Michel Planat
email: michel.planat@femto-st.fr

Hishamuddin Zainuddin

Zoology of Atlas-groups: dessins d'enfants, finite geometries and quantum commutation

Keywords: Mathematics Subject Classification: 81P45, 20D05, 81P13, 11G32, 51E12, 51E30, 20B40

Every finite simple group P can be generated by two of its elements. Pairs of generators for P are available in the Atlas of finite group representations as (not neccessarily minimal) permutation representations P. It is unusual but significant to recognize that a P is a Grothendieck's dessin d'enfant D and that most standard graphs and finite geometries G -such as near polygons and their generalizationsare stabilized by a D. In our paper, tripods P -D -G of rank larger than two, corresponding to simple groups, are organized into classes, e.g. symplectic, unitary, sporadic, etc (as in the Atlas). An exhaustive search and characterization of non-trivial point-line configurations defined from small index representations of simple groups is performed, with the goal to recognize their quantum physical significance. All the defined geometries G ′ s have a contextuality parameter close to its maximal value 1.

Introduction

Over the last years, it has been recognized that the detailed investigation of commutation between the elements of generalized Pauli groups -the qudits and arbitrary collections of them [START_REF] Planat | Pauli graphs when the Hilbert space dimension contains a square: why the Dedekind psi function?[END_REF]-is useful for a better understanding of concepts of quantum information such as error correction [START_REF]Quantum error correction for quantum memories[END_REF][START_REF] Planat | Unitary reflection groups for quantum fault tolerance[END_REF], entanglement [START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF][START_REF] Holweck | Classification of multipartite systems featuring only |W and |GHZ genuine entangled states[END_REF] and contextuality [START_REF] Howard | Contextuality supplies the magic for quantum computation[END_REF][START_REF] Winter | What does an experimental test of contextuality prove and disprove?[END_REF], that are cornerstones of quantum algorithms and quantum computation. Only recently the first author observed that much of the information needed is encapsulated in permutation representations, of rank larger than two, available in the Atlas of finite group representations [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF]. The coset enumeration methodology of the Atlas was used by us for deriving many finite geometries underlying quantum commutation and the related contextuality [START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF]- [11]. As a bonus, the two-generator permutation groups and their underlying geometries may luckily be considered as dessins d'enfants [START_REF] Lando | Graphs on surfaces and their applications[END_REF], although this topological and algebraic aspect of the finite simple (or not simple) groups is barely mentioned in the literature. Ultimately, it may be that the Monster group and its structure fits our quantum world, as in Dyson's words [11]. More cautiously, in Sec. 2 of the present paper, we briefly account for the group concepts involved in our approach by defining a tripod P -D -G. One leg P is a desired two-generator permutation representation of a finite group P [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF]. Another leg D signs the coset structure of the used subgroup H of the two-generator free group G (or of a subgroup G ′ of G with relations), whose finite index [G, H] = n is the number edges of D, and at the same time the size of the set on which P acts, as in [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF]. Finally, G is the geometry with n vertices that is defined/stabilized by D [START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF]. Then, in Sec. 3, we organize the relevant P -D -G tripods taken from the classes of the Atlas and find that many of them reflect quantum commutation, specifically the symplectic, unitary and orthogonal classes. The geometries of other (classical and sporadic) classes are investigated similarly with the goal to recognize their possible physical significance. A physically oriented survey of simple groups is [START_REF] Boya | Introduction to sporadic groups for physicists[END_REF].

Group concepts for the P -D -G puzzle

Groups, dessins and finite geometries

Following the impetus given by Grothendieck [START_REF] Grothendieck | Sketch of a programme[END_REF], it is now known that there are various ways to dress a group P generated by two permutations, (i) as a connected graph drawn on a compact oriented two-dimensional surface -a bicolored map (or hypermap) with n edges, B black points, W white points, F faces, genus g and Euler characteristic 2 -2g = B + W + F -n [START_REF] Jones | Theory of maps on orientable surfaces[END_REF], (ii) as a Riemann surface X of the same genus equipped with a meromorphic function f from X to the Riemann sphere C unramified outside the critical set {0, 1, ∞} -the pair (X, f ) called a Belyi pair and, in this context, hypermaps are called dessins d'enfants [START_REF] Lando | Graphs on surfaces and their applications[END_REF][START_REF] Grothendieck | Sketch of a programme[END_REF], (iii) as a subgroup H of the free group G = a, b where P encodes the action of (right) cosets of H on the two generators a and b -the Coxeter-Todd algorithm does the job [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF] and finally (iv), when P is of rank at least three, that is of point stabilizer with at least three orbits, as a non-trivial finite geometry [START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF]- [11]. Finite simple groups are generated by two of their elements [START_REF] Malle | Generation of classical groups[END_REF] so that it is useful to characterize them as members of the categories just described.

There are many mathematical papers featuring the correspondence between items (i) and (ii) in view of a better understanding of the action of the absolute Galois group Gal( Q/Q) -the automorphism group of the field Q of algebraic numbers-on the hypermaps [START_REF] Grothendieck | Sketch of a programme[END_REF][START_REF] Jones | Theory of maps on orientable surfaces[END_REF][START_REF] Girondo | Introduction to Riemann surfaces and dessins d'enfants[END_REF]. Coset enumeration featured in item (iii) is at work in the permutation representations of finite groups found in the Atlas [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF]. Item (i) in conjunction to (iii) and (iv) allowed us to arrive at the concept of geometric contextuality as a lack of commutativity of cosets on the lines of the finite geometry stabilized by P [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF].

