CROSSED SQUARES AND 2-CROSSED MODULES OF
COMMUTATIVE ALGEBRAS
ZEKER_IYA ARVAS_I
Transmitted by J. L. Loday
ABSTRACT. In this paper, we construct a neat description of the passage from
crossed squares of commutative algebras to 2-crossed modules analogous to that given by Conduche in the group case. We also give an analogue, for commutative algebra, of T.Porter's [13] simplicial groups to n-cubes of groups which implies an inverse functor
to Conduche's one.
Introduction
Simplicial commutative algebras play an important role in homological algebras, homo-topy theory and algebraic K-theory. In each theory, the internal structure has been studied relatively little. The present article intends to study the 3-types of simplicial algebras.
Crossed modules were initially dened by Whitehead (cf. [14]) as a model for 2-types. Conduche has dened a 2-crossed module as a model for 3-types. His unpublished work determines that there exists an equivalence (up to homotopy) between the category of crossed squares of groups and that of 2-crossed modules of groups. This construction was used by T.Porter in the work of n-Type of simplicial groups and crossed n-cubes, [13].
This result is true for the commutative algebra case.
In [3], we showed how to go from a simplicial algebra to a 2-crossed module of algebras and back to a truncated form of the simplicial algebra, and the link between simplicial algebras and crossed squares is explicitly given. It is natural for us to ask if the pas-sage from a crossed square to a simplicial algebra and hence a 2-crossed module can be performed.
The main points of this paper are thus:
i) to construct a functor from simplicial commutative algebras to crossed n-cubes
analogous to that given by T.Porter in the group case.
ii) to give a full description of the passage from a crossed square to a 2-crossed module of commutative algebras by using the Artin-Mazur \codiagonal" functor.
iii) to prove directly 2-crossed modules in a neat way.
Received by the editors 1997 May 20 and, in revised form, 1997 August 24. Published on 1997 October 5
1991 Mathematics Subject Classication : 18G30,18G55.
Key words and phrases: Simplicial Algebras, Crossed n-Cubes, Crossed Squares, 2-Crossed Modules. c
Zeker_iya Arvas_i 1997. Permission to copy for private use granted.
Acknowledgements
. The author wishes to thank Prof. T.Porter for useful conver-sations and the referee for helpful comments.1. Preliminaries
1.1. Simplicial algebras. Let
k
be a commutative ring with identity. We will use the term commutative algebra to mean a commutative algebra overk
: The category ofcommutative algebras will be denoted by
CA
.A simplicial (commutative) algebra
E
consists of a family of algebras fE ng together
with face and degeneracy maps d i =
d n i :
E n
! E n;1
; 0 i n, (n 6= 0) and s
i = s
n i :
E n
!E
n+1, 0
in, satisfying the usual simplicial identities given in Illusie
[10] for example. It can be completelydescribed as a functor
E
: op!
CommAlg
kwhere
is the category of nite ordinals [n] = f0<1<<ng and increasing maps. We will
denote the category of simplicial commutative algebras by
SimpAlg
. We have for eachk 0 a subcategory
k determined by the objects [
j] of with j k. A k-truncated
simplicial commutative algebra is a functor from (op
k) to
CommAlg
.Consider the product whose objects are pairs ([p];[q]) and whose maps are
pairs of weakly increasing maps. A functor
E.,.
: () op!
CommAlg
k is called a
bisimplicial algebra with value in
CommAlg.
To giveE.,.
is equivalent with giving for each (p;q) algebraEp;q and homomorphisms d
h i :
E p;q
!E p;1;q s
h i :
E p;q
!E p+1;q
i: 0;:::;p d
v j :
E p;q
!E p;q ;1 s
v j :
E p;q
!E p;q +1
j : 0;:::;q
such that the maps d h i
;s h
i commute with d
v j
;s v j and
d h i
;s h i (resp.
d v j
;s v
j) satisfy the usual
simplicial identities. Here d h i
;s h
i denote the horizontal operators and d
v j
;s v
j denote the
vertical operators.
By an ideal chain complex of algebras, (X ;d) we mean one in which each Imd i+1 is
an ideal of X
i. Given any ideal chain complex (
X ;d) of algebras and an integer n the
truncation, t n]
X ; of X at leveln will be dened by
(t n]
X) i =
8 < :
X
i if
i<n X
i =Imd
n+1 if i=n
0 if i>n:
The dierentiald of t n]
X is that of X for i <n; d
n is induced by the
nth dierential of X and all other are zero.
1.2. The Moore complex of simplicial algebra. We recall that given a simplicial
algebra
E
,the Moore complex (NE
;@) ofE
is the chain complex dened by(
NE
)n = n;1\
with @ n :
NE n
!NE
n;1 induced by d
n by restriction.
The nth homotopy module
n(
E) of Eis the n
th homology of the Moore complex of E,
i.e.,
n(
E)
= H
n(
NE;@) = n T i=0
Kerd n i
=d n+1 n+1(
n T i=0
Kerd n+1 i )
:
We say that the Moore complexNE of a simplicial algebra is oflength k if NE
n = 0 for
all nk+ 1 so that a Moore complex is of length k also of length r for r k:
A simplicial mapf :E!E
0 is called a n- equivalence if it induces isomorphisms
n( E)
=
n( E
0) for
n0:
Two simplicial algebrasEandE
0are said to be have the samen-type if there is a chain of n-equivalences linking them. A simplicial commutativealgebraEis ann-type if
i(
E) = 0
for i>n:
2. 2-crossed modules from simplicial algebras
Crossed modules techniques give a very ecient way of handling informations about on a homotopy type. They correspond to a 2-type (see [3]). As mentioned the above, Conduche, [5], in 1984 described the notion of 2-crossed module as a model for 3-types.
