C AHIERS DE
TOPOLOGIE ET GÉOMÉTRIE DIFFÉRENTIELLE CATÉGORIQUES
P ETER I. B OOTH
On the geometric bar construction and the Brown representability theorem
Cahiers de topologie et géométrie différentielle catégoriques, tome 39, no4 (1998), p. 271-286
<http://www.numdam.org/item?id=CTGDC_1998__39_4_271_0>
© Andrée C. Ehresmann et les auteurs, 1998, tous droits réservés.
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ON
THEGEOMETRIC
BARCONSTRUCTION
ANDTHE BROWN REPRESENTABILITY THEOREM
by
Peter L BOOTHCAHIERS’ DE TOPOLOGIE ET
GEOMETRIE DIFFERENTIELLE CATEGORIQUES
J ’olume XXXLX-4 (1998)
Resume
Cet article
poursuit
led6veloppement
d’une théorie des fibra- tions enrichies et de leursespaces
classificateurs. Pluspr6cis6-
ment, les
quasi-fibrations
enrichiesproduites
a-partir
de la con-struction "barre" de
May
sont reli6es aux fibrations enrichies d6riv6es du théorème dereprésentabilité
de Brown. Cecipermet
d’élaborer une nouvelle
approche
pour construire les espaces classificateurs des fibrationsenrichies,
tout en conservant lesprincipaux avantages
de l’une ou 1’autre des deuxapproches
mentionnées
plus
hautquant a
leursimplicite, generalite
etcalculabilite.
1 Introduction
This is one of a series of papers
following
on from[Bo2];
wenormally
usethe
terminology
introduced there. Our overallobjective
is todevelop
avery smooth
theory
of enriched fibrations and theirclassifying
spaces.Such a
theory
should combine andincorporate
many individual theo-ries, including
the "classical" ones ofprincipal,
Hurewicz and sectioned fibrations.In this paper we relate universal enriched
qu asi-fib rations - produced using
the two-sidedgeometric
bar construction of[Ma2] -
to universalenriched
fibrations
obtained via the BrownRepresentability
Theorem in[Bo3]
and[Bo4] .
Thesecomplementary
methods ofproducing classifying
spaces are blended
together, thereby producing a classification theory
with the
advantages of
bothapproaches
and thedisadvantages of
neither.We will
always
assume that E is acategory
of enrichedtopo- logical
spaces(see [Bo2, p-129], [Bo3, ch.2]).
Thus there is a faithfulunderlying
spacefunctor,
from E to theunderlying topological
cate-gory, that
forgets
any additional structure on theobjects
of £.Further,
if P is a space,Q
is an£-space
and there is ahomeomorphism
from Ponto the
underlying
space ofQ,
then there is aunique £-space
struc-ture on P such that this
homeomorphism
is theunderlying
map of an£-homeomorphism (= E-isomorphism).
We recall the
concept
of an£-overspace,
i.e. a map q : Y -> C to-gether
with an associatedE-space
structure on the fibreYlc
=q-1(C),
for each c E C. For
example,
ifQ
is anE-space
and C is a space, thenthe
projection Q
x C -> C is an9-overspace
in an obvious way.If q : Y--> C is a map and S is a
subspace
ofC,
thenY IS
will denote thesubspace q-l(S)
of Y andqlS: YlS ->
S the restrictionof q
toYlS.
If q
is an£-overspace,
thenqlS
isclearly
also an£’-overspace.
The
9-overspace q
will be said to be an£-fibration
if it satisfies the£-weak
covering homotopy
property(= £WCHP) [Bo2, p-136].
In thecase where £ consists of
topological
spaces without extra structure this is the WCHP of[Do,
section5];
fibrationssatisfying
the WCHP willbe called Dold
fibrations.
Let q
be anE-overspace
suchthat,
for each U in a numerable coverLf of
C,
there is anE-space Q
=Q(U)
such that the restrictionqlU
is£-fibre homotopy equivalent (= EFHE) [Bo2, p.130]
to theprojection E-overspace Q
x U --> U.Then q
will be said to be£-locally homotopy
trivial or ELHT
[Bo2, p.142].
Let W denote the class of all spaces
having
thehomotopy
type of aCW-complex.
If C EW,
then an£-overspace
q is an £-fibration if andonly
if it is ELHT[Bo2, thm.6.3].
We will
always
assume - unless wespecify
otherwise - that F is agiven £-space
and use to denote thecategory of fi-
.bres
containing F,
i.e. thecategory
of all£-spaces
that are9-homotopy equivalent
to F and all£-homotopy equivalences
between them.
Let F(F)
denote the monoid undercomposition
ofself-F-homotopy equivalences
ofF, topologized
as described’below.