Item (iv) may be further clarified thanks to the concept of rank of a permutation group P . First it is expected that P acts faithfully and transitively on the set Ω = {1, 2, • • • , n} as a subgroup of the symmetric group S n . The action of P on a pair of distinct elements of Ω is defined as (α, β) p = (α p , β p ), p ∈ P , α = β. The orbits of P on Ω×Ω are called orbitals and the number of orbits is called the rank r of P on Ω. The rank of P is at least two and the 2-transitive groups identify to the rank 2 permutation groups. Second the orbitals for P are in one to one correspondence with the orbits of the stabilizer subgroup P α = {p ∈ P |α p = α} of a point α of Ω. It means that r is also defined as the number of orbits of P α . The orbits of P α on Ω are called the suborbits of P and their lengths are the subdegrees of P . A complete classification of permutation groups of rank at most 5 is in the book [START_REF] Praeger | Low rank representations and graphs for sporadic groups[END_REF]. Next, selecting a pair (α, β) ∈ Ω×Ω, α = β, one introduces the two-point stabilizer subgroup

P (α,β) = {p ∈ P |(α, β) p = (α, β)}.
There exist 1 < m ≤ r such non isomorphic (two-point stabilizer) subgroups S m of P . Selecting the largest one with α = β, one defines a point/line incidence geometry G whose points are the elements of Ω and whose lines are defined by the subsets of Ω sharing the same two-point stabilizer subgroup. Thus, two lines of G are distinguished by their (isomorphic) stabilizers acting on distinct subsets of Ω. A non-trivial geometry arises from P as soon as the rank of the representation P of P is r > 2 and simultaneously the number of non isomorphic two-point stabilizers of P is m > 2.

Geometric contextuality

Let G ′ be a subgroup of the free group G = a, b endowed with a set of relations and H a subgroup of G of index n. As shown in Sec. 2.1, the permutation representation P associated to the pair (G ′ , H) is a dessin d'enfant D whose edges are encoded by the representative of cosets of H in G ′ . A graph/geometry G may be defined by taking the n vertices of G as the edges of D and the edges of G as the distinct (but isomorphic) two-point stabilizer subgroups of P.

Further, G is said to be contextual if at least one of its lines/edges corresponds to a set/pair of vertices encoded by non-commuting cosets [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF]. A straightforward measure of contextuality is the ratio κ = E c /E between the number E c of lines/edges of G with non-commuting cosets and the whole number E of lines/edges of G. Of course, lines/edges passing through the identity coset e have commuting vertices so that one always as κ < 1.

In Sec. 3 below, the contextuality parameter κ corresponding to the collinear graph of the relevant geometry G is displayed in the right column of the tables. In order to compute κ, one needs the finite presentation of the corresponding subgroup H in G ′ leading to the permutation representation P but this information is not always available in the Atlas.

A few significant geometries

There exist layers in the organization of finite geometries, see [START_REF] Batten | Combinatorics of finite geometries[END_REF] for an introduction. A partial linear space is an incidence structure Γ(P, L) of points P and lines L satisfying axioms (i) any line is at least with two points and (ii) any pair of distinct points is incident with at most one line. In our context, the geometry G that is defined by a two-generator permutation group P, alias its dessin d'enfant D, has order (s, t) meaning that every line has s + 1 points and every point is on t + 1 lines. Thus G is the geometric configuration [p s+1 , l t+1 ] (r) , with p and l the number of points and lines. The extra index r denotes the rank of P from which D arises.

We introduce a first layer of organization that is less restrictive that of a near polygon to be defined below and that of a symplectic polar space encountered in Sec. 3.3. We denote by G u = G(s, t; u) a connected partial linear space with the property that, given a line L and a point x not on L, there exist a constant number u of points of L nearest to x. A near polygon (or near 2d-gon) is a partial linear space such that the maximum distance between two points (the so-called diameter) is d and, given a line L and a point x not on L, there exists 'a unique point' on L that is nearest to x. A graph (whose lines are edges) is of course of type G 1 . A near polygon is, by definition, of type G 1 . Symplectic polar spaces are of the form G u , possibly with u > 1, but not all G u with u > 1 are polar spaces. A generalized polygon (or generalized N-gon) is a near polygon whose incidence graph has diameter d (the distance between its furthest points) and girth 2d (the length of a shortest path from a vertex to itself). According to Feit-Higman theorem [START_REF] Tits | Moufang polygons[END_REF], finite generalized N-gons with s > 1 and t > 1 may exist only for N ∈ {2, 3, 4, 6, 8}. They consist of projective planes with N = 3, and generalized quadrangles GQ(s, t), generalized hexagons GH(s, t) and generalized octagons GO(s, t) when N = 4, 6, 8, respectively. Many G ′ s have a collinearity graph that is a strongly regular graph (denoted srg). These graphs are partial geometries pg(s, t; α) of order (s, t) and (constant) connection number α. By definition, α is the number of points of a line L joined to a selected point P by a line. The partial geometries pg listed in our tables are those associated to srg graphs found in [START_REF] Brouwer | Spectra of graphs[END_REF].

A few small examples

Let us illustrate our concepts by selecting a rank 3 (or higher) representation for the group of the smallest cardinality in each class of simple groups. The notation for the simple groups and their representations are taken from the Atlas [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF].

