Mathieu Dutour and Michel Deza- Goldberg-Coxeter construction for - or -valent plane graphs

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    Goldberg-Coxeter

    construction

    for - or -valent plane graphsMathieu Dutour

    ENS/CNRS, Paris and Hebrew University, Jerusalem

    Michel Deza

    ENS/CNRS, Paris and ISM, Tokyo

    p.1/4

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    Goldberg-Coxeter for the Cube

    1,0

    p.2/4

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    Goldberg-Coxeter for the Cube

    1,1

    p.2/4

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    Goldberg-Coxeter for the Cube

    2,0

    p.2/4

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    Goldberg-Coxeter for the Cube

    2,1

    p.2/4

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    History

    Mathematics: construction of planar graphs

    M. Goldberg, A class of multisymmetric polyhedra,Tohoku Math. Journal, 43 (1937) 104108.

    Objective was to maximize the interior volume of thepolytope, i.e. to find

    -dimensional analogs of regularpolygons.

    search of equidistributed systems of points on the spherefor application to Numerical Analysis.

    p.3/4

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    History

    Biology: explanation of structure of icosahedral viruses

    D.Caspar and A.Klug, Physical Principles in the Con-struction of Regular Viruses, Cold Spring HarborSymp. Quant. Biol., 27 (1962) 1-24.

    symmetry capsid of virion

    gemini virus

    hepathite B

    , laevo HK97, rabbit papilloma virus

    , laevo rotavirus

    herpes virus, varicella

    adenovirus

    ?

    , laevo HIV-1

    p.3/4

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    History

    Architecture: construction of geodesic domesPatent by Buckminster Fuller

    EPCOT in Disneyland.

    p.3/4

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    History

    Mathematics:

    H.S.M. Coxeter, Virus macromolecules andgeodesic domes, in A spectrum of mathematics; ed.

    by J.C.Butcher, Oxford University Press/AucklandUniversity Press: Oxford, U.K./Auckland New-Zealand, (1971) 98107.

    p.3/4

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    History

    Chemistry: Buckminsterfullerene

    (football, Truncated Icosahedron)

    Kroto, Kurl, Smalley (Nobel prize 1996) syn-

    thetized in 1985 a new molecule, whose graph is

    .

    Osawa constructed theoretically

    in 1984.

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    I. ZigZags

    and

    central circuits

    p.4/4

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    Central circuits

    A 4valent plane graph G

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    Central circuits

    Take an edge of G

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    Central circuits

    Continue it straight ahead ...

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    Central circuits

    ... until the end

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    Central circuits

    A selfintersecting central circuit

    p.5/4

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    Central circuits

    A partition of edges of G

    CC=4 , 6, 82 p.5/4

    Zi Z

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    Zig Zags

    A plane graph G

    p.6/4

    Zi Z

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    Zig Zags

    Take two edges

    p.6/4

    Zi Z

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    Zig Zags

    Continue it leftright alternatively ....

    p.6/4

    Zig Zags

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    Zig Zags

    ... until we come back

    p.6/4

    Zig Zags

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    Zig Zags

    A selfintersecting zigzag

    p.6/4

    Zig Zags

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    Zig Zags

    A double covering of 18 edges: 10+10+16

    z=10 , 162zvector p.6/4

    Notations

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    Notations

    ZC-circuit stands for zigzag or central circuit in

    - or

    -valent plane graphs.

    The length of a ZC-circuit is the number of its edges.

    The ZC-vector of a

    - or

    -valent plane graph

    is thevector

    where is the number of

    ZC-circuits of length

    .

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    II. Goldberg-Coxeter

    construction

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    The construction

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    The construction

    Take a

    - or

    -valent plane graph

    . The graph

    isformed of triangles or squares.

    Break the triangles or squares into pieces:

    3valent case

    k=5

    l=2

    l=2

    k=5

    4valent case p.9/4

    Gluing the pieces

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    Gluing the pieces

    Glue the pieces together in a coherent way.

    We obtain another triangulation or quadrangulation ofthe plane.

    Case

    -valent Case

    -valent p.10/4

    Gluing the pieces

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    Gluing the pieces

    Glue the pieces together in a coherent way.

    We obtain another triangulation or quadrangulation ofthe plane.

    :

    -valent

    :

    -valent p.10/4

    Gluing the pieces

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    Gluing the pieces

    Glue the pieces together in a coherent way.

    We obtain another triangulation or quadrangulation ofthe plane.

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    Gluing the pieces

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    Gluing the pieces

    Glue the pieces together in a coherent way.

    We obtain another triangulation or quadrangulation ofthe plane.

    p.10/4

    Final steps

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    Final steps

    Go to the dual and obtain a

    - or

    -valent plane graph,which is denoted

    and called

    Goldberg-Coxeter construction.

    The construction works for any

    - or

    -valent map onoriented surface.

