Deuxième partie · Doubles viesChapitre 8
La famille de Weyl
The Weyl family
Read from the draft of 2 October 2026
Where do the twenty-eight bitangents of the Klein quartic sit in the theta structure every plane quartic carries, and what does the group of order 168 see of it?
Every plane quartic has twenty-eight bitangents. Jordan determined the group of their equation, and by Harris’s theorem the Galois group of an enumerative problem is its monodromy group: for a quartic with general rational coefficients the Galois group of the twenty-eight is , of order 1451520. The family continues through the Weyl groups of , and and the 27, 56 and 240 lines of the del Pezzo surfaces of degrees 3, 2 and 1.
The bitangents of a curve of genus 3 are its odd theta characteristics: quadratic forms on the 2-torsion of its Jacobian whose polar form is the Weil pairing. This chapter builds the family in one model, Riemann’s coordinates, with the seams between its objects, and then restricts it to the group of order 168. In that model a theta characteristic of the Klein quartic is a point and a line of the Fano plane, either possibly absent, odd exactly when the point is off the line: the book’s oldest identification, bitangents as antiflags, extended from the twenty-eight to the whole theta structure.
Under the nine objects of decompose into objects of . In particular:
(a) the even theta characteristics are , the points , an -object, the lines , , and the flags with , ; the Steiner complexes are the points, the lines, the flags and the antiflags;
(b) the Göpel subspaces transverse to both and are the graphs of the 28 nondegenerate symmetric bilinear forms on , that is the 28 polarities of the Fano plane, an -object;
(c) the object of size 8, the projective line , occurs twice: as the eight Aronhold heptads of the Cayley octad , and as the eight Desarguesian spreads that contain both and , the -structures of the Fano plane;
(d) exactly one of the 120 hexagons is -invariant;
(e) twelve of the fifteen objects of occur; those with stabilizers , and do not.
Status
The nine objects, their stabilizers and counts are classical, following Bergvall’s table, the ATLAS and Dolgachev; the del Pezzo model is Manin’s and Dolgachev’s, and the two lives of are Kneser’s, as Elkies records them. Everything was built and checked by direct computation in one model. Not found in the sources consulted: the coordinate form of the theta characteristics of the Klein quartic, where parity is non-incidence; the stabilizer classes of the restriction and several of its rows; the Coxeter graph inside the theta structure; the Galois action on the bitangents as on their labels; and the maps of in characteristic 3.
Two identifications have status type. Bergvall’s systems of Riemann–Dickson coordinates and Dye’s enneads are incarnations of the hexagons and the spreads, joined to them by seams that exist by the stabilizer principle and are not exhibited. And the 2-torsion of the Jacobian matches the two reductions of Klein’s lattice at 2 only by type; built, it would make the Coxeter pairing a statement about the curve and its Jacobian alone.
Les coordonnées de RiemannRiemann’s coordinates
Let , with elements written , the symplectic form and the quadratic form . Every quadratic form with polar form is for exactly one , and the Arf invariant of is . The group acts on the forms by .
Three odd forms are syzygetic when is odd, and azygetic otherwise. For the bitangents of a quartic this is classical geometry: three are syzygetic exactly when their six points of contact lie on a conic (Salmon, Dixon).
A theta characteristic on is a quadratic form with polar form . They are the 64 forms , ; is odd when , and there are 28 odd and 36 even ones.
Neuf objets de Sp(6,2)Nine objects of Sp(6,2)
The natural objects of have classical names: the even forms are Cayley octads, the nonzero vectors Steiner complexes, the Lagrangian subspaces Göpel subspaces, the isotropic planes syzygetic tetrads, the non-isotropic planes azygetic triads of Steiner complexes. Each stabilizer is the only conjugacy class of subgroups of its order, so each set is a rigid object, and any two of its incarnations are joined by exactly one seam.
Bergvall identifies the object of size 120 with the systems of Riemann–Dickson coordinates and the object of size 960 with Dye’s enneads. By the theorem these are incarnations of the hexagons and the spreads, joined to them by unique seams that exist by the stabilizer principle but are not exhibited: their status is type.
