R ENDICONTI
del
S EMINARIO M ATEMATICO
della
U NIVERSITÀ DI P ADOVA
D. G. H IGMAN
Coherent configurations I
Rendiconti del Seminario Matematico della Università di Padova, tome 44 (1970), p. 1-25
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D. G.
HIGMAN *)
In the
theory
ofG-spaces (G
a finitegroup)
there arise certain combinatorialconfigurations
which we call coherent[ 6 ] .
It is thepurpose of the present paper to
lay
theground
work for asystematic study
of this class ofconfigurations
in their ownright.
The first twosections, containing generalities
aboutgraphs,
incidence structures andmatrices,
are included to establish our notation and to make the paper self-contained. Coherent(and
semicoherent) configurations
are definedin §
3 and the way whichthey
arise in thetheory
ofG-spaces
is indicated. Our main line of attack instudying
theseconfigurations
isthrough
theirsemigroups
of relations and centralizerrings,
discussedin
§§
4-6together
with thedecomposition
into orbits. The methods of intersection matrices(cf. [5])
and coherentpartitions
are available forcoherent
configurations
as is shown in§§
7 and 8.In §
9 we considerthe
question
ofcoarsening
andrefining given configurations
and in§
10 we introduce a concept ofprimitivity
and consider its relation to conne~cte~dnes~s. Further workconcerning extensions, automorphism
groups, and some classification theorems will be discussed in a second paper.
Coherent
configurations generalize
the notion of association scheme(cf. [2])
and so encompass, forexample,
thestrongly regular graphs
of Bose
[1].
Additional types ofconfigurations,
forexample
the sym- metric blockdesigns,
are included as indicated at the endof §
6.*) Indirizzo dell’A.: Dept. of Mathematics University of Michigan, Ann Arbor, Michigan 48104, U.S.A.
Research supported in part by the National Science Foundation.
1.
Relations, graphs
and incidence structures.The sets
X, Y,
... considered in this paper will all be assumed to be finite. A relation from a set X to a set Y ,is ~a sub,set of X XY;
we denote the
totality
of theseby
Rel(X, Y), simplifying
the notationto Rel X in case X = Y. The converse of
fe
Rel(X, Y)
is the relationx)l(x, }
inRel (Y, X).
For xeX we putand
Relations
f e
Rel(X, Y)
and g E Rel(Y, Z)
arecomposed according
tof g = { (x,
togive f g E
Rel(X, Z).
Theidentity
relationis an
identity
for thiscomposition
~sa we have acategory,
the category of relations(between
finitesets),
which we denoteby
Rel.We denote
by Map (X, Y)
the set of maps from X toY, writing Map
X forMap (X, X),
andregard
the categoryMap
of maps(between
finitesets)
as asub~category
of Rel.With
f E
Rel(X, Y)
there is associated agraph Xf having
thedisjoint
unionX + Y
of X and Y as vertex set andf
asedge
set.The
left equivalence
kernelLt=
U(ffU)n
andright equivalence
n*o
kernel U of
f E
Rel~(X, Y), f ~ ~,
areequivalence
relationsn>0
in Rel X and Rel Y
respectively,
and We see that any two of the conditions(i)
XX, (ii) L f f = X
XY,
and(iii) Rf= Y
XY, imply
thethird; Xf
is said to be connected if these three conditions hold.An incidence
structure elf having Xf
as its Levigraph (cf. [3])
isobtained
by taking X,
Y andf respectively
as thepoints,
blocks andflags.
Assume that X=Y. With
fe REIX
there is associ,ated a secondgraph §/ having
vertex set X andedge
setf .
Thegraph lsf
is connectedif the kernel
Ef=
Ufn of f is equal
to X X X. Itis,
of course,quite
pos-m>0
sible that either one of the
graphs Rt
is connected while the other is not, but we note that( 1.1 ) If E
f is anequivalence
relationfor
somef
in RelX,
thenconnected if 3C/
is. ,2. Matrices.