Throughout this paper we denote an action of r2R on c2C by rc:
Acrossed moduleis an algebra morphism@ :C !Rwith an action ofRonCsatisfying @(rc) = r @c and @(c)c
0 = cc
0 for all c;c
0
2 M;r 2 R: The last condition is called the
Peier identity. We will denote such a crossed module by (C ;R;@):Amorphismof crossed
modules from (C ;R;@) to (C 0
;R 0
;@
0) is a pair of
k-algebra morphisms, : C ! C 0
;
: R ! R
0 such that
(r c) = (r)(c): We thus get a category XMod of crossed
modules.
Examples of crossed modules: (i) any idealI inR gives an inclusion map, inc: I !R
which is a crossed module. Conversely given an arbitrary crossed module@ :C!R; one
can easily sees that the Peier identity implies that @C is an ideal in R: (ii) Given any R-module, M; one can giveM an algebra structure by giving it the zero multiplication.
With this structure the zero morphism 0 :M !R is a crossed module.
We recall from Grandjean and Vale [8] the denition of 2-crossed module:
A 2-crossed module of k-algebras consists of a complex of C
0-algebras C
2 @
2
-C 1
@ 1
-C
0
with@ 2
;@
1morphisms of C
0-algebras, where the algebra C
0 acts on itself by multiplication,
such that
C 2
@ 2
-C
1
is a crossed module in whichC
1 acts on C
2, (we require thus that for all
x 2C 2
; y 2C 1
and z 2C
0 that (
xy)z=x(yz)), further, there is a C
0-bilinear function giving f g:C
1
C0 C
1
;!C 2
called a Peier lifting, which satises the following axioms:
PL1 : @
2 fy
0 y
1
g = y 0
y 1
;y 0
@ 1(
y 1)
;
PL2 : f@
2( x
1) @
2( x
2)
g = x 1
x 2
;
PL3 fy
0 y
1 y
2
g = fy 0
y 1
y 2
g+@ 1
y 2
fy 0
y 1
g; PL4 : fy@
2(
x)g+f@ 2(
x)yg = @ 1(
y)x;
PL5 : fy
0 y
1
gz = fy 0
zy 1
g=fy 0
y 1
zg;
for allx;x 1
;x 2
2C 2
; y; y 0
; y 1
; y 2
2C 1 and
z 2C 0
:
A morphism of 2-crossed modules of algebras can be dened in a obvious way. We thus dene the category of 2-crossed module denoting it by
X
2Mod
.We denote the category of simplicial algebras with Moore complex of length n by
SimpAlg
n in the following.In [3], we studied the truncated simplicial algebras and saw what properties that has. Later, we turned to a simplicialalgebra
E
which is 2-truncated, i.e., its Moore complex look like:;!0;!NE 2
@ 2 ;!NE
1 @
1 ;!NE
0
and we showed the following result:
2.1. Theorem. The category
X
2Mod
of 2-crossed modules is equivalent to the categorySimpAlg
2 of simplicial algebras with Moore complex of length 2.That is, this result can be pictured by the following diagram:
SimpAlg
2C
(2)K
(2)X
2Mod
I@ @
@ @
@ t
2]
Tr
2SimpAlg
: 6where
Tr
2SimpAlg
denotes the category of 2-truncated simplicial algebras.3. Cat 2
-algebras and crossed squares
We will recall the denition (due to Ellis [7]) of a crossed square of commutative algebras.
A crossed square of commutative algebras is a commutative diagram
L
-M
N
0 ?
-R
together with actions of R on L, M and N. There are thus commutative actions of M on L and N via , and N acts on L and M via and a function h : MN !L; the h-map.
These data have to satisfy the following axioms: for allm;m0
2M; n;n 0
2N; r 2R; l 2
L; k2k;
1. each of the maps ; 0; ; 0 and the composite = 0 are crossed modules,
2. the maps;0 preserve the action of R,
3. kh(m;n) = h(km;n) = h(m;kn); 4. h(m + m0;n) = h(m;n) + h(m0;n);
5. h(m;n + n0) =h(m;n) + h(m;n0);
6. rh(m;n) = h(rm;n) = h(m;rn);
7. h(m;n) = mn;
8. 0h(m;n) = n m;
9. h(m;0l) = m l;
10. h(l;n) = nl:
In the simplest example of crossed squares (cf.[3]) and are ideal inclusions and L = M\N; with h being the multiplication map. We also mentioned that if
M\N
-M
N ?
-E
?
was a simplicial crossed square constructed from a simplicial algebraE and two simplicial
ideals M and N then applying
0 to the square gives a crossed square and that up to
isomorphism all crossed squares arise his way, see [3].
Although when rst introduced by Loday and Walery [9], the notion of crossed squares of groups was not linked to that of cat2-groups, it was in this form that Loday gave their
generalisation to an n-fold structure, catn-groups (see [11]).
We recall for low dimension Ellis equivalence between the category of crossedn-cubes and that of catn-algebras is given by Ellis (cf. [7]) it was not given an explicit description
in low dimensions. We now examine this for low dimensions.
Recall from [12] that a cat1-alg is a triple, (E;s;t); where E is an k-algebra and s;t
(ii) KersKert= 0:
It was shown in [12] that setting C =Kers; B =Imsand @ =tj C ;then the action of B on C within E makes
@ :C ;!B
into a crossed module. Conversely if @ : C ! B is a crossed module, then setting E =CoB and lettings;t be dened by
s(c;b) = (0;b)
and
t(c;b) = (0;@(c) +b)
for c2C ; b2B;then (E;s;t) is a cat
1-algebra.
