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    Perspectives of New Music

    Some Compositional Uses of Projective GeometryAuthor(s): David LewinSource: Perspectives of New Music, Vol. 42, No. 2 (Summer, 2004), pp. 12-63Published by: Perspectives of New MusicStable URL: http://www.jstor.org/stable/25164553

    Accessed: 21-10-2015 00:44 UTC

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    Some Compositional Uses

    of

    Projective Geometry

    Le?7ta

    David Lewin

    Part

    I: Introduction

    to the

    Projective

    Plane;

    Diatonic Modal

    Examples

    Imagine

    a

    school

    that has

    seven

    students:

    Ann, Bill, Carol,

    Dan,

    Eve,

    Frank, and Gladys. Suppose the school offers seven courses: Latin,

    Math,

    Neurology, Psychology,

    Quantum mechanics, Russian,

    and

    Span

    ish.

    Suppose

    the enrollment of

    students

    in

    courses

    is

    given by

    Example

    1.

    On

    the

    example,

    each

    asterisk

    indicates

    that

    the

    student whose

    initial

    appears

    to

    the left

    is

    taking

    the

    course

    whose

    initial

    appears

    above.

    Thus

    Ann

    is

    taking

    Math,

    Neurology,

    and

    Quantum mechanics;

    the students

    enrolled

    in

    Spanish

    are

    Carol, Frank,

    and

    Gladys;

    and

    so

    forth.

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    ProjectiveGeometry

    13

    A

    ~B~

    ~C

    ~D

    ~E

    ~F~

    ~G

    M

    N

    Q

    R

    EXAMPLE

    1

    Example

    1

    has the

    following

    properties:

    1.

    Any

    two

    students

    have

    just

    one course

    in

    common.

    2.

    Any

    two

    courses

    have

    just

    one

    student

    in

    common.

    3.

    Every

    course

    has

    at

    least

    three

    students;

    every

    student is

    taking

    at

    least three

    courses.

    4. It is

    not

    the

    case

    that

    every

    student

    is

    taking

    every

    course.

    The

    properties

    manifest

    a

    structure

    called

    a

    "projective

    plane."

    To

    appreciate

    the

    geometric metaphor,

    we can

    replace

    the word "student"

    by

    the

    word

    "point,"

    the word

    "course"

    by

    the word

    "line,"

    and

    the

    notion

    of

    a

    student's

    taking

    a course

    by

    the notions

    of

    a

    point's "lying

    on"

    a

    line and

    (equivalently)

    of

    the line's

    "passing through"

    the

    point.

    The properties above then translate as follows:

    1.

    Any

    two

    points

    lie

    on

    just

    one

    line.

    2.

    Any

    two

    lines

    pass

    through just

    one

    point.

    3.

    Every

    line

    passes

    through

    at

    least three

    points;

    every

    point

    lies

    on

    at

    least

    three

    lines.

    4. It is

    not

    the

    case

    that

    every

    point

    lies

    on

    every

    line.

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    14

    Perspectives

    of

    New Music

    As

    translated,

    the

    properties

    suggest

    things

    we

    apprehend

    about

    "plane geometry."

    The

    things

    have

    to

    do in

    particular

    with incidence

    relations

    of

    points

    and lines.

    Only

    property

    2

    departs

    from

    Euclidean

    intuition:

    in

    Euclidean

    plane

    geometxy^parallel

    lines

    do

    not

    pass

    through

    any

    common

    point. Projective

    geometry,

    unlike Euclidean

    geometry

    (or

    "affine

    geometry")

    does

    not

    recognize

    the

    notion

    of

    parallel

    lines.

    To

    turn

    the

    Euclidean

    plane

    into

    a

    projective plane

    one can

    adjoin

    a

    "line

    at

    infinity,"

    comprising

    formal

    "points"

    where

    parallel

    lines

    meet.

    In

    the

    Euclidean

    plane

    one

    fixes

    a

    reference

    line;

    in

    a

    standard

    Cartesian

    coordinate

    system

    this could be the horizontal X axis. For each number a

    between 0 inclusive

    and

    180

    exclusive,

    stipulate

    a

    corresponding

    "point

    at

    infinity."

    Each line in the Euclidean

    plane

    will

    be

    tilted

    with

    respect

    to

    the reference

    line

    at some

    angle

    a

    degrees;

    the

    given

    line

    meets

    the

    line

    at-infinity

    at

    point

    a.

    So

    a

    line

    perpendicular

    to

    the

    reference

    line

    meets

    the

    line-at-infinity

    at

    point

    90.

    A line

    parallel

    to

    the

    reference

    line

    meets

    the

    line-at-infinity

    at

    point

    0. More

    generally,

    two

    parallel

    lines will both

    be

    tilted

    the

    same

    amount

    with

    respect

    to

    the

    reference

    line;

    if

    the

    com

    mon tilt is a degrees, then the two linesmeet at infinite-point a. The

    extended

    structure

    is called the "Real

    Projective

    Plane." The

    reader

    can

    verify

    that it satisfies

    properties

    1

    through

    4

    above.1

    A

    projective plane

    is

    highly

    structured,

    and

    that

    structure

    can

    be musi

    cally suggestive

    in

    various

    contexts.

    As

    a

    first

    illustration,

    let

    us

    return to

    Example

    1

    and

    now

    read the

    seven

    "students"

    as

    the

    seven

    white-note

    pitch

    classes.

    The

    seven

    "courses" then

    become

    a

    family

    of

    seven

    privi

    leged

    Chords,

    the

    Chords

    L

    through

    S

    displayed

    in

    Example

    2.

    The four

    properties now read:

    1.

    Any

    two notes

    belong

    to

    just

    one

    Chord.

    2.

    Any

    two

    Chords

    have

    just

    one common

    tone.

    3.

    Every

    Chord has

    at

    least

    three

    notes;

    every

    note

    belongs

    to

    at

    least

    three Chords.

    4. It

    is

    not

    the

    case

    that

    every

    note

    belongs

    to

    every

    Chord.

    L M

    N

    P

    Q

    R

    S

    EXAMPLE

    2

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    Projective Geometry

    15

    EXAMPLE

    3

    Indeed

    in

    this

    particular

    geometry

    every

    Chord

    has

    exactly

    three

    notes,

    and

    every

    note

    belongs

    to

    exactly

    three

    Chords.

    Chords

    L, M,

    and

    N,

    taken

    in

    conjunction,

    suggest

    Phrygian modality;

    Chord

    P,

    when

    suitably

    linearized,

    is

    appropriate

    for

    executing

    a

    melodic

    Phrygian

    cadence.

    Obviously

    I

    constructed

    the

    example

    with these features in

    mind/ear.

    Later

    on,

    I

    shall show how

    I

    did

    that.

    Meanwhile

    I

    shall

    present

    a

    Lehrst?ck

    that

    demonstrates

    how

    various

    aspects

    of

    the

    geometry

    can

    be

    projected compositionally.

    After

    setting

    up

    the seven-note seven-chord

    projective plane

    as in

    Examples

    1 and

    2,

    to

    build

    a

    species

    of

    "Phrygian

    mode,"

    I

    decided

    to

    write

    a

    three-part

    vocal

    piece

    where

    every

    three-note

    verticality

    would be

    a

    Chord.

    I

    decided

    to

    base this

    piece

    on a

    cantus

    firmus,

    and had the idea

    of

    com

    posing

    the

    cantus

    as

    a

    twenty-one-note

    tune

    comprising

    concatenated

    linearizations

    of the

    seven

    three-note

    Chords.

    Example

    3 shows the

    can

    tus,

    shaped

    to

    have

    a

    "Phrygian"

    character

    (and

    somewhat

    adjusted

    as

    the

    composition

    went

    into later

    stages).

    As

    shown

    by

    the brackets and

    letters at the bottom of the

    example,

    the first three notes of the cantus

    linearize

    Chord

    M,

    the

    next

    three

    linearize Chord

    L,

    and

    so

    on;

    the

    melodic cadence

    is

    achieved

    through

    a

    linearized form of Chord

    P.

    Imagining

    a

    vocal

    piece,

    I

    looked for

    a

    suitable

    text.

    I

    tried

    to

    find

    a

    stylistically appropriate

    twenty-one-syllable

    text

    that could be

    sung

    to

    the

    tune

    of the

    cantus

    firmus.

    Example

    4,

    setting

    three

    seven-syllable

    verses

    of

    text,

    seemed

    apt. (I

    modified

    my

    original

    cantus

    firmus

    slightly,

    the

    better

    to

    accommodate

    this

    text.)

    Ben

    -

    e

    -

    die

    -

    tus

    qui

    ven

    -

    it

    in

    no

    -

    mi

    -

    ne

    Do

    -

    mi

    -

    ni,

    in

    no

    -

    mi

    -

    ne

    Do

    -

    mi

    -

    ni.

    EXAMPLE

    4

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    16

    Perspectives

    of

    New

    Music

    I wanted to harmonize each note of the cantus firmuswith each of the

    three

    Chords

    to

    which

    it

    belongs. Example

    5a

    sketches the

    idea.