The category MatK of matrices in
K,
where K is a coefficientring
which we will choose to be commutative withidentity element,
has as
objects
the finite setsX, Y,
... and asmorphism
the maps X X Y ~ K. We write MatK(X, Y)
for thetotality
of these and compose MatK(X, Y) and +e
MatK( Y, Z) according
to matrixmultiplication
to obtain MatK
(X, Z).
We write MatK X for MatK(X, X).
char
The maps
Rel (X, Y) ~ MatK ’(X, Y),
wherechar f, f e
Rel(X, Y),
spt
is the characteristic function and ,spt cp, 9 c MatK
(X, Y),
is the support of cp, are such that spt o ~char=1. Of course these maps are notfunctorial, but,
e.g., if useMap~(X, Y), IE Rel (X, Z)
thenGiven
orderings
of X and Y we represent9 c MatK (X, Y) by
thematrix
We
write B
f forBo
if p=char f , IE Rel(X, Y),
sothat Jff
f hasadja-
cency matrix
(0 0 ) j ft
0and Yj
has incidence matrixB f .
In caseX = Y,
B f
is theadjacency
matrixWe see that for
IE Rel,(X, Y), blocking B
faccording
toL f
andR f corresponds
to fulldecompositions
ofB f
underpermutation equiva-
lence. In
particular
(2.1 )
Forf E
Rel(X, Y), Xt
is connectedif
andif B f
is indecom-posable
underpermutation equivalence.
If a E X and
f E
Rel(X, Y),
weput
and
(2.2)
Assumethat XI
is connected.Blocking
the rowsof B f according
to the and the columnsaccording
to thei=O, 1,
...,corresponds
totransformation
underpermutation equiva-
lenceof Bf
to theform
where
b,i
is a l-rowedmatrix,
andfor
alli,
each rowof
the block bii and each columnof
the blockbi+li
contains anWe now consider
fe
Rel X such thatE f
is anequivalence
relation.We see that a reduction of
B f
underpermutation similarity
is automati-cally
’a-decomposition
and thatblocking B f according
toE f corresponds
to full reduction of
B f
underpermutation similarity.
Inparticular (2.3) If f E
Rel X is such thatEf
is anequivalence relation,
thenthe
following
statements areequivalent.
a) gt
is connected.b) B f
is irreducible underpermutation similarity,
andc) B f
isindecomposable
underpermutation similarity.
Given
f c
Rel X land x,yeX
we define:pf(x, y) =
the leastinteger
such that
(x, y) E f L,
or 00 if no such i exists.For
i >_ 0,
thef-circle
with center x and radius i isThe diameter of the
graph gf
f is defined to be(2.4)
Assume is connected. Thenblocking Bf according
to the circles
i =1,
2, ...,for given
xeXcorresponds
to trans-formations
underpermutation similarity of Bt
to theform
in which C12 is a l-rowed
matrix,
each block cii is square, and each columnof
the block cii+l contains anentry ~ 0.
The number mof
blocks on the main
disgonal
is one greater than the diameter3. Coherent and semi coherent
configurations.
We think of
configurations consisting
of finite collections ofdisjoint
sets
together
with finite collections of relations betweenthem,
and visualize the relations in terms of the associatedgraphs
and incidencestructures as described
in §
2.By
an obvious device we can reduce the number of sets to one, so asufficiently general
definition of combina- torialconf iguration
is apair ~(X, 0) consisting
of a set X and a setQ
of relations on X. Aconfiguration go= (Xo , Oo)
will be called asubconfiguration
of g=,(X, 8),
written go g, if Xo c X and80ç 8 1 Xo ,
where
O
n(Xo
XXo) 1.
Thefull subconfiguration
onxocx is
(Xo, 8 Xo).
We now
single
out the class ofconfigurations
ofparticlar
interestto us here. Given a
configuration (X, O) and f,
g, we definean
( f ,
g,h)-triangle
to be an orderedtriple (x,
y,z)
such that(x, y) E f , (y, z) E g
and(x, z)eh.