Alternating

The smallest non-cyclic simple group is the alternating group

A 5 whose finite representation is H = a, b|a 2 = b 3 = (ab) 5 = 1 .
The permutation representations of A 5 are obtained by taking the subgroups of finite index of the free group G = a, b whose representation is H.

Table 1 list the rank r and the number m of two-point stabilizer subgroups for the permutation representations P up to rank 15.

The only non trivial permutation group has index 10, rank 3, subdegrees 1, 3, 6 with P = 10|(2, 3, 4)(5, 7, 8)(6, 9, 10), (1, 2)(3, 5)(4, 6)(7, 10) . Table 1. Parameter r and s for small index representations of A 5 .

The dessin d'enfant D corresponding to P is pictured in our previous papers, see [START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF]Fig. 10], [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF]Fig. 3j], [11,Fig. 4]. The geometries that are stabilized are the Petersen graph PG, or Mermin's pentagram MP, depending on the choice of the twopoint stabilizer subgroup. Thus A 5 features three-qubit '3QB' contextuality.

Symplectic

The smallest (simple) symplectic group is 2 list the rank r and the number m of two-point stabilizer subgroups for the permutation representations P up to rank 30.

S ′ 4 (2) = A 6 whose finite representation is H = a, b|a 2 = b 4 = (ab) 5 = (ab 2 ) 5 = 1 . Table
The smallest non trivial permutation group P has index 15, rank 3 and subdegrees 1, 6, 8 as shown in Table 2.

A 6 index 6 10 15 20 30 r 2 2 3 4 7 m 2 2 3 2 3
Table 2. Parameter r and s for the small index representations of A 6 .

The geometry that is stabilized by P is the (self-dual) generalized quadrangle GQ(2, 2), alias the graph L(K 6 ) (the complement of line graph of the complete graph K 6 ). It is known that GQ(2, 2) is a model of two-qubit '2QB' commutation, see [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF]Fig. 12]. The permutation representation of index 30 of S ′ 4 (2) stabilizes the configuration [30 [START_REF] Malle | Generation of classical groups[END_REF] , 160 3 ] of rank 7 that turns to be a geometry of type G 2 .

As for two-qutrit commutation, one uses the S 4 (3) permutation representation P of rank 3 and index 40 b found in the Atlas. The dessin d'enfant picturing P is found on Fig. 1. The dessin has signature (B, W, F, g) = (8, 28, 6, 0).

Unitary

The smallest (simple) unitary group is U 3 (3). Representations of U 3 (3) of index 28 (rank 2), 36 (rank 4), 63 (rank 4) and 63 (rank 5) may be found in the Atlas (denoted 63 a and 63 b , respectively). The most interesting ones are the 63 a , of subdegrees 1, 6, 24, 32 and the 63 b , of subdegrees 1, 6, 16 2 , 24. These representations stabilize the split Cayley hexagon GH(2, 2) (with 63 b ) and its dual (with 63 a ). The hexagon GH(2, 2) is a configuration of type [63 3 ] with 63 points on three lines and 63 lines with three points. It may be used as a model of 3QB contextuality, see [10, Fig. 5 and6] for details and plots of the corresponding dessins d'enfants.

Orthogonal

The smallest (simple) orthogonal group is O 7 (3). The Atlas lists four representations of rank 3 and index 351, 364, 378 and 1080.

We could recognize that the first representation is associated to the strongly regular graph srg(351, 126, 45, 45) and the geometry NO -(7, 3), the second representation is associated with srg(364, 120, 38, 40) and the geometry of the symplectic polar space W 5 (3), the third representation is associated with srg(378, 117, 36, 36) and presumably the partial geometry pg [START_REF] Lando | Graphs on surfaces and their applications[END_REF][START_REF] Praeger | Low rank representations and graphs for sporadic groups[END_REF][START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF], and the fourth representation is associated with srg(1080, 351, 126, 108) and the geometry NO + (8, 3), see [START_REF] Brouwer | Spectra of graphs[END_REF] for details about the undefined acronyms. The second representation corresponds to the commutation of the 364 three-qutrit '3QT' observables [START_REF] Planat | Pauli graphs when the Hilbert space dimension contains a square: why the Dedekind psi function?[END_REF]. It is found to be of type G 4 . The representation of index 1120 and rank 4 of O 7 (3) found in the Atlas is associated to the dual of W 5 (3) that is the dense near hexagon DQ(6, 3). See table 9 for further details.

Exceptional and twisted

The smallest (simple) twisted exceptional group is Sz [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF]. The representation of index 520 listed in the Atlas leads to an unconnected graph. The representation of index 560 of rank 17 and subdegrees 1, 13 3 , 26 6 , 52 7 leads to a configuration of type [560 13 , 1820 4 ] (i.e. every point is on 13 lines and there are 1820 lines of size 4). The Atlas also provides a representation of index 1456 and rank 79 that leads to another geometry, of order [START_REF] Planat | Unitary reflection groups for quantum fault tolerance[END_REF][START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF], with again 1820 lines of size 4 (see also the relevant item in

Sporadic

The smallest sporadic group is M 11 . The Atlas provides representations of rank 3 and index 55, rank 4 and index 66, and rank 8 and index 165. The first representation leads to the triangular graph T (11) = L(K 11 ). The second one leads two a non strongly regular graph with 495 edges, of girth 4 and diameter 2. The third representation leads to a partial linear space of order (2, 3) with 220 lines/triangles.