For a cat2-algebra, we again have an algebra,
E; but this time with two independent
cat1-algebra structures on it. Explicitly:
A cat2-algebra is a 5-tuple ( E;s
1 ;t
1 ;s
2 ;t
2)
;where (E;s i
;t i)
;i = 1;2;are cat
1-algebras
and
s i
s j =
s j
s i
; t i
t j =
t j
t i
; s i
t j =
t j
s i
for i;j = 1;2; i6=j:
3.1. Proposition. There is an equivalence of categories between the category of cat 2
-algebras and thatof crossed squares.
Proof. The cat
1-algebra ( E;s
1 ;t
1) will give us a crossed module @ :C ;!B
with C =Kers; B =Ims and @ = t j C ; but as the two cat
1-algebra structures are
independent, (E;s 2
;t
2) restricts to give cat
1-algebra structures on
C and B and makes@
a morphism of cat1-algebras. We thus get a morphism of crossed modules
Kers 1
\Kers 2
- Im s
1
\Kers 2
Kers 2
\Ims 1 ?
- Im s
1 \Ims
2 ?
where each morphism is a crossed module for the natural action, i.e. multiplication in
E: It remains to produce an h-map, but it is given by the multiplication within E since
if x 2Kers 2
\Ims 1 and
y 2Ims 2
\Kers 1 then
xy 2Kers 1
\Kers 2
: It is easy to check the
crossed squares axioms. Conversely, if
L
-M
?
is a crossed square, then we can think of it as a morphism of crossed modules
L M
-N?
R:?
Using the equivalence between crossed modules and cat1-algebras this gives a morphism
@ : (LoN;s;t);!(M oR;s 0;t0)
of cat1-algebras. There is an action of (m;r)
2M oR on (l;n)2LoN given by
(m;r)(l;n) = (rl + @ml + h(m;n);rn + mn):
Using this action, we thus form its associated cat1-algebra with big algebra (L
oN)o
(M oR) and induced endomorphisms s
1;t1;s2;t2:
4. Crossed n-cubes and simplicial algebras
Crossed n-cubes in algebraic settings such as commutative algebras, Jordan algebras, Lie algebras have been dened by Ellis [7].
A crossed n-cube of commutative algebras is a family of commutative algebras,MA for
A < n >= f1;:::;ng together with homomorphisms i : MA
! M
A;fig for i
2< n >
and for A;B< n >, functions
h : MA
M
B
;!M A[B
such that for all k 2k; a;a 0
2M A; b;b
0 2M
B; c 2M
C; i;j
2< n > and AB
1) ia = a if i
62A
2) ija = jia
3) ih(a;b) = h(ia;ib)
4) h(a;b) = h(ia;b) = h(a;ib) if i
2A\B
5) h(a;a0) = aa0
6) h(a;b) = h(b;a)
7) h(a + a0;b) = h(a;b) + h(a0;b)
8) h(a;b + b0) = h(a;b) + h(a;b0)
9) kh(a;b) = h(ka;b) = h(a;kb)
10) h(h(a;b);c) = h(a;h(b;c)) = h(b;h(b;c)):
A morphism of crossed n-cubes is dened in the obvious way: It is a family of com-mutative algebra homomorphisms, for A< n >; f
A :MA
;! M 0
A commuting with the
i's andh's. We thus obtain a category of crossed n-cubes denoted by Crs
Examples. (a) For n= 1; a crossed 1-cube is the same as a crossed module.
(b) For n= 2; one has a crossed square:
M <2>
2
-M
f1g
M f2g
1 ?
2
-M
; : ?
1
Each
i is a crossed module as is
1
2. The
h-functions give actions and a pairing h:M
f1g
M
f2g
;!M <2>
:
The maps 2 (or
1) also dene a map of crossed modules. In fact a crossed square can
be thought of as a crossed module in the category of crossed modules. (c) Let
E
be a simplicial algebra. Then the following diagramNE 2
=@ 3
NE 3
-NE 1
NE 1
0 ?
@
-E 1 ?
@ 0
is a crossed square. Here NE
1 =Ker d
1 0 and
NE
1 =Ker d
1 1.
SinceE
1acts on NE
2 =@
3 NE
3 ; NE
1and NE
1
;there are actions ofNE 1on
NE 2
=@ 3
NE 3
andNE 1 via
@;andNE
1 acts on NE
2 =@
3 NE
3 and NE
1 via @
0
:As@ and@
0are inclusions,
all actions can be given by multiplication. The h-map is NE
1
NE 1
;! NE 2
=@ 3
NE 3
(x;y) 7;! h(x;y) =s 1
x(s 1
y;s 0
y) +@ 3
NE 3
;
which is bilinear. Here x and y are in NE
1 as there is a natural bijection between NE
1
and NE
1 (by lemma 2.3.1 in [2]). The element
yis the image of yunder this. The reader
is referred to the author's thesis, [2], for verifying of the crossed square axioms. This last example eectively introduces the functor
M
(;;2
) :SimpAlg
-
Crs
2:
This is the 2-dimensional case of a general construction to which we turn next. By an ideal (n+ 1)-ad will be meant an algebra with n selected ideals (possibly with
repeats), (R;I 1
Let R be an algebra with ideals I 1
;:::;I n of
R. Let M
A = T
fI i :
i2Ag and M ; =
R
with A<n >:Ifi2<n >;thenM
A is an ideal of M
A;fig: Dene
i : M
A
;!M A;fig
to be the inclusion. If A;B <n >, then M A[B =
M A
\M B
;let h: M
A
M
B
;! M A[B
(a;b) 7;! ab
as M A
M B
M
A \M
B
; where a 2 M A
; b 2 M B
: Then fM A :
A < n >; i
; hg
is a crossed n-cube, called the inclusion crossed n-cube given by the ideal (n+ 1)-ad of
commutative algebras (R; I 1
;:::;I n)
: 4.1. Proposition. Let (E; I
1 ;:::;I
n) be a simplicial ideal (
n+ 1)-ad of algebras and
dene for A<n>
M A =
0
\ i2A I
i
with homomorphisms i :
M A
!M
A;fig and h-maps induced by the corresponding maps
in the simplicial inclusion crossed n-cube, constructed by applying the previous example to each level. Then fM
A :
A<n >; i
; hg is a crossed n-cube.