We call(X, O)
coherent if1) O
is apartition
of X XX,
2)
theidentity
relation Ix is a union of members ofO, 3) f E D implies
and4)
forgiven f ,
g, and(x,
the number of( f ,
g,h)- triangles (x
y,z)
isindependent
of the choice of(x, z);
we denotethins number
by
a fgh .Our motivation for this definition comes from almost obvious fact that
(3.1 ) If
X is aG-space for
some groupG,
andif OG(X )
isthe set
of
G-orbits in X X X(under componentwise action),
then(X, OG(X)) is
coherent.On the one hand this
provides
us with a rich source of coherentconfigurations,
and on the other with abridge
between grouptheory
and combinatorics. A coherent
configuration
obtained from the action of a group G on a set X as in(2.1 )
will be said to be realizedby G,
or
by
the action of G onX,
orby
theG-space
X.We carry over much of the
terminology
of thetheory
ofG-spaces (cf. [6])
togeneral
combinatorialconfigurations t3=(X, 8)
The numberI
will be called thedegree
of t3. The relations in0
will be referred to as the orbital relations of g and their numberr= ~ I 81 I
asthe rank of g. The
mapping
is called thepairing
ong. The numbers afgh of
4)
will be called the intersection numbersof
g. Association schemes(cf. [2])
arejust
those coherentconfigurations
with
Ix E O
and trivialpairing.
Assume that g is coherent. For
xeX,
the set{ f (x) ~ f E O, f (x) ~ ~ }
is a
partition
of X. Moreover(3.2)
Forf ,
g, and(x,
Hence
For some purposes it i,s convenient to
replace
condition4)
of the definition of coherentconfiguration by
4’) Given f ,
g, and(xi , i =1, 2,
there exists an( f , g, h)-triangle (xl ,
yi ,zi)
if andonly
if there exists an( f ,
g,h)- triangle (X2,
Y2,Z2);
we write or 0according
as suchtriangles
exist or not.
Of course
4) implies 4’),
with oraccording
asor We
call g
semi coherent if1), 2), 3),
and4’)
aresatisfied.
~4. The
semigroup
of relations and the centralizerring.
Let
g=(X, D)
be a semicoherentconfiguration.
Then the setR = R( g) consisting
of0
and all unions of members ofO
is a sub-semigroup
of Rel X undercomposition.
Infact, given 1),
a necessary and sufficient condition for4’)
is that R is closed undercomposition.
We refer to R as the
semigroup of
relations of g . The elements of Rwe refer as
g-relations;
in case g is realizedby
a group, these are the G-relations[ 7 ] .
Regarding
Rel X as a vector space overF2
with respect to symme~tric
difference,
so that R is thesubspace spanned by D,
theproduct off
and g inD
isIf the
pairing f
HfU
on g istrivial,
then R is commutative.From now on in this section we assume that g is
coherent,
and choose a cofficientring K,
commutative with 1. The setC = CK{ g )
ofall qE MatK X which are constant
on f
for everylEe
is a free K-sub- module of MatK X with the setI
as basis. We havef or f ,
thatso that C is a
K-subalgebra
of MatK X. We refer to C as the centralizerring of
g overK;
if g is realizedby
the action of a group G on the setX,
then C is the centralizerring
of theG-space
X. If thepairing
on g is
trivial,
then every issymmetric,
hence(4.1 ) If
thepairing
g istrivial,
then C is commutative. Since C is closed under the transpose map.(4.2) If
K is afield of
characteristic0,
thenCK(g )
issemisimple.
Taking
K to be thecomplex
number fieldC,
we have thatm
(4.3)
r = Ee12
where el , ..., em are the structure constantsof
;=i
Cc(g), i.e.,
thedegrees of
theinequivalent
irreduciblerepresentations of Cc(0).
We refer to the ei as the structure constants of g.
