C AHIERS DE
TOPOLOGIE ET GÉOMÉTRIE DIFFÉRENTIELLE CATÉGORIQUES
L EONARDO C IRLINCIONE
On a family of varieties not satisfying Stoka’s measurability condition
Cahiers de topologie et géométrie différentielle catégoriques, tome 24, n
o2 (1983), p. 145-154
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
ON A FAMILY OF VARIETIES NOT SATISFYING STOKA’S MEASURABILITY CONDITION
by
L eonardo CIRLINCIONE CAHIERS DE TOPOLOGIEET
GÉOMÉTRIE DIFFÉRENTIELLE
Vol. XXIV - 2
(1983 )
R ESUME.
On donne unpremier exemple
de famille mesurable de varietes dont le groupe attache au groupe maximal d’invariance n’ est pas mesurable.On prouve,
ainsi,
que la condition suffisante demesurabilit6,
donnée parM. I. Stoka
[3],
n’est pas n6cessaire.Let ?
be afamily
ofvarieties, depending
on the(essential)
para-meters
a1, ca2,...,
aq, of anhomogeneous
n-dimensional spaceK
andlet
Gr
be an r-dimensional Lie group of transformations ofK .
Assumethat ?
is Gr -invariant
and no element ofGr (except
theidentity map)
fixes every
variety of 1q . In case Gr
is contained in no other group hav-
ing
the sameproperties, Gr
is called the maximalgroup of
invarianceof
1q
and itssubgroups
are thegroups o f
invarianceof Fq.
Let T f
GS ,
whereGs
is an s-dimensional group of invariance ofy .
If(ai)
and(Bi) ( i
=1, ... , q )
are the parameterscharacterizing
thevarieties 0
andT(0) of 5: q
the map(ai)->(Bi)
defines an s-dimen-sional Lie group
HS (of
th e parameter spaceh q of q ), isomorphic to
Gs ([4],
page33) (the
associatedgroup of GS
wi threspect to if q ). H s
can be either a measurable Lie group
([4 ,
page12)
or not. We say thatq
has the(elementary) measure 0 (a dai ,
with respect toG ,
if H s ismeasurable, admitting O
as measure.According
to M. I.Stoka, ?
ismeasurable
ifO
is also the measure for each measurable Lie group which is associated to the same group of invariance of1q .
M.I. Stoka proves
(see [3], [41
page40)
that if the group asso- ciated to the maximal group of invarianceof 1 q
is a measurable Lie group,then ?
is measurable. This condition is also necessaryif q =
1, 2, 3([4]
page41).
Nevertheless this is notgenerally
true ; in fact wegive
anexample
of a5-dimensional
measurablefamily j= 5
of varieties ofD3 (R)
such that the group associated to the maximal group of invariance of
j= 5
is not measurable.
The first section of this article is devoted to the determination of the
subgroups
ofG 7,
thesimilarity
transformation group ofD3 (R),
de-pending
on 5 or 6 parameters. This ishelpful
in order togive
the mention-ed
example.
1. THE SIMILARITY TRANSFORMATION GROUPS OF
D3 (R)
DEPEND-ING ON 5 OR 6 PARAMETERS.
Let
G n
be an n-dimensional Lie group ofD3 (R) generated by
theinfinitesimal transformations
Xi Xn .
The operatorsdefin e an m-dimensional
subgroup Gm
ofn
iffLet be two m-dimensional
subgroups
of isconjugate
to iff there existBy supposing
in(1) ats = 0,
one canchange
Y. into(ats)-1 Ys.
Thuswe may
assume as
= I . Thenchange
Yi( i s )
into7. - ati Ys ;
we seethat it is not restrictive to put axi t = 0 .
Let
G 7
be thesimilarity
transformation group ofD3 (R).
We canwrite the
equations
ofG7
in thefollowing
way (see[4]
page154)
h ,
I,
m , n ,tl , t2, t3 E, R, h=0
andh(1+l2+m2+n2)
is the homothetic ratio.( 1) We use the Einstein’s convention.
(2) More information c an be found
in [1].
G 7
is
generated by
the infinitesimal transformationsand its group structure is
given by
REMARK 1. We
pointed
out that in( 4 ) X, f
generates the dilatation group;X2 f >, X3 f>, X4 f >
are(resp. )
the three rotation groups on the axesx , y , z and
X 5 f , X6 f , X 7 f
generate the translation group.In order to determine the
subgroups
ofG7
of dimension5,
we con-sider the transformations
where is
given by (4).
Assumethen
a75 =
0.Thus,
we may putobtaining
Under the
hypothesis
we have
Likewise one can infer the
remaining
cases :In case A (as well as in the
remaining cases),
we canagain
put the sameassumption
on the coefficients ofY4 .
