C AHIERS DE
TOPOLOGIE ET GÉOMÉTRIE DIFFÉRENTIELLE CATÉGORIQUES
P ETER I. B OOTH
Fibrations and classifying spaces : overview and the classical examples
Cahiers de topologie et géométrie différentielle catégoriques, tome 41, no3 (2000), p. 162-206
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© Andrée C. Ehresmann et les auteurs, 2000, tous droits réservés.
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
FIBRATIONS AND CLASSIFYING SPACES :
OVERVIEW AND THE CLASSICAL EXAMPLES
by
Peter I. BOOTHCAHIERS DE TOPOLOGIE ET
GEOMETRIE DIFFERENTIELLE CATEGORIQUES
.Volume XLI-3 (2000)
RESUME. Soit G un groupe
topologique.
Laconstruction
et lespropri6t6s
de1’espace
fibreprincipal
de Milnor rattaché a G sont re- connues comme étant le modèleprincipal
dans led6veloppement
des theories des fibrations et de leurs classifications.
Dans cet
article,
l’auteurd6veloppe
une telle th6orie pour des fibra- tions structur6esgenerales.
Des casparticuliers
incluent les r6sultatsanalogues
pour les fibrationsprincipales,
celles de Hurewicz et les fibrations avec sections.Certains articles ant6rieurs sur ce
sujet
ont obtenu des r6sultats aussi satisfaisants que la construction de Milnor en termes desimplicite
etde
generalite.
D’autres ont fait de même en termes degeneralite
etde
potentiel
pour lesapplications;
d’autres encore l’ont fait en termesde
simplicite
et depotentiel
pour lesapplications.
Les r6sultatspr6-
sent6s ici pour les fibrations structur6es et pour le niveau de fibra- tion considere sont les
premiers
a r6ussir dans ces trois sens a la fois.1 Introduction
Let G be a
topological
group. Milnor constructed a universalprincipal
G-bundle
[Mi]
and Dold showed that its base space acts as aclassifying
space for
principal
G-bundles[D1,
thms.7.5 and8.1].
These results haveprovided
a model for thedevelopment
ofanalogous
theories of fibrations and their associatedclassifying
spaces.This
theory
issimple
in the senses that it utilizes a standard defi- nition ofprincipal
G-bundle and classifies such bundles up to the most naturalequivalence
relation between such bundles. Thetheory
is gen-eral,
in that it is valid forarbitrary topological
groups G.Classifying
spaces are
produced by
arelatively simple procedure,
i.e. asquotients
ofjoins
ofcopies
of G. The details of this construction aredirectly
usefulin
applications
of thiswork,
i.e.they
enhance theapplicabzlity
of thewhole
theory.
The
analogous problems
ofclassifying
the threetypes
of classicalfibrations,
i.e.principal,
Hurewzcz and sectionedfibrations,
have beenconsidered
by
numerous authors.Principal
and sectioned fibrations have been defined in different ways in differentpublications.
Each type of classical fibration has been classifiedby
means of more than oneequivalence
relation. In some cases thedistinguished
fibre isarbitrary,
in others it is
required
tosatisfy
atopological
condition. Some of theclassifying
spaces areproduced by geometric
bar construction or GBCprocedures,
othersby
methods that may be lesshelpful
whenapplica-
tions are involved.
Also,
when the BrownRepresentability
Theorem orBRT is
used,
theproof
oftenincorporates
a set theoreticaldifficulty.
Wewzll show that none
of
these results have all threeof
the above desirablefeatures of
the Milnor-Doldtheory.
We now consider theories that describe structured
,fibrations
in gen- eral. It isobviously important
for them toincorporate satisfactory
versions of the classical theories as
particular
cases. Toclarify this,
weneed a few ideas
concerning categories
of enriched spaces. Moreprecise explanations
of the concepts involved will begiven
in section 2.Let .6 denote a
category
of enrichedtopological
spaces and F be agiven e-space.
we define the associatedcategory of fibres
T as con-sisting
of allE-spaces
that are of the samee-homotopy
type as F and allE-homotopy equivalences
between suchE-spaces.
Thene- fcbratzons
are fibrations whose fibres are
prescribed
to lie in E. Different choices of E lead into discussions of different types of fibrations. Thustaking
E to be a suitable
category
ofG-spaces
andG-maps,
thecategory
ofspaces and maps and the
category
ofpointed
spaces andpointed
maps,we obtain theories of
principal G-fibrations,
Hurewicz fibrations and sectionedfibrations, respectively.