    Wsym

    bolizes

    the

    note

    of

    the

    cantus

    firmus;

    the lines

    on

    Example

    5

    a

    indicate

    the three Chords

    containing

    W,

    that

    is

    {W,

    XI,

    X2],

    {W,

    Yl,

    Y2\,

    and

    [W,Z1,Z2\.

    a)

    b)

    c)

    /W\ ,WV /Wl

    W2

    XI Yl Zl XI-Yl-Zl XI-Yl-W3

    III

    III II

    XI Yl 72 X2?Y2-22 X2-Y2-W3

    EXAMPLE

    5

    It is

    not

    hard

    to

    see

    that

    the

    seven

    "points"

    of

    Example

    5a

    must

    be

    the

    seven

    distinct

    notes

    of the

    mode.2

    One

    naturally

    hopes

    to

    be

    able

    to

    arrange

    matters

    as

    in

    Example

    5b,

    so

    that

    {XI,

    Yl,

    Zl]

    and

    {X2,

    T2,

    Z2\

    will

    be

    Chords

    (i.e.,

    "lines"

    of the

    geometry), projected

    as

    vocal lines in

    the

    two

    accompanying

    voices.

    But

    this

    is

    not

    possible.

    The line deter

    mined

    by

    XI

    and

    Yl will

    indeed contain

    one

    of

    the

    Z-points,

    but that

    same

    Z-point

    (not

    the

    other

    one)

    will also be the

    third

    point

    on

    the

    X2

    72 line.3

    This feature

    of

    the

    system suggests

    the

    compositional algorithm

    sketched

    by Example

    5c.

    Here Wl

    symbolizes

    the

    present

    note

    of the

    cantus

    firmus,

    and

    W2

    symbolizes

    the

    next

    note

    of

    the

    cantus.

    (The

    can

    tus was

    constructed

    so

    as

    not to

    have

    repeated

    notes.)

    If

    W3

    is the

    third

    note

    of

    the Chord

    containing

    Wl

    and

    W2

    (the

    third

    point

    on

    the

    line

    containing

    Wl and

    W2),

    then the

    X-notes

    and

    T-notes

    can

    be

    arranged

    so

    that

    X1-Y1-W3

    is

    a

    geometric

    line

    (i.e.,

    a

    Chord),

    and

    X2-Y2-W3

    is

    also a geometric line (a Chord). Indeed, this arrangement isunique, up

    to

    contrapuntal

    inversion of "voice

    1"

    and "voice

    2,"

    and/or

    exchange

    of

    notes

    Xn

    with

    notes

    Tw.4

    The basic

    algorithm

    of

    Example

    5

    c

    produced

    the

    compositional

    study

    of

    Example

    6.

    Other

    features

    of

    the

    projective

    geometry suggest

    other

    compositional

    possibilities.

    Consider for

    instance the fact

    that

    every

    pair

    of distinct

    notes

    belongs

    to

    exactly

    one

    Chord,

    to

    which

    exactly

    one

    other

    note

    also

    belongs.

    This

    enables

    one to

    add

    a

    third

    part automatically,

    to

    any two-part

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    Projective

    Geometry

    17

    nit,

    ui

    ve

    -

    -

    -

    nit,

    n

    m

    mi

    -

    -

    ni_

    Do-mi

    ni,_Do

    -

    mi

    -

    ni,

    _

    Do

    - -

    mi

    -

    ni,.

    in_

    no

    -

    -

    mi

    -

    - -

    ne inno

    -

    mi

    -

    ne

    _

    EXAMPLE

    6

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    18

    Perspectives

    of

    New Music

    example

    7

    diatonic

    counterpoint

    that does

    not

    contain

    a

    vertical

    octave

    or

    unison.

    Example

    7

    illustrates,

    adding

    a

    third

    part

    to

    an

    example

    from

    Zarlino.5

    The example illustrates his "third mode"; given our particular Chord

    vocabulary,

    it is

    of

    course

    natural

    to

    select

    a

    two-part

    model

    from

    one or

    another E-final mode. The exercise could be made

    more

    elegant

    if

    it did

    not

    cling

    so

    doggedly

    to

    the

    notion

    that

    every

    three-note

    verticality

    had

    to

    be

    a

    Chord

    of the

    geometric

    system;

    protocols

    for non-Chordal verti

    calities

    in

    three

    voices

    could

    of

    course

    be

    worked

    out.

    Another

    resource

    for

    composition

    in

    our

    geometric

    mode

    is

    "modula

    tion"

    to

    secondary

    modes. This

    can

    be

    accomplished

    in

    several

    ways. First,

    the Chords of

    Example

    2

    can

    all

    be

    transposed by

    a

    fixed number of semi

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    Projective

    Geometry

    19

    a) b)

    L'

    W

    N'

    P'

    ?r

    R' S' V

    M' N' P'

    Q

    R'

    S'

    (M)

    (Q)

    (R)

    (Q)

    (P)

    EXAMPLE

    8

    tones,

    introducing

    ficta

    as

    appropriate.

    An

    appropriate

    interval

    of

    transpo

    sition is

    five

    semitones

    (Example

    8a):

    that

    is

    because

    the

    two

    harmonic

    triads

    of

    themode

    are

    related

    by

    T5;

    also the

    transposition

    introduces

    only

    one ficta tone. The a-minor triad serves as

    pivot:

    Chord V of the trans

    posed

    mode

    coincides with

    Chord

    M

    of

    the

    original

    mode.Example

    8b

    shows

    the

    original

    mode

    transposed

    by

    T2.

    This introduces ficta

    tones

    F|

    and

    C|.

    Chord

    5'of the

    transposed

    mode

    coincides with Chord

    Q

    of the

    original

    mode.

    Example

    8c

    shows

    a

    particularly

    idiomatic

    pitch-class

    inver

    sion of

    the

    original

    mode,

    inversion-about-D. No

    ficta

    tones

    are

    intro

    duced,

    and

    there

    are

    many

    pivot-Chords:

    P'and

    il'coincide

    with R and P

    respectively;

    Q

    'coincides with

    Q.

    The

    mode

    of

    Example

    8c could be taken

    in itself as a sort of

    "Ionian/C-major"

    structure.

    That

    suggests

    another

    sort

    of

    modulation

    one can

    make,

    from the

    original

    mode

    of

    Example

    2.

    Namely,

    one can

    modulate

    to

    other diatonic

    modes,

    modes

    given

    by

    other choices of

    Chords,

    to

    realize

    a

    projective

    plane

    with the

    seven

    white

    notes

    as

    "points."

    One

    can

    easily

    construct

    large

    numbers of such modes.

    For

    that

    purpose,

    the

    abstract

    configura

    tion of

    Example

    9 is useful.

    First

    one

    selects three basic

    Chords,

    which

    one

    might

    think

    of

    as

    "pri

    mary." These are the Chords corresponding to lines 123, 345, and 561

    on

    the

    figure.

    The

    primary

    Chords

    must

    be

    selected

    so

    that

    any

    two

    of

    them

    have

    exactly

    one common

    tone.

    C-, G-,

    and

    F-major

    triads could

    not

    be selected

    as

    the

    three

    Chords,

    because the G

    and the F triads

    have

    no

    common

    tone.

    One

    could,

    however,

    select

    {C,

    E,

    G}, {F,A,

    C},

    and

    {G, F,

    B}.

    Arranging

    the

    notes

    to

    suit

    the

    configuration

    of

    Example

    9,

    one

    could take

    C

    =

    1,

    G

    =

    3,

    F

    =

    5,

    E

    =

    2,

    B

    =

    4,

    A

    =

    6. Then

    the

    remain

    ing

    note,

    D,

    would be

    number 7 in

    the

    example.

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    20

    Perspectives

    of

    New Music

    If

    123, 345,

    and

    561

    are

    all

    formal

    "lines"

    of

    the

    geometry,

    then

    so are

    174,

    376, 572,

    and 246.

    example

    9

    The choice of the "basic triangle" on Example 9 exhausts six notes of

    the

    mode.

    The seventh

    note

    appears

    at

    the

    center

    of the

    triangle.

    It

    must

    be

    the

    case

    that

    174, 376,

    and 572

    are

    all formal

    "lines" of

    the

    geometry;

    the

    corresponding

    notes

    will then be

    formal Chords

    of

    the

    system.6

    Finally,

    it

    must

    be the

    case

    that 246 is

    a

    formal

    "line";

    the

    corresponding

    notes

    then

    form the

    seventh

    Chord.7

    (a) (b)

    (c)

    "Ionian/Cmaj";

    "Dorian";

    primary "Mixolydian";

    primary

    Chords

    CEG,

    Chords

    DFA, GBD,

    primary

    Chords

    GBD,

    FAC, GBF;

    other

    EGA;

    other

    Chords

    DFA, GAC;

    other

    Chords

    BCD,

    DGA,

    CDE, ABC, FGC,

    Chords

    CDE, EFG,

    DEF,

    EAB.

