Coherent Configurations with Two Fibers

Total Page:16

File Type:pdf, Size:1020Kb

Coherent Configurations with Two Fibers Coherent Configurations 7: Coherent configurations with two fibers Mikhail Klin (Ben-Gurion University) September 1-5, 2014 M. Klin (BGU) Configurations with two fibers 1 / 62 Fibers An association scheme is a particular case of coherent configuration (briefly CC): all loops form one basic graph. In general, in a coherent configuration the full reflexive relation is split into a few parts, each one corresponds to a fiber. A fiber is a combinatorial analogue of an orbit of a permutation group. M. Klin (BGU) Configurations with two fibers 2 / 62 Two fiber coherent configurations In a series of papers, D. Higman attacked coherent configurations of \small type", that is non-trivial types of coherent configurations with two fibers, each of rank at most three. Following Higman, we investigate irreducible ones, that is those that can not be decomposed as direct or wreath products of configurations of a smaller order. M. Klin (BGU) Configurations with two fibers 3 / 62 The type of a CC W with two fibers is a a b matrix , where a is the rank of the c AS on the first fiber, c on the second fiber, b the amount of relations from first to second fiber. Thus rank(W ) = a + 2b + c. Clearly a ≥ 2, c ≥ 2, and for non-trivial cases, b ≥ 2. M. Klin (BGU) Configurations with two fibers 4 / 62 In addition, we require that the AS on each fiber be symmetric. 2 2 The smallest non-trivial type is . 2 It is easy to understand that it is equivalent to the case of symmetric block designs. M. Klin (BGU) Configurations with two fibers 5 / 62 The next interesting \small" type is 2 2 . 3 It is equivalent to quasi-symmetric block designs. This case was carefully investigated by A.R. Calderbank, A. Neumaier, J.J.Seidel, M.S. Shrikhande et al. M. Klin (BGU) Configurations with two fibers 6 / 62 Example 1 Hyperovals in the projective plane Π of order 4. Start from any quadrangle Q in Π, Q = fA; B; C; Dg: Two more points E, F are not collinear with any two elements of Q. M. Klin (BGU) Configurations with two fibers 7 / 62 fA; B; C; D; E; F g is an example of a (hyper-) oval. 21·20·16·9 There are 4! = 2520 quadrangles. 6 Each oval contains 2 = 15 quadrangles. 2520 There are 15 = 168 ovals. M. Klin (BGU) Configurations with two fibers 8 / 62 More about ovals: The simple group PSL(3; 4) of order 20160 acts transitively on points of Π and has 3 orbits of equal size 56 on the set of ovals. Pick one such orbit X . Two ovals from X are adjacent if they are disjoint. M. Klin (BGU) Configurations with two fibers 9 / 62 Now points of Π are points of the design D, ovals from X are blocks of D. We get a biplane D with 21 points and 56 blocks. On blocks we have a primitive triangle-free SRG(56; 10; 0; 2), the Gewirtz graph.. Altogether we have a quasisymmetric BIBD. M. Klin (BGU) Configurations with two fibers 10 / 62 Strongly regular designs We consider the third type (due to 3 2 Higman), that is ( 3 ), which was called by him strongly regular designs (SRD). These are rank 10 coherent configurations with two fibers. They will be subject of main attention in this lecture. M. Klin (BGU) Configurations with two fibers 11 / 62 Each fiber in an SRD induces an SRG (that is, an AS with two classes, or a rank 3 AS). Extra special requirements imply axiomatics of partial geometries. Very beautiful and quite rare structures. M. Klin (BGU) Configurations with two fibers 12 / 62 Example 2 (Partial geometry pg(8; 9; 4)) Start with the Fano plane F , also known as PG(2; 2). 3 5 6 7 1 4 2 Aut(F ) =∼ PSL(3; 2) is a simple group of order 168. M. Klin (BGU) Configurations with two fibers 13 / 62 Add one more point 8 to the point set of F . Consider the action of the alternating group A8 on all images of such a structure (under S8). There are two orbits of equal length 8! 