Theorem 7.1.There exists a simplicial closed model category structure on the category
of
simplicial spaces, called the Segal space model category
structure, with the following properties.
(1)
The cofibrations are precisely the monomorphisms.
(2)
The fibrant objects are precisely the Segal spaces.
(3)
The weak equivalences are precisely the maps such that
is a weak equivalence of spaces for every Segal
space .
(4)
A Reedy weak equivalence between any two objects is a weak
equivalence in the Segal space model category structure, and if both
objects are themselves Segal spaces then the converse holds.
Moreover, this model category structure is compatible with the
cartesian closed structure on in the sense of
Section 2.
Theorem 7.2.There exists a simplicial closed model category structure on the category
of
simplicial spaces, called the complete Segal space model category
structure, with the following properties.
(1)
The cofibrations are precisely the monomorphisms.
(2)
The fibrant objects are precisely the complete Segal spaces.
(3)
The weak equivalences are precisely the maps such that
is a weak equivalence of spaces for every
complete Segal space .
(4)
A Reedy weak equivalence between any two objects is a weak
equivalence in the complete Segal space model category structure, and if both
objects are themselves complete Segal spaces then the converse holds.
Moreover, this model category structure is compatible with the
cartesian closed structure on in the sense of
Section 2.
Proof.This is a direct consequence of the compatibility of these model
category structures with the cartesian closure, since any object is
cofibrant in either of these model category structures.
∎
We would like to understand the relationship between the model category
structures for Segal spaces and for complete Segal spaces.
We say a map of Segal spaces is a Dwyer-Kan
equivalence if
(1)
the induced map on homotopy
categories is an equivalence of categories, and
(2)
for each pair of objects the induced function on
mapping spaces
is a weak
equivalence.
For a Segal space let denote the set of objects of
modulo the equivalence relation of homotopy equivalence (or
equivalently, the set of isomorphism classes in ).
If we define a condition 1’ by
1’.
the induced map on equivalence
classes of objects is a bijection,
then it is not hard to see that conditions 1’ and 2 together are
equivalent to conditions 1 and 2.
Proof.It is clear that a Reedy weak equivalence between any two Segal spaces
is a Dwyer-Kan equivalence.
Conversely, suppose is a Dwyer-Kan equivalence
between complete Segal spaces. Then and by
(6.5), so that is a bijection. In the commutative diagram
the right-hand square is a homotopy pullback (since the induced maps
of fibers are of the form , which is
assumed to be a weak equivalence), and the
large rectangle is a homotopy pullback (since by
(6.4) the induced maps of
fibers are of the form , which is
also a weak equivalence). We conclude that is a
weak equivalence, and therefore that is a weak equivalence.
Since both and are Segal spaces, it follows that the map
is a
Reedy weak equivalence as desired.
∎
Theorem 7.7.Let be a map between Segal spaces. Then is a
Dwyer-Kan equivalence if and only if it becomes a weak equivalence in
the complete Segal space model category structure.
Remark 7.8. Note that if is a category, then the natural inclusion
of simplicial spaces is a Dwyer-Kan
equivalence; thus by (7.7) this map is a
weak equivalence in the complete Segal space model category structure.
Corollary 7.9.The homotopy category of complete Segal spaces may be obtained by
formally inverting the Dwyer-Kan equivalences in the homotopy category
of Segal spaces.