Now suppose that X is a set #0 and
em
is a subset ofMatzX
such thata) cp(x, y)e(0, 1’} 1
for allcpecm
and all x,b) £ y)=1
for all x,yeX, c)
char Ix is a sum members ofc%, d) qEB implies
ande)
theZ-submodule
B ofMatz X spanned by B
is asubalgebra.
Then it is not difficult to see that
g = (X, .9),
whereis a coherent
configuration
withC2(g)=B.
5. Orbits.
Let
g=~(X, 8)
be a semicoherentconfiguration.
Thenwhere the Ei are
uniquely
determined elements ofO.
We havedom Ei=range Ei ,
anddenoting
thi,s setby Xi ,
E; induces theidentity
relation on Xi . The Xi , which we refer to as orbits of g, or the
g-orbits,
constitute a
partition
ofX;
in case g is realizedby
a group, the Xiare the G-orbits in X. We call g transitive
if ~ ~- ~ , i.e.,
ifIx E O.
Thedegree
of X = is defined to beX I,
andWe now observe that
(5.2)
Forfee, dam Xi
and rangef = X; for
somei, j.
PROOF. We have for some
i,
and thenIf xe
dom f ,
there exists an element zeX such that(x, z)ef.
Theremust exist an
f , f)-triangle (x,
y,z)
and hence xedom E1= Xi ,
That is
Again,
if xedom f
and(x, z)Ef,
then(x,
z,x)
is an( f , fU, Ei)- triangle,
soaffUEi
=1. Hence ifyEXi,
there must exist an(f, fu, Ei)- triangle (y,
w,y),
and hence ye,dom f.
Thusdom f = X i ,
and rangef =
for some
j.
We
put
and rangef = X; },
so that{ Oi’ ~ I
isa
partition
ofO by (5.2).
Note thatif f ,
g, thenimplies
that
geeik
andheÐik
for somei, j,
k. The numberÐii I
will be called the rank of the
pair Xi , X; ;
in case g is realizedby
a groupG, ri;=rankG (Xi , Xi) (cf. [6]).
We haveIt is clear that full
subconfiguration
on the union of anynonempty
set of orbits of a
(semi)
coherentconfiguration
g is(semi)
coherent.In
particular,
the fullsubconfiguration gi
on Xi is(semi)
coherent ofdegree ni
and rank rii , and is transitive.For the rest of this section we assume that g is coherent.
For
and if we put
I f(x) 1,
thenIn
particular,
n f isindependent
of the choice of soMoreover
The numbers n f ,
fEO
are called thesubdegrees
of g.If
f ,
g, and there exi.stsxe dom f n dom h,
then .afghnh = the number of
( f ,
g,h)-triangles (x,
y,z)
= the number of
~(h, gu, f )-triangles (x,
z,y)
=ahgUfnf.
In
particular
Two further relations for the intersection numbers are
and
and
6.
Decomposition
of the relationsemigroup
and centralizerring.
Assume that g is semi coherent. The
semigroup
R of relationsdecomposes
into adisjoint
unionwhere Rii is the
Frsubs.pace
of Rspanned by
We haveFurthemore Rzi is
isomorphic
with thesemigroup
of relations of0~.
Now assume that C is coherent.
Taking
a commutative coefficientring
K withidentity element,
we obtain a similardecomposition
of thecentralizer
ring by putting I spt
XX; } .
ThenCij is a K-submodule of C with K-basis and
as a K-module. We have Cij Ch k = 0 and Ctt is
isomorphic
with the centralizerring
ofgi.
Taking
anordering
of X consistent with thepartition }
andassociating
with eachtpec
the matrix we see that forcp E Ci’, Bo
has the formFrom
(5.12)
and(5.13)
it f ollows that iff ,
thenBcp
has row sum n f and column sum ntu . Inparticular,
(6.1 )
Each Cii has a linearrepresentation.
From
(4.3)
and(6.1 )
we see that(6.2) I f
rii 4, then Cii is commutative.(If
g is realizedby
a group, then Czi is commutative for rii=5too.)
