A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
J EAN J ACQUES M OREAU
Jump functions of a real interval to a Banach space
Annales de la faculté des sciences de Toulouse 5
esérie, tome S10 (1989), p. 77-91
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- 77 -
Jump functions of
areal interval
to aBanach
spaceJEAN
JACQUES MOREAU(1)
Annales Faculte des Sciences de Toulouse
Les fonctions a variation localement bornée dans un intervalle reel I, , a valeurs dans un espace de Banach X, forment 1’espace vectoriel Ibv(I,X), sur lequel une topologie est définie par la famille de semi-normes
f ~--~ var( f; a, b), a E I, b E I. Par definition, les fonction de saut sont les elements de Fadherence de 1’espace des fonctions localement en escalier.
On construit la decomposition de toute f E Ibv(I,
X)
en somme d’unefonction de saut et d’une fonction continue. Entre autres propriétés, on
etudie comment cette decomposition se réflète sur la fonction variation indefinie Vf de f. . Le lien avec la decomposition d’une mesure réelle sur
I en somme d’une mesure diffuse et d’une mesure atomique est explicite.
ABSTRACT.- On the space Ibv(I, X) of the functions of a real interval I to
a Banach space X, with locally bounded variation, a topology is defined by
the semi-norms f t2014~ var( f a, b), a E I, b E I. By definition jump functions
are the elements of the closure of the space of local step functions. The
decomposition of every f E Ibv(l, X) into the sum of a jump function and
a continuous element of lbv(I, X ) is constructed. Among other properties,
it is studied how this decomposition is reflected on the real function Yf, ,
the indefinite variation of f. The connection of what precedes with the decomposition of a real measure into the sum of a diffuse measure and an
atomic measure is investigated.
(1) Laboratoire de Mecanique generale des Milieux Continus U.S.T.L., 34060 Montpellier cedex, France.
1. Introduction
Real functions of a real variable with bounded variation are a standard to-
pic. Elementarily,
a functionbelongs
to this class if andonly
if itequals
thedifference of two
nondecreasing
real functions. In thatcontext,
the decom-position
of any element of the class into the sum of a continuouscomponent
and an element of thespecial
sort called ajump function
iseasily
derived.From the real valued case, the
concept
of bounded variation may be extended to functions with values in R~by referring
to theircomponents.
Actually,
manyproperties
discovered in that way arefound, through
theuse of different
techniques,
to hold also forfunctions,
with values in anarbitrary
Banach space X. This is thesetting
of thepresent
paper, devoted toextending
the abovedecomposition property
and todeveloping
some ofits
topological
features.The author’s
primary
motivation lies in NonsmoothDynamics,
i.e. thestudy
of MechanicalSystems
whose motion is notregular enough
foraccelerations to exist. The
velocity
isonly
assumed to be a vector functionof time with
locally
boundedvariation;
this allows for a vector measure, on the considered timeinterval,
toplay
the role of acceleration.Accordingly,
the
system dynamics
isgoverned by
a mesuredifferential equation
or, if such mechanical effect as unilateral contact,possibly
with Coulombfriction,
aretaken into account, a measure
differential
inclusion[6].
On this purpose, achapter
of a recent book[5]
has been devoted toexposing
some old and newproperties
of the(locally)
b.v. functions of a real interval to a Banach space X and of the associated vector measures. Thepresent
paper is intended tocomplement
this text.Let I denote a real
interval,
not empty nor reduced to asingleton. By f
EIbv(I,X)
it is meant thatf
is a function of I to X withlocally
boundedvariation,
i.e. it has bounded variation on every compact subinterval of I(in [2],
this is called a function withfinite variation).
Trivialinequalities concerning
variationsimply
thatl bv(I, X )
is a vector space andthat,
forevery compact subinterval
[a, b]
ofI,
themapping var( f;
a,b)
is asemi-norm on this space. If
[a, b]
rangesthrough
thetotality
of thecompact
subintervals of
I,
orequivalently through
someincreasing
sequence of such subintervals with unionequal
toI,
the collection of thecorresponding
semi-norms defines on
lbv(l’, X )
a(non Hausdorff) locally
convextopology
thatwe shall call the variation
topology.
The closure in this
topology equals
thesubspace
ofconstants ; by going
to thequotient,
one obtains a metrizablelocally
convex Hausdorffspace.