    BEF.

    EAB,

    BCF.

    EXAMPLE

    10

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    11/53

    Projective Geometry

    21

    Example 10a shows themode generated by the "primary Chords" {C,

    E,

    G},

    {F,A, C},

    and

    {G,

    F,

    B},

    as

    begim

    above.

    This

    turns

    out

    to

    be the

    "Ionian/C-maj"

    mode

    encountered earlier in

    Example

    8c;

    it

    was

    the

    inversion

    of

    our

    original

    "Phrygian"

    mode about

    D.

    Example

    10b shows

    a

    "Dorian"

    mode

    generated by

    taking

    {D, F,

    A},

    {G, B, D},

    and

    {E,

    G,

    A}

    as

    primary

    Chords.

    Example

    10b

    inverts about D

    to

    yield

    Example

    10c,

    a

    "Mixolydian"

    mode with

    primary

    Chords

    {G, B, D},

    {D,

    F,

    A},

    and

    {G,

    A,

    C}.

    Chords

    DFA,

    GBD,

    and

    CDE

    serve as

    pivots

    between

    our

    Dorian

    and

    Mixolydian modes;

    FGC

    pivots

    as a

    Chord

    for

    both

    our

    Phrygian

    and

    our

    Dorian mode.

    There

    is

    of

    course

    little

    reason,

    other than

    historicist

    sentimentality,

    to

    assign

    special priority

    to

    harmonic

    triads

    as

    Chords,

    "primary"

    or

    other

    wise,

    in

    constructing

    any

    formal

    diatonic mode

    (i.e.,

    geometry).

    Further

    techniques

    of

    "modulation"

    are

    available.

    Some mathemati

    cally

    idiomatic

    ones

    will

    be

    discussed

    later,

    "collineations"

    in

    particular.

    * *

    In

    any

    projective

    plane,

    there

    are

    many

    ways

    of

    choosing

    a

    structure

    almost

    like that of

    Example

    9,

    a

    structure

    consisting

    of

    seven

    points

    {1,2,

    3, 4,

    5,

    6, 7}

    in

    which

    123, 345, 561,

    174, 376,

    and

    572

    are

    all

    formal

    "lines" of

    the

    geometry.

    In

    general,

    246 need

    not

    be

    a

    formal

    line.

    We

    shall

    call

    any

    such

    structure

    a

    "reference

    quadrangle."

    A

    generic

    reference

    quadrangle

    may

    be

    constructed

    as

    follows.

    Given

    any

    projective plane

    (whether

    a

    seven-point

    plane

    or

    some

    other),

    select

    "1" and "3" as any two distinct

    points.

    (Any line contains at least three

    distinct

    points.)

    Since

    not

    all

    points

    of

    the

    plane

    lie

    on one

    line,

    select

    "5"

    as

    any

    point

    not

    on

    the

    line 13.

    The

    lines

    13, 35,

    and 15

    are

    all distinct.

    (If

    any

    two

    coincided,

    then

    points

    1,3,

    and 5 would all

    be

    collinear,

    and

    point

    5

    would lie

    on

    line

    13,

    contrary

    to

    construction.)

    So,

    in

    particular,

    lines

    13 and 15

    are

    dis

    tinct. Let

    L

    be

    a

    third line

    passing

    through

    point

    1.

    (Every point

    lies

    on

    at

    least

    three

    distinct

    lines.)

    Take "4"

    to

    be the

    point

    where

    line

    L

    meets

    line 35. Point 4 isnot the same as point 3, since Lis distinct from line 13.

    Point

    4

    is

    not

    the

    same as

    point

    5,

    since

    L

    is

    distinct from

    line

    15.

    Line L

    contains

    at

    least three

    distinct

    points,

    including

    points

    1

    and 4.

    Take "7"

    to

    be

    a

    third

    point

    on

    line L.

    Then 7

    cannot

    lie

    on

    any

    of

    the

    other lines

    so

    far constructed

    (13,

    15,

    or

    35).

    If

    7

    were on

    line

    13,

    then

    line

    17,

    which is

    L,

    would

    be the

    same

    as

    line 13?but L

    was

    taken

    to

    be

    distinct from

    line 13. If

    7

    were on

    line

    15,

    then

    line

    17,

    which

    is

    L,

    would be

    the

    same as

    line

    15?but

    L

    was

    taken

    to

    be

    distinct

    from

    line

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    12/53

    22

    Perspectives

    of

    New Music

    Jl

    =

    [p2,p3, ql, ri} Kl

    -

    [pi, ri, s2, s3)

    J2

    =

    [pi,

    p3, q2,

    r2\

    K2

    =

    [p2,

    r2, si,

    s3}

    J3

    =

    [plyp2,

    q3,

    r3]

    K3

    =

    [p3,

    r3,

    si,

    s2]

    Ll

    =

    [pi, ql,

    si,

    t)

    Ml

    =

    [q2, q3,

    ri,

    si)

    L2

    =

    [p2,

    q2,

    s2, t)

    M2

    =

    [ql,

    q3,

    r2,

    s2\

    L3

    =

    [p3, q3,

    s3,

    t]

    M3

    =

    [ql,

    q2,

    r3,

    s3)

    N=[rl,r2,r3,t\

    EXAMPLE

    11

    15. If 7

    were on

    line

    35,

    7 would be the

    point

    where

    L

    meets

    line

    35?

    but that

    point

    is

    point

    4,

    and

    7

    was

    chosen

    to

    be

    distinct

    from

    4.

    Take

    "2"

    to

    be the

    point

    where line 57

    meets

    line

    13. Point

    2

    is

    dis

    tinct from

    point

    3: if2

    =

    3,

    then line 25

    =

    line

    35,

    and

    point

    7 would lie

    on

    line 35?which it doesn't. Point 2 is distinct from

    point

    1:

    if 2

    =

    1,

    then line 25

    =

    line

    15,

    and

    point

    7 would lie

    on

    line 15?which

    it

    doesn't.

    So

    1, 2,

    and 3

    are

    different

    points

    of line 13.

    In like

    manner,

    taking

    "6"

    to

    be the

    point

    where line 37

    meets

    line

    15,

    we see

    that

    1,

    6,

    and 5

    are

    distinct

    points

    of

    line

    15.

    In

    sum,

    points

    1

    through

    7

    are

    all

    distinct; 123, 345,

    561,

    275,

    471,

    and

    673

    are

    all dis

    tinct lines.

    In

    the

    general

    projective

    plane,

    it

    need

    not

    be the

    case

    that

    points

    2, 4,

    and 6

    are

    collinear.

    Part

    II:

    Some Other

    Projective

    Planes,

    with

    Musical Applications

    A

    generic thirteen-point projective plane

    can

    be

    conceptualized

    as

    fol

    lows. Let the

    "points"

    of

    the

    system

    be

    symbolized

    as

    pi, p2, p3, ql, q2,

    q3,

    rl, r2,

    r3,

    si,

    s2,

    s3,

    and

    t.

    Then take

    as

    the thirteen "lines"

    the

    sets

    of

    points

    J1,J2,

    etc.

    given by Example

    11.

    The given thirteenpoints, togetherwith the stipulated thirteen lines,form

    a

    projective plane.

    The reader

    may

    check

    the four

    required properties:

    1.

    Any

    two

    points

    lie

    on

    just

    one

    line.

    2.

    Any

    two

    lines

    pass

    through

    just

    one

    point.

    3.

    Every

    line

    passes

    through

    at

    least three

    points;

    every

    point

    lies

    on

    at

    least

    three lines.

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    13/53

    Projective Geometry

    23

    4. It is

    not

    the

    case

    that every point lies

    on

    every line.

    In the

    thirteen-point

    plane,

    every

    point

    lies

    on

    exactly

    four lines and

    every

    line

    passes

    through

    exactly

    four

    points.

    The

    thirteen-point plane

    can

    be used

    to

    structure

    "chromatic"

    modes,

    if

    one

    adjoins

    a

    special

    symbol

    $

    to

    the

    twelve

    chromatic

    pitch

    classes.

    The

    special

    symbol

    could

    be realized

    musically

    as

    silence,

    or as a non

    pitched

    event,

    or as a

    wild card.

    Example

    12

    shows the

    structure

    of

    one

    such

    mode.

    pl=B,p2

    =

    G,p3=?, ql=D,

    #2=Bt,

    q3

    =

    G$,

    ri=C, r2=E,

    r3-Cf,

    ?i=Et,?2=Ff,.tf

    =A,?

    =

    $.

    /i={G,F,D,C}

    tfi?{B,C,Ff,A}

    J2

    =

    {B,

    F,

    Bt,

    E}

    K2

    =

    {G,

    E,

    Et,

    A}

    J3

    =

    {B,G,

    Gf, Cf}

    K3

    -

    {F,

    Cf,

    Et, Ff}

    LI -

    {B,

    D,

    Et,

    $}

    Ml =

    {Bt,Gt,

    C,

    Et}

    L2

    =

    {G,

    Bt,

    F|,

    $}

    M2

    -

    {D,

    Gf,

    E,

    Ff}

    L3

    =

    {F,

    Gf,

    A, $}

    M3

    =

    {D,

    Bt, C|,

    A}

    tf={C,E,Cf,$}

    EXAMPLE

    12

    To

    construct

    the

    mode of

    Example

    12

    I

    proceeded

    as

    follows.