We now consider the case in which g has twoorbits, i.e., t = 2,
so
that,
in terms ofmatrices,
the centralizering C=Cc(g)
is a semi-simple subalgebra
ofCan
andand C~ are
semisimple,
and weregard
C12 as a module over the semi-simple ring
Then we see withoutdifficulty
that the decom-position
.of Ci‘ into
simple
two-sidedideals,
and thedecomposition
of el2 into
simple
submodules over can be soarranged
thatC«2
is faithful for 1 a s. Hence we see that thesimple
components of C are
where
together
withCii, i =1,
2.This means that
( 6.3 ) If
t=2, then the structure constants eia., 1for gi, i =1, 2,
can be so numbered that the structure constantsfor
g are eta. + e2a., s 1 a s,together
with eix, s -i-1 a mi ,i =1,
2, and thenThus,
forexample,
if rli = 2 andr22 = 3,
thenby (6.2)
and(6.3),
r12 2.We have remarked
in §
3 that the transitiveconfiguration
withtrivial
pairing
arejust
the association schemes. Ingeneral,
if thepairing
on g is
trivial,
g coherent theng’
is an associationscheme,
and ifwe put then
I
i,s a concordantfamily
ofgraphs
in the sense of Bose and Mesner[2],
andOf
is a
partially
balancedincomplete
blockdesign.
At this
point
we lookbriefly
at the types ofconfigurations arising
for somespecial
values of r.Let g
= (X, 8)
be a coherentconfiguration
ofdegree
n and rankr, with t orbits
Xl , X2 ,
..., Xt .1)
The extremepossibilities
for r are r =1 and If r =1then n =1 so this case is included in the case r = n2. If
r = n2,
thenO
is the
totality
of one-element subsets of X XX,
the orbits are the one- element subsets ofX,
so that t = n. R is the fullsemigroup
Rel X ofrelations on X and C is the full matrix
ring
Matx X. In this case werefer to g as a trivial
configuration.
It is realizedby
any group Gacting trivially
on X.2)
There isjust
one coherentconfiguration
of rank 2 on agiven
set1 X I, )Xj~2.
It is realizedby
any group Gacting doubly transitively
on X. Here and C , K (D K.3) If
r=3, then s~aI x E O,
and0 = { I x , f , g } .
If thepairing
istrivial,
so that andg= gU,
then thegraphs §/
and~g
are a
complementary pair
ofstrongly regular graphs. Conversely, given
a
strongly regular graph
with vertex set X andedge
setf ,
the confi-guration (X, O),
is coherent of rank 3.
Any
rank 3permutation
group of even order realizes aconfiguration
of this type, while the rank 3 groups of odd order realize rank 3configurations
with non trivialpairing.
4)
Ifr:58,
then t 2. If r7 and t = 2 then r12=1 so that the two orbits arejoined together
in a trivial way. The firstinteresting
case in which t = 2 is r=8 with m=r22=n2==2. If we write
0~2 = { f , g} }
and and
g = g n (X i X X2)
then andelf
are acomplementary pair
of(possibly degenerate)
blancedincomplete
blockdesigns
which aresymmetric
if andonly
if ni = n2 .7. Intersection matrices.
We consider once more a coherent
configuration 0 =(X, O), maintaining
the notation of thepreceding
two sections. For purposes ofcomputation
we take anordering
of X consistent with the decom-potision
intoorbits,
and anumbering
of the elements of eachsuch that
where,
of course, thepairing ~(i) :
a - a’depends
on i. We writeni=1 Xi I
and so thatand
By (7.1)
and(5.6),
(This
accounts for all the non zero intersection numbers. The arrange- ment ofsubscripts
is because of our ultimate interest in theregular representation
ofC.)
The matrix
B~
has the formand
The
following properties
of theMf
are i-mmediate.Mf
has rowsum na
and column sumna .
where
J
has all entries 1.a
Conversely,
it is not difficult to see that a setof
(0, 1 )-matrices satisfying (7.6) through (7.9),
with the coefficients in(7.6) nonnegative
rationalintegers,
is associated with a coherentconfiguration.