Brief summary

The results of this subsection are summarized in Table 3. Observe that the smallest simple linear group is equivalent to A 5 and that the smallest untwisted group G 2 (2) ′ is similar to U 3 [START_REF] Planat | Unitary reflection groups for quantum fault tolerance[END_REF]. Except for M 11 and Sz(8) all these 'small' groups occur in the commutation of quantum observables. Further relations between the geometry of simple groups and the commutation of multiple qudits are given at the next section.

Atlas classes and the related geometries

Alternating

The non trivial configurations that are stabilized by (low rank) small simple alternating groups are listed in It has been shown at the previous section that A 5 and A 6 are associated to threequbit contextuality (via Mermin's pentagram) and two-qubit commutation (via the generalized quadrangle of order two GQ(2, 2)), respectively. Since A 8 encodes the 35 lines in P G(3, 2), the corresponding configuration may be seen as a model of four-qubit contextuality, see [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF]Sec. 4] for the recognition of P G(3, 2) as a model of a 4QB maximum commuting set and [START_REF] Lévay | Grassmannian Connection Between Three-and Four-Qubit Observables, Mermin's Contextuality and Black Holes[END_REF] for an explicit reference to the O + (6, 2) polarity.

As the permutation representation is not in the Atlas, we provide a few details below. The permutation representation on 35 points of A 8 is The representation is of rank 3, with suborbit lengths [START_REF] Planat | Pauli graphs when the Hilbert space dimension contains a square: why the Dedekind psi function?[END_REF][START_REF] Malle | Generation of classical groups[END_REF][START_REF] Praeger | Low rank representations and graphs for sporadic groups[END_REF], and corresponds to a dessin D of signature (B, W, F, G) = (9, 15, 5, 4)), that is, of genus 4, and cycles [6 4 3 3 1 2 , 3 10 1 5 , 7 5 ]. The two-point stabilizer subgroups are of order 32 and 36. The group of order 36 is isomorphic to the symmetry group Z 2 3 × Z 2 2 of the Mermin square (a 3 × 3 grid), see [START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF]Sec. 4.4]. The edges of the collinearity graph of the putative geometry G are defined as sharing the same stabilizer subgroup of order 36, up to isomorphism, but acting on different subsets. The graph is srg of spectrum [16 1 , 2 20 , -4 14 ] and can be found in [START_REF] Brouwer | Spectra of graphs[END_REF]. The lines of G are defined as the maximum cliques of the collinearity graph. In the present case, the lines do not all share the same stabilizer subgroup. One gets G = [35 8 , 56 5 ] (3) , a finite geometry of type G 2 . The collinearity graph associated to the stabilizer subgroup of order 32 is the complement of the collinearity graph of G and the corresponding geometry is Ḡ = [35 6 , 30 7 ] (3) , a configuration of type G 3 , and a model of the O + (6, 2) polarity.

P =< 35|(3,

Linear

The non trivial configurations that are stabilized by (low rank) small simple linear groups are listed in Table 5.

As for a relation to physics, we already know that the linear group L 2 (4) = L 2 (5) = A 5 is associated to a 3QB pentagram and that L 2 (9) = A 6 is associated to 2QB commutation. Then the group L 5 (2) is associated to 5QB contextuality through lines in P G(4, 2). The other configurations in table 5 lack a physical meaning. Table 5. The non trivial configurations stabilized by small simple linear groups and their rank. The configuration [21 2 , 14 3 ] (6) configuration corresponds to the thin generalized hexagon GO(2, 1) (see Fig. 6 of [START_REF] Planat | Geometric contextuality from the Maclachlan-Martin Kleinian groups[END_REF]).

group L n (m) geometries (rank) G (r) κ L 2 (4) = L 2 (5) = A 5 MP, T (

Symplectic

The symplectic class of simple groups is a very useful one for modeling quantum commutation of multiple qudits. At the previous section, we already met groups S ′ 4 (2) and S 4 (3) associated to two-qubits and two-qutrits, respectively.

The group S 4 (3).

Let us go back to the group S 4 (3) whose finite representation is H = a, b|a 2 = b 5 = (ab) 9 = [a, b] 3 = [a, bab] 2 = 1 . Apart from GQ(3, 3) associated to twoqutrits other geometries exist for this group as shown in Table 6.

A few remarks are in order. Stricto sensu, only the generalized quadrangles GQ(2, 4) and GQ(3, 3) are 'stabilized' by the corresponding permutation representations P (and dessins d'enfants D -their signature is given at the second column). The lines of each of the two geometries are defined as having two-stabilizer subgroups acting on the same subsets of points. In a weaker sense, the permutation representation for index 36, 40 a and 45 'define' the geometries OA(6, 3), the dual of GQ(3, 3) and GQ(4, 2) from the collinearity graph, its srg spectrum (shown at the third column) and the structure of its maximum cliques. In these last cases, not all lines of the geometry have their pair of points corresponding to the same two-stabilizer subgroup. Observe that case 40 a and case 40 b are isospectral but with a distinct D-signature.

S 4 (3) index D-
The group S 6 (2). Another group of rich structure is the symplectic group S 6 (2) whose finite representation is H = a, b|a 2 = b 7 = (ab

) 9 = [ab 2 ] 12 = [a, b] 3 , [a, b 2 ] 2 = 1 .
The smallest non-trivial permutation representation P of S 6 (2) stabilizes the symplectic polar space W 5 (3) associated to three-qubits [START_REF] Planat | Pauli graphs when the Hilbert space dimension contains a square: why the Dedekind psi function?[END_REF]. The small permutation representations of S 6 (2) are shown on Table 7 The meaning of bold notation is as in Table 6.