Then7(Fl’
willdenote
F(F)
with a whisker grown at itsidentity
1F. We notice that.F(F)’
also carries the structure of atopological
monoid. It can be used with the bar construction to construct an associatedF-overspace,
i.e.a universal
F-quasi-fibration
qF :Y F -> C17 (see §3
for moredetails).
May
used either ar-completeness [Ma2, def.5.1]
or aF’- complete ness [Ma2, def.5.4] assumption
to convert his qF into a universalF -fibration
rqf
orr’qT [Ma2,
thm.9.2(a)
and(b)].
Thistheory
can be very usefulin the area of
applications (see,
forexample, [Ma3]).
The r- and r’-completeness assumptions also, however,
have the drawback that theiruse detracts from the
simplicity
andgenerality
of the classification result obtained.The Brown
Representability
Theoremapproach, given
in[Bo3]
and[Bo4],
allows the construction of an alternative universal F-fibration pT:X F -> Byr (see §3
for moredetails). Further,
thisprocedure
avoidsthe above
problems (compare [Bo4, thm.5.3]
with[Ma2, thm.9.2, (a)
and
(b)]).
On the otherhand,
pF cannot beapplied
in the same directand flexible fashion that is
possible
with the formerapproach.
Theseand other
issues, concerning
the merits ofdiffering approaches
to theclassification
problem,
will be reviewed in[Bo5].
We use a fibred
mapping
spaceargument
toequate
PF and qF.In
particular,
weequate
theclassifying
spacesB F
andC F.
Neithera
r-completeness
nor ar’-completeness
condition is assumed. Thenproperties of
the bar construction can be usedfor applications,
in thesimplified
and moregeneral
Brown’s theorem context.If
p:X->B and q : Y - C
are maps, and h : X - Yand g: B -> C
are maps such that
qh
= gp, then we write thath, g>
is apairwise
map
from
p to q.If p
and q are£-overspaces
andhl(Xlb): Xlb-> Ylg(b)
is an
£-map
for each b EB,
then we will write thath, g>
is an£-pairwise
mapfrom
p to q. In section 2 we consider some relevantproperties of fibred mapping
spaces,leading
to theorem 2.7 whichgives
sufficient conditions for the existence of an
F-pairwise
map from agiven
F-fibration to a
given F-overspace.
Thisresult, together
with the prop-erties of the
geometric
bar construction and of the Brown’s theorem universal fibration that are reviewed in section3,
enables us to show in section 4(theorem 4.2)
that there is anF-pairwise
maph, g>
from p F to qF. Further h :X F -> Yjr and g : B F --> C F
are weakhomotopy
equivalences.
Thus we have achieved ourobjective.
It follows
(corollary 4.3)
that the bar construction spaceC.F
acts asa
classifying
space for F-fibrations It does so without therequirement
of a
topological condition,
such as compactness orbelonging
toW,
onthe
underlying
spaces of the fibres involved.Our discussion should be taken to be in the context of the
category
T ofcompactly generated
or cg-spaces([Bo2, p.128-129]
and[V, sec.5, ex.(ii)]).
Thus if X and Y are cg-spaces, thenT(X,Y)
willdenote the space of all maps from X to Y
equipped
with thecg-ified
modification
[Bo2, p. 129]
of thecompact-open topology. F(F)
will betopologized
in the same fashion.We recall that a space B is weak
Hausdorff [Bo2, p.129]
if thediago-
nad subset
AB
={(b, b) lb
EB}
is closed in the(cg-ified) product
spaceBxB.
Lemma 1.1
If B
is a weakHausdorff
space and S is asubspace of B,
then S is weak
Hausdorff.
Proof.
Thediagonal
subsetAs
=(S x S)
nAB
is closed in S x S.2 Fibred Mapping Spaces and Structure
Preserving Maps
We will assume,
throughout
thissection,
that B is a weak Hausdorff space and thatp : X - B and
q : Y -3 C are£-overspaces.
We recall the
concept
of theE-overspace
qg: Y n D -->D,
inducedby pulling
q back over the map g : D --7 C[Bo2, p.130].
Also that there is afibred
mapping
space XDY withunderlying
setUbEB,cECE E(XlblYlc)
and a map
pDq: XDY --> B x C,
with(pDq)(f)
=(b, c),
wheref
EE(Xlb, Ylc),
b E B and c E C[Bo2, p.131-132]. We use pDlq:
XD Y -> B andpD2q: XDY --> C
to denote the maps that are thecomposites
ofpDq
with theprojections
7rB: B x C - B and 7rc: B x C -C,
respec-tively. So if f E E(Xlb, Ylc)
where b E B and c EC,
then(pD 1q) (f)
= band
(pD2q)(f)
= c.In this section we
develop
some basicproperties
ofpolq.
Versionsof some of these
(theorem 2.1,
corollaries 2.2 and 2.4 and a weaker form ofproposition 2.6)
have beengiven
elsewhere(see [BHP1], [BHP2],
[BHMP]
and[Bol]).