The proof is straightforward and so has been omitted.
Up to isomorphism, all crossed n-cubes arise in this way. In fact any crossed n-cube
can be realised (up to isomorphism) as a
0of a simplicialinclusion crossed
n-cube coming
from a simplicial ideal (n+ 1)-ad in which
0 is a non-trivial homotopy module.
In 1991, T. Porter described a functor, [13], from the category of simplicial groups to that of crossed n-cubes of groups, based on ideas of Loday. Here, we adapt that
description to give an obvious analogue of this functor for the commutative algebra case. The functor here constructed is dened using the decalage functor studied by Illusie [10] and Duskin [6] and is a
0-image of a functor taking values in a category of simplicial
ideal (n+ 1)-ads.
Thedecalage functor forgets the last face operators at each level of a simplicial algebra
E and moves everything down one level. It is denoted by Dec. Thus
(DecE) n =
E n+1
:
The last degeneracy ofEyields a contraction of Dec 1
Eas an augmented simplicialalgebra,
Dec1
E'K(E 0
;0);
by an explicit natural homotopy equivalence (cf. [6]). The last face map will be denoted
0 : Dec 1
Iterating the Dec construction gives an augmented bisimplicial algebra
[:::Dec 3
E
-- Dec
2
E
0
1 -Dec
1
E
]which in expanded form is the total decalage of
E:
[::: Dec 3
E
--Dec
2
E
0
1
- Dec 1
E
]0
-
E
:(
see [6] or [10] for details). The maps from DeciE
to Deci;1E
coming from thei last face
maps will be labelled 0
;:::;
i;1 so that
0 = d
last ;
1 = d
last butone and so on.
For a simplicial algebra
E
and a given n, we writeM
(E
, n) for the crossed n-cube,arising from the functor
M
(;;n
) :SimpAlg
;!Crs
n;
which is given by
0(Dec
E
;Ker0
;:::;Ker n;1)
: The following propositions and their
proofs aim to explore this compressed denition, giving an `elementary' specication of the construction.
4.2. Proposition. If
E
be a simplicial algebra, then the crossed n-cubeM
(E
,n) isde-termined by:
(i) for A <n >;
M
(E
;n) A =T
j2AKer d
n j;1 d
n+1 n+1(Ker
d n+1 0
\f T
j2AKer d
n+1 j
g);
(ii) the inclusion
\ j2A
Kerd n j;1
;! \ j2A;fig
Kerd n j;1
induces the morphism
i :
M
(E
;n)A
;!
M
(E
;n) A;fig;(iii) the functions, for A;B <n>;
h:
M
(E
;n) AM
(E
;n) B;!
M
(E
;n) A[Bgiven by
h(x;y) =xy ;
where an element of
M
(E
;n)A is denoted by
x with x2 T
j2AKer d
n j;1
Proof. First some explanation of the denition of M(;;n) as
0(Dec
E
; Ker0
; :::; Ker n;1)
:
For each simplicial algebra,
E
;we start by looking at the canonical augmentation map 0:Dec1
E
;!
E
; which has kernel the simplicial algebra, Kerdlast mentioned above. Then
take the simplicial inclusion crossed module Ker 0
;! Dec
1
E
to beM(
E
;1) deningthus a functor
M( ;1) :
SimpAlg
;!Simp
(IncCrs
1):
Then it is easy to show that
0(Ker
0)
;! 0(Dec
1
E
)is precisely
M
(E
;1): The higher order analoguesM
( ;n) are as follows:For each simplicial algebra,
E
, there is a functorial short exact sequence Ker0
-Dec 1
E
0
-
E
:This corresponds to the 0-skeleton of the total decalage of
E
;[:::Dec 3
E
-- Dec
2
E
0
1 - Dec
1
E
]0 -
E
:
Forn = 2; the 1-skeleton of that total decalage gives a commutative diagram
Dec2
E
0 - Dec
1
E
Dec1
E
1 ?
0
-
E
: ?0
Here 1 is
d n
n;1 in dimension
n whilst 0 is
d n n
: Forming the square of kernels gives
Ker 0
\Ker 1
-Ker
1
Ker 0 ?
- Dec 2
E
: ?
Again,
0 of this gives
M
(E
;2): In general, we use the (n ; 1)-skeleton of the total
decalage to form an n-cube and thus a simplicial inclusion crossed n-cube corresponding
to the simplicial ideal (n+ 1)-ad
(Decn
E; Ker n;1
; :::; Ker 0)
This simplicial inclusion n-cube will be denoted by M(E;n), and its associated crossed n-cube by
0(
M(E;n)) =M(E;n):
The result now follows by direct calculation on examining the construction of
0 as the
zeroth homology of the Moore complex of each term in the inclusion crossedn-cube,M(E, n).