The geometry of multiple qudits.

We define the multiple qudit Pauli group P q (q = p n ) as the n-fold tensor product between single p-dit Pauli operators with ω = exp( 2iπ p ) and p a prime number. Observables of P q /Center(P q ) are seen as the elements of the 2n-dimensional vector space V (2n, p) defined over the field F p . The commutator [., .] : V (2n, p) × V (2n, p) → P ′ q induces a non-singular alternating bilinear form on V (2n, p), and simultaneously a symplectic form on the projective space P G(2n -1, p) over F p .

The |V (2n, q)| = p 2n observables of P q /Center(P q ) are mapped to the points of the symplectic polar space W 2n-1 (p) of cardinality |W 2n-1 (p)| = p 2n -1 p-1 ≡ σ(p 2n-1 ), (where σ(.) is the sum of divisor function of the argument) and two elements of [P q /Center(P q ), ×] commute if and only if the corresponding points of the polar space W 2n-1 (p) are collinear [START_REF] Planat | Pauli graphs when the Hilbert space dimension contains a square: why the Dedekind psi function?[END_REF].

A subspace of V (2n, p) is called totally isotropic if the symplectic form vanishes identically on it. The number of such totally isotropic subspaces/generators g e (of dimension p n -1) is Σ(n) = n i=1 (1 + p i ). A spread s p of a vector space a set of generators partitioning its points. One has

|s p | = p n +1 and |V (2n, p)|-1 = |s p |×|g e | = (p n + 1) × (p n -1) = p 2n -1.
A generator g e corresponds to a maximal commuting set and a spread s p corresponds to a maximum (and complete) set of disjoint maximal commuting sets. Two generators in a spread are mutually disjoint and the corresponding maximal commuting sets are mutually unbiased.

The symplectic polar spaces W 2n-1 (p) at work, alias the commutation structure of n p-dits may be constructed by taking the permutation representation of index σ(p 2n-1 ) of the symplectic (rank 3) group S 2n (p) available in the Atlas. The special case of twoqubits [with S ′ 4 (2)], two-qutrits [with S 4 (3)], three qubits [with S 6 (2)]. For the group S 6 (3), one finds two permutation representations of index 364 and 1120 that are similar to the ones of the same index found for the group O 7 (3) (see Sec. 2, item 'Orthogonal' and Table 9). The representation of index 364 corresponds to the commutation structure of three qutrits and the one of index 1120 is the dual geometry encoding the nonintersection of the 1120 maximum commuting sets of size 26 built with the three-qutrit observables.

The collinearity graph of the polar space

W 2n-1 (p) is a srg(a, pb, b -2, b), with a = a(n) = σ(p 2n-1 ) and b = b(n) = σ(p 2n-3 ). The corresponding geometric configuration is of the form [a(n) Σ(n-1) , Σ(n) (p n -1)/(p-1) ].

Unitary

The unitary class of simple groups is a very rich one. It defines many generalized quadrangles, the hexagons GH(2, 2) associated to 3-qubit contextuality (as shown in Sec. 2, table 3), and two near hexagons including the largest of 'slim dense' near hexagons on 891 points, as shown in Table 8 [START_REF] Bruyn | Near polygons[END_REF]. Whether such configurations have a physical relevance is unknown at the present time. Since unitary groups play a role as normalizers of Pauli groups, it may be expected that some of these geometries occur in the context of quantum error correction and Clifford groups [START_REF] Planat | Unitary reflection groups for quantum fault tolerance[END_REF].

Orthogonal

The geometries carried by orthogonal simple groups of small index are listed in Table 9. It is noticeable that some representations are associated to the non-intersection of maximum commuting sets for three qubits 2]. The srg's are identified in [START_REF] Brouwer | Spectra of graphs[END_REF]. The near hexagon O - 8 (2) There exists a near polygon (thus of type G 1 ) built from O - 8 (2) (on 765 points) that seems to have been unnoticed. The configuration is of the type [765 7 , 1071 5 ] (4) with collinearity graph of spectrum [28 1 , 11 84 , 1 476 , -7 204 ] and diameter 3 corresponding to a near hexagon of order [START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF][START_REF] Howard | Contextuality supplies the magic for quantum computation[END_REF]. Since the permutation representation is a subgroup of the modular group Γ = P SL(2, Z), it is possible to see the dessin D as an hyperbolic polygon D H . As in [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF]11] This closes our investigation between simple groups and finite geometries. The contextuality parameter κ, when it is known, is the highest (exceeding 0.97) for graphs associated to standard representations of L 2 (32), U 3 (4), U 3 [START_REF] Winter | What does an experimental test of contextuality prove and disprove?[END_REF], exceptional groups 2F ′ 4 (2) and Sz(8), and sporadic groups such M 23 , M 24 , Co 2 , McL, He, F i 22 , T , etc.

