G/S4b73113110101001G/G111111111111111
Plate 3.4The three Gassmann pairs: rows that agree on the shaded cyclic columns 1, C2C_2, C3C_3, C4C_4, C7C_7, so share a permutation character, and differ in the column V4aV_4^a, boxed in blue.

Read along its cyclic columns, the table gives the permutation characters, and three pairs of objects share theirs: (G/V4a,G/V4b)(G/V_4^a,G/V_4^b), (G/A4a,G/A4b)(G/A_4^a,G/A_4^b) and (G/S4a,G/S4b)(G/S_4^a,G/S_4^b). The reason is conceptual. The outer automorphism exchanges the two members of each pair and fixes every conjugacy class of elements except 7A7A and 7B7B; V4V_4, A4A_4 and S4S_4 contain no element of order 7, so the two members meet every class of GG in equally many elements, which is the condition for equal permutation characters. Since the outer automorphism sends 7A7A to 7B=7A−17B=7A^{-1}, this is an instance of the Galois gap of Chapter 17: counting cannot hear a twist that acts on the classes as Galois acts.

The column V4aV_4^a separates them: within each pair its marks differ, 6 and 0 on the objects of size 42, 2 and 0 on those of size 14, 1 and 3 on the sevens. By Burnside’s theorem the two members of a pair are not isomorphic, no seam joins them, and every bridge between them, for one marking, is refuted. In the language of Chapter 2 each pair is a separating absence whose imprint is the column V4aV_4^a, which separates all three at once. The pair of S4S_4‘s is the classical one, the points and the lines of the Fano plane.

Proposition(The Gassmann pairs of PSL(2,7)PSL(2,7)) proved

Two distinct objects of GG have the same permutation character exactly for the three pairs (G/V4a,G/V4b)(G/V_4^a,G/V_4^b), (G/A4a,G/A4b)(G/A_4^a,G/A_4^b) and (G/S4a,G/S4b)(G/S_4^a,G/S_4^b). Every bridge between the two members of such a pair, for one marking, is refuted.

Proof

The coincidences are read off the table of marks. The two members of each pair are not isomorphic GG-sets, since their marks at V4aV_4^a differ, so no seam joins them.

Le premier blocThe first block

points88 · 7:3pairs2828 · S3three-subsets5656 · C3four-subsets7042 · C414 · A4a14 · A4bbisections3521 · D87 · S4a7 · S4b
Plate 3.5The natural figures of P1(F7)\Proj^1(\F_7) split into orbits, each drawn by one representative and labelled with its size and stabilizer class: one orbit of points, of pairs and of three-subsets; three of four-subsets and three of bisections.

In each of five theories take natural sets of figures, let the theory’s group act through its marking, split the sets into orbits, and compute the stabilizer class of each orbit. An orbit is then an incarnation of the object of that class, and two orbits with the same class are joined by the explicit seam gx↦gygx\mapsto gy for points with equal stabilizers, so every entry of the table has status built. The markings are μA\mu_A for the Fano plane and the graphs, the identity for the projective line and the group, and Klein’s ρ\rho for the quartic.

On the projective line the figures are subsets, pairs of pairs and vectors. The 8 points are one orbit, of class 7:37{:}3; the 28 pairs one orbit, S3S_3; the 56 three-subsets one orbit, C3C_3. The 70 four-subsets split into three: 42 in the orbit of {0,1,2,3}\{0,1,2,3\}, class C4C_4, and 14 each in the orbits of {0,1,2,5}\{0,1,2,5\} and {0,1,2,4}\{0,1,2,4\}, classes A4aA_4^a and A4bA_4^b. The 35 bisections, partitions into two sets of four, split as 21+7+721+7+7, classes D8D_8, S4aS_4^a and S4bS_4^b. The 24 nonzero vectors of F72\F_7^2 up to sign, on which GG acts through SL⁡(2,7)\SL(2,7), are the object of size 24, and the ordered triples form two regular orbits, of (0,1,2)(0,1,2) and of (0,1,3)(0,1,3).

The other columns are as concrete. In the Fano plane: frames, flags and antiflags, ordered pairs of points and of lines, oriented quadrangles and quadrilaterals, and cyclic labellings, bijections to Z/7\Z/7 carrying the lines onto the translates of {0,1,3}\{0,1,3\} or of {0,4,6}\{0,4,6\}. In the group: elements and subgroups under conjugation, and pairs of commuting involutions. On the Klein quartic: its flexes and their tangents, the bitangents with their poles and points of contact, the centres and axes of the involutions, self-polar triangles, the eight flex triangles, and two families of invariant conics. In the graphs: Coxeter vertices, arcs, edges and heptagons, and Heawood edges, hexagons and perfect matchings.

Sutures internes à une théorieSeams inside one theory

1234567
Plate 3.6A flag of the Fano plane and the undirected 4-cycle on the quadrangle off its line: the flag (1,123)(1,123) and the cycle 4,6,5,7, whose diagonals 45 and 67 meet at 1.

Some relations between entries are seams that hold for every marking, because they are made from the figures alone. A quadrangle is the complement of a line, and an undirected 4-cycle on it has its two diagonals in one parallel class of the affine plane off the line, which is a point of the line: undirected 4-cycles are flags. Directing the cycle halves the stabilizer, D8D_8 becoming C4C_4.