    I

    decided

    to

    make the

    special

    symbol

    $

    the

    point

    t

    of

    Example

    11. I

    then

    considered

    the

    four

    lines

    of

    Example

    11

    that

    would contain the

    special

    symbol

    t

    =

    $.

    These four

    formal lines would be realized

    in

    the musical

    mode

    by

    formal

    Chords

    thatwould each

    comprise

    three

    "genuine

    notes"

    plus

    the

    special

    effect.

    I

    decided

    to structure

    the mode

    so

    that those four

    Chords

    would be

    transposed

    or

    inverted

    forms,

    each of

    any

    other.

    I

    spe

    cificallydecided thatLI

    =

    [pi, ql, si, t)would be {B,D, Et, $}, that L2

    =

    [p2, q2,

    s2,

    t)

    would be

    {Ff,

    G,

    Bt,

    $},

    that L3

    =

    [p3,

    q3,

    s3,

    t)

    would be

    {F,

    Gf,

    A,

    $},

    and

    that

    N

    -

    [rl,

    r2,

    r3,

    t)

    would be

    {C,

    Cf,

    E,

    $}.

    Thus

    the three

    notes

    B, D,

    and

    Et

    would

    be

    assigned

    in

    some

    order

    as

    the

    points

    pi,

    ql,

    and si

    of

    Example

    11;

    likewise the

    three

    notes

    Ff,

    G,

    and

    Bt

    would

    be

    assigned

    in

    some

    order

    as

    the

    points

    p2, q2,

    and s2

    of

    Example

    11,

    and

    so

    forth.

    Playing

    around with

    various

    possibilities

    for

    those

    assignments,

    considering

    the other

    Chords

    that

    Example

    11

    would

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    24

    Perspectives

    of

    New Music

    generate in each case, I arrived

    at

    themode of Example 12. Evidently

    an

    enormous

    number of such modes

    can

    be

    constructed.

    (t-1-1)-1-p3-s3v

    rl

    r

    -s

    /-qJv pi-p

    I-r3-(q3-q3-q3-q3)

    rl-p

    I-P3-(ql?ql-ql-ql)-J--ql

    r3-ql-$3'

    s2-rl-qV

    si

    EXAMPLE

    13

    Example

    13 demonstrates

    an

    algorithm

    for

    harmonizing

    certain

    types

    of

    cantus

    firmus.

    The

    example

    supposes

    the

    succession

    t,

    q2, q3

    as a

    seg

    ment of such a cantus firmus.All vertically aligned sets of four events in

    the

    example

    are

    Chords of the

    generic

    system.

    At the

    left,

    the

    cantus

    fir

    mus

    event

    tis harmonized

    by

    the four vertical Chords that contain it:

    {t,

    rl,

    r2, r3}, {t,

    si,

    pi,

    ql],

    {t,

    q3, p3,

    s3],

    and

    (moving

    onwards)

    {t,

    p2, q2,

    s2).

    The

    voice

    leading

    can

    be

    arranged

    so

    that the three

    accompanying

    voices

    of the first three chords all form formal lines with

    q2,

    the

    next

    event

    of the

    cantus

    firmus. That

    is?as

    indicated

    by

    the horizontal and

    diagonal

    lines

    in

    Example

    13?[rl,

    si,

    q3, q2)

    is

    a

    formal

    line;

    so

    is

    \r2,

    pi, p3, q2}y

    and

    so

    is

    [r3,

    ql,

    s3,

    q2\. q2

    now

    takes

    over as

    cantus

    firmus

    event,

    and it is first armonized

    by

    the

    (unique)

    chord that contains both

    q2

    and

    t.

    The

    process

    then

    repeats,

    aiming

    at

    q3,

    the

    next event

    of

    the

    cantus

    firmus.

    Evidently,

    in

    this

    arrangement,

    it is

    necessary

    for

    q3

    not to

    be

    p2

    or

    s2?i.e.,

    q3

    must not

    lie

    on

    the

    line

    defined

    by

    t

    and

    q2.

    And

    of

    course

    t

    and

    q2

    must

    be

    distinct.

    The

    cantus

    is thus

    constrained

    as

    follows:

    it

    must

    contain

    no

    immediately

    repeated

    events,

    and

    no

    three consecutive

    events

    may

    be collinear.

    In

    Example

    13, the three initial lines of "alto," "tenor," and "bass"

    voices,

    under

    t

    in the

    cantus

    firmus,

    become

    verticalities when

    q2

    takes

    over

    the

    cantus

    role:

    the

    alto's initial

    line

    rl-sl-q3-q2

    becomes the last

    four-point

    verticality

    shown

    in

    the

    example;

    the tenor's

    initial

    line

    r2-pl

    p3-q2

    becomes the fifth four-note

    verticality,

    and

    so

    forth. This

    is

    a

    fea

    ture

    of the

    algorithm.

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    Projective

    Geometry

    25

    * *

    *

    The

    thirteen-point

    plane

    can

    also be

    applied

    to

    other musical

    phenom

    ena.

    For

    instance,

    there

    are

    exactly

    thirteen

    of what

    Larry Polansky

    calls

    "ternary

    contours."8

    These

    are

    illustrated

    in

    Example

    14. The

    thirteen

    point

    plane

    will

    organize

    these

    contours

    into

    mathematical

    "lines,"

    each

    of

    which

    is

    a

    group

    of

    four

    contours.

    Example

    11 will

    help

    the

    reader

    experiment

    with

    various modes

    of

    such

    grouping, assigning

    the

    symbols

    ply p2,

    etc.

    in

    various

    ways

    to

    the thirteen

    symbols

    of

    Example

    14.

    EXAMPLE

    14

    * * *

    There

    is

    a

    twenty-one-point projective plane;

    every

    line therein has

    exactly five points, and every point lies on exactly five lines. A generic

    structure

    for

    the

    plane

    can

    be

    obtained

    by

    algebraic

    techniques

    to

    be dis

    cussed later. The

    geometric

    structure

    could be

    applied,

    in various

    "modes,"

    to

    the

    family

    of

    twenty-one

    diatonic unordered

    dyads.

    There is also

    a

    thirty-one-point projective plane;

    every

    line therein has

    exactly

    six

    points,

    and

    every

    point

    lies

    on

    exactly

    six

    lines. The

    structure

    might

    be of

    interest

    to

    those who

    are

    interested in the

    thirty-one-tone

    scale;

    the

    geometry

    would

    single

    out

    a

    privileged

    family

    of

    thirty-one

    hexachords

    as

    formal "lines" of the

    system.

    The

    thirty-one privileged

    hexachords

    could be chosen

    in

    a

    vast

    variety

    of

    different

    "modes."

    Part

    III: Algebraic

    Structure

    of the

    Projective

    Plane

    There is

    a

    common

    algebraic

    structure

    underlying

    all

    projective planes,

    a

    structure

    which is

    very

    helpful

    for

    constructing

    a

    "generic" specimen

    of

    a

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    16/53

    26

    Perspectives

    of

    New

    Music

    given plane, along the lines of Example 11 earlier. To grasp suchmatters,

    one

    must

    first

    nderstand the

    notion

    of

    an

    algebraic

    "skew-field."

    By

    that

    term,

    a

    mathematician

    understands

    a

    set

    F

    of

    objects

    x,

    y,

    etc.,

    upon

    which

    two

    binary

    combinations

    are

    defined.

    The

    combinations

    are

    usually

    denoted

    using

    conventional

    symbols

    for

    addition

    and

    multiplica

    tion:

    thus

    objects

    x

    and

    ymay

    be

    combined

    so as

    to

    yield

    a

    formal

    "sum"

    x

    +

    y,

    and

    a

    formal

    "product"

    xy.

    In

    order

    to

    constitute

    a

    "skew-field,"

    the

    system

    must

    satisfy requirements

    1, 2,

    and

    3

    following.

    1. Pis

    a

    commutative

    group

    under addition.

    The

    identity

    element is

    denoted

    by

    0;

    the additive

    inverse

    of

    element

    a;

    is

    denoted

    "-#".

    2.

    The

    non-zero

    elements

    of F

    form

    a

    group

    under

    multiplication.

    The

    identity

    element of the

    group

    is

    denoted

    by

    1;

    the

    multiplicative

    inverse of

    a

    non-zero

    #is denoted

    by

    "aT1"

    or

    by

    "1/V\

    3.

    Multiplication

    distributes

    over

    addition,

    according

    to

    the

    laws

    x(y

    +

    z)

    =

    xy

    +

    xz\ (x +y)z

    =

    xz

    +yz.