Conclusion

We explored two-generator permutation representations of simple groups, as listed in the Atlas [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF], with the viewpoint of Grothendieck's dessins d'enfants and the finite geometries associated to them, as started in our earlier work. A strong motivation for this work is the understanding of commutation structures in quantum information and their contextuality [START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF]- [11], [START_REF] Lévay | Grassmannian Connection Between Three-and Four-Qubit Observables, Mermin's Contextuality and Black Holes[END_REF][START_REF] Planat | Geometric contextuality from the Maclachlan-Martin Kleinian groups[END_REF]. A wealth of known and new point-line configurations G, and as much as possible their contextuality parameter κ, are defined from permutation representations P and their corresponding dessin D, using the methodology described in Sec. 2. It is intriguing that the concept of a near polygon, defined in Sec. 2.3, may be usefully expanded to that of a geometry of type G i (i > 1) to qualify some of the new configurations we found. Looking at unitary groups of table 8, one observes that most configurations we obtained are of the near polygon type (that is of type G 1 ) or have a strongly regular collinearity graph. But we do not know how to unify both aspects. To some extent, orthogonal simple groups, as well as exceptional groups of Lie type, have this common feature (as shown in Tables 9 and10, respectively). It is much more involved to recognize the regularities of geometries defined from (small) sporadic groups (see tables 11 to 13). Many sporadic groups (including the Monster) are subgroups of the modular group, or even of the Hurwitz group G = a, b|a 2 = b 3 = (ab) 7 [START_REF] Wilson | The Monster is a Hurwitz group[END_REF]. It is a challenging question to relate the symmetric genus of such structures to the (much smaller) genus of the corresponding dessin d'enfant (and modular polygon) [11]. Our down-to-earth approach of understanding quantum commutation and contextuality from representations of some simple groups is of course far from the concept of a VOA (vertex operator algebra) which is related to string theory and generalized moonshine [START_REF] Gannon | Monstrous moonshine: the fist twenty-five years[END_REF]. As final note, let us mention F. J. Dyson again. So far as we know, the physical universe would look and function just as it does whether or not the sporadic groups existed. But we should not be too sure that there is no connection • • • We have strong evidence that the creator of the universe loves symmetry, and if he loves symmetry, what lovelier symmetry could he find than the symmetry of the Monster? [START_REF] Dyson | Unfashionable pursuits[END_REF].

Figure 1 .

 1 Figure 1. The dessin d'enfant stabilizing the generalized quadrangle GQ(3, 3) (a model of two-qutrit '2QT' commutation). The dessin corresponds to the Sp(4, 3) permutation representation of index 40 b found in the Atlas. Only black points are shown: white points are implicit at the mid-edges or at the ends of half-edges.

  [from O + 8 (2) : 2)] and three qutrits [from O 7 (3) or O + 8 (3)]. These geometries are introduced in [1, Table

Figure 2 .

 2 Figure 2. A schematic of the hyperbolic polygon on 765 tiles corresponding to the permutation group of O - 8 (2). The picture is split into two horizontal parts.

table 10 )

 10 . The physical meaning of both representations, if any, has not been discovered.

	type	group	m r	G	physics	κ
	alternating	A 5	10 3	PG = L(K 5 ) MP in 3QB 0.767
	linear	L 2 (5) = A 5	. .	.	.	;
	symplectic	S ′ 4 (2)	15 3 GQ(2, 2) = L(K 6 )	2QB	.
	.	S 4 (3)	40 3	GQ(3, 3)	2QT	0.800
	unitary	U 3 (3)	63 4	GH(2, 2)	3QB	0.704
	orthogonal	O 7 (3)	364 3	W 5 (3), G 4	3QT	0.846
	except. untwist. G 2 (2) ′ = U 3 (3)	. .	.	.	.
	except. twist.	Sz(8)	560 17	[560 13 , 1820 4 ] (17)	?	0.971
	sporadic	M 11	55 3	T (11) = L(K 11 )	?

Table 3 .

 3 A few characteristics of a index m and rank r = 3 (or higher) representation of the simple group of smallest cardinality in each class. The characteristics of the Sp(4, 3) representation for two qutrits is added to this list. The question marks point out that a physical interpretation is lacking.

Table 4 .

 4 The alternating group A 7 is missing because no non-trivial geometry has been recognized. Permutation groups for alternating groups A n , n > 8 are those listed in the Atlas. T (8) (3) , ([35 6 , 30 7 ] (3) : srg, G 3 , S(2, 3, 15), lines in P G(3, 2), O + (6, 2)) 0.684, 0.737 A 9 T (9) (3) , [126 5 , 315 2 ] (5) , [280 3 , 84 10 ] (5) , [840 4 , 1120 3 ] (12) A 10 T (10) (3) , [126 10 , 210 6 ] (4) : srg), [210 15 , 1575 2 ] (5) , [945 10 , 3150 3 ] (7) A 11 T (11) (3) , [165 8 , 330 4 ] (4) , [462 6 , 1386 2 ] (6) A 12 T (12) (3) , [220 9 , 495 4 ] (4) , [462 12 , 792 7 ] (4)

	The A 8 configuration on 35 points

Table 4 .

 4 The non trivial configurations stabilized by small simple alternating groups and their rank r given as an index. The notation T (n) = L(K

n ) means the triangular graph and S(2, k, v) means a Steiner system, that is, a 2 -(v, k, 1) design

[START_REF] Brouwer | Spectra of graphs[END_REF]

. The symbol srg is for a strongly regular graph. A description of the A 8 configuration on 35 points is given in the text.

Table 6 .