Equivalently,
we shall once for all choose in I areference point,
say p, and restrict ourselves to1 bvo (I, X), namely
thesubspace
oflbv(I, X) consisting
of functions which vanish atpoint
p. This linear space will be shown in Sec. 2 to becomplete
in the variationtopology.
Denoting
the Banach norm inX,
oneobviously has,
for everyf
Elbvo (I, X )
and every[a, b]
C Icontaining
p,Therefore,
in the space1 bvo (I, X ),
the variationtopology
isstronger
thanthe
topology
of the uniform convergence oncompact
subsets of I.One denotes
by bv(I, X )
thesubspace
ofIbv(I,X)
constitutedby
thefunctions whose total variation on I is finite. Its
subspace bvo (I, X ),
consis-ting
of the elements which vanish atpoint
p, is a Banach space in the normf H var ( f ; I )
.By writing s
EIst(I, X ),
we shall mean that s is a localstep function
inthe
following
sense : there exists alocally
finitepartition
of the interval I into subintervals of any sort(some
of thempossibly
reduced tosingletons),
on each member of which s
equals
a constant. Such functions make a linearsubspace
oflbv(I, X ), easily proved
to be dense relative to thetopology
of uniform convergence on the
compact
subsets ofI. But,
in the variationtopology,
the closure oflst(I, X )
is aproper subspace
oflbv(I, X ),
whoseelements, by definition,
are thejump functions.
. A series ofpropositions
established in Sec. 3 below
yield
theproof
of :THEOREM 1.2014
Every f
Elbv(I, X )
possesses aunique decomposition
into the sum
of
ajump function vanishing
atpoint
p, sayJo( f ),
and acontinuous element
of lbv(I, X ),
sayC( f ).
Themappings Jo
and Care linearprojectors of lbv(I, X )
intoitself,
continuous in the variationtopology.
On may call
Jo( f )
thejump
component off
inlbvo(I, X ). Changing
thereference
point p
results inadding
constants toJo ( f )
ande(f).
With every
f
Elbv(I, X ),
there is associated its variationfunction, vanishing
atpoint
p,namely
thenondecreasing
elementV f
ofIbvo(I, R)
defined as
We shall establish in Sec. 4 : _
THEOREM 2. The nonlinear
mapping f
HVf
is continuousof lbv(I, X )
tolbvo(I, R)
in therespective
variationtopologies of
these spaces.THEOREM 3.
If
the notations C andJo
are alsoapplied
to elementsof lbv(I, R)
one has =C(Vf)
and =.Io(Vf).
Theorems 1 and 3
clearly yield Vf
= + so, for every~a, b~
CI
,Actually,
thisequality
will in thesequel
be established asProposition 3.2, prior
toproving
Theorem 3.Theorem 3 also
implies
that an elementf of lbv(I, X ) is a jump function if
andonly if
the same is truefor Vf.
Infact,
ifVf
is ajump function, C(V f)
=equals
a constant(in
factzero),
soe(f)
is aconstant, making of f a jump
function.Conversely,
iff
is ajump function, e(f)
is aconstant,
soC(Vf) equals
zero,making
ofV~
ajump
function.Symmetrically, f
is continuous if andonly
if the same is true forVI;
;this is
elementarily
established in[5]
and will be used in thesequel prior
toproving
Theorem 3.The most common reason one has for
being
interested in lbv functions(letting
alone NonsmoothDynamics)
lies in the factthat,
with everyf
El bv(I, X ),
an X-valued measure on the interval I isassociated, usually
denoted
by df
orD f
, called thedifferential
measure(or
theStieltjes measure)
off
A connection isnaturally expected
between Theorem 1 anda
property which,
at least in the real-valued case, isclassical, namely
thedecomposition
of a measure into the sum of twocomponents,
on of whichis
diffuse
and the other atomic.Actually, properties
of both sorts cannot bestrictly equivalent,
since thecorrespondence
between X-valued measures and elements ofIbv(I,X)
is notone-to-one. In
fact,
if an lbv functionf
is discontinuous at somepoint
a,the measure
df
isexpected
to exhibit at thispoint
an atom with massequal
to the total
jump
off i.e.
the diference between theright-limit f +(a)
andthe left-limit
f -(a).