Thus,
for a result at the structured fibrationlevel,
there is an im-portant unity
condition. Ingeneral
terms, theclassifying
result forstructured fibrations should do a very
good job
ofunifying
theclassify- ing
results for the classical fibrations.We do not claim that an
optimal theory
of fibrations would match that of Milnor-Dold in allrespects.
Thus[D1, thm.8-11
showed that the total space of Milnor’s universalprincipal
G-bundle is contractible.However,
a result of thistype
forprincipal
G-fibrations - such as[F, thm.p.334] -
has bothadvantages
anddisadvantages.
Let G be atopo- logical
monoid and pG :XG - BG
be aprincipal G-fibration,
withXG
contractible. It
follows,
via[Va, thm.1.3].
and[BHMP, lem.3.2],
that thecoboundary
mapQBG ->G is a homotopy equivalence
and anH-map.
So G has a
homotopy
inverse. Weprefer
to avoid thisapproach since,
as we
explain
in the discussion beforeproposition 5.10,
the condition onG may fail to hold in some relevant
examples.
A space X will be said to be
weakly
contractible if it ispath
connectedand all of its
homotopy
groups are zero. To avoid the aforementioned limitation onG,
weprefer
to use weakcontractibility
inplace
of con-tractibility.
Weexpect
that atheory
ofprincipal fibrations,
or atheory
of structured fibrations that includes
principal fibrations,
shouldsatisy
a weak
contractibility condition,
i.e. that the total spaces of universalprincipal
fibrations should be at leastweakly
contractible.There are three classification results for structured fibrations in gen-
eral,
i.e. a result from[B3] (=
theorem 2.3 of thispaper)
and twoGBC
style
results’of[M1].
Thus theorem9.2(i)
of that paper - parts(a) (i)
and(b) (i)
to beprecise -
classifies such fibrations up to a form of fibrewise weakhomotopy equivalence.
Theorem9.2(ii) - actually (a)(ii)
and
(b) (ii) -
classifies such fibrations up to a form of fibrewisehomotopy
equivalence.
We will show that noneof
these accounts have allof
thepreviously
listed desirablefeatures.
One of the main aims of this series of papers, i.e.
[Bl], [B2], [B3], [B4]
and this paper, can be summarized as follows.Objective
A We wish todevelop
atheory of
structuredfibrations
andtheir
classifying
spaces that will meet the seven criteria that we list in section 3. These include theaforementioned simplicity, generality,
en-hanced
applicability, unity
and weakcontractibility
conditions.Results Obtained This
objective
is achievedby further developing
thetheory of
our theorem 2.3. Theclassifying
spaces anduniversal
struc-tured
fibrations of
theorem4.7
will be shown tosatisfy
allof
our criteria.A
general theory
of fibrations andclassifying
spaces should do muchmore that
upgrade existing theories;
it should facilitate thedevelopment
of new theories. This leads to a second
major goal
of this work.Objective
B Ourtheory
shouldprovide
themachinery for manufactur- ing classifying
spacesfor
agreat variety of types of
structuredfibrations. : Further,
the conditions that have to beverified,
i. e. to show that it isapplicable
tospecific types of
structuredfibration,
should beuncompli-
cated and
easily managed.
Results Obtained This
objective
is metby
our theorems4.7
and 6.6.We have
already explained
that suitable choices of E allow us to derive theories ofclassifying
spaces for the classical theories of fibrations:There are many other
examples
ofcategories 9
for which the associated f-fibrations havegood
theories ofclassifying
spaces. Theseexamples
include the cases where E is
(i)
thecategory
ofpairs
of spaces and maps ofpairs [Sp, p.22-23], (ii)
thecategory
of spaces under a fixed space and maps under that space,(iii)
the fibrewisecategory,
i.e. thecategory
of spaces over a fixed space and maps over that space, and
(iv)
thecategory
whoseobjects
are Dold fibrations that are also identifications and whosemorphisms
arepairwise
maps between such fibrations.These lead us into classification theories for
(i) pairs
offibrations,
(ii)
fibrations that extend trivialfibrations, (iii)
fibrations overprod-
uct spaces and
(iv) composites
of Doldfibrations, respectively.
Theseextensive and
interesting
theories arebeyond
the scope of this paper.However,
somepreliminary
ideas on thesetopics
aregiven
in section 8of [B1].
The
techniques
of this present group of papers makeheavy
use ofconcepts
from[Ml],
eventhough
our methods ofproof
arequite
dif-ferent from those used there. Thus our terms
categories
of fibresf,
f-fibrations and f-fibre
homotopy equivalence
derive from -although they
do not coincide with - thecorresponding concepts
of that memoir.The use of the GBC construction of
classifying
spaces,however,
trans-fers
directly
to this paper. Thefollowing
account of the use of thatprocedure
to define universal0-quasifibrations
is a condensed versionof material in section 3 of
[B4].