 6 , 1 20 , -5 6 ] [27 5 , 45 3 ] (3) : GQ(2,4) 0.785 36 (8, 24, 4, 1) [15 1 , 3 15 , -3 20 ] [36 15 , 135 4 ] (3) : OA(6,3) 0.833 40 b (8, 28, 6, 0) [12 1 , 2 24 , -4 15 ] [40 4 ] (3) : GQ(3,3) , 3 20 , -3 24 ] [45 3 , 27 5 ] (4) : GQ(4,2) 0.855 Characteristics of small index representations of S 4 (3) and their geometry. The bold notation correspond to geometries that are 'stabilized' by the corresponding permutation representation P. The other geometries that are only 'defined' from the collinearity graph associated to P.

		signature	spectrum	geometry	κ
	27	(7, 15, 3, 2)	[10 1 0.704
	40 a	(8, 24, 8, 1) [12 1 , 2 24 , -4 15 ] [40 4 ] (3) : GQ(3,3) dual 0.825
	45	(9, 29, 7, 1) [12 1

Table 7 .

 7 . The one of index 135 is associated to the near quadrangle DQ(6, 2) [24, chap. 6]. , 5 35 , -1 84 , -7 15 ] [135 7 , 315 3 ] (5) : Characteristics of small index representations of S 6 (2) and their geometry.

	S 6 (2)	D-signature	spectrum	geometry	κ
	63	(9, 47, 7, 1)	[30 787
	120	(16, 60, 14, 15)	[56 1 , 8 35 , -4 84 ]	[120 28 , 1120 3 ] (3)	0.847
	126	(18, 64, 14, 16)	[64 1 , 8 27 , 0 63 , -8 33 ]	[126 64 , 2688 3 ] (5)	0.766
	135	(21, 75, 15, 13)	[14 1 DQ(6,2) 0.794
	240	(36, 120, 28, 29)	[126 1 , 6 84 , 0 120 , -18 35 ]	[240 17280 , 518400 8 ] (5)	0.894
	315	(45, 195, 37, 20)	[18 1 , 9 35 , 3 84 , -3 195 ]	[315 7 , 135 3 ] (5)	0.909
	336	(48, 216, 40, 17)	[20 1 , 8 35 , 2 168 , -4 105 , -8 27 ]	[336 10 , 1120 3 ] (5)	0.918
	960	(138, 480, 114, 115)	[56 1 , 8 385 , -4 504 , -16 70 ]	[960 28 , 8960 3 ] (6)	0.961

1 , 3 35 , -5 27 ] [63 15 , 135 7 ] (3) : G 3 , W 5 (2) 0.

  , the genus g of D equals that of the hyperbolic polygon D H , a face of

	group	D-signature	geometry	κ
	G 2 (2) ′	U 3 (3) in table 8	srg, [63 3 ]; GH(2, 2), GH(2, 2) dual 0.846, 0.820
	G 2 (4)	(88, 224, 32, 37)	[416 8400 , 698830 5 ] (3) : srg, part of Suz graph
		(273, 725, 105, 132)	[1365 5 ] (4) : GH(4, 4)
		(277, 693, 105, 146)	[1365 5 ] (4) : GH(4, 4) dual
	2 F 4 (2) ′ (585, 923, 135, 57)	[1755 5 , 2925 3 ] (5) : GO(2, 4) (Ree-Tits)	0.988
	Sz(8)	(146,288,112,8])	[560 13 , 1820 4 ] (17)	0.971
		(370,736,292,30)	[1456 5 , 1820 4 ] (79)	0.980
	3D 4 (2)	(95,419,63,122)	[819 9 , 2457 3 ] (4) : GH(2, 8)

Table 10 .

 10 Small non-trivial configurations 'defined' by exceptional groups of Lie type. The most remarkable configurations are generalized hexagons, their duals and generalized octagon GO[START_REF]Quantum error correction for quantum memories[END_REF][START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF].Finally, small index representations of small sporadic groups lead to geometries of various types. The results are split into three tables: configurations arising from Mathieu groups in table 11, from Leech lattice groups in table 12 and the remaining ones -small sections of the Monster group and pariahs-in table[START_REF] Lando | Graphs on surfaces and their applications[END_REF]. Niticeable geometries arising from sporadic groups are the M 24 near hexagon NH(2, 14) on 759 points, the J 2 near octagon NO(2, 4) on 315 points and Tits generalized octagon GO[START_REF]Quantum error correction for quantum memories[END_REF][START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF] on 1755 points. Another remarkable geometry is the one built from the McL graph on 275 points, which is found to be of type G 2 , see also https://www.win.tue.nl/∼aeb/graphs/McL.html for details about the McL graph.

	3.7. Sporadic

Table 12 .

 12 Small non-trivial configurations 'defined' by Leech lattice groups. Noticeable geometries are the J 2 near octagon on 315 points and the Co 2 geometry that is locally the U 6 (2) near hexagon. Another remarkable configuration of type G 2 is attached to the permutation representation on 275 points of the McL group. , 2926 3 ] (22) (780, 520, 220, 11) [1540 19 , 14630 2 ] (21) (532, 804, 228, 17) [1596 11 , 8778 2 ] (19) Ru (1054, 2030, 316, 331) srg, index 4060 T= 2 F 4 (2) ′ (585, 923, 135, 57) [1755 5 , 2925 3 ] (5) : GO(2, 4) [21] 0.988 (774, 1152, 180, 100) [2304 26 , 14976 4 ] (7) 0.988

	group	D-signature	geometry	κ
	He	(294, 1106, 122, 269)	[2058 4896 , 3358656 3 ] (5) 0.984
	Fi 22	(270, 2102, 320, 410)	[3510 891 , 142155 22 ] (3) : srg 0.997
	Fi 23	(10575, 16183, 1163, 1876)	srg, index 31671
	Fi ′ 24	(102312, 155224, 10584, 19409)	srg, index 306936
	J 1	(92, 138, 38, 0)	[266 11 , 1463 2 ] (5) : Livingstone graph
		(355, 525, 151, 8)	[1045 8 , 4180 2 ] (11)
		(491, 747, 209, 9)	[1463 6

Table 13 .