    If

    multiplication

    is

    commutative,

    the

    skew-field

    is

    called

    a

    "field."

    The

    real

    numbers

    form

    a

    field.

    So

    do the rational

    numbers?those

    which

    can

    be

    expressed

    as

    quotients

    of

    integers.

    So

    do

    the numbers

    of

    form

    a

    +

    b(Jl),

    where

    a

    and

    b

    are

    rational

    numbers

    and

    Jl

    is

    the

    (irrational)

    square

    root

    of

    2.

    The

    multiplicative

    inverse

    of

    a non-zero a +

    b(

    Jl

    )

    is

    (a

    -b(j2))/(aa-

    2bb)?the

    denominator

    cannot

    vanish because

    a2

    cannot

    possibly equal

    2e2,

    a

    and b

    being

    rational and

    not

    both

    zero.9

    The integersmod 2 form a field. Those are the integers 0 and 1with

    all

    arithmetic reduced modulo

    2?e.g.,

    1

    +

    1

    =

    0. The

    integers

    mod 3

    are

    also

    a

    field,

    that is the

    symbols

    0,

    1,

    and

    2

    with

    arithmetic

    reduced

    mod

    ulo

    3:

    2

    +

    1

    =

    0,

    2 2

    =

    1

    (4

    is

    one

    more

    than

    some

    multiple

    of

    3),

    and

    so

    forth.

    The

    integers

    mod 5

    are a

    field,

    that is

    the

    symbols

    0,1, 2, 3,

    and

    4,

    with

    all arithmetic reduced

    modulo

    5.

    (4

    3,

    for

    instance,

    =

    2,

    since

    12

    is

    two

    more

    than

    some

    multiple

    of

    5.)

    In

    general,

    for

    any

    prime

    number

    p,

    the

    integers

    mod

    p

    form

    a

    field.

    There

    are

    other

    finitefields

    as

    well. For

    instance,

    there is

    a

    field

    of four

    elements which

    one can

    denote

    as

    0,1,

    a,

    and

    a

    +

    1. In

    this

    field,

    anything

    added

    to

    itself

    produces

    0,

    and

    a2

    equals

    a +

    1.

    These

    properties

    enable

    one

    to

    carry

    out

    the

    necessary arithmetic,

    to

    verify

    that

    the

    structure

    is

    a

    field. For

    instance,

    a(a

    +

    1)

    =

    a2

    +

    al

    =

    (a

    +

    I)

    +

    a

    =

    I

    +

    a

    +

    a

    =

    1.

    Then

    (a

    +

    l)(a

    +

    1)

    =

    a(a+

    1)

    +

    l(a+

    1)

    =

    (I)

    +

    (a

    +

    1)

    =

    1

    +

    1

    +

    a

    =

    a.

    The

    cardinality

    of the field

    just

    studied,

    four,

    is

    not

    a

    prime

    number,

    but it

    is

    a

    power

    of

    a

    prime.

    In

    general,

    for

    any

    prime

    number

    p

    and

    any

    positive integer

    ?,

    there will be

    a

    field

    of

    cardinality

    p^.

    Furthermore, any

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    Projective Geometry

    27

    finite fieldmust be one of those. Indeed, any finite skew-field must be

    one

    of

    those,

    since

    a

    remarkable theorem shows

    that

    any

    finite skew-field

    must

    be

    a

    field.

    * * *

    Now

    we are

    ready

    to

    construct

    a

    generic projective plane.

    Let

    F

    be

    some

    skew-field

    (any

    skew-field).

    Consider the

    family

    of all

    ordered

    triples

    formed from members

    bl, b2,

    and b3 of F.

    We

    stipulate

    that

    two

    such

    triples,

    say

    and

    ,

    are

    "left-equivalent"

    if

    there is

    some non-zero

    number k in

    F

    such that bl'

    =

    k

    -

    bl,

    b2'

    =

    k

    -

    b2,

    and b3'

    =

    k b3. This

    in

    indeed

    an

    equivalence

    relation

    among

    the

    triples.

    The relation is

    reflexive

    (bj-

    1

    bj,forj

    =

    1, 2,

    3);

    it is

    symmetric

    (if

    bj'=

    k

    -

    bj,

    then

    bj

    =

    (l/k)

    bjy,

    the relation is also

    transitive

    (if

    bj"

    =

    h

    bj',

    then

    bj"

    =

    (hk)

    bj).

    The

    points

    of the F

    Projective

    Plane

    are

    labeled

    by

    the

    non-zero

    left

    equivalence-classes

    of

    F-triples.

    That

    is,

    is excluded

    as a

    "point"

    of

    the

    geometry,

    but

    every

    other

    F-triple

    represents

    a

    point;

    among

    those

    triples

    and

    represent

    the

    same

    point

    if

    and

    only

    if

    there

    is

    some

    non-zero

    ?in F such

    that

    cj

    =

    k-

    ?/for

    each

    y

    =

    1,2,3.

    We shall label the

    formal lines

    of the

    F

    Projective

    Plane

    by

    the

    non

    zero

    right equivalence-classes

    of

    F-triples,

    which

    we

    shall write

    using

    square

    brackets:

    the

    triple

    [XI, X2, X3]

    is

    r^i-equivalent

    to

    the

    triple

    [XI

    ',

    T, X_H

    if there is

    some non-zero

    k in

    _Fsuch that

    Xj'

    =

    Xj

    k,

    for

    each

    j

    =

    1,

    2,

    3.

    Every

    non-zero

    triple

    represents

    a

    line; among

    those

    triples [XI, X2, X3] and [Tl, T2, T3] represent the same line ifand

    only

    if there is

    some non-zero

    k in _Fsuch that

    Yj

    =

    Xj-

    k,

    for each

    j

    =

    1,2,3.

    The

    point

    b=

    lies

    on

    the line

    X=

    [XI,

    X2,

    X3]

    if

    and

    only

    if

    he sixnumbers

    atisfy

    he

    equation (bl)(Xl)

    +

    (b2)(X2)

    +

    (b3)(X3)

    =

    0 in the skew-field

    F.

    One

    sees

    that if b'

    is

    left-equivalent

    to

    b,

    and/or

    right-equivalent

    to

    X,

    the numbers

    ?y'and Xj'wi? satisfy

    the

    same

    equa

    tion. Hence the relation

    "? lies

    on

    _?" is

    well-defined for

    points

    and lines.

    The known

    algebraic

    behavior of such

    equations

    in

    skew-fields

    guaran

    tees that the "points" and "lines" of the "F Projective Plane," as defined

    above,

    do indeed constitute

    a

    projective

    plane.

    That is:

    1.

    Any

    two

    points

    lie

    on

    just

    one

    line.

    2.

    Any

    two

    lines

    pass

    through just

    one

    point.

    3.

    Every

    line

    passes

    through

    at

    least

    three

    points;

    every

    point

    lies

    on

    at

    least three lines.

    4. It isnot the case that every point lies on every line.

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    18/53

    28

    Perspectives

    of

    New

    Music

    The Property of Desargues (discussed in note 1) also obtains. Remark

    ably

    enough,

    every

    projective plane

    (i.e.,

    every

    aggregation

    of

    formal

    points

    and

    formal

    lines

    satisfying

    the

    four

    properties

    above

    and the

    Prop

    erty

    of

    Desargues)

    can

    be

    labeled

    by

    numbers from

    some

    F

    Projective

    Plane

    so as

    to

    realize the

    algebraic

    structure

    described

    above.

    That

    is,

    every

    Desarguesian) Projective

    Plane

    "is"

    in

    fact

    an

    F

    Projective

    Plane,

    for

    some

    suitable F.

    If

    the

    Pis

    finite

    (and

    hence

    a

    field)

    we

    can

    count

    the

    number of

    points

    in

    the

    F

    Projective

    Plane.

    Say

    the

    cardinality

    of Pis

    q,

    where

    q

    is

    a

    power

    of

    some

    prime

    p

    (as

    earlier).

    The

    number

    of

    F-triples

    is

    then

    q3,

    and the

    number of

    non-zero

    F-triples

    is

    q3

    -

    1.

    Of

    those,

    each

    is

    equivalent

    to

    q

    1

    others,

    since each

    triple

    can

    be

    multiplied

    by

    any

    of

    the

    q

    -

    1

    non-zero

    members of F

    to

    form

    an

    equivalent

    triple.

    The

    number

    of

    non-zero

    equivalence

    classes

    is then

    q*

    -

    1

    divided

    by

    q

    -

    1.

    That

    number is

    equal

    to

    1

    +

    q

    +

    q2,

    which

    will

    be the

    number of

    points

    in

    the

    corresponding

    projective plane.

    If

    #

    =

    2,l

    +

    #

    +

    #2

    =

    l+2

    +

    4

    =

    7;

    the

    mod-2

    projective

    plane

    is

    our

    seven-point

    "diatonic"

    plane.