This in turn derives from section 7 and remark 9.3 of[M1].
Let G be a
topological
monoid with astrongly non-degenerate
basepoint;
If X is aright G-space
and Y is a leftG-space,
then there is anassociated
GBC-space B(X, G, Y).
This construction is functorial so,given
a leftG-space F
and the mapF-*,
there is an associated map p*,F :B(*, G, F) -4 B(*, G, *).
If G isgrouplike.,
i.e. such thatII0(G)
with the induced
operation
is a group, then p*,F is aquasifibration.
If X is a
pointed
space, then X’ will denote X with a unit interval"whisker" grown at its
distinguished point.
The basepoint
ofX’,
i.e.the
point
at the end of thatwhisker,
isstrongly non-degenerate.
LetG be a
grouplike topological monoid,
with theidentity
asdistinguished point.
Then G’ is agrouplike topological monoid,
with theoperation
that extends theoperation
on G andmultiplication
on the unit intervalI ,
as well assatisfying tg = gt =
g, where t c Iand g
E G.There is a canonical action of
0(F)’
onF,
withf(F) acting by
evaluation and the whisker
acting trivially.
This action determines aGBC-space B(*,f(F)’, F).
The map F ->* then induces aquasifibra-
tion
P*,F: B(*,f(F)’, F)’,F)->B(*,f(F)’,*),
withf-space
fibres. Fur-ther,
thisf-quasifibration
isuniversal,
in the sense thatlB1ay’s
universalf-fibrations
correspond
to and derive from suchquasifibrations.
A
key
difference between theapproaches
ofMay
and the present au- thor can now be clarified. Thus[Ml, thm.9.2]
usesT- completeness
and ir’-completeness assumptions
to transform universal0-quasifibrations
p*,F into universal f-fibrations
T(p*,F)
orF’(p*,F),
over thecorrespond- ing classifying
spacesB(*,f(F)’, *).
We construct universal fibratio’nsby
the BRTapproach [B2, thm.8.1].
We prove that these f-fibrationsare
equivalent
to universalF- qu asifibrat ions by
means of a fibred map-ping
spaceargument (see [B4, thm.4.2]).
Hence we are able toeq.uate
our BRT
classifying
spaces to thecorresponding
spacesB(*, 7(F)’, *).
This
procedure
is akey step
in ourargument.
It enables us to blend the two theoriestogether.
Thus we are able tomanufacture
atheory
withthe
advantages of
bothapproaches
and thedisadvantages of
neither.We discuss
terminology
and notation in section 2. Thestrengths
and weaknesses of the
existing general
theories of structured fibrationsare reviewed in section 3. This leads to our list of seven criteria - includ-
ing
the five discussedpreviously -
that describe what weregard
as thedesirable characteristics of a classification theorem for structured fibra- tions. In section 4 we establish such a result for classes of f-fibrations
(theorem 4.7);
this result is later shown to meet all of our criteria. This theorem isapplied
toprincipal,
Hurewicz and sectioned fibrations in sections5,
7 and8, respectively.
Areview
of what was knownprevi- ously
is included in each of these three last mentioned sections. We note that our results are, in each case,improvements
on those results.Section 6 looks at relations between structured fibrations and their as-
sociated
principal
fibrations.The author thanks the referee for
making
numeroushelpful
com-ments on
papers
in this series.2 Terminology and Notation
Our
terminology
and notation grows outof,
and in most cases coincideswith,
thatdeveloped
in[Bl], [B2], [B3], and [B4].
We will work in the context of the
category
T of weakHausdorff compactly generated
spaces and maps between such spaces[Bl, p128-
129].
Thesymbol
W will be used to denote the class of such spaces thathave the
homotopy types
ofCW-complexes.
Let A be a
given
space. Then a space(X, i)
under A consists of aspace X and a
homeomorphism
i from A onto a closedsubspace
of X.Maps
under A are defined in the usual and obvious fashion. We will useA
to denote thecategory of
spaces under A and maps under A.We recall the
concept
of acategory of
enriched spaces(9, U),
whereE is a
category
and U : £ -3T
is a faithful functor. Theunderlying
spacefunctor
U is such that if Y is an9-object,
S is a space andf :
S - UYis a
homeomorphism
onto the spaceUY,
then there exists aunique
e-object
X and aunique 6-isomorphism
g : X - Y such that UX = S andUg
=f (see [B2, p.86]).