However this material is not all in oneplace,
thedetails of the
proofs
are sometimes ratherskimpy
and the results areoften based on data somewhat different from ours.
Theorem 2.1 : Fibred
exponential
law. Letf : D -> B
be a map.Then there is a
bijective correspondence
between:(i)
the setof £-pairwise
mapsh, g> from p f
to q and(ii)
the setof
maps ho: D XCIY overB,
i. e. relative tof
andpolq,
determined by h(x, d)
=ho(d)(x)
and g =(pD2q)hO,
wherep(x)
=f (d).
Proof.
This isjust
aslight
modification of theproof
of another fibredexponential law,
i.e. theorem 2.2 of[Bo2];
we notice that B isrequired
to be weak Hausdorff in that result.
If s : D - B and t : D - C are maps then the map
D -> B x C,
withd->(s(d), t(d))
where d ED,
will be denotedby (s, t).
Leth,
g>be
an
£-pairwise
map fromp f
to q. Then there is a mapho: D -> XOY,
defined
by
theequality specified above,
and such that(pDq)hO = ( f, g) (see [Bo2, thm.2.2]).
So(pDlq)h° = 7rB(pDq)hO = 7rB(f,g)
=f,
and h°is a map over B as
required.
Conversely,
let ho: D -> XDY be a mapsatisfying (pO,q)h’ = f .
Then
(pDq)ho = (pD1q,pD2q)ho = ((pDlq)hO, (pD2q)hO) = (f, g),
where9 =
(pD2q)ho:
D -> C. So ho satifies the conditionspecified
in[Bo2, thm.2.2],
the associated h is well defined andh, g>
is asrequired.
Corollary
2.2 There is abijective correspondence
between :(i)
the setof £-pairwise
mapsh, g> from p
to q, and(ii)
the setof
sections ho topDlq,
determined by hl(Xlb)
=ho(b)
and g =(pD2Q)hO,
where b E B.Proof.
This follows from theorem 2.1 if we take D =B, f
=1B
andidentify p f
with p.Corollary
2.3If S is a subspace of B,
then(XOY)IS = (pD1q)-1(S)
and
(XlS)DY
areidentical,
and(pDlq)IS = (pIS)Dlq.
Proof. Clearly
theunderlying
sets of the two spaces coincide and the functions(pO1q)l,S
and(plS)D1q
are identical. Let us consider any(of
course
cg-)
spaceD,
mapf :
D -> S and function k : D -->(X DY) lS
thatis over S. We will prove that k is continuous into
(X DY) lS
if andonly
if it is continuous into
(XlS)DY.
The result will then follow.Let i :
S -> B and j : (X DY)l S ->
X DY denote the inclusions. If k is continuous into(XDY)IS,
it follows thatjk :
D -> X OY is a map overB,
relative to the mapsi f : D -> B and pD14q: XDY ->B. Applying
our fibred
exponential law,
there is acorresponding E-pairwise
maph , g
> fromPi f
to q, determinedby h(x, d)
=k(d) (x),
wherep(x)=
if (d)
=f(d) and g
=(Po2q)jk.
The£-overspaces pi f : X
n D - Dand
(plS) f : (XlS)
n D -> D areidentical,
soh , g >
is an£-pairwise
.map from
(p/s)f
to q. Now S is weak Hausdorff(lemma 1.1),
and so itfollows from theorem 2.1 that there is a map L : D ->
(X /S)[]Y
overS,
i.e. with
((p/S)[]1q)l
=f. Further, l(d)(x)
=h(x, d)
=k(d)(x)
wheref(d)
=p(x),
so l = k and k : D ->(X /S)[] Y
is continuous.Now each
step
in the aboveparagraph
isclearly reversible,
so thecontinuity
of k in the two senses isequivalent
and theproof
iscomplete.
The subset
Uc E
C£(F, Ylc)
of the setT(F, Y)
determines a sub- spacePrinFY
of the spaceT(F, Y).
Then thecomposite
of the inclu- sion mapPrinFY -> T(F, Y),
the mapT(F, Y )->
Y that evaluates atan
arbitrarily
chosenpoint
of F and q : Y - C is the obviousprojection prinFq:
PrinFY -> C. Hence thisprojection
is continuous.Corollary
2.4If bE B,
then thefibre of pOlq
over b isPrin XlbY’
Proof.
It follows fromcorollary
2.3 that the fibre ofpF-l 1 q
over b EB, i.e. (X[]Y)/b,
is(Xlb)DY.