Thus one findsFrom
Aa
it followsNow
Aal splits again
in four cases. Consider the firstI n view of
( 5), ( 2 ) yields
whence
These
equations
arecompatible
ifTherefore . As it is not restrictive to set
a 1
=1,
we have the first5-dimensional subgroup
ofG 7
In the second case,
Aa 1 (II), we have
From it follows that
A
simple computation
leads toThus one finds the
family
of5-dimensional
groupsIn the case
Aa1 (III) we may assume a11 =
0 . For supposing a11=
0
and
a31=
0(then
it must benecessarily a41# 0 )
we obtain aspecial
caseof
Aa1 ( I ) (since it is not restrictive to put also a 4 - 0 ),
while if a31=
0
a
particular
case ofAa 1( II ) occurs. Therefore
Compute
as usual( Yi Y) ;
then( 2 )
and( 5 ) imply
Thus
Hence we have the
family
ofsubgroups
of GAal (IV) splits further in three cases: yet they
fall under those
above examined. The
study
of theremaining
cases is a routinecomputation.
One finds that the
early
groups fill up the class ofsubgroups
ofG 7
de-pending
on five parameters.THEOREM 10 Let
G5
be a5-dimensional subgroup of
thesimilarity
trans-formation group G 7 o f (t 3 (R).
Th enGS
isconjugate
inG7
toG3( 5
b ,c),
for
suitableb,
c E R.PROOF. The
change
of coordinatesT (x, y, z )= (z, x, y)
induces theoperator
permutation
Thus we note that
(G15) T = G25(0).
Likewise one checks thatG25(a)
isconjugate
toG35(a, 0).
We can make use of the same processes of Theorem 1 to
classify
the 6-dimensional
subgroups
ofG 7.
Thefollowing
theorem is the result weobtain :
THEOREM 2. There exists
exactly
one6.dimensional subgroup o f G 7
theorthogonal group
2. A 5-DIMENSIONAL MEASURABLE FAMILY OF VARIETIES OF
(f3(R)
Let 0
be thevariety
of8 (R)
where a
i R
andClearly (9)
is apair
oforthogonal
planes
ofD3(R).
Let ?
=O G7
be thefamily
of varieties obtainedfrom 0 through
the transformations of
G7.
The maximal group of invarianceof ? is,
ofcourse,
G7.
We proveTHEOREM 3. The
group
associated toG7,
withrespect
toF5,
is a non-measurable
group.
PROOF. Let T be the transformation
(3)
ofG7 .
The parameters(3
i ofthe
variety T(O)
define the associated groupH7 :
The coefficients of the infinitesimal transformations
generating H7
areH7
is a measurable group if thefollowing
system ofequations
admits
exactly
one non-trivial solution(up
to aconstant),
see Deltheil[2]
page 28.The last three
equations
of (11 )
areequivalent
toClearly
theequations (12)
and the firstequation
of(11)
form a system ofequations admitting
no solution. ThereforeH7
is not measurable.R EMARK 2. The first
equation
of (11 )
arises from the dilatation parameter, while theremaining equations correspond,
in order of sequence, to the ro-tation and translation parameters.
Let
Gn
be an n-dimensional group ofG7,
where n 5 and letHn
be the associated group with respect to9r .
If n 4 ,then H n
is in-transitive,
whence it is not measurable([4]
page15).
In case n =
5 ,
from Theorem 1 it follows thatGn
isconjugate
toG35 (b, c ) ,
for suitable parametersb,
c E R . In view of Remarks 1 and2,
we note that the Deltheil’s system of
H5
contains the first and the lastthree
equations
of (11 ).
But we havealready
seen in theproof
of Theorem3 that
they
admit no solutions. Therefore :PROPOSITION 1.
Y5
admits no measure withrespect
to anyn-group of
invariance, if
n 5 .We turn now to the
orthogonal
groupG6 . Let H6
denote the cor-responding
associated group. On theground
of Remark2,
we can obtainthe Deltheil’s system of
H6 by suppressing
in (11 )
the firstequation.
It is not difficult to check that this system has
only
one solution(up
to aconstant)
Hence we have
PROPOSITION 2. With
respect
to theorthogonal group Y5
admits the ele- mentary measureAs a consequence we have the main result
(see
also Theorems2,
3 andProposition 1) :
COROLL ARYo The
family of
varietiesF5
is measurable inspite of
thenon-measurability of
thegroup
associated to its maximalgroup of
in-variance.
REFERENCES.
1. BIANCHI L., Lezioni sulla teoria dei
gruppi
continuifiniti
ditransformazioni,
Zanichelli,Bologna
1928.2. DELTHEIL R., Sur la théorie des
probabilités géométriques,
Thèse, Ann. Fac.Sc. Univ. Toulouse (3) 11
(1919), 1- 65.
3. STOKA M.I., Geometria
integrale
in unospazio
EuclideoEn,
Boll. Un. Mat.Ital. 13- 4 ( 1958), 470- 485.
4. STOKA M. I., Geometria
integrale,
Ed. Acad. R. S. Romania, Bucarest 1967.Istituto di Matematica dell’Universita Via Archirafi 34
90123 P ALERMO. ITALIE