Theobjects
andmorphisms
of such £ will henceforth be calledE-spaces
andE-maps, respectively.
Inpractise
wewill
frequently simplify
ourterminology by omitting
reference to U.Thus we may state that E is a
category
of enriched spaces when wereally
mean that(E, U)
is acategory
of enriched spaces.If X and Y are
E-spaces
and there is ane-map
i : X - Y such that Ui : UX - UY is ahomeomorphism into,
then the6-space
X will besaid an
e-subspace
of theE-space
Y.A
category of
well-enriched spaces under A[B2, def.2.3]
is atriple (6, UA, IX xE I}).
In thissituation, 9
is acategory
andUA:.E -4 A
is an
underlying
space under Afunctor. Further,
for each£ -space X ,
there is an associatedE-space
Xxg I,
i.e. the£-cylinder
of X. These data arerequired
tosatisfy
conditions that E andUA
are well behaved withregard
toC-subspaces, E-cylinders, and £-mapping cylinders.
It is known that every
category
of well-enriched spaces also carries the structure of acategory
of enriched spaces[B2, lem.2.4].
We now review a number of definitions that
apply
in the context ofa
category
of enriched spaces, and therefore also in acategory
of well enriched spaces.An
E-overspace
is a map q : Y - Ctogether with,
for each c E C,an associated structure of an
e-space
on thefibre Ylc = q-1(c).
If VT isa
subspace
ofC,
thenY I V
=q-1(V).
The restrictionqlV : Y lV ->
V isclearly
also an£-overspace.
Given an
E-overspace q :
Y-+C and a mapf : B->C,
we can formthe associated
pullback
space YnB.Then q f
will denote theprojection
and induced
9-overspace
Y n B -> B. Theprojection
Y n B -> Y will be denotedby fq.
Let p: X -> B
B and q: Y -+ C be67overspaces.
AnE-pairwise
mapf , g
> from pto q
consists of mapsf :
X -> Y and g: B - C. These mustsatisfy
the conditions thatq f
= gp andthat,
for eachb E B,
f I(Xlb): Xlb
->Ylg(b)
isan,6-map.
An
9-pairwise
map with domain thee-overspace
p x1I
will be calledan
e-pairwise homotopy.
Taking
B = C andfixing g
to belc,
the9-pairwise
mapconcept
reduces toe-map
over C ore-fibrewise
map.Taking
B to be C x Iand
fixing g
to be theprojection
C x I ->C,
there is an obviousassociated
concept of E-homotopy overC,
and henceof.6-fibre homotopy Equivalence
or £FHE over C.We recall the
concepts
of£-covering homotopy property
or eCHP and E-weakcovering homotopy property
or SWCHP. Theseideas,
theE-versions of the CHP and WCHP of
[Dl],
are described in sections 3 and 4 of[B1], respectively.
AnE-fibration
is an£-overspace
that satisfies the EWCHP. We recall that if q : Y->C is an9-overspace
and C EW, then q
is an E-fibration if andonly if q
isE-locally homotopy
trivial orELHT
(see [B1, p.142
andthem.6.3],
and also[Bl, p.141]
fornumerably contractible).
Given an
object
F inS,
then there is an associatedcategory of fibres
f in
E, consisting
of allE-spaces
that areE-homotopy equivalent
toF and all
E-homotopy equivalences
between such spaces. The monoidof self -f-homotopy equivalences of F,
undercomposition,
will be de- notedby f(F).
It carries thecg-ified compact-open topology,
i.e. thecompact-open topology
modified in standard fashion to make it com-pactly generated [B1, p.129].
Let
q: Y -> C
is anf-overspace.
We definePrinF(Y)
to be thespace
with underlying
setU CECf(F, Ylc)
and thecg-ified
compact-open
topology.
There is aprincipal
overspaceprinf (q) : PrinF(Y) -> C,
defined
by prz*nf (q) (f )
= c, wheref
Ef(F, Ylc) [B4, p. 276].
If we take £ = T and U to be the
identity
functor onT,
then wehave a
category
of enriched spaces(T, U)
andT-fibrations
are Doldfibrations,
i.e. fibrationssatisfying
the WCHP of[D1]. However,
we arealso interested in
classifying
Hurewiczfibrations,
a proper subclass of the class of Dold fibrations. In a similar way ourpreferred
definition ofprincipal
fibration involves aglobal
action on the total space and ourpreferred
definition of well sectioned fibration involves the sectionbeing
a cofibration.