Let
X;) and, using
the notationof § 1, put
0 mii
Then
giia
hasadjacency
matrixm
orMaii according
as ori=i.
-
( m
a 11 0The
regular representation
of C is theisomorphism
of C onto asubalgebra
C of MatK Q such that forIn terms of
matrices, Bij
maps ontoBx
of the formwhere the blank entries are all zero,
and
We refer to the matrices as the intersection matrices for g.
If we
put
then the restriction of the
regular representation
of C toCi’ gives
ahomomorphism
which is the
regular representation
of Cii in case and isbijec-
tive in case k = i or
k = j.
Now we summarize the
properties
of intersection numbers in termsof our
present
notation.According
to(5.10)
and(5.11)
that is
By (5.4)
and(5.5)
By (3.3)
By (2.8)
From
( 7 .12 )
and( 7 .15 )
we getand in
particular
nik is ale f t eigenvector o f
witheigenvalue
For convenience of reference we note
explicitly
certain of the sim-plifications
in notation which can be made in case g is transitive. Herewe
drop
thesuperscripts, writing
we
drop
thesuperscripts, writing O = { f 1 , f 2 ,
...,fr) }
withf i = Ix
andf ~~
=f a- ,
and so thatWe write Ba for
Bfa
and Ma for thecorresponding
intersectionmatrix,
so that
and
where We have
and
i.e.,
In
particular,
since mp = mo, ,Under the
regular representation,
B(1. maps onto Ma so(7.27) If F(t)eC[t]
is such thatF(M(1.)=O,
andif
0 is a rootof F(t) of multiplicity
m, thenis a rational
integer.
In
fact,
11e is themultiplicity
of 0 as aneigenvalue
of B~ .8. Coherent
partitions.
In this section
g = (X, O)
denotes a coherentconfiguration.
Werefer to a
pair (x, y) E f
as anf-edge.
Apartition 9
of X is coherentif,
forf E Q, S,
and the number ofledges (x, y)
withyeT
isindependent
of the choice of This number isIn
particular, 9
is coherent if andonly
if each block of each matrixBp , cpEC,
when blockedaccording
to9,
has constant row(and column)
sum.
Let 9
be a coherentpartition
of X and let See.for
some i,
and if andy E S,
then the number ofEi-edges
fromx to
S, namely
1, isequal
to the number from y to S. HenceyEXi
Z andIn
particular I
is apartition
of Xi and isclearly
coherent for
g i.
The
following simple
fact is useful.(8.1 ) Let 9 be a
coherentpartition of X, and, for 9 e C,
S, andXES,
putThen
- qpgp is a K-algebra homomorphism of
C onto asubalgebra C~ o f
PROOF. is well-defined because of the coherence of
~,
andis
clearly
K-linear. Take cp,S,
and thenHence
proving (7.1 ).
The matrix of is obtained from
Bcp by blocking according to #
and
replacing
each blockby
its row sum.Certain coherent
partitions
arealways available, namely,
chooset
and We know is a
partition
7=1
of X. For
/e9
and g, the number off -edges
fromxEg(Xk)
toh(xk)
is ’which is
independent
of the choice ofx E g(xk).
Hencegk
iscoherent,
andwe see that in terms of matrices in the notation
of § 7,
mapsonto
that
is,
if Pi is thepermutation
matrix of thepairing ~(i) :
a ~oc’,
thenFrom
(8.2)
we see that the statements(2.1 ) through (2.4)
con-cerning connectedness,
etc., asapplied
to thegraph
hold with theintersection matrix
M’j’
i inplace
ofMii.
(HereMa plays
the role of the matrixB f of § 2.)
Moreprecisely,
(8.3) If j,
then is connectedif
andonly if Ma
is indecom-posable
underpermutation equivalence.