But the very value thatf
takes atpoint
a bears nonrelationship
withdf.
.The diferential measures of the elements of
l bv(I, X)
are characterizedby
thefollowing property, which,
for infinite-dimensionalX,
makes of thema
special
class of vector measures :they
have bounded variation(concerning
this
concept,
see e.g.[3])
on everycompact
subinterval of I. In[2],
suchvector measures are said to have
finite
variation; the corresponding concept
in Bourbaki’s construction of measure
theory ~1~
is that of amajorable
vector measure. This
property implies
the existence of thenonnegative
realmeasure the modulus measure of
df (also
called the variation measure or the absolute value ofdf ).
In Sec.5,
we shall prove :THEOREM 4. - An element
f of lbv(I, X )
is ajump functio n if
andonly if
thenonnegative
real measure|df|
is atomic.Equivalently,
thenonnegative
real measuredVf
is atomic.2. The variation
topology
At the first
stage,
let us consider functions whose total variation on I is finite.PROPOSITION 2.1. The vector space
bv0(I,X)
is a Banach space inthe norm : = var
( f, I).
Proo f
. Let( f n )
be aCauchy
sequence in this norm. There exists M > 0 such thatIn view of
inequality (1.1), ( f n )
is also aCauchy
sequence relative to the supremum norm(~ . ~~ ~,
so it converges in the latter norm to some functionf~ : I -~ X,
with = 0.For every finite ordered set of
points
ofI,
say S To Tl ... Tv , and everyf
: I --~X, let
usput
the notationSince,
at everypoint
T= ofS,
the element of Xequals
the limit ofin norm, one has
Due to
(2.1),
this ismajorized by
M whatever isS,
hencefoo
Ebvo(I, X ).
Finally,
let us prove thatf n
converges tofoo
in norm. Let6 >
0 ;
in view of the assumedCauchy property,
there exists n E N such thathence,
for everyp >
n,One
readily
checksthat,
for fixedS,
themapping f - V ( f S)
.is a semi-norm. Therefore
By letting
p tend to +00, one concludesV(/n
-S)
~ for every finite sequence5’,
hence var( f n
-foo, I)
~Let us now
drop
theassumption
of finite total variation on I. The variationtopology
onlbvo(I, X )
is definedby
the collection of semi-normsf H Nk(f) :
= var( f Kk ),
where(Kk)
denotes anondecreasing
sequence ofcompact
subintervals whose unionequals
I. Inaddition,
on may assume that all intervalsKk
arelarge enough
to contain g.Therefore,
theresulting topology
is metrizable and Hausdorff.PROPOSITION 2.2.2014 The variation
topology
makesof lbvo(I, X )
a com-plete
metrizablelocally
convex vector space(i.
e. a Fréchetspace).
Proof . - Let ( f n )
be aCauchy
sequence int bvo (I, X ) By definition,
forevery
U,
aneighborhood
of theorigin
in this space, there exists n E N such thatBy taking
as U the semi-ballwith k E N and e >
0,
thisyields
theimplication
Therefore the restrictions of the functions
( fn)
toKk
make aCauchy
sequence in
bvo(Kk,X),
In view ofProp. 2.1,
this sequence converges tosome element
f k
of the latter space. If the same construction is effected foranother interval with k’ >
k,
theresulting
functionfk’ : Kk~ -~ X is
an extension of
f k. Inductively,
a functionf
is constructed on the whole ofI,
which constitutes the limit of the sequence( f n )
in the variationtopology.
D
3. Construction of the
jump component
Without
assuming
that I iscompact,
let us first consider the case wheref
: I --~ X has finite total variation on the whole interval. Asbefore,
areference
point (}
is chosen in I. With everye E I,
let us associate thesingle-step function
se : I -~ X definedby
thefollowing
conditions.The
function
severifies
and admits e as its
unique possible discontinuity point,
with the samejumps
as
f
at thispoint,
i. e.Here,
thenotations +
and - refer to theright-limit
and theleft-limit
of theconsidered functions at the considered
point. By convention, f -(e)
=f (e) if
thepoint
eof
~happens
to be theleft
endof
this interval andf "~’(e)
=f (e) if it happens
to be theright
end.Clearly,
se Ebvo(I, X );
; itequals
the zero constant if andonly
iff
iscontinuous at
point
e.For every finite subset F of
I,
let us consider thestep
functionCall ~’ the
totality
of the finite subsets of I. The inclusionordering
makesof 7 a directed set
[4]
and onereadily
checks that themapping
of
(~’, ~)
to R isnondecreasing
and boundedby
var( f, I).
