Discrete Mathematics
North-Holland
111 (1993) 131-136
A homotopy
matroids
131
theorem on oriented
R. Cordovil zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
Centro de M atemirtica e Aplica@ es Fundamentais, Au. Prof. Gama Pinto,
2. 1699 Lisboa Codex, Portugal
M.L. Moreira”
Centro de M atemirtica da Unio. do Porte, P. Games Teixeira, 4000 Porte, Portugal
Received
22 July 1991
Abstract
Cordovil, R. and M.L. Moreira,
111 (1993) 131-136.
A homotopy
theorem
on oriented
matroids,
Discrete
Mathematics
Consider a finite family of hyperplanes
_%?= {Hi, . _., H,} in the finite-dimensional
vector space IWd.
We call chambers (determined by 2) the connected components
of W”\ U y=, Hi. Galleries are finite
families of chambers (C,,,C,,
, C,), where exactly one hyperplane
separates Ci+i from Ci, for
O <i<m, and exactly m hyperplanes
separate C, from C,. Using oriented matroid theory, we
prove that any two galleries with the same extremities can be derived from each other by a finite
number of deformations
of the same kind (elementary deformations). When the chambers
are
simplicial cones, this is a result of Deligne (1972). Our theorem generalizes also a result of Salvetti
(1987).
1. Introduction and notations
Let 2={CH,,H2,...
a real vector space
,H,} be a finite family of homogeneous
hyperplanes
of
V of finite dimension.
Call Vc the complexification
of V.
H. When the chambers (i.e., connected
Let X= K\IJHEX He: and Y= V\u,,,
components)
of Y are simplicial cones, Deligne ([7]) has proved that ni(X)=O
for i> 1, i.e., the space X is a K(rc, 1). A combinatorial
result that turns out to
be important
in this paper is that any two galleries (i.e., minimal paths) linking
chambers of Y with the same extremities can be obtained from each other using
a finite number of deformations
of a certain kind, called elementary deformations
(see zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
C71).
*Partially
supported
0012-365X/93/$06.00
by a grant
Q
from I.N.I.C.
1993-Elsevier
Science Publishers
B.V. All rights reserved
132
R. Cordovil, M.L. Moreira
zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
Our theorem
generalizes
for oriented
matroids
Deligne’s
ticular that his restriction-‘the
chambers of Y are simplicial
Note that the ‘realizable oriented matroid’ case was proved
Arrangement
of hyperplanes
occurs
in several
branches
result, showing
in par-
cones’-is
not essential.
by Salvetti [14].
of mathematics
(see
[13-151). We suppose that the basic notions and results from oriented matroid theory
are familiar to the reader (see [l, 9, ll]), and we recall here only those which are
directly related to this paper.
We begin by associating with the set Y of chambers an oriented matroid in the
following
way: We fix a point
a chamber
ldidn,
&E Y; to each CE Y, we assign a zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIH
signed vector QE { +, - }“, where, for any i,
(Vc)i=+Ox(C)
x(C) in the interior
and x(C,)
of each chamber
are in the same connected
component
C of Y and
of V\Hi.
The family of signed vectors w = { Vc: CEY} is the family of maximal elements of the
cocircuit span of the (realizable) oriented matroid Jz’ of the linear dependencies
on a set u2/ of vectors orthogonal
to the hyperplanes
of the arrangement
2,
,n,
such
that
uilHi
for
every
i=l,...,
n.
q={“i}i=l,.
The elements of w have been studied in oriented matroid theory under the name of
of oriented matroids using this
topes or non-Radon partitions ([2,8]). A xiomatizations
family are also well known ([4, 5, 10, 121).
In what follows, the elements of w= “K(A) will be called maximal covectors or,
shortly, covectors of the oriented matroid &‘. By rank ofW we will mean the rank of
the matroid JH and note by v the signed covector whose entries are symmetric to
those of VGT. It is known that -Ilr itself is symmetric, i.e., ?.V= “@ = { v: VFW ” }. We
will suppose w.1.o.g. that w has no parallel elements, i.e., for each i, 1 <i < n, there are
two covectors V and V’ in w, with I/‘ # v satisfying K=- Vi.
2. The results
Let ?V c { +, -}” be the family of maximal covectors of a simple (i.e., with no loops,
parallel or antiparallel
elements) oriented matroid on the set E.
Definition 2.1. A family G = ( V,, VI, . . . , V,,) of n + 1 covectors of -1y- is a gallery with
initial point VO,endpoint
V, and length n if:
(1) vi+ 1 differs from K in exactly one entry, for any i, 1 < i < n;
(2) V, differs from V, in exactly n entries.
Definition 2.2. Two galleries with the same extremities
G =( VO, VI, . . . , Vn) and
G’=( V0 = V,, Vi, . . , Vn= Vn) can be obtained from each other by an elementary
deformation if:
(1) There are two integers p and q, with O<p < q < n, such that vj= Vi, for any
j satisfying
O<j<p
or qdj<n;
A homotopy theorem on oriented matroids
133
(2) The two galleries G1 = ( zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
VP, VP+1, . . . , V,) and G I= ( Vb= VP, VP+ 1, . . . , Vb = V,)
are unique in w with these extremities.
Two galleries in -ly- are equivalent if they can be obtained
number of elementary deformations.
Remark 2.3. Note
that (1) for any two covectors
from each other by a finite
V and
v’ of @‘“, there is always
a gallery in YY linking them ([3, Lemma 3.71);
(2) given two covectors V and v’ of %‘“,there are exactly two galleries with them as
extremities if and only if, with A={eEE:
V,=- Vk} and B=(eEE:
a rank 2 face of the acyclic oriented matroid BJ&‘.