2·168 = 120. Pick one such orbit V . M. Klin (BGU) Configurations with two fibers 14 / 62 Define a graph Γ with vertex set V . Two copies of F are adjacent () they do not share a common line. Get an SRG Γ with parameters (120; 63; 30; 36): M. Klin (BGU) Configurations with two fibers 15 / 62 The graph Γ contains 2025 cliques of size 8. Among the orbits of A8 on these cliques there are orbits of lengths 120 and 15. Pick these orbits and get a set L of size 135 consisting of 8-element subsets of V . M. Klin (BGU) Configurations with two fibers 16 / 62 The structure (V ; L) provides an example of a partial geometry pg(8; 9; 4). Details will be communicated during the exercises. This model is due to Klin-Reichard (1997). M. Klin (BGU) Configurations with two fibers 17 / 62 Extra comments ∼ 6 In fact, Aut(Γ) = (Z) :A8. There are altogether four partial geometries with the same point graph Γ, having groups 1 of order 28!, 1440, 1344 (twice). The graph Γ was discovered by Brouwer-A.V. Ivanov-Klin (1989). M. Klin (BGU) Configurations with two fibers 18 / 62 Altogether (up to isomorphism) there are eight known pg(8; 9; 4). Contributions by A.M. Cohen, R. Mathon and A.P. Street. Full list of all pg(8; 9; 4) is not yet known. M. Klin (BGU) Configurations with two fibers 19 / 62 An SRD is called proper if it does not come from a partial geometry. An SRD is called primitive if both point and line graphs are primitive SRG's. M. Klin (BGU) Configurations with two fibers 20 / 62 Structure of SRDs Each fiber in SRD induces a strongly regular graph (that is, a rank 3 scheme). Higman required that both SRGs are primitive. This is a strong requirement: there are just three parameter sets on up to 1000 vertices (for certain proper cases, those that are not coming from partial geometries). We omit requirements of primitivity. M. Klin (BGU) Configurations with two fibers 21 / 62 Results The list of feasible parameter sets increases drastically. Let n1; n2 be the sizes of the two fibers, n = max(n1; n2). Then we get 22 parameter sets for n ≤ 20, 318 for n ≤ 100 and 869 for n ≤ 200. Using computer, smallest parameter sets were investigated, all SRDs were classified (a few feasible parameter sets were killed). M. Klin (BGU) Configurations with two fibers 22 / 62 Recall that a graph Γ is called coherent if it is a basic graph of its WL-closure W (Γ). Special interest goes to coherent non-Schurian graphs. We combine this requirement with consideration of an incidence graph of an SRD. M. Klin (BGU) Configurations with two fibers 23 / 62 Thus we consider the incidence structure (P; B; F ), where P is a set of points, B a set of blocks, and F a set of flags, here F ⊆ P × B, and P and B are disjoint non-empty sets. The dual incidence structure is (B; P; F T ), where F T = f(y; x)j(x; y) 2 F g. M. Klin (BGU) Configurations with two fibers 24 / 62 A strongly regular design (SRD) is a finite incidence structure with n1 points and n2 blocks which satisfies the following conditions (together with the corresponding conditions, formulated for their duals): 1 Each block is incident to S1 points. 2 Two distinct blocks are incident with either a1 or b1 points, a1 > b1, and both cases occur. M. Klin (BGU) Configurations with two fibers 25 / 62 This allows us to define the block graph Γ2 to be the graph whose vertices are blocks, two distinct blocks being adjacent if they are incident with a1 common points. 3 The number of blocks incident with a point x and adjacent to a block y is N2 or P2, according as x and y are incident or not. M. Klin (BGU) Configurations with two fibers 26 / 62 There are also the dual conditions 1', 2', 3': we understand the same conditions 1, 2, 3, just formulated for the dual structure. In the constants applying to the dual we change the index from 1 to 2 or vice versa. Thus, by definition the SRD's form a self-dual class of designs. M. Klin (BGU) Configurations with two fibers 27 / 62 An SRD Γ is called algebraically (or formally) self-dual (or symmetric) if all parameters of Γ coincide with the corresponding parameters of its dual ΓT . A symmetric SRD (SSRD) Γ is (combinatorially) self-dual if it allows a duality, that is, if Γ and ΓT are isomorphic incidence structures. M. Klin (BGU) Configurations with two fibers 28 / 62 Higman lists 15 numerical equations for the parameter sets of an SRD. Unfortunately there is a (typographical?) mistake in the formulation of Condition 15. This is why in our consideration we were omitting this Condition 15. M. Klin (BGU) Configurations with two fibers 29 / 62 The first job was to generate the list of feasible parameters of SRD's with n up to 200, n = max(n1; n2). The list contains for each of the two designs Γ and ΓT the parameters (ni ; si ; ai ; bi ; Ni ; Pi ), i = 1; 2, as well as the parameters (k; λ, µ, r; s; f ; g) for both accompanying SRG's (point and block graphs).