So,
in each of the classical cases, we have to deal with asubclass of the class of all
E-fibrations,
for a suitable choice of E. Hencewe will
develop
atheory
thatclassifies
such subclassesof E -fibrations.
Let .6 be a
category
of enriched spaces andSE fibn
be aparticular
class of E-fibrations. The members of
SE fibn
will be calledSE-fibrations.
The class of all 9-fibrations will be denoted
by Efibn.
Definition 2.1
Sgfibn
will be said to be a closed classof E-fibrations if, whenever q: Y -> C
is aSE -fibration
andf : B -> C
is a map, the inducedE-fibration q f : Y n B -> B is
also anS£-fibration.
Let F be a
given E-space,
f be thecategory
of fibres determinedby F
andS£ fibn
be a closed class of E-fibrations. We defineSf fibn
tobe the intersection of
SE fibn
with the class of all f-fibrations. Hencean
Sf-fibration
is an S£-fibration that is also an f-fibration.Clearly Sf fibn
inherits the closed classproperty
fromSgfibn.
Given a space
B,
thenSTFHE(B)
will denote the set -assuming
that it is a set - of all FFHE-classes of Sf-fibrations over B.
If,
for everyB E W, STFHE(B)
is a set, thenSFfibn
will be said to be STFHE set-valued. Inparticular, fFHE(B)
will denote the set -again
if it isa set - of fFHE-classes of f-fibrations over B.
If,
for every B CW,
F F H E(B)
is a set, thenFfibn
will be said to be fFHE set-valued.If B C W and
0fibn
is TFHEset-valued, then fFHE(B)
is a set andits subclass
SJ’FHE(B)
is a set.Hence,
iff fibn
is fFHEset-valued,
then
Sffibn
will be SF F H E set-valued. In that case,SfFFHE(-)
is acontravariant functor from the
homotopy category
of spaces in W to thecategory
of sets and functions(see
theparagraph
before[B2, defs.2.2]).
We are now
ready
to commence a discussion ofuniversality amongst
Sf-fibrations.Definition 2.2 Let S be a
category of
erzriched spaces, F be agiven
£ -space,
T be thecategory of fibres
in £ that i.s determinedby F, S£fibn
be a closed class
of £ -fibrations
and r : Z - D be aSf-fibration.
Wezuild assume that
Sf fibn
is SF F H E set-valued.Then r will be said to be
free
universalamongst Sf-fibrations,
orto be a
free
universalSf-fibration, if
the naturalfunction
is a
bijection for
all B E W.Further,
D will then be said to be aclassify- ing
spacefor S.F-fibrations
andf
aclassifying
mapfor
theSf-fibrations
in the fFHE class
[rf ].
Let be a
category
of well enriched spaces under the space A.If,
for every choice of a
category
of fibres f in E and of a space X underA,
the class of all associated
f-space
structures on X is a set, then £ will be said to be proper.The
following
classification result for f-fibrations is theorem 5.3 of[B3]
and theorem 3.2 of[B4].
It is the main classification result derived from the BRTapproach
of[B2]
and[B3]
and is the foundation of our main line ofargument
in section 4.Theorem 2.3 Let £ carry the structure
of
a propercategory of
well-enriched spaces under a space
A,
F bean E-space
and F be the associ- atedcategory of fibres.
Then there existsan f-fibrataion,
pf :X, - B,,
that is
free
universalamongst
allf-fibrations,
whereB,
is apath
con-nected
CW -complex.
We conclude this section
by reviewing
someterminology
from[M1].
An
[Mij-sense category of fibres
F has a faithfulunderlying
space functor 0 - T and adistinguished object
F. It satisfies the conditionthat,
for eachobject
X inf,
the associatedproducts
withone-point
spaces, i.e.
spaces X
x * and * xX,
are in 0. Also the evident home-omorphisms
between these spaces and X are in f.Further,
every map in f is a weakhomotopy equivalence, f(F, X)
isnon-empty
for eachspace X in
f,
andcomposition with 0
is a weak
homotopy equivalence,
foreach 0
Ef(F, X).
In this case theobjects
of f will be called[Mi]-,sense f-spaces.
A
given
map q : Y - C will be said to be an[Mil-sense f-overspace (called
anf-space
in[M1]) if,
for each c EC,
there is an associated[M1]-sense 7-spacJ
structure on the fibreYlc.
Let
p : X -
C and q : Y - C bef-overspaces
in the[M1]-sense.