4.3. Lemma. If E is a simplicial algebra with A<n>; A6=<n >; then
d n
\ i2A
Kerd n i
= \
i2A
Kerd n;1 i;1
:
Proof. Ifi 2A; then
d n
\ i2A
Kerd n i
\ i2A
Kerd n;1 i;1
;
since d i;1
d n =
d n;1
d i;1
:
Conversely, we suppose that xis an element in T
i2AKer d
n;1
i;1 and consider the element y=s
n x;s
n;1
x+:::+ (;1) n;k
s k
x= n;k X i=0
(;1) i+1
s i+k
x;
where k is the rst integer in < n > nA: Then d n
y = x and d i
y = 0for all i 2 A and
hence y2 T
i2AKer d
n
i implies x2d
n( T
i2AKer d
n
i) as required.
This lemma gives the following proposition:
4.4. Proposition. If E is a simplicial algebra, then
i) for A<n>; A6=<n>;
M(E;n) A
= \
i2A
Kerd n;1 i;1
so that in particular, M(E;n) ;
=E
n;1; in every case the isomorphism is induced by d
n ;
ii) if A6=<n >and i2<n>;
i :
M(E;n) A
;!M(E;n) Anfig
is the inclusion of an ideal, iii) for j 2<n>;
j :
M(E;n) <n>
;! \ i6=j
Kerd n+1 i
is induced by d n
Proof. By proposition 4.2 and the previous lemma, one can obtain, for A 6=<n>; M(E;n)
A = T i2AKer d n i;1 d n+1 (Kerd
n+1 0 \f T i2AKer d n+1 i g) = T i2AKer d n i;1 Kerd n 0 \( T i2AKer d n i;1 ):
The epimorphism d n :
E n
! E
n;1, which is split, d
n s
n;1 = id, can be restricted to an
epimorphism \ i2A Kerd n i;1 ;! \ i2A Kerd n;1 i;1 ;
by lemma 4.3 It follows then that Ker \ i2A Kerd n i;1 d n ;! \ i2A Kerd n;1 i;1
= Kerd n 0 \ \ i2A Kerd n i;1 :
which completes the proof of (i):
(ii) and (iii) are now consequences.
Expanding this out for low values of n gives:
1) For n= 0, M(E;0) =E 0 =d 1(Ker d 0) = 0(
E) =H 0(
E):
2) For n= 1; M(E;n) is the crossed module
1 : Ker d 1 0 =d 2 2( NE 2) !E 1 =d 2 2(Ker d 2 0) :Since d 2 2( NE
2) =Ker d 1 0Ker d 1 1
;this implies :NE
1 =Kerd
1 0Ker
d 1 1
;!E 0
:
3) For n= 2; M(E;n) is
Kerd 2 0
\Kerd 2 1 =d 3 3(Ker d 3 0
\Kerd 3 1
\Kerd 3 2) 2 - Ker d 2 0 =d 3 3(Ker d 3 0
\Kerd 3 1) Kerd 2 1 =d 3 3(Ker d 3 0
\Kerd 3 2) ? 1 2 -E 2 =d 3 3(Ker d 3 0) : ? 1
By proposition 4.4, this is isomorphic to
Here the h-map is
h : Kerd1 0
Kerd 1 1
;!NE 2=d
3 3(NE
3)
given by
h(x;y) = s1x(s1y ;s
0y) + @3NE3:
where x;y2NE 1:
5. 2-crossed modules from crossed squares
Conduche constructed (in a letter to R.Brown in 1984) the 2-crossed module from a crossed square
L - M
N 0
?
-R
?
as
L (;;
0) - M
oN +
- R:
This construction can be briey described as follows: apply the nerve in the both directions so as to get a bisimplicial algebra, then apply either the diagonal or the Artin-Mazur `codiagonal' functor to get to a simplicial algebra and take the Moore complex.
We saw above the category of crossed modules is equivalent to that of cat1-algebras.
Ellis (cf. [7]) generalised this equivalence to the dimensionn; i.e., the equivalence between crossed n-cubes and catn-algebras.
We form the associated cat2-algebra. This is
(LoN)o(M oR) s
-t-N oR
M oR
s0 ??
t0
sM
-tM
- R:
sN ??
tN
The source and target maps are dened as follows:
s((l;n);(m;r)) = (n;r) t((l;n);(m;r)) = (0l + (m)n;(m) + r)
s0((l;n);(m;r)) = (m;r) t0((l;n);(m;r)) = (l + m;(n) + r)
sM(m;r) = r tM(m;r) = (m) + r
for l2L;m 2M;n2N and r2R:
We now take the binerve, that is the nerves in the both directions of the cat2-algebra
constructed. This is a bisimplicial algebra. The rst few entries in the bisimplicial array are given below (where AB:=A
oB)
--(L
N) o((L
N) o(M
R))
-- N o(N oR)
((LL)
oN)o((M M)
oR) ???
-- (L
N) o(M
R) ???
--N
oR ???
M o(MoR) ??
-- M
oR ??
--R
??
Some reduction has already been done. For example, the double semi-direct product represents the algebra of pairs of elements ((m1;r1);(m2;r2))
2 M oR where (m 1) +
r1 = r2: This is the algebra M
o(M oR) where the action is M oR on M given by
(m;r)m
0= (m + r)m0:
We will recall the `Artin-Mazur' codiagonal functor r (cf. [1]) from bisimplicial
alge-bras to simplicial algealge-bras.