Recommended publications
  • Finite Projective Geometries 243
    FINITE PROJECTÎVEGEOMETRIES* BY OSWALD VEBLEN and W. H. BUSSEY By means of such a generalized conception of geometry as is inevitably suggested by the recent and wide-spread researches in the foundations of that science, there is given in § 1 a definition of a class of tactical configurations which includes many well known configurations as well as many new ones. In § 2 there is developed a method for the construction of these configurations which is proved to furnish all configurations that satisfy the definition. In §§ 4-8 the configurations are shown to have a geometrical theory identical in most of its general theorems with ordinary projective geometry and thus to afford a treatment of finite linear group theory analogous to the ordinary theory of collineations. In § 9 reference is made to other definitions of some of the configurations included in the class defined in § 1. § 1. Synthetic definition. By a finite projective geometry is meant a set of elements which, for sugges- tiveness, are called points, subject to the following five conditions : I. The set contains a finite number ( > 2 ) of points. It contains subsets called lines, each of which contains at least three points. II. If A and B are distinct points, there is one and only one line that contains A and B. HI. If A, B, C are non-collinear points and if a line I contains a point D of the line AB and a point E of the line BC, but does not contain A, B, or C, then the line I contains a point F of the line CA (Fig.
    [Show full text]
  • Con Gurations in Quantum Information
    Congurations in Quantum Information Kate Blancheld Department of Physics Stockholm University Licentiate thesis Thesis for the degree of Licentiate in Physics Department of Physics Stockholm University Sweden ⃝c Kate Blancheld 2012 ⃝c Elsevier (papers) ⃝c American Physical Society (papers) iii Abstract Measurements play a central role in quantum information. This thesis looks at two types: contextual measurements and symmetric measurements. Con- textuality originates from the Kochen-Specker theorem about hidden variable models and has recently undergone a subtle shift in its manifestation. Sym- metric measurements are characterised by the regular polytopes they form in Bloch space (the vector space containing all density matrices) and are the subject of several investigations into their existence in all dimensions. We often describe measurements by the vectors in Hilbert space onto which our operators project. In this sense, both contextual and symmetric measurements are connected to special sets of vectors. These vectors are often special for another reason: they form congurations in a given incidence geometry. In this thesis, we aim to show various connections between congurations and measurements in quantum information. The congurations discussed here would have been well-known to 19th and 20th century geometers and we show they are relevant for advances in quantum theory today. Specically, the Hesse and Reye congurations provide proofs of measurement contextu- ality, both in its original form and its newer guise. The Hesse conguration also ties together dierent types of symmetric measurements in dimension 3called SICs and MUBswhile giving insights into the group theoretical properties of higher dimensional symmetric measurements. iv Acknowledgements Thank you to Ingemar for being an excellent supervisor.