Hence we have to prove that(X/b)[]Y =
Prin XlbY’ Clearly the underlying
sets are identical,
so we just
have to
prove that the
topologies
agree. Let D be a space and h° : D ->(X/b)[]Y
be a function. We will show that
ho
is continuous into(Xlb)[]Y
if andonly
if it is continuous intoPrinXlbY’
The result then follows. Let usapply
the fibredexponential
law to h° : D ->(Xlb)[]Y,
considered as amap over a
point,
and the"ordinary" exponential
law[Bo2, (0.1)]
toh° : D -
Prin XlbY
C7(Xlb, Y).
We see that in each case the conti-nuity
of h° isequivalent
to thecontinuity
ofh:(Xlb)xD->Y,
whereh(x, d)
=hO(d)(x),
with x E X and d E D. Hence theproof
iscomplete.
If b E
B,
thenqlb :
F - F x{b}
will denote thehomeomorphism
de-termined
by qlb(z) = (z, b),
where z E F. It follows - from the definition ofcategory
of enriched spaces - that there is aunique £-space
structureon
Fx{b}, making Ob
into anE-homeomorphism
for each b E B. We recall that this allows us to view theprojection
7rB : F x B -t B as anE-overspace.
Corollary
2.5 Let II:(PrinFY)
x B -3 B denote theprojection.
Thereis a
homeomorphism O: (FX B)DY Q£ (PrinFY)x B,
that is over B inthe sense that IIO = 7rBDiq.
Proof.
Ifb E B,
c E C andg e E(F x {b}, Ylc),
then9Ob e E(F, Y/c)
CPrinFY.
We define the function O:(F x B)[]Y -> (PrinFY)xB by
therule
O(g)= (9Ob, IIB[]1q(g)).
ThenIIO(g) = II(9Ob, (IIB[]1q) (g))
=(IIB[]:1q)(g),
so IIO =7rBcllq
and the function (D is over B.Let
Ob : Fx{b}
-> F denote thehomeomorphism Ob (z, b)
= z, wherez E F and b E B. Then
’l/Jb
is theE-homeomorphism
that is inverse toOb.
If f E PrinFY
andb e B,
thenf wb e E(Fx {b}, Ylc)
C(Fx B)DY,
where c =
(prinFq) (f).
Let V :(PrinFY)x B -> (FxB)DY
be the func- tion withw(f,b)
=fOb-
It iseasily
seen that TO and Ow areidentity functions,
so 0 and W are inversebijections.
On
applying
theorem 2.1 to theidentity
on(FxB)DY,
we obtain anE-pairwise
map e,IIB[]2q>
from(IIB) (IIB[]1q)
to q. The evaluation, mape: (F x B) n ((F x B)[]Y) ->
Y is determinedby e(z, b, g)
=g(z, b),
with z E
F,
b E B and g EE (F x {b}, Y/c)
for some c E C.Further,
thereis a
homeomorphism ((FxB)[]xF = (FxB)
n((FxB)[]Y)
deter-mined
by
the rule(g, z)
-3(z, b, g),
where b =(IIB[]1q)(g).
Hence we see,by composition,
that there is a map((F x B)[]Y)
x F -Y, (g, z)
-g(z, b).
Applying
theexponential
law of[Bo2, (0.1)]
to this map, the ruleg->(z->g(z,b))
determines a map(FxB)DY --+ T(F, ¥).
In this caseg E (F x B)[]Y, z E F and b = (IIB[]1q)(g).
Nowg(-, b) : F -> Y/c,
whichtakes z to
g(z,b),
is90b
EE(F, Ylc),
where c =(7rBD2q)(g).
So we havea map
(F x B) []Y -> PrinFY,g-> 9Ob
and it follows that O is continu-ous.
We now define maps
e’,
Àand p
such thate’ À,
u> is an£-pairwise
map
corresponding
to T. If theordinary exponential
law isapplied
tothe inclusion
PrinFY
C7(F, Y),
we obtain an evaluation map:where
f
EPrinFY
and z E F. Let us defineby A ((z, b), (f, b)) = ( f, z), where z E F,
b E B andf E PrinFY,
andby
where
f E PrinFY
and b E B. Soqe’À(z,b,f,b)
=qf (z) = (prinFq)(f)
=
1u(f,b) = u((IIB)II(z, b, f, b)),
wherez E F,
b E B andf E PrinFY.
Hence
e’À,tt>
is an£-pairwise
map from(IIB)II
to q.Applying
theo-rem 2.1 there is a map
(PrinFY) x B -> (F x B) [] Y,
determinedby
therule
( f, b)->((z, b)->f (z)),
wheref
EPrinFY,
b E B and z E F. Nowthis is
T,
so T is continuous. Hence 4D is ahomeomorphism
over B.Proposition
2.6If B is
aCW-complex,
p: X -> B is an£-fibration and q : Y - C is
an£ -overspace,
thenpO 1 q
is a Doldfibration.
Proof.