    If

    #=3,

    1

    +

    ^

    +

    ^

    =

    1

    +

    3

    +

    9

    =

    13;

    themod-3

    projective plane

    is our

    thirteen-point

    "chromatic"

    or

    "ternary

    contour"

    plane.

    If

    q

    =

    4,

    we

    obtain

    the

    twenty-one-point

    plane;

    if

    q

    =

    5,

    we

    obtain

    the

    thirty-one-point

    plane.

    Six is

    not

    a

    prime

    power;

    there is

    no

    six-element

    (skew-)field,

    so

    there is

    no

    forty-three-point

    pro

    jective

    plane.

    But

    there

    is

    a

    seven-element

    field,

    so

    there

    is

    a

    fifty-seven

    point

    projective

    plane. Eight

    and nine

    are

    each

    prime

    powers,

    so

    there

    is

    a

    seventy-three-point

    plane,

    and

    a

    ninety-one-point plane.

    Part

    IV:

    Applications?Mathematical

    and

    Musical?of Part

    III

    to

    the

    Twenty-One-Point

    Plane

    21

    =

    1+4+16;

    the

    twenty-one-point

    projective plane

    "is"

    in

    fact the

    F4

    Projective

    Plane,

    where F4 is

    the four-element

    field

    discussed in

    Part III.

    F4

    =

    (0,1,?,#+1};

    anything

    added

    to

    itself

    is

    0;

    a +

    1

    =

    02.

    One

    verifies

    that

    0(0

    +

    1)

    =

    (0

    +

    1)0

    =

    03

    =

    1;

    (0

    +

    l)2

    =

    0;

    (0

    +

    l)3

    =

    1.

    1

    +

    (0

    +

    1)

    [= 1 + 1 + 0]

    =

    a, and so forth.

    Given

    a

    twenty-one-point projective

    plane,

    we

    shall

    now see

    how it

    manifests

    the

    structure

    of

    the F4

    Projective

    Plane.

    Using

    the

    method

    dis

    cussed

    at

    the

    end of

    Part

    I

    earlier,

    we

    select

    any

    "reference

    quadrangle"

    in

    the

    plane;

    let its

    points

    and

    lines be

    denoted

    as

    in

    Example

    15:

    points

    pi,

    p2,

    p3,

    q,

    rl,

    r2,

    and

    r3\

    lines

    Jl,

    J2,

    J3,

    Ml, M2,

    and

    M3,

    each line

    containing

    inter

    alia

    the

    points specified

    on

    the

    figure.

    Now,

    using

    numbers

    from

    F4,

    we

    label

    pi

    =

    ,

    p2

    =

    ,

    p3

    =

    ,

    and

    q

    =

    . The

    algebraic

    structure

    of the F4 Plane

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    Projective

    Geometry

    29

    Jl=[p2,p3,rl,

    J2

    =

    [p3,pl,r2,

    J3

    =

    [pl,p2,r3,

    Ml

    =

    [pl,

    q,

    rl,

    M2

    =

    [p2, q, r2,

    M3

    =

    [p3,

    q,

    r3,

    EXAMPLE

    15

    tells

    us

    what

    the

    line coordinates for

    Jl

    will

    be. Both

    p2

    and

    p3

    have

    first

    coordinate

    equal

    to

    zero.

    That

    is,

    both

    are

    points

    b

    =

    satisfy

    ing the equation bl

    -

    0. Thus, both points satisfythe equation (bl)(Xl)

    +

    (b2)(X2)

    +

    (b3)(X3)

    =

    0,

    where

    XI

    =

    1,

    X2

    =

    0,

    and

    X3

    =

    0. We

    know,

    from

    the

    algebraic

    structure

    developed

    in Part

    III,

    that

    the

    coordinates

    for

    Jl

    will

    then

    be

    [1,

    0, 0]:

    Jlis

    that line

    containing exactly

    such

    points

    b

    as

    satisfy

    bl =0

    (more

    explicitly,

    bl

    1,

    plus

    b2

    0,

    plus

    b3

    0

    equals

    0).

    Similarly,

    J2

    =

    [0,1,

    0];

    J2

    contains

    just

    those

    points

    b

    satisfying

    b2

    =

    0.

    And

    J3

    =

    [0, 0, 1];

    J3

    contains

    just

    those

    points

    b

    satisfying

    b3

    ?

    0.

    Example

    16

    updates Example

    15

    to

    display

    the

    new

    information.

    pl

    -

    ,

    pl=,p3

    =

    q-

    /Z-[1,0,0]

    J2

    =[0,1,0]

    J3

    =

    [0,0,1]

    Ml=[pl,q,rl,.

    M2

    =

    [ply

    q,

    rl,

    .

    M3

    =

    [p3y

    }

    r3,

    .

    EXAMPLE

    16

    [pl,p3,rl,..

    [p3,pl,rl,..

    [pl

    l(W-O)

    .K*2-0)

    p2yv3y...

    }(b3=0)

    Next

    we

    shall find

    the line

    coordinates

    for

    Ml

    in

    F4.

    The

    lineMl

    =

    [XI,

    X2,

    X3]

    passes

    through

    the

    points pl

    =

    and

    q

    =

    .

    Accordingly,

    we

    must

    have

    1 XI

    plus

    0

    X2

    plus

    0

    X3

    equal

    to

    0

    (since

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    30

    Perspectives

    of

    New

    Music

    pi lies onMl), and also 1 XI plus 1 X2 plus 1 X3 equal to 0 (since q

    lies

    on

    Ml).

    That

    is,

    we

    must

    have

    XI

    =

    0,

    XI

    +

    X2

    +

    X3

    =

    0. Or: XI

    =

    0,

    X2

    =

    X3.

    Accordingly

    Ml

    =

    [0,

    1,

    l].10

    In similar

    fashion,

    we see

    thatM2

    =

    [1, 0, 1],

    and

    that

    M3

    =

    [1,

    1, 0].

    The

    new

    information

    is

    displayed

    in

    Example

    17.

    pi

    =

    ,

    p2

    =

    ,

    p3

    =

    ,

    q

    =

    /i-

    [1,0,0]

    /2

    =

    [0,1,0]

    J3

    =

    [0,0,1]

    {p2,p3,rl,.

    [p3,pl,r2,.

    \pl,p2,r3,.

    ?fi-[0,1,1]:

    {?I,

    ft ri,.

    ?I?

    -

    [1, 0,1]:

    {?2,

    ftr2,.

    M3-[l,l,0]:f^,ftr3,.

    (M-0)

    (?2=0)

    (W-0)

    (b2

    =

    b3)

    (bl=b3)

    (bl=b2)

    EXAMPLE 17

    Now

    we

    shall find the

    point

    coordinates

    for

    point

    rl.

    Suppose

    those

    coordinates

    are

    . Since rl lies

    on

    line/i

    =

    [1,

    0,

    0],

    we

    have

    bl

    =

    0. Since

    rl

    lies

    on

    lineMl

    =

    [0,

    1,

    1],

    we

    have b2

    +

    b3

    =

    0,

    whence b2

    =

    b3

    (in F4).

    In

    sum:

    bl

    =

    0;

    b2

    =

    ?3.

    ri is

    then labeled

    by

    the

    triple

    .

    Similarly,

    r2

    is

    labeled

    by

    the

    triple

    ,

    and

    r3 is

    labeled

    by

    the

    triple

    .

    Example

    18

    updates

    Example

    17

    with

    the

    new

    information.

    In the

    particular

    field

    F4,

    1 + 1 = 0.

    Therefore,

    in the

    particular

    sys

    tem

    we are now

    considering,

    the

    sum

    of rl's

    three coordinates

    is

    zero.

    So

    is the

    sum

    of r2's

    three

    coordinates,

    and

    so

    is the

    sum

    of

    r3,s

    three

    coor

    dinates. That

    is,

    the

    points

    rl, r2,

    and

    r3 all

    satisfy

    the

    equation

    bl

    +

    b2

    +

    b3

    =

    0.

    (This

    would

    not

    be

    the

    case

    in

    a

    field where

    things

    added

    to

    themselves

    were

    not

    zero.)

    Hence

    the three

    r-points

    all lie

    on

    the line

    L

    =

    [1,

    1, 1].

    Example

    19

    updates Example

    18 with the

    new

    information.

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    Projective

    Geometry

    31

    pl

    =

    ,

    p2

    =

    ,

    p3

    =

    ,

    q

    =

    rl

    =

    ,

    r2

    =

    ,

    r3

    =

    Jl

    =[1,0,0]:

    [p2,p3,rl,.

    J2

    =

    [0,1,0]:

    [p3,pl,

    r2,

    .

    J3

    =

    [0,0,1]:

    [pl,p2,r3,.

    Ml

    =[0,1,1]:

    [pl,q,rl,.

    M2

    =

    [1,0,1]:

    [P2,q,r2,.

    M3 =

    [1,1,0]:

    [p3,q,r3,.

    (bl=0)

    (b2=0)

    (b3

    =

    0)

    (b2

    =

    b3)

    (bl=b3)

    (bl=b2)

    EXAMPLE

    18

    Example

    19,

    we

    now

    see,

    realizes

    a

    seven-point plane

    embedded

    within

    the

    twenty-one-point

    plane.