(8.4) Assuming
that is connectedfor
some then(2.2)
holds withM’j’
i inplace of
(8.5)
Thefollowing
areequivalent:
a) is
connected,
b)
is irreducible underpermutation similarity,
andc)
isindecomposable
underpermutation similarity.
(8.6)
Assume that~x
is connected. Then(2.4)
holds with inplace of
9.
Automorphisms,
refinements andcoarsenings.
An
automorphism
of aconfiguration
g =(X, c9)
is apermutation
ofthe elments of X which permutes the elements of D under
component-
wise action on X X X . Anautomorphism
is strict if thepermutation
in-duced on
D
is trivial. The strictautomorphisms
of g constitute a nor-mal
subgroup
Aut * g of the group Aut g of allautomorphisms
of g .We say that a group G is
represented
in the(strict) automorphism
group of g if G acts on X in such a way that the
permutations
of Xassociated with the elements of G are
(strict) automorphisms
of g, or,what is the same
thing,
if there is ahomomorphism
of G into(Aut
*g )
Aut g. The
configuration
g is realizedby
the action of a group G onX, i.e., O = OG(X),
if andonly
if G isrepresented
in the strictautomorphism
group of g and rank G X=r
(where
r is the rank ofg ).
Suppose given configurations O1) and g 2 = (X, 02)
such that81
and(92
arepartitions
of X X X. We call gi a refinement of g2 if81
is arefinement
of82;
if inaddition,
gi is(,semi) coherent,
we say that gl is a(semi)
coherentrefinement
of g2 . It is clear that(9.1 ) If g 1 is a
coherentrefinement of
a coherentconfiguration
g, the the orbits
of
g constitute a coherentpartition of
g(in
the senseo f § 8).
An immediate but useful remark is
studying automorphism
groups ofconfigurations
is(9.2)
It a group G isrepresented
in the strictautomorphism
groupof a configuration g= (X, 8),
then theconfiguration (X, OG(X))
is acoherent
refinement of
g. Inparticular, if
g iscoherent,
then the G-orbits in X constitute a coherentpartition of
X.If gi is a refinement of g2 , then 92 will be called a
coarsening
of B]1 ;if,
inaddition,
02 is(semi)
coherent it will be called a(semi)
cohe-rent
coarsening of
g 1.(9.3) If g is a
transitive coherentconfiguration
such that its cen-tralizer
ring Cz (g )
iscommutative,
thengl = (X, 81),
whereO1=
coherent
coarsening of
t3.The
proof
of(9.3)
is astraightforward application
of the conditionsa) through e) given
at the endof §
4,together
with the fact that theassumed
commutativity
and(3.3) imply
that afuguhu=afgh forf,
g,h E O.
We can
replace
coherentby
semi coherent in(9.3)
if we assume commu-tativity
ofR(g)
instead ofCz(g).
As a sort of dual to
(9.2)
we have(9.4)
Let G berepresented
in theautomorphism
groupof
a tran-sitive coherent
configuration g=(X, 0).
ThenO1),
where(9i={ I
UI
coherentcoarsening of
g .,7eG
The
proof
is similar to that of(9.3), using
the fact that for C1E Autg, and f ,
g, Coherent can bereplaced by
semi coherent in
(9.4).
10.
Prbmitivity
and connectedness.In this section
g = (X, O)
denotes a semi coherentconfiguration.
We call g
primitive
if theonly equivalence
relations in R are Ix andX X X;
thisimplies
that g is transitive. We call gimprimitive
if it istransitive and not
primitive.
These definitions are consistent with themeaning
of these terms in thetheory
ofG-spaces
in case g is realizedby
a group.( 10.1 ) If g is
coherent andtransitive,
thenfor f E O,
the kernelEl of f
is anequivalence
relation.PROOF. Since R is closed under union and
composition, E f
is inR. Hence ...
-~- f n ,
soI
isindependent
ofxeX. If
yeEf(x),
thenEf(y)g;Et(x)
and henceE f(y) = E f(x).