We know that p is £LHT. Thus there is a numerable cover U of Band,
for each U ELf,
there is anobject Q
of £ such thatplU
is £FHE to the
E-overspace
andprojection
7ru :Q X U ->
U. Itfollows,
via
corollary 2.3,
that(p[]1q)lU
=(plU)[]1q,
which in turn is FHE to(IIU)[]1q.
We see from lemma 1.1 that U is weakHausdorff,
and hencefrom
corollary
2.5 that(7ru)Olq
ishomeomorphic
over U to the pro-jection PrinQ (X ) x U -> U.
HencepOlq
islocally homotopy trivial,
i.e.TLHT,
and therefore a Dold fibration.The last
result,
which was announced withoutproof
in[Bo1, (7.2)],
should not be confused with certain similar
published
results. Thusall of
[Bo2, prop.4.5], [BHPI, prop.6], [BHP2,
axiomA4]
and[BHMP, prop.2.3]
state that if p and q are(in
somesense) £-fibrations,
thenpDq
is(some
sortof)
a fibration. These results prove,by composition
with
IIB: BxC -> C,
thatpO l q
is a fibration.However, they
assumesomething
that we cannot assume about q, i.e. that it is at least an£-fibration. The fact that q need not possess such a
property
is crucialfor our verification of theorems 2.7 and 4.2.
From this
point
on ourargument
willusually
focus on acategory
of fibres7,
rather than onE;
the E ofprevious
resultscan, of course, be taken to be such an F. So X[]Y and
PrinFY
willnow consist
entirely
of7-homotopy equivalences
between spaces thatare
always 7-homotopy equivalent
to F.A space S will be said to be
weakly
contractible if7r;(S)
=0,
for allnon-negative integers
i.Theorem 2.7 Let B be a
CW-complex,
p : X -> B be anF-fibration
and q : Y -> C be an
F-overspace. If FrinFY
isweakly contractible,
then there is an
F-pairwise
mapfrom
p to q.Proof.
It follows fromproposition
2.6 thatpDlq
satifies the WCHP.The fibre of
p[]1q
over b E B isPrinXIbY (corollary 2.4), which has
the
homotopy
type ofPrinFY
and is therefore aweakly
contractible space.Considering
the exacthomotopy
sequenceof p[]1q,
we see thatthis map is a weak
homotopy equivalence. Factoring pDig
as the com-posite
of ahomotopy equivalence
X []Y -> R and a Hurewicz fibration p : R ->B,
we see via[Do, thm.6.1]
that p is FHE top[] 1q.
Hence p is aweak
homotopy equivalence and, by [Sp, thm.7.6.23],
p has ahomotopy section,
i.e. a map 0’ such that p6 = 1B.Applying
the CHP we seethat p has a
section,
hence so also doespdlq.
The result follows fromcorollary
2.2.3 Constructing Classifying Spaces
We will now
quote
someresults
from[Ma2].
Theconcept
ofcompactly
generated
space, as used in thatmemoir, incorporates
the weak Haus- dorffness condition.Hence,
from thispoint
on, our discussion shouldbe taken to be in the context of the
category
of weak Hausdoffcg-spaces [Mc,
section2].
Let G be a
topological
monoid that isgrouplike,
i.e.II0(G)
with theobvious induced
operation
is a group.Further,
let us assume that theidentity
element t of G is astrongly non-degenerate
basepoint,
in thesense that
(G, ftl)
is astrong NDR-pair (see [Mal,
definitionA.1]).
Let X and Y be left and
right G-spaces, respectively.
Then[Ma2, p.31]
describes a two-sidedgeometric
barconstruction,
that defines aspace
B(Y, G, X). Further,
if * is aone-point
space, there is aunique
left action Gx * - * and the map X ->* induces a
quasi-fibration
py,x:
B(Y, G, X) - B(Y, G, *) [Ma2, p.34].
Then pY,X has fibres home-omorphic
to X[Ma2, p.35].
If H is any
(of
coursecg-sense) topological monoid,
we will use H’to denote the space
consisting
of H with a whisker(= I)
grown atits
identity
t. Thus wesimply identify t
with 0. Then H’ carries the structure of atopological monoid,
under theoperation
that extends both theoperation
on H andmultiplication
onI,
and has th = ht = h for all t E I and h E H. Theidentity
for H’ is of course 1. If H is agrouplike topological monoid,
then we notice that H’ is also agrouplike topological
monoid. The relevance of H’ lies in the fact that it has astrongly non-degenerate
basepoint (see [Mal,
definitionA.8]
for furtherdetails).
The evaluation map
e:F(F)
x F -F, e( f, z)
=f(z)
wheref
Ef(F)
and z E
F,
and thecomposition
mapc:f(F)
xf(F) ->f(F), c(f, 9) = fg
wheref
andgEf(F),
are left actions off(F)
on F andf(F), respectively.