    That

    is

    because the two-element field

    F2

    =

    {0, 1}

    is

    a

    subfield

    of F4. The

    seven

    points

    and

    seven

    lines of

    Example 19 are exactly those points and lineswhose coordinates can be

    written

    using

    only

    numbers from F2.

    Since

    our

    original

    choice of refer

    ence

    quadrangle

    was

    arbitrary,

    we can

    pause

    to

    note

    the

    interesting

    fact:

    any

    choice

    of reference

    quadrangle

    in

    the

    twenty-one-point projective plane

    realizes the

    seven-point

    plane.

    The visual

    image

    of

    Example

    19,

    on

    the

    Euclidean

    plane

    of

    the

    page,

    begins

    to

    be

    deceptive

    now?for

    instance

    it does

    not

    show

    us

    that

    rl, r2,

    and r3

    are

    collinear.11

    So

    we

    shall continue onwards

    from

    Example

    19

    purely algebraically, adjoining

    other

    points

    and

    lines

    of

    the

    twenty-one

    point plane using number-triples

    of F4. The

    coordinates

    of

    our new

    points

    and lines

    will

    all

    involve numbers of

    F4 that

    are

    not

    numbers of

    F2;

    thus

    they

    will all involve

    the

    number

    a

    of F4.

    Example

    20 lists the

    twenty-one

    points

    of the

    plane,

    identifying

    them

    with

    twenty-one

    non-equivalent

    number-triples

    from F4. And

    Example

    21

    lists the

    twenty-one

    lines

    of the

    plane, giving

    their line coordinates

    in

    square brackets;

    Example

    21

    also

    shows

    which

    points

    of

    Example

    20 lie

    on

    which of

    those

    lines.

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    22/53

    32

    Perspectives of

    New Music

    pi

    =

    ,

    p2

    =

    ,

    p3

    =

    ,

    q

    =

    ri

    ?

    ,

    r2

    =

    ,

    r3

    =

    Jl=[l,0,0]:{p2,p3,rl,..

    J2

    =

    [Q,l,0]:{p3,pl,r2,..

    J3

    =

    [0,0,1]:

    [pl,p2,r3,.

    .

    L-[l,

    1,1]:

    [ri, r2,r3,...

    Ml=[0,l,l]:[pl,q,rl,..

    M2

    =

    [l,Q,l]:{p2,q,r2,..

    M3

    =

    [l,l,0]:{p3,q,r3,..

    .}(W-0)

    .}(f?-0)

    .}(f??0)

    }(M

    +

    *2

    +

    *3-0)

    . }(t?-*3)

    ,

    }(M-*3)

    .

    )(W-t?)

    EXAMPLE

    19

    ?i=,

    ri=l>)

    si

    =,

    ii'

    =

    ,

    tl

    =,

    fi'

    =

  • 7/23/2019 Lewin - Some Compositional Uses of Projective Geometry

    23/53

    Projective Geometry

    33

    Jl

    =[1,0,0]

    J2

    =

    [0,1,0]

    /5

    =

    [0,0,1]

    ?

    =

    [1,1,1]:

    Ml

    =[0,1,1]

    Ml-

    [1,0,1]

    M3

    =

    [1,1,0]

    M

    =[0,0,1]

    #2

    =

    [0,0,1]

    N3

    =

    [0,1,0]

    ATi'

    -[0,*

    +

    l,l]

    N2'

    =

    [0 +1,0,1]

    AT3'

    =

    [0

    +

    1,1,0]

    ?-[^,1,1]

    K2-[1,*>1]

    K3-[l,l,*]

    Kl'

    =[0

    +

    1,1,1]

    Kl' =[1,0 + 1,1]

    K3'

    =[1,1,0

    +

    1]

    G

    =

    [l,0,0

    +

    1]:

    #=[1,0

    +

    1,0]:

    [p2yP3ytlySlySV\

    [plyp3yrlyslysi]

    [pl,pl,r3,s3,s3'}

    [rly

    rly r3y

    u,

    v)

    [plyqyTlytlyt?]

    [pl,

    qy

    rly tly

    ti

    }

    [p3y

    y

    r3y 3y

    3'

    )

    [Ply

    Sly

    t?

    yt3yU)

    [flySlyt? yt3yV)

    [p3y

    3y ly

    t?

    y

    U)

    [plySl'

    ytlyt3' yV)

    [fly

    S?

    y

    lyt3'

    y

    U)

    [p3yS3'

    ytlyti yV)

    [rlySlyS3y

    i'

    yt? }

    [Tly

    ly

    S3'

    y

    i'

    y

    3'

    }

    [r3ySl'

    y

    ?

    yti yti

    [rly

    S?

    y

    3'

    y

    ly

    t3\

    [rlyS3ySly tly t3\

    [r3,

    Sly

    Sly

    tly

    tl\

    [sly

    i

    y

    3'

    y

    } u)

    [Sly

    S3y

    S?

    y

    ,

    V)

    (arithmetic nF4(\))

    (W-0)

    (?2-0)

    (?5=0)

    (bl+bl

    +

    b3

    =

    0)

    (bl

    =

    b3)

    (bl=b3)

    (bl-bl)

    (b3-a-bl)

    (b3?a-bl)

    (bl-a-bl)

    (b3-(a

    +

    l)-bl)

    (b3

    =

    (a

    +

    l)-

    bl)

    (bl=(a

    +

    l)-bl)

    (a-bl-bl

    +

    b3)

    (a-bl-bl+bJ)

    (a-b3

    =

    bl+bl)

    ((a

    +

    l)bl=bl

    +

    b3)

    ((a + l)bl

    =

    bl+b3)

    ((a

    +

    l)b3-bl+b2>)

    (bl+a(bl)

    +

    (a

    +

    l)b3=0)

    (bl+(a

    +

    l)bl

    +

    a(b3)

    =

    0)

    EXAMPLE

    21

    points listed in Example 20. One strategy?not the only one ?is to

    begin

    with

    a

    reference

    quadrangle.

    Example

    22

    assigns

    to

    Example

    19

    the values

    pl

    =

    {CE},

    pl

    =

    {FA},

    p3

    =

    {GB},

    r3

    =

    {EG},

    rl

    =

    {DA},

    r2

    -

    {BFU

    =

    {AC}.

    EXAMPLE

    22

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    34

    Perspectives

    of

    New Music

    These assignments give

    a

    "C-major"

    sort

    of reference

    to

    thequadrangle?a

    feature evident

    in

    Example

    23a,

    where the bracketed

    segments

    are

    collinear.

    pi

    r3

    pi

    rl

    p3

    rl

    pi

    pi

    q

    rl

    r3

    q

    p3 p2

    q

    r2 r3

    rl

    p3

    rl

    pi

    EXAMPLE 23

    Example

    23b

    projects

    the

    same

    formal

    "lines"

    as

    verticalities,

    indicat

    ing

    another

    textural

    possibility.

    No

    rhythm

    is

    indicated.

    I

    have

    not

    exer

    cised

    any

    special

    control

    over

    the

    voice

    leading

    here,

    simply

    trying

    to

    project

    vaguely Stravinskyish spacings

    of the

    dyad-triples.

    Example

    23

    illustrates how the reference

    quadrangle

    of

    Example

    22

    yields

    a

    seven-point subplane

    of the

    twenty-one-point plane. In the

    present

    context,

    it is natural

    to

    arrive

    at

    the full

    plane

    by

    "diminuting"

    Example

    23a. To

    see

    what that

    means,

    consider the first three

    dyads

    of

    Example

    23a. These

    dyads,

    playing

    the roles of

    pi,

    r3,

    and

    p2,

    all lie

    on

    line

    J3

    of the

    full

    plane,

    but

    they

    do

    not

    constitute the

    entire

    line

    J3

    of

    that

    plane.

    The

    full line

    J3,

    as we see

    in

    Example

    21,

    contains

    not

    only

    the

    points

    pi,

    r3,

    and

    r2,

    but

    also the

    points

    s3 and

    s3',

    points

    not

    appearing

    on

    the reference

    quadrangle.

    We

    can

    naturally

    imagine

    dyads

    s3 and

    s3',

    in

    this

    context,

    appearing

    "in

    passing"

    to

    elaborate the

    pro

    gression pi,

    r3,

    p2

    of

    Example

    23a. The

    first

    phrase

    of

    Example

    24a

    materializes

    that

    notion.

    In

    that

    phrase,

    the

    progression pi,

    r3,

    p2,

    which

    began

    Example

    23a,

    is

    diminuted

    by

    transitional

    dyads

    {CG}

    and

    {EB}

    that

    appear

    on

    the off

    beat

    eighths.

    To subsume those

    dyads

    onto

    line

    J3,

    we

    assign

    them the

    point-values

    s3

    and

    s3',

    the other

    points

    of line

    J3.