Theorem 2.4. Any two galleries
covectors
of an oriented
with the same extremities
A is
V,=-},
in the set $T of the maximal
matroid _4? are equivalent.
For the particular case rank(w)=
3, Theorem 2.4 is implicit in [3], Theorem 2.1.
Indeed, the following theorem, which is stronger than our theorem for rank 3, is also
implicit therein.
Theorem 2.5. Let TUTbe the family
with n points and 1 lines. Let
a gallery
linking
equivalent
of maximal
V be a covector
V to v. W ith G’ =( Vb = v,,
and can
be
obtained
from
each
covectors
of a rank 3 oriented
matroid
of PY and G=( V= V,, VI, . . . , V,= v)
V; = v,_ 1, . . . , V:, = &), G and G’ are
other
by
using
exactly
1 elementary
deformations.
Note
that,
under
the conditions
of Theorem
2.5, 1 is the minimal
number
of
elementary deformations
required to obtain one of the galleries from the other. This
result also suggests the following problem, for which a positive answer would allow us
to generalize Theorem 2.4 in the spirit of Theorem 2.5.
Problem 2.6. Let w = w(A)
be the family
of maximal
covectors
of an oriented
matroid
A&’ with rank, at least, three; let G be any gallery in YY linking two
opposite covectors V and l? Is there any subset PV’ of covectors of -1y- containing
the covectors of G and being the family of maximal covectors of a rank 3 oriented
matroid A’?
3. Proofs
Let A’(E) be a simple and acyclic oriented matroid and ~2 = {ACE:
a_&’ is
With each AE~, we associate a graph G(A) whose vertices (edges) are the
flats of & with rank 1 (rank 2) included in A and belonging to &‘.
acyclic}.
134
R. Cordooil. ML.
Moreira
Proposition 3.1. G(A) zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
is a connected graph.
We remark
extremal
that, when all the acyclic reorientations
points (the hypothesis
considered
of AZ”have exactly rank(A)
by Deligne
[7]), the connectivity
of G(A)
can be easily proved; indeed, in this case G(A) is a complete graph.
Note also that if A is a flat of &, since Ad,
A is a face of A’, i.e., A is a union of
positive cocircuits of A; thus, the graph G(A) is the l-skeleton of the face lattice of the
submatroid
A’(A). This lattice being a combinatorial
its l-skeleton is connected (see, e.g., [6]).
manifold,
Proof of Proposition 3.1. We will prove it by induction
it is well known
that
on )A I. When 1A 1Q 2, there is
nothing left to prove. Suppose now that the proposition
is true for any Aed with
1A I< n and let B be any element of d such that IBI = n + 1. We assume that B is not
a face of the matroid A! since otherwise, as we noted, the result follows.
Now take a vertex x of G(B) and let p be the Mobius function on d, thought of as
a partially ordered set by inclusion. It is known (see [S] and the extension to oriented
matroids
in [4, Corollary
2.101) that, for each XL&,
.
L- l)rank(X) zt,“,r;is;
P(8, x)=
face of A,
i
It follows from the definition
La
a=-
1
P(0,
of the Mobius
function
that
X)
XfB
and, in particular,
J, A02Xl=
c zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
A02X)=0.
XCB\(xJ
ac
XX
Using these equalities
and the result above, we have
xsFfB
F
zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA
is a face of .X
and, thus, as B is not a face of A!,
c
XEFFB
F is a face
148,F)=O
of
.X
Since ~(0, {x})=1, there must be a face F, of A strictly containing
{x> and being
strictly contained in B. Therefore, by the Jordan-Dedekind
property of the lattice of
faces of an oriented matroid (see [ 1 l]), we may say that there is a face F : of A! such
that
XEF;G
F,
and
rank(F:)=2.
135
A homotopy theorem on oriented matroids
This means that there is an edge of G(B) with x for vertex, i.e., G(B) has no isolated
vertices. In view of [3, Lemma 3.71, since BE&, we can choose XEG(B) such that
B\ (x}E&‘. By induction, G(B\ (x}) IS connected. Since all the edges of G( B\(x)) are
edges of G(B) and
connected.
0
G(B) has only one more,
nonisolated,
vertex,
it must
also be
Proof of Theorem 2.4. We proceed by induction
on the length of the galleries. Let
G and G’ be two different galleries with the same extremities V, and V2. Its length
must be at least equal to three. If it is equal to three, clearly G=( V,, A, V2) and
G’ = ( VI, B, V2) are unique with these extremities and they can be obtained from each
other by one elementary deformation.
Suppose now that the theorem is true when the length of the galleries is less or
equal to n- 1, and take any two different
galleries
G =( Ve, Vi, . . . , V,) and
G’=(&=V,,
I’;,...,
VI,= V,) with the same extremities
and length
n.
By taking, if necessary, a reorientation
of the matroid
&‘, we can suppose,
w.l.o.g., that all entries of the covector V, are positive. We call AE& the set of
negative entries of V, and a (b) the unique negative entry of Vi ( VI). By the
connectivity
graph.
of G(A), it is sufficient
to consider
the case where {a, b} is an edge of this
Let U be the covector of W whose negative entries are the elements of E belonging
to the 2-face {a, b} of JZ. According to Remark 2.3(2), there are exactly two galleries
Gi and G2 with extremities VOand U. Call Gr3 and Gz3 to the galleries linking V, with
V, and obtained by composing, respectively, Gi and G2 with some gallery G3 joining
U to V,. It is clear that Gr3 and Gz3 can be obtained from each other by one
elementary
deformation.
Noting that the galleries G and Gr3 have the two first
vertices in common, it follows from the induction hypothesis that they are equivalent;
the same argument
galleries.
0
yields for the galleries G’ and Gz3. Hence, G and G’ are equivalent
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