Let us now define amorphism
oftopological monoids,
i.e.
(3: f(F)’ -> f(F), by B(t) =1F
and(3(h)=h,
where t E I andh
~ f(F).
Then there are left actions ofe ( jS
x1F):f(F)’
x F -+ Fof
T(F)’
onF,
andc(B x 1.f(F)) F( F)’ x f(F) -> f(F)
of,f(F)’
on-T(F).
The above left action
F(F)’x F -> F
and the left andright
actionsof
f(F)’
on * determine a mapp*,F:B(*,f(F)’/,F)->B(*,f(F)’,*);
we use gf:
Y, - Cir
to denote this map.Then
C F
=B( *, F( F)/, *)
is thegeometric
bar construction classi-fying
spacefor
f.Proposition
3.1 The map qg7 is aquasi-fibration
and carries the struc-ture
of
anf-overspace.
The mapprinF(qF): PrinF(Yf)-> CF
is aquasi-fibration
with a contractible total spacePrinF(Y F).
Proof.
The first two conditions arejustified because,
asexplained
pre-viously,
any pY,X is aquasi-fibration
with fibreshomeomorphic
toX;
PrinF(qf)
is aquasi-fibration by [Ma2, prop.7.10].
We
just
have toverify
thecontractibifity
condition. We see, via[Ma2, prop.7.10],
that the spacePrinF(YF)
=PrinF(B(*,f(F)’, F))
is
homeomorphic
toB(*,f(F)’, f(F)).
The latter bar construction space is definedusing
the above left actionf(F)’xf(F) ->f(F).
Ithas the
homotopy
type of the spaceB(*,f(F)’, f(F)’),
that is obtainedusing
theoperation
onf(F)’ (see [Ma2, prop.7.3(ii)]). This,
in turn,can be seen to be contractible
(take
Y = * in[Ma2, prop.7.5]).
HencePrinF(Yf)
is contractible.We now turn to a
completely
different construction ofclassifying
spaces, i.e. the Brown
Representability
Theoremapproach
of[Bo3]
and[Bo4].
Thearguments
of those papers are valid in the world of weak Hausdorff cg-spaces, if a suitableadjustment
is made to the definition of"space
under agiven
spaceA",
as stated in[Bo3,
section2].
We will assume that
(X, i)
is a space under A now means thati : A - X is a
homeomorphism
of A onto a closedsubspace
of X. Thisensures that all
adjunction
spaces, that appear in thisfamily
of papers,are defined
using
a map out of a closedsubspace
of agiven
space. It followsthat,
in our newcontext,
all of theseadjunction
spaces are weak Hausdorff(see [Mc, props.2.4
and2.5]).
The fibredmapping
spaces that appear in thisfamily
of papers may,temporarily,
take us outside thecategory
of weak Hausdorff spaces.However,
that does notprevent
usfrom
drawing
conclusions thatapply
in thatcategory.
An f-fibration p : X -> B will be said to be universal if it is universal in the
weakly
contractible sense, i.e. ifPrinF(X)
isweakly
contractible.It is a shown in
[Bo4, prop.3.7] that,
if such a p exists and a spaceD E W,
then the collection7FHE(D)
of all fFHE classes of f- fibrations over D is a set.Further,
such a p is alsofree
universalamongst
f-fibrations.
Thus there is abijection
that is
natural,
relative to D in W(see [Bo3, prop.7.4]
and[Bo4, thm.3.4]).
We recall the
concept
of Ecarrying
the structure of acategory of
well enriched spaces under a
given
space A[Bo3, def.2.3].
Thus£,
with its
underlying
spacefunctor,
is acategory
of enriched spaces that possesses well behavedsubspaces, cylinders
andmapping cylinders,
allin the under A sense.
Further,
thecategory
of enriched spaces structureon & is derived from the well enriched structure on that
category (see [Bo3, lem.2.4]).
If,
for every choice of acategory
of fibres f in 9 and of a space Z underA,
the class of all associated,f-space
structures on Z is a set, then E will be said to be proper[Bo4, def.5.1(ii)].
Theorem 3.2
(see [Bo4, thm.5.3]J
Let E carry the structureof
a propercategory of
well enriched spaces under a spaceA,
F be an£-space
andf be the
category of fibres
determinedby
F. Then there exists a uni- versal7-fibration pf-:Xf-> Bf
over apath
connectedCW-complex Bir.
The above is a consequence of Brown’s
theorem,
so the spaceB F
willbe said to be a Brown
Representability
Theoremclassifying
spacefor f.
4 Main Result
Lemma 4.1
If q : Y - C
is anF-fibration,
thenprin,Fq
is a Doldfi-
bration.
Proof.
Let us take W to be agiven
space, and g : W x{0} -> PrinFY
and G : W x I-> C to be maps such that
(prinFq)g
=GI(W
x{0}).