    The first

    ive

    dyads

    of

    Example

    24a will then

    project

    line

    J3

    in

    its

    entirety.

    In

    like

    spirit,

    the

    second five

    dyads

    of

    Example

    24a take the

    progression

    p2,

    rl,

    p3

    from

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    Projective

    Geometry

    35

    pi

    r3

    p2 p2

    rl

    p3 p3

    r2

    pi pi

    q

    ri r3

    q

    p3

    p2

    q

    r2 r2

    r3

    rl

    s3 s3'

    si si'

    s2 s2'

    tl tl'

    t3 t3' t2

    t2'

    v u

    EXAMPLE

    24

    Example

    23a,

    and diminute

    it

    by

    inserting

    transitional

    dyads

    {FG}

    and

    {CD}

    on

    the

    off-beat

    eighths;

    the

    transitional

    dyads

    are

    then

    assigned

    as

    points

    si and

    si',

    so

    the

    phrase

    as a

    whole

    projects

    line

    Jl

    =

    {p2,

    p3,

    rl,

    si,

    si'}

    in

    its

    entirety.

    Example

    24a

    proceeds

    in

    the

    same

    spirit through

    out.

    It

    turns

    out

    (in

    this

    plane )

    that

    every

    remaining point

    of the

    plane

    will be referenced exactly once, by diminuting Example 23a in such a

    way.

    One

    can

    see

    that

    by

    inspecting

    Example

    21;

    there

    one

    sees

    that the

    lines

    Jl,

    J2, J3,

    L, Ml, M2,

    and M3

    collectively

    reference

    point

    u,

    point

    v,

    each

    ?-point,

    each s'

    -point,

    each

    i-point,

    and each t'

    -point

    exactly

    once.

    And those

    are

    the lines

    which

    appear

    in

    part

    on

    Example

    23a,

    as

    progres

    sions

    to

    be

    "diminuted."

    Example

    24b

    realizes the

    five-dyad

    lines

    as

    verticalities,

    elaborating

    the

    three-dyad

    verticalities of

    Example

    23b.

    The

    new

    dyads

    are

    shown with

    filled-in

    noteheads.

    Orchestration

    and/or

    other

    compositional

    means

    (dynamics,

    order of

    entrance

    and

    exit,

    amount

    of

    sustained

    time,

    etc.)

    could

    be used

    to

    project

    the

    idea that the

    open-notehead

    parts

    of each

    sonority

    is

    more

    in

    the

    nature

    of

    a

    Zentralklang,

    while

    the filled-in

    noteheads

    project

    Akzidentien}2

    On the

    other

    hand,

    a

    composer

    might

    not

    choose

    to

    project

    explicitly

    the

    "referentiality"

    of

    Example

    23b,

    treating

    that

    only

    as

    a

    work

    ing

    method

    to

    arrive

    at

    the full

    twenty-one-point

    structure.

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    26/53

    36

    Perspectives

    of

    New

    Music

    DEFGABEFGABFGAB

    CCCCCCDDDDDEEEE

    si'

    pi

    t3' s3

    q

    tT t2' s2' t3 rl t3

    u

    r3

    v

    s3'

    G

    A B A B B

    F F F G G A

    si

    p2

    r2 s2

    p3

    t2

    EXAMPLE

    25

    Example

    25 shows

    the

    assignment

    of

    dyads

    to

    points,

    that

    eventuates

    from the diminutions of

    Example

    24. In

    working

    out

    those

    diminutions,

    it is

    helpful

    of

    course to

    keep

    a

    running log

    of

    Example

    25

    as

    it

    develops,

    to

    be

    sure

    that each

    dyad

    is

    used,

    and used

    only

    once.

    Now

    that

    we

    have

    assigned

    a

    dyad

    to

    each formal

    point

    of

    Example

    20,

    we

    automatically

    know

    the formal lines of

    Example

    21?in

    particular

    the

    fourteen lines of that example not yet involved in the constructions of

    Example

    24.

    t3 si

    u

    tT

    pi

    v

    t3'

    tl

    pi

    si' rl

    si

    s3 t3' tT

    EXAMPLE

    26

    Example

    26a

    projects

    lines

    Nl,

    Nlf,

    and

    Kl

    of

    Example

    21 into

    the

    musical

    texture

    of

    Examples

    23a and

    24a,

    loosening

    up

    the

    rhythm

    and

    "bowing"

    a

    bit.

    Example

    26b

    imagines

    a more

    flexible

    texture

    than

    any

    so

    far

    presented;

    in that

    texture

    it

    projects

    lines

    J3,

    G,

    and

    if

    as

    indicated.

    The interested reader, taking hints from this example, will quickly dis

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    Projective

    Geometry

    37

    cover

    many

    other

    textures

    inwhich

    to

    project formal

    lines

    of the plane,

    and

    many

    other

    musical

    resources

    for

    linking

    the lines

    together.

    Many,

    many

    other "modes"

    are

    of

    course

    available for

    assigning

    dia

    tonic

    dyads

    to

    the formal

    points

    of

    Example

    20. The

    choice of

    our

    "C

    major"

    mode

    was

    only

    to

    facilitate

    hearing

    for

    the

    first

    such

    mode

    to

    be

    studied.

    Within

    a

    composition,

    one

    could

    "modulate"

    between

    different

    such

    modes,

    particularly

    if

    they

    have formal

    lines

    in

    common,

    with

    which

    to

    "pivot."

    Or

    one

    could

    transpose

    a

    mode via

    any

    number of

    semitones,

    introducing

    new

    tones.

    Example

    24a,

    using

    a

    ficta

    F|

    within

    our

    mode,

    suggests

    one

    such

    possibility.

    Finally

    one

    can use

    mathematical transfor

    mations that

    are

    particularly

    characteristic for

    projective planes.

    Part

    V: Collineations

    in the

    Projective

    Plane

    It is

    time

    now

    to

    bring

    such

    transformations

    into the

    picture.

    A

    collinea

    tion

    is

    a

    function f that

    permutes

    the

    points

    of

    a

    projective plane

    among

    themselves in such fashion

    that,

    whenever

    points

    p,

    q,

    and r are

    collinear,

    so are

    ?(p),

    ?(q),

    and

    f(r).

    Loosely

    speaking,

    a

    collineation

    is

    an

    operation

    on

    points

    that

    "preserves

    lines."

    If

    point

    p

    varies

    along

    line

    L,

    then

    f(L),

    the

    locus of the

    points f(p),

    will

    itself be

    a

    line.

    f(Z)

    may

    or

    may

    not

    be

    the

    same

    line

    as

    L.

    Obviously,

    collineations

    are

    particularly

    idiomatic

    sorts

    of

    transforma

    tions

    to

    consider,

    given

    the

    points

    of

    a

    projective plane.

    The

    collineations

    form

    a

    group

    of

    operations.13

    Here is the basic theorem concerning collineations: letpl, p2, p3, and

    p4

    be

    points,

    no

    three of which

    are

    collinear;

    let

    pi, p2',

    p3',

    and

    p4'

    also

    be

    such

    a

    quartet

    of

    points;

    then there exists

    a

    collineation

    f

    such

    that

    f(pl) =pl',

    f(p2)

    =

    pi, f(p3)

    =

    p3',

    and

    ?(p4)

    =

    p4'.

    In

    this

    context

    the

    p'

    -points

    may

    all

    be distinct from the

    ^-points,

    or

    various of

    the

    p'

    -

    points

    may

    be the

    same as

    various

    of the

    ^-points;

    the

    theorem obtains

    in

    any

    case.14

    As

    one

    intuits from

    the

    theorem,

    there

    are a

    "large

    number" of

    col

    lineations

    on a

    given plane. To sharpen that intuition, letus examine col

    lineations

    on

    the

    seven-point plane.

    For that

    purpose

    Example

    27

    essentially

    reproduces

    an

    earlier

    sche

    matic for the

    plane.

    Points

    1,

    3,

    and 5 of the

    example

    are

    non-collinear;

    we

    can

    take them

    as

    the

    generic

    "pl,

    p2,

    and

    p3"

    of

    the

    theorem.

    We

    are

    also

    to

    consider

    a

    generic

    "?>4"

    not

    lying

    on

    line

    13,

    or on

    line

    35,

    or

    on

    line

    51.

    Point 7 is

    the

    only possible

    such

    p4,

    for this

    plane.

    Given

    points

    pi,

    pi,

    p3',

    and

    p4'

    as

    stipulated,

    let

    us

    find

    a

    collineation f

    as

    in the

    theorem.

    We

    know that

    any

    such

    f

    must

    satisfyf(l)

    =

    pl ', f(3)

    =

    pi, f(5)

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  • 7/23/2019 Lewin - Some Compositional Uses of Projective Geometry

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    38

    Perspectives

    of

    New

    Music

    A

    seven-point plane:

    123, 345,

    and

    561

    are

    all formal "lines" of the

    geometry;

    so are

    174, 376, 572,

    and 246

    example

    27

    =

    p3', f(7)

    =

    p4'. Subject

    t


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