Each S3S_3-orbit of perfect matchings of P1(F7)\Proj^1(\F_7) contains a distinguished pair, the one its stabilizer fixes, and that is its seam to the pairs; the two 7-orbits of matchings are the two families of K4K_4‘s inside the twenty-eight. On the quartic, the stabilizer of a bitangent is an S3S_3 whose subgroup of order 3 fixes both points of contact and whose involutions exchange them, the stabilizer of a point of contact being only C3C_3. So a point of contact is a bitangent together with one of its two points of contact, and sending it to its bitangent is the natural GG-map G/C3→G/S3G/C_3\to G/S_3, with fibres of size two. Each centre lies on exactly four bitangents, which the two elements of order 4 fixing it pair into the two Coxeter edges there.

Cases vides par nécessitéCells that are empty by necessity

1G7S4a7S4b87:314A4a14A4b21D824C728S342C442V4a42V4b56C384C21681classes of elementsor of subgroupspoints of the planeP2(C), under ρpoints of theKlein quartic
Plate 3.7The negative space of three kinds of figure. Gold dots are incarnations of the fifteen objects; blue hatching marks the cells that are empty by necessity.

Every row of the Fano, projective-line and Klein columns is filled, but inside a column particular kinds of figure can realize only some classes, and these restrictions are theorems. A conjugacy class of elements is an incarnation of G/CG(x)G/C_G(x), and the centralizers are GG, D8D_8, C3C_3, C4C_4, C7C_7, C7C_7; a class of subgroups is an incarnation of G/NG(H)G/N_G(H), and the normalizers are GG, D8D_8, S3S_3, 7:37{:}3, S4aS_4^a, S4bS_4^b. So the objects with stabilizers 1, C2C_2, V4aV_4^a, V4bV_4^b, A4aA_4^a, A4bA_4^b are incarnated by no conjugacy class at all.

Under Klein’s ρ\rho no point of P2(C)\Proj^2(\C) has its stabilizer in the classes V4aV_4^a, V4bV_4^b, A4aA_4^a, A4bA_4^b, 7:37{:}3, S4aS_4^a, S4bS_4^b or GG. This absence has an imprint, the self-polar triangle: the object G/V4G/V_4, which no point can carry, is carried by ordered pairs of vertices of a self-polar triangle. A point of the Klein quartic itself has stabilizer 1, C2C_2, C3C_3 or C7C_7, with orbits of 84, 56 and 24 points beside the regular ones.

Two further families come from the literature. Klein’s map of type {7,3}\{7,3\} on the quartic has 24 heptagonal faces, 56 vertices and 84 edges, and GG acts by rotations about their centres: the face centres are the flexes, the vertices are the points of contact of the bitangents, and the midpoints of the edges are the points with stabilizer C2C_2. The 24 cusps of the modular curve X(7)X(7), the preimage of the cusp of X(1)X(1), are the object of size 24 again, and return in Chapter 4.

Proposition(Forced gaps) proved

(a) The objects with stabilizers 1, C2C_2, V4aV_4^a, V4bV_4^b, A4aA_4^a, A4bA_4^b are incarnated by no conjugacy class of elements or of subgroups. (b) No point of P2(C)\Proj^2(\C) has stabilizer, under ρ\rho, in the classes V4aV_4^a, V4bV_4^b, A4aA_4^a, A4bA_4^b, 7:37{:}3, S4aS_4^a, S4bS_4^b or GG, and the same holds for lines. (c) The stabilizer of a point of the Klein quartic is 1, C2C_2, C3C_3 or C7C_7.

Proof

(a) Under conjugation the stabilizer of an element is its centralizer and that of a subgroup its normalizer. (b) A point fixed by KK is a line of C3\C^3 invariant under ρ(K)\rho(K). The character of ρ\rho restricted to A4A_4, S4S_4 and 7:37{:}3 has norm 1 (for 7:37{:}3, (9+3∣α∣2+3∣αˉ∣2)/21=1(9+3|\alpha|^2+3|\bar\alpha|^2)/21=1, as ∣α∣2=2|\alpha|^2=2), so these restrictions are irreducible and fix no point, and neither does any subgroup containing one of them. The involutions of a Klein four-group have eigenvalues 1,−1,−11,-1,-1 and are simultaneously diagonal; their common eigenlines are the centres of the three involutions, each with stabilizer the centralizer, a D8D_8. For lines, apply the same argument to the contragredient representation, which is ρ\rho composed with an outer automorphism. (c) By Elkies’s description of the orbits on the quartic; that the stabilizers are cyclic is general, since a finite group fixing a point of a Riemann surface acts faithfully on the tangent line there.

The table is filled: every object has a built incarnation in the Fano plane, on the projective line and on the Klein quartic, and the graphs reach the rest once their cycles and distances are read. What the table does not settle is which of the several seams between two incarnations of a non-rigid object the theories themselves choose. Chapter 4 takes the nine non-rigid rows one by one, beginning with the object of size 24, and adds a second block of columns, the integral octonions and a finer reading of the two graphs.

Introduced here
forced gap