Itfollows from the
exponential
law(0.1)
of[Bo2]
that there is a mapg’ : F
x W x101
-3Y,
determinedby
the ruleg’(z,
w,0)
=g(w, 0) (z),
where w E W and z E F. If II : F x W -> W denotes the
projection,
thenqg’(z,w,0)
=q(g(w, 0)(z))= (prinFq)g(w,0) = G(w,0)
=G(II X 1I)(z,w,0). Further, g’(-, w, 0)
=g(w,0)
Ef(F,YlG(w,0)),
and so
g’, GI(W
x{0})>
is anf-pairwise
map from 7r x1{0}
to q.Now q
has the7WCHP,
so there is amap H’ :
F x W x I -Y,
suchthat
H’,
G> is anf-pairwise
map from 7r x II to q. We see, via the or-dinary exponential law,
that there is a map H : W x I -7"(F, Y),
whereH(w, t)(z)
=H’(z, w, t)
for all w EW, t E
I and z E F. Then the abovef-pairwise
condition ensures that H factorsthrough PrinFY,
and wecan take H to be a
homotopy
W x I ->PrinFY.
So(prinFq)H(w, t)
=q(H(w, t)(z))
=qH’(z,
w,t)
=G(7r
x1I)(z,
w,t)
=G(w, t),
for all w EW,
t E I and z E F. Hence
(prinFq)H
= G.Further, H(w, 0)(z)=
H’(z, w, 0)
=g’(z, w, 0)
=g(w, 0)(z),
for all w E W and z E F. SoH(w, 0)
=g(w, 0),
for all w E W.Theorem 4.2 Let £ carry the structure
of
a propercategory of
wellenriched spaces under a space
A,
F be agiven E-space
and f be thecategory of fibres
determinedby
F. Then:(i)
there is anf-pairwise
maph,
g>from
PF to qF such that the maps h :X, - Yjr
and g :Bf-> C F
are weakhomotopy equivalences.
(ii) If 7(F)
EW, then g
is ahomotopy equivalence; if also F E W,
then h is a
homotopy equivalence.
Proof. (i)
It follows from theorem2.7, proposition
3.1 and theorem 3.2 that there is anf-pairwise
maph, g> : pf-> qf.
The maph:Xf->Yf
induces a maph#: PrinF(Xf) ->PrinF(Yf), h# (f)
=(hl(Xflb))f,
wherefEPrinF(XF)
and b =(prinF(Pf))(f).
Thenh# ,
g> is apairwise
map fromprinF(PF)
toprinF(qf).
The mor-phisms
of f aref-homotopy equivalences,
sohl(Xflb): Xf lb -> Yflb
is an
f-homotopy equivalence,
for all b E B. Hence the induced maph# lF(F, Xflb) : f(F, Xf lb) -> f(F, Yf lb),
wheref-+(hl(XFlb)j
forall b E
Bf,
is ahomotopy equivalence.
NowPrinF(Xf)
isweakly
con-tractible
(theorem 3.2)
andPrinF(Y F)
is contractible(proposition 3.1),
so
h#
is a weakhomotopy equivalence.
AlsoB F
andC F
arepath
con-nected
(theorem
3.2 and[Ma2, prop.7.1]).
It follows from the "ladder" of exacthomotopy
sequences associated with the Dold fibrationprinF(PF)
(lemma 4.1),
thequasi-fibration prinF(qF) (propopsition 3.1),
and thepairwise
maph# ,
g> ,that g
is a weakhomotopy equivalence.
A similar
argument, applied
to the ladder associated with thepair-
wise map
h ,
g> from PF to qjr, now shows that h is also a weakhomotopy equivalence.
(ii)
Iff(F)
E Wthen, using
theretraction B:F(F)’->f(F),
wesee that
7(Fl’
E W. SoC F
is in W[Ma2, prop.7.2].
Wealready
know that
BF
is aCW-complex,
so g is a weakhomotopy equivalence
between spaces in W and hence is a
homotopy equivalence [Sp, 7.6.24].
If the base space and fibres of a Hurewicz fibration are both in
W ,
then so also is the total space
[Sc, thm.2]. Any
map factors as thecomposite
of a Hurewicz fibration and ahomotopy equivalence;
if themap is a Dold
fibration,
then thehomotopy equivalence
is an FHE[Do, thm.6.1].
Hence theresult, just
stated forHurewicz
fibrationsand spaces in
W,
alsoapplies
when the fibrations arejust
assumedto
be Dold fibrations. NowPf: X f -> Bf
is anf-fibration,
so itis a Dold fibration
[Bo2, prop.4.3].
AlsoBT
is aCW-complex,
so ifF E W then
Xjr
E W. If alsof(F)
EW,
thenf(F)’
E W andYT
=B(*,.F(F)’, F)
E W[Ma2, prop.7.2].