Let E.,. be a bisimplicial algebra. Put
E(n) = M p+q =n
Ep;q
and dene r n
E
(n) as follows: An element (x
0;:::;xn) of E
(n) with x p
2 E
p;n;p is in r
n if and only if
dv 0x
p =d h p+1x
p+1 for p = 0;:::;n ;1:
Next, dene the faces and degeneracies Dj :
r n
!r n;1
Sj : r
n !r
n+1 j = 0;:::;n
by
Dj(x) = (d v jx
0;d v j;1x
1;:::;d v 1x
j;1;d h jx
j+1;d h jx
j+2;:::;d h jx
n)
Sj(x) = (s v jx
0;s v j;1x
1;:::;s v 0x
j;1;s h jx
j;s h jx
j+1;:::;s h jx
n):
Thus r(E:;:) =fr
n:Dj;Sj
g is a simplicial algebra.
We now examine this construction in low dimensions:
Example: Forn = 0;E(0)=E
0;0: For n = 1; we have r
1 E
(1)=E1;0 E
where
r 1 =
(e1;0;e0;1) :d h 0e
1;0=d v 1e
0;1
together with the homomorphisms D1
0(e
1;0;e0;1) = (d v 0e
1;0;d h 0e
0;1)
D1 1(e
1;0;e0;1) = (d v 1e
1;0;d h 1e
0;1)
S0 0(e
0;0) = (s v 0e
0;0;s h 0e
0;0):
Forn = 2; we have
r 2
E (2)=
M p+q =2
Ep;q =E2;0 E
1;1 E
0;2
where
r 2 =
(e2;0;e1;1;e0;2) :d h 0e
2;0=d v 1e
1;1; d h 0e
1;1=d v 2e
0;2 :
We use the `Artin-Mazur' codiagonal functor to obtain a simplicial algebra A(of some
complexity);
The base algebra is still A0
= R: However the algebra of 1-simplices is subset of E1;0
E
0;1= (M
oR)(N oR);
consisting of elements ((m;r);(n;r0)) where (m) + r = r0; i.e.,
A1 =
f((m;r);(n;r
0)) :(m) + r = r0 g:
Let us see what the composite of two such elements
((m1;(m1) +r1);(n1;r1))and ((m2;(m2) +r2));(m2;r2))
becomes:
((m1;(m1) +r1);(n1;r1)) ((m
2;(m2) +r2));(m2;r2))
= (m1;(m1) +r1) (m
2;(m2) +r2) ((n
1;r1) (m
2;r2))by the inter-change law
= ((m1m2+m1((m2) +r2) +m2((m1) +r1);((m1) +r1)((m2) +r2));
n1n2+n1r2+n1r1;r1r2):
This means that the subalgebraA1 is M
o(N oR) where the action of NoR on M via
R is the obvious one. Thus A1
= M o(N oR) =f(m;n;r) : m2M;n2N;r2Rg:
We next turned to the algebra of 2-simplices which is the subset A2 of
E2;0 E
1;1 E
0;2= (M
o(M oR))((LoN)o(M oR))(N o(N oR));
whose elements ((m2;m1;r);(l;n;m;r 0);(n
2;n1;r
00)) are such that (m
2;m1+r) = (m;r 0)
and (0l + n;m + r0) = (n 1;r
By similar calculation given above, the composition of two such elements ((m2;m1;r);((l;n);(m2;m1+r));(n2;(
0
l + n;m + r0)))
and
((m0 2;m
0 1;r
1);((l
0;n0);(m0 2;m
0 1+r
1));(n 0 2;(
0l0+n0;m0+r0 1)))
becomes such an element (
l
;m
;n
;r
)2Lo(M o(N oR)) wherel
2L;m
2M;n
2 Nand
r
2R: This is the algebra Lo(Mo(N oR)) where the action of M o(N oR) onL is the obvious one. Thus
A2
= Lo(M o(NoR)):
Therefore we can get a 2-truncated simplicial algebra
A
(2) that looks likeA
(2) : Lo(M o(N oR))
d2 0;d
2 1;d
2 2
s1 0;s
1 1
M o(N oR)
d1 0;d
1 1
s0 0
R:
with the faces and degeneracies d1
0(m;n;r) = r
d1
1(m;n;r) = (m) + r
0 where r0 =(n) + r
s0
0(r) = (0;n;r)
and
d2
0(l;m;n;r) = (m;n;r)
d2
1(l;m;n;r) = (m;n;r)
d2
2(l;m;n;r) = (
;(l) + m;
0(l) + n;(m) + r0); where r0=(n) + r
s1
0(m;n;r) = (0;m;n;r)
s1
1(m;n;r) = (0;m;n;r):
Loday,[11], dened a mapping cone of a complexwhich is analogous to the construction of the Moore complex of a simplicial group. One can easily give an obvious description for commutative algebras.
We next give a mapping cone of a crossed square of algebras as follows:
5.1. Proposition. The Moore complex of the simplicial algebra
A
(2) is the mapping
cone, in the sense of Loday, of the crossed square. Furthermore, this mapping cone complex has a structure of 2-crossed module of algebras.
Proof. Given the 2-truncated simplicial algebra
A
(2) described the above and look at its
Moore complex:
Of course NA0 = A0
= R: The second term of the Moore complex is NA1 =Kerd0:
The d0 map is d0 on N
oR; that is it picks out the point r; i.e., d
0(n;r) = r: Thus
the kernel of d0 is the subalgebra of M
M oN = NA
1 =Kerd0: The map d1 jKer
d0 is d
1(m;n;0) = (m) + (n): This is d1 on
M oR; which is (m) + r
0 where r0 =(n) + r; and of course r = 0:
It is not hard to see that the kernel ofd0 andd1 is the subalgebra ofL
o(Mo(NoR))
where m = 0; n = 0; r = 0: This is the algebra L: In other words NA2 = L: The map
d2 jKer
d 0
\Kerd 1 is
d2(l;0;0;0) = ( ;l;
0
l;0); This is @2 =d2 on L; which is, @2l = (
;l; 0l):
Next we will see that @1@2 = 0;
@1@2(l) = @1( ;l;
0l)
= (;l) +
0l
= ;(l) + (l) by =
0
= 0: Thus, if given a crossed square
L - M
N 0
?