Amap X -> Y over
C,
whose restrictions to individual fibres are inT,
willbe called an an
[M1]-sense f-map
over C.An
[Mi]-sense f-fibration
is an[M1]-sense f-overspace
that satisfies thecorresponding
version of the fCHP.If a
pair
of[M1]-sense
7-fibrations over C areequivalent
under theequivalence
relationgenerated by [M1]-sense f-maps
overC,
thenthey
will be said to be
f-fibre
weakhomotopy equivalent
or fFWHE.A
category
of fibresf,
in our sense, isclearly
an[M1]-sense category
of fibres. For such
7,
many[M1]-sense 7-concepts
coincide with thecorresponding concepts
in our sense. The[Ml]-sense
7-fibration idea then agrees with ourconcept
of anf-overspace satisfying
the fCHP.3 Assessing theories of Structured Fibra- tions and their Classifying Spaces
In this section we will compare three "free
universality style"
classifica- tion results for7-fibrations,
i.e. our theorem 2.3 andparts (i)
and(ii)
of
[Ml, thm.9.2].
In later sections we will compare numerouspublished
classification results for the classical fibrations. Our method will involve
listing
seven desirable criteria that can be used to assess and evaluate the basic characteristics of such theories. We will determine the extent to which the results meet - or fail to meet - the criteria. This willhelp us
decide what is
required of
a "smoother"account,
i. e. one that combinesadvantageous aspects of
eachapproach.
In the case of the two
general
results of[M1],
terms such ascategory
of fibres 7 and f-fibration should be understood in the sense of
[M1].
Let £ be a
category of
enriched spaces, f be thecategory of fibres determined by
agiven 9-space
F andS£fibn
be a classof £-fibrations.
Our criteria will
refer
to aclassification
theoremfor Sf-fibrations.
The three aforementioned results
classify
f-fibrations.So,
in re-viewing
theseresults,
we will beasking
whether or notthey satisfy
the critieria in the case where
S£fibn
meansEfibn,
Sf-fibration means f-ffibration andSFFHE(B)
meansfFHE(B) .
Our first criterion is
just
a statement of theproblem
considered.(1) Simplicity.
Ourpreferred
result willclassify Sf-fibrations,
or atleast those that are over spaces in
W,
up to fFHE.This condition is satisfied
by
theapproach
of our theorem 2.3.Theorem
9.2(i)
of[Ml]
classifiesMay’s
f-fibrations up toTFWHE,
which does not in
general
conform to condition(1).
Theorem
9.2(ii)
of[Ml] requires
thatcategories
of fibres be eitherr-complete
in W[Ml, def.5.1]
orIncomplete
in W[Ml, def.5.4].
Sothe spaces of f must be in W. Hence the
morphisms
of f are bothf-maps
andhomotopy equivalences (see [Sp, cor.7.6.24]),
but may notbe
7-homotopy equivalences.
So theequivalence
relation that classifies f-fibrations may not be fFHE and(1)
has not beenjustified.
Our next two conditions are valid
for,
andstrong points of,
bar con-struction
approaches
to the classification of fibrations. Inparticular,
this
applies
to the twoapproaches
of[Ml].
(2)
Firm Foundations.Any theory of Sf-fibrations,
and their clas-sifying
spaces, should include averification
thatSfFHE(B)
isa set, for
all choicesof
B E W.This is not a
problem
with the bar constructionapproach since,
inthat case, every Sf-fibration over B is 7FHE to one of a constructible set of f-fibrations. In fact this set theoretical
difficulty
arisesonly
whenthe BRT
approach
is used.However,
on theapproach
of our theorem2.3, (2)
follows from[B3, prop.3.7]
and the existence(see
theproof
of[B3, thm.5.3])
of aweakly
contractible universal f-fibration.(3)
EnhancedApplicability. Classifying
spacesfor Sf-fibrations
should be constructed
by
ageometric
bar constructionprocedure.
This is
advantageous,
because knownproperties
of such construc-tions can sometimes be used in
applications.
We are notclaiming
that(3)
is an absoluteprinciple.
If an alternative construction ofclassifying
spaces were to be
found,
that wasadvantageous
in tems ofapplications,
then that construction would be
preferable.
It is shown in
[B4, thm.4.2]
that(3)
is within range ofbeing
validfor our
theory,
i.e. that ourclassifying
spaces have the weak homo-topy types
of thecorresponding
bar construction spaces. In fact thisdeficiency
of our theorem 2.3 will be eliminated in theorems 4.5 and 4.7.(4) Generality
of Fibres. Aclassification
theoremfor SF-fibrations
should not
require
that any unnecessarytopological
condition beimposed
on any
fibre
orfibres.