So h is a weakhomotopy equivalence
between spaces in W and hence ahomotopy equivalence.
We have not shown that there is a universal f-fibration over
Cf
ingeneral,
however we do have thefollowing
result.Corollary
4.3(i)
There is abijection [D, Cf] -> fFHE(D)
that isnatural in
D,
where D E W .(ii) If f(F)
EW,
then there is a universalf-fibration
overC F.
Proof. (i)
It follows from[Sp, cor.7.6.23]
that the weakhomotopy equiv-
alence g :
Bj7 -+ CF
determines abijection
9#:[D, BF] -+ [D, dr] by
the rule
g# [f]
=[9 f],
where[f]
E[D, B f].
The result followsby
com-posing
the inverseof g#
with thebijection O(p F) : [D, B f] -> fFHE(D).
(ii)
Iff(F)
EW,
then g is ahomotopy equivalence. Taking
k to bea
homotopy
inverseof g,
then(p F) k : X fn Cf -> CT
is an f-fibration.Let k_ denote the
projection Xf
nC F -+ Xf.
We then have ane-pairwise
mapk_,
k> from(PJr)k
to p.F whichinduces, by
compo-sition,
apairwise
mapk-#,
k> :prinF((PF)k) -+prinF(PF).
NowPrinF(Xf)
isweakly contractible,
so it follows from the exact ho- motopy ladder associated withk-#
, k> thatPrinF(X F
flCf)
isweakly
contractible. Hence(PF) k
is universal.[Ma2,
thm.9.2(a)(ii)
and(b)(ii)]
are similar toparticular
cases of(ii) of
the lastcorollary,
with A= 0
in the former case and A = a onepoint
space in the latter-case.References
Bo1. P. I.
BOOTH, Equivalent homotopy
theories and groups of self-equivalences,
Lecture Notes in Math. vol. 1425(1990), 1-16, Springer-Verlag,
Berlin.Bo2. P. I.
BOOTH,
Local toglobal properties
in thetheory of fibrations,
Cahiers de
Topologie
et Géométrie DifférentielleCatégoriques,
XXXIV-2
(1993),
127-151.Bo3. P. I.
BOOTH,
Fibrations andclassifying
spaces: an axiomatic ap-proach I,
Cahiers deTopologie
et Géométrie DifférentielleCatégori-
ques, XXXIX
(1998),
83-116.Bo4. P. I.
BOOTH,
Fibrations andclassifying
spaces: an axiomatic ap-proach II,
Cahiers deTopologie
et Géométrie DifférentielleCatégori-
ques, XXXIX
(1998),
181-203.Bo5. P. I.
BOOTH,
Fibrations andclassifying
spaces: overview andexamples (to appear).
BHMP. P.
BOOTH,
P.HEATH,
C. MORGAN and R.PICCININI,
H-spaces of
self-equivalences
of fibrations andbundles,
Proc. LondonMath. Soc. 49
(1984),
111-124.BHP1. P. I.
BOOTH,
P. R. HEATH and R. A.PICCININI,
Fibre pre-serving
maps and functional spaces, Lecture Notes in Math. vol.673
(1978), 158-167, Springer-Verlag,
Berlin.BHP2. P. I.
BOOTH,
P. R. HEATH and R. A.PICCININI,
Characteriz-ing
universalfibrations,
Lecture Notes inMath.
vol. 673(1978),
168-184, Springer-Verlag,
Berlin.Do. A.
DOLD,
Partitions ofunity
in thetheory
offibrations,
Ann. ofMath. 78
(1963),
223-255.Ma1. J. P.
MAY,
Thegeometry
of iteratedloop
spaces, Lecture Notes inMathematics,
vol.271 (1972), Springer-Verlag,
Berlin.Ma2. J. P.
MAY, Classifying
spaces andfibrations,
Mem. Amer. Math.Soc.
vol.155, Providence,
1975.Ma3. J. P.
MAY,
Fibrewise localization andcompletion,
Trans. Amer.Math. Soc. 258
(1980),
127-146.Mc. M. C.
McCORD, Classifying
spaces and infinitesymmetric prod-
ucts, Trans. Amer. Math. Soc. vol. 146(1969),
273-298Sc. R.
SCHÖN,
Fibrations over aCWh-base,
Proc. Amer. Math.Soc. 62
(1977),
165-166.Sp.
E. H.SPANIER, Algebraic Topology, McGraw-Hill, NewYork,
1966.
V. R. M.
VOGT,
Convenientcategories
oftopological
spaces for ho-motopy theory,
Arch. Math 22(1971),
545-555.DEPARTMENT OF MATHEMATICS AND STATISTICS MEMORIAL UNIVERSITY OF NEWFOUNDLAND ST.