-R
?
then its mapping cone is
L @2
-M
oN @ 1
- R
where @1(m;n) = (m) + (n) and @2l = ( ;l;
0l):
Now we will show the second part of the proof of result:
The semi-direct product M oN can be formed by making N act on M via R;
nm = (n)m
where theR-action is the given one. The fact that @2 and@1 are algebra homomorphisms:
(m;n)(m0;n0) = (n m
0+n0
m + mm
0;nn0)
= ((n)m0+(n0)m + mm0;nn0)
Thus, (i)
@1((m;n)(m
0;n0)) = @
1((n)m
0+(n0)m + mm0;nn0)
= ((n)m0+(n0)m + mm0) +(nn0)
= (n)(m0) +(n0)(m) + (m)(m0) +(n)(n0)
= ((m) + (n))((m0) +(n0))
and similarly of course
@1((m;n) + (m
0;n0)) = @
1(m + m
0;n + n0)
= (m + m0) +(n + n0)
= ((m) + (n)) + ((m0) +(n0))
= @1(m;n) + @1(m 0;n0)
(ii) ifl1;l2
2L; then
@2(l1l2) = ( ;(l
1l2); 0(l
1l2))
= (;(l
1l2); 0(l
1) 0(l
2))
whilst
@2(l1)@2(l2) = ( ;l
1; 0l
1)( ;l
2; 0l
2)
= ((0l 1)
(;l
2) + ( 0l
2) (;l
1) + ( ;l
1)( ;l
2); 0(l
1) 0(l
2))
but 0 =; so the rst coordinates are equal. Similarly
@2(l1+l2) = ( ;(l
1+l2); 0(l
1+l2))
= (;l 1;
0l 1) + (
;l 2;
0l 2):
= @2(l1) +@2(l2):
These elementarycalculations are useful as they pave the way for calculation of the Peier multiplication of x = (m;n) and y = (c;a) in the above complex:
hx;yi = @ 1x
y;xy
= ((m) + (n))(c;a);(m;n)(c;a)
= (((m) + (n))c;((m) + (n))a);(nc + am + mc;na)
= (am;((m) + (n))a;na) since any dependence on cvanishes
= ((a)m;(m)a + (n)a;na) by denition of action
= ((a)m;(m)a + na;na) since is a crossed module
= ((a)m;(m)a): Thus the Peier lifting
f g: (MoN)(M oN);!L
for this structure is given by
fxyg=h(m;na):
It is immediate that this works: @2
fxyg = (;h(m;na);
0h(m;na))
= ((;m)na;(na)m)
= (;(na)m;(m)(na))
We will not check all the axioms for a 2-crossed module for this structure, but will note the proof for two or three of them as it illustrates the connection between theh-map and the Peier lifting.
PL2: f@ 2(l0)
@ 1(l1)
g =l 0l1:
As @2l = ( ;l;
0l); this needs the calculation of
h(;l 0;
0
(l0l1))
but the crossed square axiomh(l;n) = nl; and h(m;
0l) = m
l; together with the fact
that the map : L!M is a crossed module give: f@
2(l0) @
1(l1)
g = f(;l 0;
0l 0)
(;l 1;
0l 1)
g
= h(;l 0;
0(l 0l1))
= ;l
0 (l
0l1)
= l0l1 PL3: fy
0 y
1y2
g=fy 0
y 1y2
g+@ 1y2
fy 0
y 1y2
g , where y
0 = (m0;n0); y1 = (m1;n1)
and y2 = (m2;n2)
2M oN fy
0 y
1y2
g = f(m 0;n0)
(m
1;n1)(m2;n2) g
= f(m 0;n0)
(n 1
m 2 +n2
m
1+m1m1;n1n2) g
= h(m0;n0n1n2)
whilst
fy 0
y 1y2
g+@ 1y2
fy 0
y 1y2
g=f(m
0;n0)(m1;n1) (m
2;n2) g
+@1y2 f(m
0;n0) (m
1;n1)(m2;n2) g
=h(n0 m
1 +n1 m
0;n0n1(n2)) +h(m0;@1y2 (n
0n1))
and this simplies as expected to give the correct result.
PL4: fx@
2l g+f@
2l
xg = f(m;n)(;l; 0l)
g+f(;l; 0l)
(m;n)g
= h(m;n0l) + h( ;l;
0(l)n)
= h(m;0(n
l)) + h(;l; 0(n
l)) by
0 cros. mod.
= ((m) + (n))l
= @1(m;n) l
= @1x l
We thus have two ways of going from simplicial algebras to 2-crossed modules (i) directly to get
NE2
@2NE3
;!NE 1
;!NE 0;
(ii) indirectly via the square axiomM(E;2) and then by the above construction to get
NE2
@2NE3
;!Kerd 0
oKerd 1
and they clearly give the same homotopy type. More preciselyE
1 decomposes as Ker d
1 o s
0 E
0 and the Ker d
0 factor in the middle term of (ii) maps down to that in this
decompo-sition by the identity map. Thus d
0 induces a quotient map from (ii) to (i) with kernel
isomorphic to
0;!Kerd 0
=
;!Kerd 0
which is thus contractible.
Remark. The situation in this paper can be summarised in the following diagram:
SimpAlg
2; ;
; ;
;
M
(;;2
)Crs
2( )2 -
X
2
Mod
;K
(2)6 ?