 13 Non-trivial configurations 'defined' by small sections of the Monster group, the Pariah groups J 1 and Ru, and Tits group T .

Acknowledgements

The interaction of the two authors was made possible thanks to grants ERGS 1-2013-5527178 and FRGS 11-2014-5524676. Part of the work was completed during the visit of the first author to the Universiti Putra Malaysia in the context of SEAMS School: Algebra and their applications, Nov. 3 to 10 (2015).

group

D-signature geometry κ U 3 (3) [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF][START_REF] Bruyn | Near polygons[END_REF][START_REF] Howard | Contextuality supplies the magic for quantum computation[END_REF]0) [36 28 , 336 3 ] (4) [START_REF] Lando | Graphs on surfaces and their applications[END_REF]35,[START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF][START_REF]Quantum error correction for quantum memories[END_REF] [63 3 ] (4) : GH(2,2) 0.846 [START_REF] Jones | Theory of maps on orientable surfaces[END_REF]35,[START_REF] Planat | Quantum contextual finite geometries from dessins d'enfants[END_REF][START_REF] Planat | Unitary reflection groups for quantum fault tolerance[END_REF] [63 3 ] (5) : GH(2,2) dual 0.820 U 3 [START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF] (70, 112, [START_REF] Malle | Generation of classical groups[END_REF][START_REF] Howard | Contextuality supplies the magic for quantum computation[END_REF] [208 6 , 416 3 ] (5) : conf. over F 16 [START_REF] Brouwer | A construction of the sporadic Suzuki graph from U 3 (4)[END_REF] 0.970 U 3 (5) [START_REF] Planat | Geometry of contextuality from Grothendieck's coset space[END_REF][START_REF] Batten | Combinatorics of finite geometries[END_REF][START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF][START_REF] Winter | What does an experimental test of contextuality prove and disprove?[END_REF] [50 7 , 175 2 ] (3) : Hoffmann-Singleton U 3 [START_REF] Winter | What does an experimental test of contextuality prove and disprove?[END_REF] [START_REF]Quantum error correction for quantum memories[END_REF][START_REF] Batten | Combinatorics of finite geometries[END_REF], respectively: see [START_REF] Bruyn | Near polygons[END_REF] for details about the notation.

Let us feature the U 3 (4) configuration. One defines the 3-dimensional unitary space U over the field F 16 , the projective space P(U) and a nondegenerate Hermitean form (., .) on U. The space P(U) consists of 65 isotropic points x satisfying (x, x) = 0, x = (0, 0, 0), and 208 non-isotropic points satisfying (x, x) = 0. There exist 416 orthogonal bases, that is, triples of mutually orthogonal non-isotropic points. The resulting configuration [208 6 , 416 3 ] (5) has been shown to be related to a 3 -(66, 16, 21) design used to construct the Suzuki sporadic group Suz [START_REF] Brouwer | A construction of the sporadic Suzuki graph from U 3 (4)[END_REF] (see also table 12).

In passing, it is noticeable to feature the hyperplane structure of the U 3 (4) configuration. A basic hyperplane is defined from points of the collinearity graph that are either at minimum or maximal distance from a selected vertex. There are 208 such hyperplanes. The other hyperplanes may be easily built from Velkamp sums H ⊕ H ′ of the basic hyperplanes H and H ′ , where the set theoretical operation ⊕ means the complement of the symmetric difference (H ∪ H ′ ) \ (H ∩ H ′ ) (as in [START_REF] Saniga | Veldkamp-space aspects of a sequence of nested binary Segre varieties[END_REF]). One finds 10 distinct classes of hyperplanes totalizing 2 16

where f is the number of fractions, c is the number of cusps, ν 2 and ν 3 are the number of elliptic points of order two and three of D H , respectively. In the present case, the polygon D H is associated to a non-congruence subgroup of level 17 of Γ and (n, g, ν 2 , ν 3 , c, f ) = (765, [START_REF] Gannon | Monstrous moonshine: the fist twenty-five years[END_REF][START_REF] Lando | Graphs on surfaces and their applications[END_REF][START_REF] Praeger | Low rank representations and graphs for sporadic groups[END_REF]45,250). A schematic of D H is shown in Fig. 2.

Exceptional

A few exceptional groups of low index and low rank are defining well known generalized polygons GH(2, 2) and its dual, GH(4, 4) and its dual, GH [START_REF]Quantum error correction for quantum memories[END_REF][START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF], the Ree-Tits octagon GO [START_REF]Quantum error correction for quantum memories[END_REF][START_REF] Jozsa | Quantum factoring, discrete logarithms and the hidden subgroup problem[END_REF], as well as two extra G 1 geometries [coming from Sz [START_REF] Wilson | ATLAS of Finite Group Representations -Version 3[END_REF]]. This is summarized in Table 10.