This is valid for our theorem
2.3,
where no conditions areimposed
on the spaces of f.
The criterion holds when
[M1, thm.9.2(i)]
isapplied
to the threeclassical theories
(see
"reviews"(iv), (vi)
and(ii)
ofchapters 5,
7 and8,
respectively). However,
it is not clear that it holds for[Ml, thm.9.2(i)]
in
general.
In the case of
[M1, thm.9.2(ii)],
it isrequired
that JF should be eitherr-complete
in W orf’-complete
in W. Thisrequires that,
for all Y in0,
thespaces X
andf(F, X)
should be inW,
so the criterion doesnot hold. The space
f(F, X),
ofmorphisms
from F toX,
carries thecg-ified compact-open topology.
(5)
TheEquivalence
of Theories of Structured andPrincipal
Fibrations. Let £ be a
category of
enriched spaces, f be thecategory of fibres
determinedby
aparticular £-space F, SE fibn
be agiven
classof E -fibrations
and r be arcSf-fibration.
Then r should be
free
universalamongst Sf-fibrations if
andonly if prinF(r)
isfree
universalamongst principal f(F) -fibrations.
This will be verified on our
approach
in theorem6.4(i).
It tells usthat the theories of f-fibrations and
principal f(F)-fibrations
are, in asense,
equivalent.
Thus(ii)
and(iii)
of theorem6.4,
whichexplain
thisequivalence, depend
on(5).
Similar
arguments apply
in the two cases of[M1, them.9.2].
Howeverthe limitations on
F,
referred to under(4), prevent
us fromachieving
full
generality.
(6) Unity
of Theories. For eachspecific type of
classicalfibration,
a suitable choice
of 9
andS£fibn
should ensure that theSE-fibration concept
coincides with a standard oroptimal definition of
thattype of
classical
fibration.
Ourgeneral classification
theorem should thenimply
that the conditions
(1), (2),
...(5)
are valid in the contextof
each suchtheory of
classicalfibrations.
We
explained
in our Introduction that[Ml, thm.9.2(i)]
isactually
two
disjoint results,
i.e.parts (a)(i)
and(b)(i)
of that theorem.[M1, thm.9.2(ii)]
is also twodisjoint results,
i.e.parts (a)(ii)
and(b)(ii)
ofthat theorem. In each case,
(a)
refers to the situation where the corre-sponding
space A isempty
andapplies
to bothprincipal
and Hurewiczfibrations,
and(b)
to the situation where A is a onepoint
space andapplies
to sectioned fibrations. So these twogeneral results,
in the formgiven,
do not meet(6)
since neither is asingle
theorem that covers all of the classical theories.We
delay
further discussion of(6)
until sections5,
7 and 8.Our final criterion refers
only
toprincipal
G-fibrations and is the fibrationanalogue
of[DI, them.7.5].
It is not verified in any of the three accounts of structured fibrations. However it isshown,
in each case, that there areweakly
contractible universalprincipal
G-fibrations thatare also free universal. The criterion will be
verified,
for ourapproach,
in
corollary
6.2.Proposition 5.10(i),
inconjunction
with(5), implies
that an
assumption
that G isgrouplike
isrequired
in ourtheory.
(7)
WeakContractibility.
Let G be atopological
monoid. Aprinci- pal G-fibration
should befree
universalif
andonly if
its total space isweakly
contractible.Our first
objective
can now be made moreprecise.
Clarified Statement of
Objective
A. We wish todevelop
atheory of S£-fibrations
and theirclassifying
spaces thatsatisfies
our criteria(1), (2),
...(7).
Review of
Progress
made towardsachieving Objective
A. Itshould be understood
that,
in some of the cases where agiven published theory
is not shown tosatisfy
agiven criterion,
the criterion can be verified withoutmajor changes
to the work inquestion. However,
thecritical
difficulty
with the BRTapproach
lies inensuring
that(2)
and(3)
are satisfied. The criticaldifficulty
with the GBCapproach
lies inensuring
that(1), (4)
and(6)
are satisfied. It wasexplained,
in theprevious section,
that earlier papers of this series havesimplified
thesituation. Thus
(2)
has been resolved and(3) partly
resolved for ourversion of the BRT
approach.
In the case of(3),
this was doneby equating
the twotypes
ofclassifying
spaces.The
remaining problem
consistsof modifying
theorem 2.3 to obtaina
classification
resultfor f-fibrations
thatsatisfies (3), extending
thatresult to
classify
subclassesSf fibn of f-fibrations, noticing
that(1)
to(4)
remain valid in theSfFfibn context,
andverifying (5), (6)
and(7)
in that context.