    [Show full text]
  • COMPUTERS in SCIENTIFIC DISCOVERY 6 (CSD6) Portorož, Slovenia, 21 – 25 August 2012
    Abstracts of the Workshop COMPUTERS IN SCIENTIFIC DISCOVERY 6 (CSD6) Portorož, Slovenia, 21 – 25 August 2012 UP IAM August 2012 Abstracts of the Workshop Computers in Scientific Discovery 6 (CSD6) Portorož, Slovenia, 21 – 25 August 2012 UP IAM August 2012 WELCOME We thank all of you for coming and wish you a pleasant and successful workshop in Portorož. Computers and Scientific Discovery 6 aims to continue the deliberately multidisciplinary emphasis of these conferences, provide space for collaborations and follow-up on results of the previous meetings, and expand even further the range of topics covered. As the first of the series to be held in Slovenia, CSD6 will benefit from the strong local tradition of research in pure and applied graph theory. Much of the importance of interdisciplinary meetings comes from their influence in break- ing down "language barriers" between fields, and in opening the eyes of researchers in one field to the expertise and challenges available in another. Our workshop format, which com- bines formal presentations from invited speakers with contributed talks, and builds in plenty of time for free discussion between active researchers, is designed to facilitate these aims. Tomaž Pisanski Klavdija Kutnar Patrick Fowler Portorož, August 21, 2012 CONTENTS CSD6 5 Welcome .......................................................5 Contents . .7 General Information . .9 Special Events . 11 Past Workshops . 13 A few words about the University of Primorska . 15 Abstracts 17 Keynote Talks . 17 Oswin Aichholzer: The Order Type Data Base ........................... 18 Alexandru Balaban: Dualists of Two-Dimensional and Three-Dimensional Classes of Molecules: Benzenoids and Diamondoids ......................... 19 Gunnar Brinkmann: Snarks – and Beyond? ...........................
    [Show full text]
  • Marston D. E. Conder · Antoine Deza Asia Ivić
    Springer Proceedings in Mathematics & Statistics Marston D. E. Conder · Antoine Deza Asia Ivić Weiss Editors Discrete Geometry and Symmetry Dedicated to Károly Bezdek and Egon Schulte on the Occasion of Their 60th Birthdays Springer Proceedings in Mathematics & Statistics Volume 234 [email protected] Springer Proceedings in Mathematics & Statistics This book series features volumes composed of selected contributions from workshops and conferences in all areas of current research in mathematics and statistics, including operation research and optimization. In addition to an overall evaluation of the interest, scientific quality, and timeliness of each proposal at the hands of the publisher, individual contributions are all refereed to the high quality standards of leading journals in the field. Thus, this series provides the research community with well-edited, authoritative reports on developments in the most exciting areas of mathematical and statistical research today. More information about this series at http://www.springer.com/series/10533 [email protected] Marston D. E. Conder • Antoine Deza Asia Ivić Weiss Editors Discrete Geometry and Symmetry Dedicated to Károly Bezdek and Egon Schulte on the Occasion of Their 60th Birthdays 123 [email protected] Editors Marston D. E. Conder Asia Ivić Weiss Department of Mathematics Department of Mathematics University of Auckland and Statistics Auckland York University New Zealand Toronto, ON Canada Antoine Deza Department of Computing and Software McMaster University Hamilton, ON Canada ISSN 2194-1009 ISSN 2194-1017 (electronic) Springer Proceedings in Mathematics & Statistics ISBN 978-3-319-78433-5 ISBN 978-3-319-78434-2 (eBook) https://doi.org/10.1007/978-3-319-78434-2 Library of Congress Control Number: 2018939138 Mathematics Subject Classification (2010): 05B40, 05B45, 52A10, 52A21, 52A35, 52B10, 52B11, 52B15, 52C15, 52C17, 52C20, 52C35, 52C45, 90C05, 90C27 © Springer International Publishing AG, part of Springer Nature 2018 This work is subject to copyright.