Hence thismapping
is aconvergent
net of real numbers.Let us show that the net F - sF is
Cauchy
in the Banach norm ofbvo (I, X ).
Let 6 >0;
due to the convergence of the net(3.4)
inR,
thereexists F such
that,
for every F’containing F,
one hasthis is the sum of two
step
functions withdisjoint dicontinuity sets,
thereforewhich,
in view of(3.5)
and(3.6), yields
By
thetriangle inequality,
there comes outthat,
for every F’ and F" in7,
both
containing F,
one hasthis is the
Cauchy property
for the net F - sF in the Banach spacebvo(I,X).
It secures the existence in this space of the elementIf,
moregenerally
thanabove,
thegiven
functionf belongs
tolbv(I, X ),
one may cover I with a
nondecreasing
sequence ofcompact
subintervalsKk,
all
containing
~o. Thepreceding
construction will beapplied
to the restriction off
toKk, yielding
as the limit in(3.8)
somefunction j f
Ebvo(Kk, X ).
Observe that the
single-step
function se vanishesthroughout Kk
if the element e of I is not adiscontinuity point
of the restriction off
toKk.
.When Kk is
replaced by
alarger
subintervalKk
ofI,
the step functions F
previously
considered isreplaced by
some extension of it to For Franging
in~’,
the limit found in is an extension of the functionprecedingly
obtained.By
this process, anelement j f
oflbvo(I, X )
isinductively defined, equal
to the limit of the net F H sF in this Frechet space.
DEFINITION 3.1. For every
f
EIbv(1,X) (resp. f
Ethe
function jf
constructed above is called thejump component of f
inX ) (resp
. in000(1, X )~.
Clearly,
when the referencepoint
o ischanged,
thefunction j
f is alteredby
the addition of a constant. .PROPOSITION 3.2. - The
function
ci =f - j f
is continuous.For every
[a, b~
CI,
one hasProof. - It
isenough
to consider the casef
Ebv ( I , X )
. Lett E I
; thepart
of Fconsisting
of the finite subsets of I which include t is cofinal in(~’, C).
Therefore in(3.8),
one mayindifferently impose
on F the condition ofincluding
t. Under thiscondition,
the functionf -
sF is continuousat t,
since
by
constructionf - st
is so, as well as all the functions se fore ~
t.Now, continuity
atpoint t
ispreserved
whentaking
the limit(3.8),
becausethe on
bvo majorizes
the norm of uniform convergence. This proves the first assertion.In order to establish
(3.9),
we shall first showthat,
for every g Ebv(I, X)
and every
single-step function se
such that g - se is continuous at e, onehas
In
fact, supposing
e E[a, b] (otherwise
theequalities
that follow aretrivial)
one
has,
in view of[5], Prop. 4.3,
Now,
since seequals
a constant in[a, t],
the twofunctions g
and g - se have the same variation on thisinterval,
whileThis proves that
(3.10)
holds when[a, b]
isreplaced by [a, e] ;
similarreasoning applies
to~e, b~
and(3.10)
followsby
addition.Applying (3.10) inductively,
one seesthat,
for every finite subset F ofI,
Due to the definition
of j f
in(3.8)
and to thecontinuity
of themapping
g - var
(g; a, b)
in the variationtopology,
thisyields equality (3.9). 0
PROPOSITION 3.3.2014 The
mapping Jo
:f
~--~j f of Ibv(I,X)
tolbvo(I,X) is linear, idempotent
and continuous in the variationtopology.
Proof
. It isenough
to consider the bv case. From(3.1), (3.2)
and(3.3)
it follows that the
mapping f ~
se is linear.By addition,
the same is truefor
f H
s F .Linearity
ispreserved
under the process ofgoing to the limit,
used in order to
construct j
f.Equality (3.9) implies I ) var( f, I), securing
thecontinuity
ofJo.
ThatJo
isidempotent
results fromProp. 3.2 ;
infact,
whenapplied
to acontinuous function such as c f, the process
generating
thejump component clearly yields
the zero constant. DPROPOSITION 3.4. - The range
of Jo
is a closedsubspace of lbv(I, X )
in the variation
topology.