4 On the Classification of Structured Fi- brations
We now introduce three more universal Sf-fibration
concepts,
the sec- ond of thembeing closely
related to our criterion(3).
Definitions 4.1 Let 9 be a
category of
enriched spaces, F be agiven
£-space,
f be thecategory of fibres
in 9 that is determinedby F, S£fibn
be a closed class
of £-fibrations
and r : Z - D be anSf -fibration.
(i)
TheSf-fibration
r will be said to beweakly
contractible universalif PrinF(Z)
is aweakly
contractible space.(ii)
We recall that there is a "univeral"f-overspace
andquasifibra- tion P*,F: B(*, f(F)’, F) -> B(*,f(F)’,*) (see
theintroduction).
Thenr urill be said to be bar construction universal
if
there are weakhomotopy
equivalences,
h : Z -B(*, f(F)’, F)
and k : D -B(*,f(F)’, *),
such thath,
k > is anf-pairwise
mapfrom
r to P*,F..(iii)
AnSf -fibration
will be said to be atriple
universalSf -fibration,
or to be
triple
universalamongst Sf-fibrations, if
it is universal in thefree, weakly
contractible and bar constructions senses.We now determine some relations between our various
types
of uni-versality,
a discussion that iscompleted
in theorem 6.1.Proposition
4.2 Let £ be acategory of
enriched spaces, F be agiven 9 -space,
f be thecategory of fibres
in E that is determinedby F, S£ fibn
be a closed class
of £-fibrations
and r : Z -> D be aSf -fibration.
Thenthe conditions:
(i)
The classSf fibn
is Sf FHE set-valued and r is afree
universalSF -fibration,
(ii)
r isweakly contractible universal, (iii)
r is bar constructionuniversal,
and(iv)
r is atriple
universalSf -fibration
are related
according
to the scheme:If D E W,
then this relation becomes:Proof. (ii)
=>(i).
This is similar to theproof
of[B3, thm.3.4], except
that we nowforget
about basepoints
and fibrationsbeing grounded.
The closed condition ensures that the
argument
is valid in the context of Sf-fibrations.(iii)
=>(ii).
We recall thatprinF(p*,F)
is aquasifibration [M1, prop.7.10].
Thef-pairwise
map of our data induces apairwise
map fromprinF(r)
andprinF(p*,F).
This in turn induces a sequence ofhomomorphisms
from the groups in the exacthomotopy
sequence ofprinF(r)
to the groups in the exacthomotopy
sequence ofprinF(P*,F).
The
homomorphisms
between thehomotopy
groups of the base spaces and thehomomorphisms
between thehomotopy
groups of the fibresare all
isomorphisms.
In the former case this follows from thedata;
in the latter case it is a consequence of the
morphisms
of f all be-ing f-homotopy equivalences.
It thenfollows, using
the 5-lemma and thepath-connectedness of B(*, 7(F)’, *) [M1, prop.7.1],
that the homo-morphisms
between thehomotopy
groups of the total spaces are alsoisomorphisms.
Now the total space ofprinF(p*,F)
is contractible[B4, prop.3.1],
hence the total spaceof prinF(r)
isweakly
contractible.(ii)
=>(iii),
where D E W. This is similar to theproof
of[B4, thm.4.2(i)].
The reader will notice that thisargument
uses thepath connectivity
of the base space. This last fact follows from the freeuniversality
of thegiven fibration,
since there isjust
asingle
JFFHEclass of f-fibrations over a
point.
The conditions
involving (iv)
are immediate from the definition of thatconcept
and the otherparts
of this result.For a
triple
universal Sf-fibration with BRTtype classifying
spaces,these spaces are
CW-approximations
to thecorresponding GBC-spaces B(*, (f(F))’,*) [B4, thm.4.2(i)].
Hence such BRT spaces are deter- mined up tohomotopy type.
We willspecify
aCW-approximation
toB(*, (7(F) )’, *)
and utilize it as ourpreferred classifying
space.Given any space
X,
we will use|S(X)|
to denote Milnor’s geo- metric realization of thesingular complex S(X).
Then)S(X))
is aCW-complex
and there is an associated weakhomotopy equivalence j = jx : |S(X)|->X [FP, thm.4.5.30].
Definition 4.3 For each
topological
monoidG,
wedefine
the associatedgeometric
bar constructionCW- complex BG
to beI S(B (*, G’, *))|.
Proposition
4.4If
G is atopological monoid,
thenBG
ispath
con-nected.