    [Show full text]
  • Marston D. E. Conder · Antoine Deza Asia Ivić Weiss Editors Dedicated To
    Springer Proceedings in Mathematics & Statistics Marston D. E. Conder · Antoine Deza Asia Ivić Weiss Editors Discrete Geometry and Symmetry Dedicated to Károly Bezdek and Egon Schulte on the Occasion of Their 60th Birthdays Springer Proceedings in Mathematics & Statistics Volume 234 Springer Proceedings in Mathematics & Statistics This book series features volumes composed of selected contributions from workshops and conferences in all areas of current research in mathematics and statistics, including operation research and optimization. In addition to an overall evaluation of the interest, scientific quality, and timeliness of each proposal at the hands of the publisher, individual contributions are all refereed to the high quality standards of leading journals in the field. Thus, this series provides the research community with well-edited, authoritative reports on developments in the most exciting areas of mathematical and statistical research today. More information about this series at http://www.springer.com/series/10533 Marston D. E. Conder • Antoine Deza Asia Ivić Weiss Editors Discrete Geometry and Symmetry Dedicated to Károly Bezdek and Egon Schulte on the Occasion of Their 60th Birthdays 123 Editors Marston D. E. Conder Asia Ivić Weiss Department of Mathematics Department of Mathematics University of Auckland and Statistics Auckland York University New Zealand Toronto, ON Canada Antoine Deza Department of Computing and Software McMaster University Hamilton, ON Canada ISSN 2194-1009 ISSN 2194-1017 (electronic) Springer Proceedings in Mathematics & Statistics ISBN 978-3-319-78433-5 ISBN 978-3-319-78434-2 (eBook) https://doi.org/10.1007/978-3-319-78434-2 Library of Congress Control Number: 2018939138 Mathematics Subject Classification (2010): 05B40, 05B45, 52A10, 52A21, 52A35, 52B10, 52B11, 52B15, 52C15, 52C17, 52C20, 52C35, 52C45, 90C05, 90C27 © Springer International Publishing AG, part of Springer Nature 2018 This work is subject to copyright.
    [Show full text]
  • Arxiv:Math/0507118V1
    CONFIGURATIONS OF LINES AND MODELS OF LIE ALGEBRAS L. MANIVEL Abstract. The automorphism groups of the 27 lines on the smooth cubic surface or the 28 bitangents to the general quartic plane curve are well-known to be closely related to the Weyl groups of E6 and E7. We show how classical subconfigurations of lines, such as double-sixes, triple systems or Steiner sets, are easily constructed from certain models of the exceptional Lie algebras. For e7 and e8 we are lead to beautiful models graded over the octonions, which display these algebras as plane projective geometries of subalgebras. We also interprete the group of the bitangents as a group of transformations of the triangles in the Fano plane, and show how this is related to an interpretation of the isomorphism P SL(3, F2) ≃ P SL(2, F7) in terms of harmonic cubes. 1. Introduction Such classical configurations of lines as the 27 lines on a complex cubic surface or the 28 bitangents to a smooth quartic plane curve have been extensively studied in the 19th century (see e.g. [21]). Their automorphism groups were known, but only at the beginning of the 20th century were their close connections with the Weyl groups of the root systems E6 and E7, recognized, in particular through the relation with Del Pezzo surfaces of degree three and two, respectively [8, 9]. Del Pezzo surfaces of degree one provide a similar identification of the diameters of the root system E8, with the 120 tritangent planes to a canonical space curve of genus 4.
    [Show full text]
  • The Generalized Reye Configuration
    Also available at http://amc.imfm.si ISSN 1855-3966 (printed edn.), ISSN 1855-3974 (electronic edn.) ARS MATHEMATICA CONTEMPORANEA 3 (2010) 21–27 The generalized Reye configuration Brigitte Servatius , Herman Servatius Mathematics Department, Worcester Polytechnic Institute 100 Institute Road, Worcester, MA 01609-2280, USA Received 29 June 2009, accepted 29 November 2009, published online 28 January 2010 Abstract Given an embedding in the plane of the vertices of a cube, we consider conditions on the embedded vertices such that they are the projection of the vertices of a 3 dimensional polyhedron combinatorially equivalent to the cube. We are particularly interested in con- ditions expressible as incidence conditions for the lines induced by the given vertex set in the plane. We show that the vertices and their incidences extend to a Reye configuration in the plane if and only if the vertices are the projection of a parallelepiped. More generally, the positions of the embedded vertices result from projecting a polyhedron combinatori- ally equivalent to the cube if and only if they belong to a plane configuration we call the generalized Reye configuration. Keywords: Reye’s configuration, generic picture, sharp lift. Math. Subj. Class.: 51A05, 51A20, 51D20 1 Introduction In [6], Theodor Reye addressed several questions concerning configurations and in [7] he examined what is now called Reye’s configuration. An exposition of its properties is contained in [4,5,3] and a historical account is contained in [2]. For a modern application to quantum mechanics see [1]. A point–line configuration of type (pn; lm) is a finite set of p points and l lines such that on each line there are m points and through each point there are n lines.