Itequals
the closureof
the setof
thestep functions vanishing
atpoint
~O.The
mapping id - Jo f
-C f is
a linearprojector,
continuous in thesame
topology.
Its rangeequals
thetotality of
the elementsof lbv(I, X )
whichare continuous
throughout
I.Proof.
-Every
element g of the range ofJo equals
the limit of a net(equivalently
a sequence, since we areworking
in metrizablespaces)
ofstep
functionsvanishing
at g. Infact,
asJo
isidempotent, g equals
thecorresponding jg , which, by construction, equals
such a limit.That every continuous element of
t bv( I, X ) belongs
to therange
ofid -
Jo
follows from the construction of thejump component :
in fact thisconstruction
yields
the zero constant whenperformed
upon a continuous function. D4. Variation functions
Theorem
2,
which states thecontinuity
of themapping f ~--~ V f
in therespective
variationtopologies
ofl bvo (I, X )
andl bvo (I, R)
is a consequence of thefollowing. Incidentally,
thevanishing
of the considered functions atpoint {]
is not needed here.PROPOSITION 4.1. Let
f
and gbelong
tolbv(I, X),
with v and w asrespective
variationfunctions. Then, for
every~a, b~
CI,
one hasProof.
- Let E >0 ;
there exists a finite sequence ofpoints
of~a, b~,
say To Tl ... Tn, such thatFor every i E
(1, 2,..., n~,
there exist a~ and~3=
in[0, ~/2n~
and a sequencewhere the
integer
pdepends
oni,
such thatThen
Now
Therefore,
theexpression
in(4.2)
ismajorized by
Finally,
sinceê/2n,
As e is
arbitrary,
this establishes theexpected inequality.
0To prove Theorem
3,
there now remains toinvestigate
how hedecompo-
sition
f = j f ~-
c f is reflected on adecomposition
of the variation functionVf :
: I - R(vanishing
atpoint ).
Denoteby Vj
andVc
therespective
variation functions
(vanishing
atpoint
and c f Fromequality (3.9)
it follows that
An element of
lbv(I, X )
is continuous if andonly
if its variation function is continuous[5] ;
thusVc
is continuous.Furthermore, Vy
is a realjump
function. In
fact, j f equals
thelimit,
in the variationtopology,
of a sequenceof X - valued
step
functions. Thecorresponding
variation functions are realstep
functionswhich,
due toProposition 4.1,
converge toVy
in the variationtopology. Using Proposition
3.3 with X =R,
one concludes thatVc
andVj respectively equal
the continuouscomponent
and thejump component
ofVf
.,
5. Differential measures
As recalled in the
Introduction,
with everyf
Elbv(I, X )
there isassociated its differential measure
df,
an X-valued measure on the interval I.Characteristically,
for everycompact
subinterval[a, b]
ofI,
one hasHere
again,
it isagreed that,
if thepoint
b of Ihappens
to be theright
end ofthis
interval,
thenby
conventionf +(b)
=f (b); symmetrically, f -(a)
=f (a)
if a is the left end of I.
In
particular, by taking
as[a, b]
asingleton ~a},
there comes out thatOne thus observes
that,
whenf
is discontinuous atpoint
a, the proper valuef (a)
of the function bears norelationship
with the measuredf.
.Consequently,
even if one agrees to treat asequivalent
two functions whichdiffer
only by
a constant, thecorrespondence
betweenf
anddf
cannot beone-to-one.
As standard sources
concerning
thetheory
of measures with values in aBanach
space, one may referto 1 J , [2], [3].
The measuredf
introduced aboveI~s
thespecial property
ofbeing majorable
in the sense of~1J,
i.e. in theterminology
of[2]
and[3],
this vector measure hasfinite
variation on everycompact
subinterval of I. Thisimplies
the existence of thenonnegative
realmeasure on I called in
[3]
the variation measure ofdf
or, in[2]
and[5],
themodulus measure of
df.