The nine sets, the odd theta characteristics (28), the even ones (36), the nonzero vectors (63), the split Cayley hexagons whose lines are isotropic lines (120), the Lagrangian subspaces (135), the Aronhold heptads (288), the isotropic planes (315), the non-isotropic planes (336) and the Desarguesian symplectic spreads (960), are transitive; each stabilizer fixes no other point of its set and is the only class of subgroups of its order. So each is a rigid object. Moreover:
(a) of the 3276 triples of odd forms, 1260 are syzygetic and 2016 azygetic; (b) the syzygetic tetrads , 315 of them, correspond bijectively to the isotropic planes by ; (c) the Aronhold heptads are the 7-sets of odd forms with every triple azygetic, the sum of a heptad’s seven forms is an even form, and each even form is the sum of exactly 8 heptads.
L’octade de CayleyThe Cayley octad
is a hyperbolic quadratic space, so it is the space of the Klein quadric of chapter 6, and the stabilizer of the even form is . There the 28 nonsingular vectors are the pairs of letters; here they are the vectors with odd. So an even theta characteristic is a labelling of the 28 bitangents by the pairs of eight letters: the classical Cayley octad.
Conwell’s eight heptads are exactly the eight Aronhold heptads whose sum is . If for , then , so every triple is azygetic; the heptads with sum form an orbit of 8 under , and Conwell’s form such an orbit, so the two coincide. The two families of 15 planes of the Klein quadric make one orbit of 30 under and split under .
(a) The stabilizer of an odd form , a group , has orbits on the odd forms, 36 on the even, on the nonzero vectors, the 27 being the singular points of , and on the isotropic planes, the 45 being the totally singular lines of , which with the 27 points form the generalized quadrangle .
(b) The stabilizer of the even form , a group , has orbits 28 on the odd forms, on the even, on the nonzero vectors, on the Lagrangians, the 30 being the planes totally singular for , and on the heptads.
Les surfaces de del PezzoDel Pezzo surfaces
Let have basis with , , and let . Exceptional classes have , roots and , and is generated by the reflections in and . The lines of a del Pezzo surface of degree 3, 2, 1 are its 27, 56, 240 exceptional classes.
The family is seamed by blowing down: is the stabilizer of in . In degree 2 the 56 lines lie in pairs over the 28 bitangents of the branch quartic, exchanged by the Geiser involution , and the bitangents are the 28 pairs of opposite minimal vectors of , not pairs of roots; the 63 pairs of roots are the Steiner complexes. Each of the 27 bitangents other than contains exactly one class orthogonal to , a line of the cubic surface obtained by blowing down.
(a) For there are 27, 56, 240 exceptional classes and 72, 126, 240 roots, and , 2903040, 696729600. The Geiser involution () and the Bertini involution () are central in , acting as on ; the centre of is trivial.
(e) Under the exceptional classes split as and the Bertini pairs as . Under the exceptional classes split as , the bitangents as , the roots as and the pairs of roots as .
Les réseaux réduitsThe root lattices reduced
Reduced modulo 2, the root lattice gives the theta characteristics back. On with the polar form has a one-dimensional radical with ; acts with image of order 1451520 and kernel , so . For an exceptional class the hyperplane of the with even misses , and restricted to it is the theta characteristic of the bitangent : of the 64 hyperplanes missing the nucleus, the 28 hyperplanes are elliptic and the other 36 hyperbolic.
has two lives of this kind, as a group of forms in characteristics 2 and 3. They are not double lives in the sense of chapter 6, whose families are and ; they are double lives among the groups of forms, as is the coincidence of the types and in characteristic 2.
Let , the lattice . (a) In characteristic 2, with is a nondegenerate elliptic quadratic space of dimension 6 on which acts faithfully, so . The map carries the 27 lines onto the 27 singular points and the 45 tritangent trios onto the 45 totally singular lines, and the 36 pairs of roots go onto the 36 nonsingular points.
(b) In characteristic 3, is 5-dimensional, is nondegenerate on it, and acts faithfully on its 121 points, so . The points form three orbits: 36 with , the pairs of roots; 45 with , onto which carries the tritangent trios; and 40 singular, onto which the subsystems map bijectively.
Les thêtas de la quartique de KleinThe theta characteristics of the Klein quartic
Label each bitangent of the Klein quartic by its antiflag , through the unique seam from the bitangents to the antiflags, and write for the vector whose first component is the point and whose second is the linear form vanishing on the line, so that is 1 exactly when . Let act on by .
The conic criterion was checked by exact computation: for one triple in each of the 29 orbits of on triples of bitangents, the determinant of the conic monomials at the six points of contact was computed in , and the 1260 triples where it vanishes are carried by the seam exactly onto those with .