    Operation

    p.11/4

    Example of

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    Example of

    p.12/4

    Example of

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    Example of

    p.12/4

    Example of

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    Example of

    p.12/4

    Example of

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    p

    p.12/4

    Example of

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    p

    p.12/4

    Example of

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    p

    p.12/4

    Example of

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    p

    p.12/4

    Properties

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    p

    One associates

    (Eisenstein integer) or

    (Gaussian integer) to the pair

    in

    - or

    -valent case.

    If one writes

    instead of

    , then onehas:

    If

    has

    vertices, then

    has

    vertices if

    is

    -valent,

    vertices if

    is

    -valent.

    If

    has a plane of symmetry, we reduce to

    .

    has all rotational symmetries of

    and all

    symmetries if

    or

    . p.13/4

    The case

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    Case

    -valent Case

    -valent

    p.14/4

    The case

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    Case

    -valent Case

    -valent

    p.14/4

    The case

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    Case

    -valent

    is called leapfrog

    (=Truncation of the dual)

    Case

    -valent

    is called medialBonjour

    p.14/4

    Goldberg Theorem

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    is the class of

    -valent plane graphs having only

    -and

    -gonal faces.

    The class of

    -valent plane graphs having only

    - and

    -gonal faces is called Octahedrites.

    Class Groups Construction

    ,

    Tetrahedron

    ,

    Cube

    ,

    Prism

    !

    ,

    Dodecahedron

    Octahedrites "

    ,

    Octahedron

    p.15/4

    The special case

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    Any ZC-circuit of

    corresponds to

    ZC-circuits of

    with length multiplied by

    .

    If the ZC-vector of

    is

    , then the ZC-vector

    of

    is

    .

    p.16/4

    The special case

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    Any ZC-circuit of

    corresponds to

    ZC-circuits of

    with length multiplied by

    .

    If the ZC-vector of

    is

    , then the ZC-vector

    of

    is

    .

    p.16/4

    The special case

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    Any ZC-circuit of

    corresponds to

    ZC-circuits of

    with length multiplied by

    .

    If the ZC-vector of

    is

    , then the ZC-vector

    of

    is

    .

    p.16/4

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    III. The

    -product

    p.17/4

    The mapping

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    We always assume

    if

    if

    is bijective and periodic with period

    .Example: Case

    ,

    :

    operations:

    p.18/4

    The

    -product

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    Definition 0 (The

    -product)If

    and

    are two elements of a group,

    and

    ; we define

    by

    and

    .Set

    if

    and

    if

    ;then set

    By convention, set

    and

    .For

    ,

    , one gets the expression

    A similar notion is introduced by Norton (1987) inGeneralized Moonshine for the Monster group.

    p.19/4

    Properties

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    If

    and

    commute,

    Euclidean algorithm formula

    if

    if

    If

    and

    do not commute, then

    .

    p.20/4

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    IV. ZC-circuits

    in

    p.21/4

    Position mapping, -valent case

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    A zigzag in

    0GC (G )5,2

    p.22/4

    Position mapping, -valent case

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    Put an

    on it

    Orientation

    p.22/4

    Position mapping, -valent case

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    e

    1 2 3 4 5

    6

    7

    A directed

    edge e

    A position p=3

    Encoding:

    a pair ( e, 3)

    p.22/4

    Position mapping, -valent case

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    1 2 3 4 5

    6

    7

    k=5

    l=2

    e

    Go to the

    Dual !

    p.22/4

    Position mapping, -valent case

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    l=2

    k=5

    1

    6

    7

    5432

    3 4 521

    is

    1f

    Image of ( e, 3)

    ( f , 5)

    1 e

    p.22/4

    Position mapping, -valent case

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    l=2

    k=5

    1

    6

    7e

    5432

    is

    2 3 4 5

    6

    7

    f2

    Image of ( e, 6)

    ( f , 1)

    2

    p.22/4

    Iteration

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    Position mapping is denoted

    =

    or

    =

    . So, one defines Iterated position

    mapping as

    .

    is the set of directed edges of

    .

    is a

    permutation of

    .

    For every ZC-circuit with pair

    denote

    the smallest

    , such that

    .

    For any ZC-circuit of

    one has:

    =

    -valent case

    =

    -valent case

    The [ZC]-vector of

    is the vector

    where is the number of ZC-circuits with order . p.23/4

    The mappings and

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    and

    are the following permutation of

    with

    and

    being the first and second choice.Example of Cube

    Dual Cube

    p.24/4

    The mappings and

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    24 Directed Edges

    p.24/4

    The mappings and

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    L(e)

    L(L(e))

    e

    Successive images of e by L

    p.24/4

    The mappings and

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    R(e)

    R(R(e))

    e

    Successive images of e by R

    p.24/4

    Moving group and Key Theorem

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    is the moving groupIn Cube: a subgroup of

    .

    For

    , denote

    the vector

    with multiplicities

    being the half of the number ofcycles of length in the permutation acting on the set

    .In Cube:

    Key Theorem One has for all

    - or

    -valent plane graphs

    and all

    of

    p.25/4

    Solution of the Cube case

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    and

    do not commute

    .

    =

    normal subgroup of index

    of

    .

    is of order

    .

    divisible by

    Elements of

    have order

    . Elements of

    have order

    .