    [Show full text]
  • [Math.AG] 18 Apr 2003
    ABSTRACT CONFIGURATIONS IN ALGEBRAIC GEOMETRY I. DOLGACHEV To the memory of Andrei Tyurin Abstract. An abstract (vk,br)-configuration is a pair of finite sets of cardinalities v and b with a relation on the product of the sets such that each element of the first set is related to the same number k of elements from the second set and, conversely, each element of the second set is related to the same number r of el- ements in the first set. An example of an abstract configuration is a finite geometry. In this paper we discuss some examples of abstract configurations and, in particular finite geometries, which one encounters in algebraic geometry. CONTENTS 1. Introduction 2. Configurations, designs and finite geometries 3. Configurations in algebraic geometry 4. Modular configurations 5. The Ceva configurations 6. v3-configurations 7. The Reye (124, 163)-configuration 8. vv−1-configurations 9. The Cremona-Richmond 153-configuration 10. The Kummer configurations 2 11. A symmetric realization of P (Fq) arXiv:math/0304258v1 [math.AG] 18 Apr 2003 1. Introduction In this paper we discuss some examples of abstract configurations and, in particular finite geometries, which one encounters in algebraic geometry. The Fano Conference makes it very appropriate because of the known contribution of Gino Fano to finite geometry. In his first published paper [18] he gave a first synthetical definition of the projective plane over an arbitrary field. In [18] introduces his famous Fano’s Postulate. It asserts that the diagonals of a complete quadrangle do not intersect at one point. Since this does not hold for the projective plane over a finite field of two elements (the Fano plane), the postulate 1 2 I.
    [Show full text]
  • CONFIGURATIONS from a Graphical Viewpoint
    1 CONFIGURATIONS From a graphical viewpoint Tomaˇz Pisanski1 IMFM Oddelek za teoretiˇcnoraˇcunalniˇstvo Univerza v Ljubljani Jadranska 19, 1111 Ljubljana Slovenija [email protected] and Brigitte Servatius WPI USA [email protected] Copyright °c , TomaˇzPisanski, Brigitte Servatius 1999–2004 Ljubljana, 2004 2 The first author used the notes as a reading material for students of a graduate course Konfiguracije in grafi (Configurations and Graphs) at the University of Ljubljana, Slovenia, 1999–2000. Several people contributed to these notes. Aleksandar Juriˇsi´c suggested several important references. Several co-authors allowed him to include parts of our joint work verbatim in the earlier versions of the manuscript. We are grateful to Anton Betten, Marko Boben, Gunnar Brinkmann, Marston Conder, Milan Hladnik, Ante Graovac, Harald Gropp, Aleksander Malniˇc, Dragan Maruˇsiˇc,Alen Orbani´c, Marko Petkovˇsek, PrimoˇzPotoˇcnik,Milan Randi´c,Steve Wilson, and Arjana Zitnikˇ , for that. We would like to thank Marko Boben, J¨urgen Bokowski, Chris Godsil, Josef Leydold, Alen Orbani´c, Marko Petkovˇsek, Bor Plestenjak, John Shawe-Taylor, for reading several versions of the manuscript or prats of the manuscript, giving some very interesting suggestions. After finishing teaching the course T.P. ceased working on the manuscript for about seven months. When he started preparing these notes he was un- aware of some of the most recent work on configurations of Branko Gr¨unbaum. We would like to thank him for sharing his work with us. After receiving his notes for a graduate course on configurations [45] T.P. resumed his work on the manuscript in January 2001 and began adjusting terminology with that of Gr¨unbaum in all feasible cases.