We shall denote itby
It isnaturally
involved insome
inequalities,
with the consequencethat,
in the sense of theordering
ofreal measures, the differential measure of the variation function
V f
satisfiesIt is established in
[5] that,
whenf
hasaligned jumps,
i.e. for every a E I the valuef(a) belongs
to the linesegment
of X withendpoints f -(a)
andf+(a),
then|df|
=dVf (conversely,
thisequality implies jump alignment, provided
theBanach
space X isstrictly
convez, i.e thetriangle inequality
in this space holds as
equality
for flattriangles only).
The
following
is classical in the context ofnonnegative
real measureson
arbitrary
spaces : such a measure is saiddiffuse
if ityields
zero asthe measure of every
singleton.
Incontrast,
thenonnegative
measure issaid atomic if it
equals
the supremum of a collection ofnonnegative point
measures. It is found that a
nonnegative
measurebelongs
to one of thesetwo classes if and
only
if it issingular relatively
to every element of the other.Furthermore,
everynonnegative
real measure letaitself
beuniquely
decomposed
into the sumof
adiffuse
measure andof
an atomic measure.Since
f
can differ fromf - only
at itsdiscontinuity points,
which form acountable subset of
I,
oneeasily
obtains : :LEMMA 5.1.2014 For every
f
EIbv(I,X)
thedifference f
-f - (resp.
thedifference f
-f+)
is ajump function.
This lemma allows one to restrict the
proof
of Theorem 4 to the casewhere
f = f -,
sof trivially
hasaligned jumps,
a circumstance which makesIdfl = dVf.
As observed inIntroduction,
Theorem 3implies
thatf
is ajump
function if and
only
if the same is true forVI;
so we are reduced to thestudy
of the
latter,
anondecreasing
real functionwhich,
in the present case, is left- continuous[5].
Inparticular,
when the interval I is bounded from theright
and contains its
right end,
say r, theleft-continuity
ofV f
secures thatdV f
has no atom at this
point.
Recall in addition thatV~
has been assumed to vanish atpoint
e.Therefore, Vi
may be recovered fromdV’f trough
thefollowing
process, aspecial
case of a constructioninvestigated
in detail in[2]
or[5].
Let us denote
by
M the linear spaceconsisting
of the real measures onI with no atom at the
possible right
end of this interval. Let us call L the linearoperation associating
with every element ofM ,
saydw,
the functionw : I --~ R defined as
One may check
(see
e.g.[2]
or[5] ;
a similar situation is alsoclassically
met in
Probability)
that L is a linearbijection
of M to thesubspace
W ofIbvo(I, R) consisting
of the left-continuous elements.Trivially
w hasaligned jumps,
so|dw| = dVw and,
for everycompact
subinterval[a, b]
ofI,
This
readily yields that,
when W is endowed with the variationtopology
oflbv(I, R)
and M with thestrong topology
of the space of real measures, L is bicontinuous.By using
thesetopologies,
sinceVw
=L(dVw),
onecompletes
theproof
of Theorem 4
through
thefollowing
remarks :1° An element of W is a
jump
function if andonly
if itequals
the sumof a series of
single-step
functions.2° An element w of W is a
single-step
function if andonly
if dw is apoint
measure.3° An element of M is an atomic measure if and
only
if itequals
thesum of a series of
point
measures.- 91 -
Bibliographie
[1]
BOURBAKI (N.).- Intégration, Hermann(Paris),
Chap. 1, 2, 3, 4(2d
ed.), 1965, Chap. 5, 1956; Chap. 6, 1956; Chap. 7,8, 1963.[2]
DINCULEANU (N.).2014 Vector Measures, Pergamon (London, New-York), 1967.[3]
DUNFORD (N.), SCHWARTZ (J.T.).- Linear Operators, Part I : General Theory,Interscience (New York), 1957.
[4]
KELLEY (J.L.).- General topology, Van Nostrand Reinhold (New York), 1955 . [5] MOREAU (J.J.).- Bounded variation in time, in : Topics in Nonsmooth Mecha-nics, (Ed. J.J. Moreau, P.D. Panagiotopoulos and G. Strang), Birkhäuser (Basel, Boston, Berlin), 1988, p. 1-74.
[6]
MOREAU (J.J.).2014 Unilateral contact and dry friction in finite freedom dynamics,in : Non-smooth Mechanics and Applications, (Ed. J.J. Moreau and P.D. Pa-
nagiotopoulos), CISM Courses and Lectures n°302, Springer-Verlag (Wien, New York), 1988, p. 1-82.