    Cube

    has [ZC]=

    if

    and [ZC]=

    ,

    otherwise

    p.26/4

    Possible [ZC]-vectors

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    Denote

    the set of all pairs

    with

    .

    Denote

    the smallest subset of

    , which

    contains the pair

    and is stable by the twooperations

    and

    Theorem: The set of possible [ZC]-vectors of

    is equal to the set of all vectors

    ,

    with

    .Computable in finite time for a given

    .

    p.27/4

    Examples

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    Dodecahedron

    of order

    . Order ofelements different from

    are

    ,

    or

    .Possible [ZC] are

    or

    or

    .

    Klein Map

    =

    of order

    "

    . Order ofelements different from

    are

    ,

    ,

    or

    .Possible [ZC] are

    or

    .

    Truncated Icosidodecahedron

    has size "

    p.28/4

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    V. action

    p.29/4

    action?

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    is the set of pairs

    . One has

    and

    The matrices

    and

    generate

    .

    We want to define

    , such that

    (i)

    is a group action of

    on

    (ii) If

    , then the mapping

    satisfies

    This is in fact not possible!

    p.30/4

    action

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    is generated by matrices

    and

    all relations between

    and

    are generated by therelations

    and

    We write

    p.31/4

    action (continued)

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    By computation

    Group action of

    on

    .

    If preserve the element

    in

    ,then for all pairs

    :

    and

    have the same [ZC]-vector. This define a

    finite index subgroup of

    p.32/4

    Conjectured generators

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    Graph

    Generators of

    Dodecahedron

    ,

    ,

    Cube

    ,

    Octahedron

    ,

    ,

    p.33/4

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    VI. Remarks

    p.34/4

    transitive

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    is the set of all directed edges of

    .

    : all rotations in automorphism group

    .

    its action on

    is free.

    action of

    and

    on

    commute.

    If

    is transitive on

    , then its action onZC-circuit is transitive too and

    defined by

    , is an injective groupmorphism.

    is normal in

    .

    p.35/4

    Extremal cases

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    non-trivial

    restrictions on

    .

    transitive on

    =

    (

    -valentcase) or

    (

    -valent case).

    is formed of even permutation on

    or

    directed edges.

    In some cases

    .

    We have no example of

    -valent plane graph

    with

    . p.36/4

    commutative

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    commutative

    is either a graph

    , agraph

    or a

    -hedrite.

    Class

    (Grunbaum-Zaks): Goldberg-Coxeter of the

    Bundle

    Class

    (Grunbaum-Motzkin)

    Class

    -hedrites

    (Deza-Shtogrin)

    No other classes of graphs or

    -hedrites is known toadmit such simple descriptions.

    p.37/4

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    VII. Parametrizing

    graphs

    p.38/4

    Parametrizing graphs

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    Idea: the hexagons are of zero curvature, it suffices to giverelative positions of faces of non-zero curvature.

    Goldberg (1937): All

    ,

    or

    of symmetry (

    ,

    ),

    (

    ,

    ) or (

    ,

    ) are given by Goldberg-Coxeterconstruction

    .

    Fowler and al. (1988) All

    of symmetry

    ,

    or

    are described in terms of

    parameters.Graver (1999) All

    can be encoded by

    integerparameters.

    Thurston (1998) The

    are parametrized by

    complexparameters.

    Sah (1994) Thurstons result implies that the Nrs of

    ,

    ,

    ,

    ,

    . p.39/4

    The structure of graphs

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    triangles in

    The corresponding trian-gulation

    The graph

    p.40/4

    Tightness

    A railroad in a

    -valent plane graph

    is a circuit of

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    p g p

    hexagons with any two of them adjacent on oppositeedges.

    They are bounded by two zigzags.A graph is called tight if and only if it has no railroads.

    If a

    - (or

    -)valent plane graph

    has no -gonal faces

    with

    =

    (or

    ) and

    then

    is tight. p.41/4

    - and railroad-structure of graphs

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    All zigzags are simple.The -vector is of the form

    with

    the number of railroads is

    .

    has

    zigzags with equality if and only if it is tight.If

    is tight, then

    (so, each zigzag is aHamiltonian circuit).

    All

    are tight if and only if

    is prime.

    There exists a tight

    if and only if

    is odd.

    p.42/4

    Conjecture on

    are described by two

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    complex parameters. They exists if and only if

    and

    "

    .

    with one zigzag The defining triangles

    !

    #

    $

    exists if and only if

    %

    &

    '

    !

    (

    )1

    2

    3 4

    $

    ,% 5 (.

    If % increases, then part of

    $

    amongst

    !

    !

    $

    goes to 100%

    p.43/4

    More conjectures

    All

    with only simple zigzags are:

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    ,

    and

    the family of

    with parameters

    and

    with

    and

    "

    They have symmetry

    or

    or

    Any

    with one zigzag is a

    .

    For tight graphs

    the -vector is of the form

    with

    or

    with

    Tight

    exist if and only if

    , they arez-transitive with

    iff

    and, otherwise,

    iff

    p.44/4

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    The End

    p.45/4