(a) The six points of contact of three bitangents with labels lie on a conic if and only if , which holds for 1260 of the 3276 triples; four bitangents whose labels sum to 0 have their eight points of contact on a conic, and these are the 315 syzygetic tetrads.
(b) Sending a pair of bitangents to the sum of their labels identifies with , -equivariantly, and the Weil pairing with . The theta characteristic of the bitangent is , so the 64 theta characteristics of are the forms with and arbitrary, odd exactly when , and .
(c) is the only -invariant theta characteristic, and it is even. and are the only -invariant Lagrangian subspaces of : the natural module of and its dual.
Le groupe d’ordre 168 dans Sp(6,2)The group of order 168 in Sp(6,2)
Restricted to , each of the nine objects is a sum of the fifteen objects of , labelled and as the seam table labels them. The bitangents are one orbit of 28 with stabilizer , which is the book’s identification of bitangents and antiflags; the Cayley octads are , the points, the lines and the flags; the Steiner complexes are the points, the lines, the flags and the antiflags.
A Göpel subspace transverse to is the graph of a symmetric , transverse to exactly when is invertible; there are 28 such , the polarities of the Fano plane, and the stabilizer of is the group of permutation matrices, an . The sky occurs twice, as the eight heptads of the Cayley octad and as the eight -structures of the Fano plane, its Singer cycles.
Le graphe de Coxeter dans les thêtasThe Coxeter graph in the theta characteristics
The centre of an involution of is the isolated fixed point of in Klein’s plane, and four bitangents pass through it. Their labels sum to 0, so they form a syzygetic tetrad, and its three nonzero differences are , and , where is the flag of centre and axis of the elation . Of the three ways of splitting the four into two pairs, the pairing by gives the two Coxeter edges at the centre, the pairing by joins bitangents whose antiflags share their line, and the pairing by those that share their point.
So the Coxeter pairing is described without group elements: of the three classes by which the four concurrent bitangents pair off, it is the one lying in neither -invariant Lagrangian. If those Lagrangians are the kernels and of the complex multiplication, an identification of status type, this uses only the curve and its Jacobian.
(a) The four bitangents through a centre have labels summing to 0 and form a syzygetic tetrad, paired as above. (b) Every Coxeter edge spans an isotropic line whose third point is a flag class; for each , nine odd have this property, and the three Coxeter neighbours among them are those for which the cross classes and are odd. (c) Exactly one split Cayley hexagon is -invariant. Its lines are the 21 lines , , and the 42 lines over the Coxeter edges; its 35 points with form a geometric hyperplane, and its collinearity graph on the other 28 points, the bitangents, is the Coxeter graph.
Le groupe de Galois des bitangentesThe Galois group of the bitangents
Take over . For let send , and let be on . The line is a rational bitangent and Klein’s matrices are stable under the Galois group, so acts on as conjugation by and on the bitangents as acts on their labels; the rational bitangent’s label is , which every fixes. The normalizer of in is , acting on the labels.
Three groups act on one set of 28. The Galois group of a general quartic, , is its monodromy group; the symmetry group is also the only nontrivial monodromy of the family of quartics with that symmetry; and the arithmetic group of the model over is . They are nested, , with , and is the quadratic character of .
(a) All 28 bitangents are defined over , and acts on them as acts on their labels in . The action is faithful, so the bitangents generate , and the image is the cyclic group of order 6 fixing 0 and ; acts by elements of , and complex conjugation by an outer automorphism.
(b) The Galois orbits on the bitangents have sizes 1,3,6,6,6,6. The line is the only rational bitangent; its three Coxeter neighbours , , form an orbit, each defined over , and these four are the real bitangents.
(c) On the Galois group fixes exactly one nonzero class, an antiflag class, and exactly two theta characteristics, and . Complex conjugation fixes exactly 7 nonzero classes, so by Zeuthen’s classification the real locus of is a single oval.
The seam out of the group of order 168 into the Weyl family is built from the curve: a theta characteristic of the Klein quartic is a point and a line of the Fano plane, odd exactly when the point is off the line, and every natural object of restricts to a sum of the book’s objects, twelve of the fifteen occurring. The Klein quadric of chapter 6 is the stabilizer of the one invariant even form, and the sky appears in the theta world twice.
What stays at status type is the match of the two invariant Lagrangians with the two reductions of Klein’s lattice at 2 (chapter 9). The arithmetic behind , the simple group , belongs to the type law, which reads its two lives through over (chapter 6).