C
(2)where ( )2 is given by Proposition 5.1. The diagram is commutative, linking the
con-structions of section 4 and 5 with those given here.
References
[1] M. Artin and B. Mazur. On the Van Kampen theorem, Topology,
5
, 179-189 (1966).[2] Z. Arvasi.Applications in commutativealgebra of the Moore complexof a simplicial
algebra, Ph.D. Thesis, U.C.N.W. Maths Preprint, 94.09.
[3] Z. Arvasiand T. Porter. Freeness conditions for 2-crossed modules of
commuta-tive algebras, Applied Categorical Structures, (to appear).
[4] R. BrownandJ-L. Loday. Van Kampen theorems for diagram of spaces,Topology
26
(1987) 311-335.[5] D. Conduche.Modules croises generalises de longueur 2, J. Pure Applied Algebra,
34
(1984), 155-178.[6] J. Duskin.Simplicial methods and the interpretation of triple cohomology,Memoirs A.M.S. Vol. 3
163
(1975).[7] G.J. Ellis. Higher dimensional crossed modules of algebras. J. Pure and Appl. Algebra
52
(1988) 277-282.[8] A.R. GrandjeanandM.J. Vale.2-Modulos cruzados en la cohomologia de
[9] D. Guin-Walery and J.L. Loday. Obstructions a l'excision en K-theories
algebrique. In: Friedlander, E.M.,Stein, M.R.(eds.) Evanston conf. on algebraic K-theory 1980. (Lect. Notes Math., vol. 854, pp. 179-216) Berlin Heidelberg New York: Spinger 1981.
[10] L. Illusie. Complex cotangent et deformations, I, Lectures Notes in Math. 239
(1971); II, 283 (1972).
[11] J.L. Loday. Spaces with nitely many non-trivial homotopy groups. J. Pure and
Appl. Algebra 24 (1982) 179-202.
[12] T. Porter. Homology of commutative algebras and an invariant of Simis and
Vas-conceles.J.Algebra 99 No:2 (1987).
[13] T. Porter. n-Type of simplicial groups and crossed n-cubes. Topology 32 5-24
(1993).
[14] J.H.C. Whitehead. Combinatorial homotopy. Bull. Amer. Math. Soc 55 (1949)
453-496.
Department of Mathematics Faculty of Science
Osmangazi University 26480, Eskisehir Turkey
Email: zarvasi@mail.ogu.edu.tr
This article may be accessed via WWW athttp://www.tac.mta.ca/tac/ or by anonymous
signicantly advance the study of categorical algebra or methods, or that make signicant new contribu-tions to mathematical science using categorical methods. The scope of the journal includes: all areas of pure category theory, including higher dimensional categories; applications of category theory to algebra, geometry and topology and other areas of mathematics; applications of category theory to computer science, physics and other mathematical sciences; contributions to scientic knowledge that make use of categorical methods.
Articles appearing in the journal have been carefully and critically refereed under the responsibility of members of the Editorial Board. Only papers judged to be both signicant and excellent are accepted for publication.
The method of distribution of the journal is via the Internet toolsWWW/ftp. The journal is archived
electronically and in printed paper format.
Subscription information. Individual subscribers receive (by e-mail) abstracts of articles as they are published. Full text of published articles is available in .dvi and Postscript format. Details will be e-mailed to new subscribers and are available byWWW/ftp. To subscribe, send e-mail totac@mta.ca
including a full name and postal address. For institutional subscription, send enquiries to the Managing Editor, Robert Rosebrugh,rrosebrugh@mta.ca.
Information for authors. The typesetting language of the journal is TEX, and LATEX is the
preferred avour. TEX source of articles for publication should be submitted by e-mail directly to an appropriate Editor. They are listed below. Please obtain detailed information on submission format and style les from the journal's WWW server at URL http://www.tac.mta.ca/tac/ or by anonymous ftp
fromftp.tac.mta.ca in the directorypub/tac/info. You may also write totac@mta.ca to receive details
by e-mail.
Editorial board.
John Baez, University of California, Riverside: baez@math.ucr.edu
Michael Barr, McGill University: barr@triples.math.mcgill.ca
Lawrence Breen, Universite de Paris 13: breen@math.univ-paris13.fr
Ronald Brown, University of North Wales: r.brown@bangor.ac.uk
Jean-Luc Brylinski, Pennsylvania State University: jlb@math.psu.edu
Aurelio Carboni, Universita della Calabria: carboni@unical.it
P. T. Johnstone, University of Cambridge: ptj@pmms.cam.ac.uk
G. Max Kelly, University of Sydney: kelly m@maths.su.oz.au
Anders Kock, University of Aarhus: kock@mi.aau.dk
F. William Lawvere, State University of New York at Bualo: mthfwl@ubvms.cc.bualo.edu
Jean-Louis Loday, Universite de Strasbourg: loday@math.u-strasbg.fr
Ieke Moerdijk, University of Utrecht: moerdijk@math.ruu.nl
Susan Nieeld, Union College: nieels@gar.union.edu
Robert Pare, Dalhousie University: pare@cs.dal.ca
Andrew Pitts, University of Cambridge: ap@cl.cam.ac.uk
Robert Rosebrugh, Mount Allison University: rrosebrugh@mta.ca
Jiri Rosicky, Masaryk University: rosicky@math.muni.cz
James Stashe, University of North Carolina: jds@charlie.math.unc.edu
Ross Street, Macquarie University: street@macadam.mpce.mq.edu.au
Walter Tholen, York University: tholen@mathstat.yorku.ca
Myles Tierney, Rutgers University: tierney@math.rutgers.edu
Robert F. C. Walters, University of Sydney: walters b@maths.su.oz.au