    [Show full text]
  • Danzer's Configuration Revisited Arxiv:1301.1067V2 [Math.CO] 6 Jan 2015
    Danzer's configuration revisited Marko Boben G´abor G´evay Faculty of Computer Science Bolyai Institute University of Ljubljana University of Szeged 1000 Ljubljana, Slovenia Aradi v´ertan´uktere 1. and 6720 Szeged, Hungary University of Primorska, IAM [email protected] Muzejski trg 2 6000 Koper, Slovenia [email protected] TomaˇzPisanski∗ Faculty of Mathematics and Physics University of Ljubljana 1111 Ljubljana, Slovenia and University of Primorska, FAMNIT Glagoljaˇska 8 6000 Koper, Slovenia [email protected] June 5, 2018 arXiv:1301.1067v2 [math.CO] 6 Jan 2015 ∗The first and third author were supported in part by the ARRS of Slovenia, grants: P1- 0294 and N1-0011: GReGAS, and by the European Science Foundation. The second and third author were supported by the European Union and co-funded by the European Social Fund; project title: \Telemedicine-focused research activities on the field of Mathematics, Informatics and Medical Sciences"; project number: TAMOP-4.2.2.A-11/1/KONV-2012-´ 0073. 1 Dedicated to the memory of Ludwig Danzer (1927-2011) Abstract We revisit the configuration of Danzer DCD(4), a great inspiration for our work. This configuration of type (354) falls into an infinite series of geometric point-line configurations DCD(n). Each DCD(n) is characterized combinatorially by having the Kronecker cover over the Odd graph On as its Levi graph. Danzer's configuration is deeply rooted in Pascal's Hexagrammum Mysticum. Although the combina- torial configuration is highly symmetric, we conjecture that there are no geometric point-line realizations with 7- or 5-fold rotational sym- metry; on the other hand, we found a point-circle realization having the symmetry group D7, the dihedral group of order 14.
    [Show full text]
  • 1 Introduction
    The Tomotope Barry Monson University of New Brunswick, Fredericton, New Brunswick, Canada E3B 5A3 Daniel Pellicer Instituto de Matem´eticasUNAM - Unidad Morelia, M´exico Gordon Williams University of Alaska Fairbanks, Fairbanks, Alaska 99775-6660 Keywords: abstract regular or uniform polytopes. Abstract Every abstract 3-polytope M, in particular, every polyhedral map, has a unique minimal regular cover, and the automorphism group of this cover is isomorphic to the monodromy group of M. Here we demonstrate that the situation for polytopes of higher rank must be very different: the tomotope T is a small, highly involved, abstract uniform 4-polytope. It has infinitely many distinct minimal regular covers. 1 Introduction The monodromy group is a most useful tool when one tries to understand com- binatorial properties of maps, such as coverings, automorphism groups, flag orbits, stellations, and so forth; see [10, x3] and [8], for example. Changing our structural viewpoint a little, we may consider polyhedral maps, at least, to be abstract 3-polytopes. This paper arose as a by-product of a wider effort [17] to understand basic combinatorial constructions for abstract polytopes in all ranks. In this setting, the monodromy group already appeared in [5] (as the image of the ‘flag action'). One of our concerns is to understand how an n-polytope P, with no particu- lar attributes of symmetry, can be covered by a regular n-polytope R. When P has rank n = 3, there is a minimal such regular cover, intimately related to the monodromy group of P. (This fact seems to be well-known, but we must refer to [17] for an easy proof.) On the other hand, our attempts to extend the result to higher ranks are thwarted by that best of all reasons, a counterexample.
    [Show full text]
  • Russell's Theory of Geometry in the Principles of Mathematics
    Toward a topic-specific logicism? Russell’s theory of geometry in the Principles of Mathematics Sébastien Gandon To cite this version: Sébastien Gandon. Toward a topic-specific logicism? Russell’s theory of geometry in the Principles of Mathematics. Philosophia Mathematica, Oxford University Press (OUP), 2008, 16 (3), pp.1-39. halshs-00326371 HAL Id: halshs-00326371 https://halshs.archives-ouvertes.fr/halshs-00326371 Submitted on 17 Oct 2008 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Toward a topic-specific logicism? Russell’s theory of geometry in the Principles of Mathematics. Sébastien Gandon PHIER, Université Clermont-Ferrand II, 4 rue Ledru, 63000 Clermont-Ferrand, FRANCE “The tragedy of Russell’s paradox was to obscure from Frege and from us the great interest of his actual positive accomplishment”. ([Boolos, 1998], p. 267) ABSTRACT: Russell’s philosophy is rightly described as a programme of reduction of mathematics to logic. Now, the theory of geometry developed in 1903 does not fit this picture well, since it is deeply rooted in the purely synthetic projective approach, which conflicts with all the endeavours to reduce geometry to analytical geometry. The first goal of this paper is to present an overview of this conception.
    [Show full text]