SoE f
issymmetric
and hence anequivalence
relation.( 10.2) If g is coherent,
then g isprimitive if
andonly if
thegraphs ~ f ,
are all connected.PROOF. Assume that g is
primitive
and take ThenE f ~ Ix
soEf=X
X X which meansthat Ot
f is connected. On the otherhand,
suppose that E is anequivalence
relation in R and assume thatE ~ Ix . Then ...
+fm
with/ïEÐ and,
say, Thenso that is
connected,
X XLet E be an
equivalence
relation on X and let x : X -X/E
bethe natural map. For
IE
Rel X putI/E=’1tutrc,
so thatf /E E
RelX/E.
(10.3) I f g = (X, O) is
semicoherent andtransitive,
andif
E is anequivalence
relation inR(g ),
theng /E = (X /E, D/E),
whereO/E =
semicoherent and transitive.
PROOF. To show that
g/E
is semi coherent weverify
the condi-tions
1), 2), 3)
and4’) of §
4.1)
If(S, T)eX/E
XX/E,
take andyeT.
Then(x, y)ef
for some
fe(9,
so(S, r)~//B. Suppose
thatf, g~9.
Then so
f c EgE (since
HenceEfEçE2gE2==.EgE,
and
similarly
so thatE f E = EgE
and henceflE = glE.
HenceO/E
is apartition
ofX/E
XX/E
and1)
holds.2)
Since g istransitive, Ix E O
and hence3)
so3)
holds.4’)
Let thenR/E
is theF2-subspace
ofRel
(X/E) spanned by O/E.
Toverify 4’)
it suffices to show thatR/E
is closed under
composition.
Iff, geR,
thenwhich is in
R/E
asrequired.
Since
g/E
is transitive.In case g is realized
by
aG-space X,
so that then anecessary and sufficient condition for the
imprimitivity
of g in the sensedefined here is that X be an
imprimitive G-space.
In this caseg/E (as
well asg )
is coherent sinceO/E= OG(X/E).
( 10.4)
Let(9t),
2, be semi coherent and letf E Rel (Xl , X2),
such thatfURlfçR2
andfR2fuçRI,
whereThen
f
induces anisomorphism of g 1/L f
onto(j2IRf.
PROOF. Let 1CL: Xi and TCR : X2 --~
X21Rt
be the natural maps.By
the Fundamental Theorem onRelations,
is a
bijection.
Ifg E 81,
thenHence and the reverse
inequality
holdssimilarly.
(10.4) Applies,
forexample,
if gi and g2 are the fullsubconfigu-
rations on orbits Xi and X2 of a semi coherent
configuration
g andfeR12-
.As a
corollary
to(10.4)
we remark( 10.5)
Let t3l and g xand f
be as in(10.4)
and assume that g ~ isprimitive
and 92 is transitive. Theneither Xf
f is connected orf
inducesan
isomorphism of
gi ontog2/Rf .
PROOF. Since t3i 1 is
primitive,
etherLf=X
X X orL f = I x .
In thefirst case,
~f
is connected since 02 is transitive. In the second casef
induces an
isomorphism
of gi ontog2/R f by (10.4).
REFERENCES
[1] BOSE R. C.: Strongly regular graphs, partial geometries and partially balanced designs, Pacif, J. Math. 13 (1963), 389-419.
[2] BOSE R. C.: and MESNER DALE M.: On linear associative algebras corre- sponding to association schemes of partially balances designs, Ann. Math.
Stat. 30 (1959), 21-38.
[3] DEMBOWSKI PETER: Finite Geometries, Berlin, New York, Springer, 1968.
[4] HIGMAN D. G.: Finite permutation groups of rank 3, Math. Z. 86 (1964),
145-156.
[5] HIGMAN D. G.: Intersection matrices for finite permutation groups, Journal
of Algebra 6 (1967), 22-42.
[6] HIGMAN D. G.: Combinatorial Theory of finite G-spaces, in preparation.
Manoscritto pervenuto in redazione il 3 dicembre 1969.