231-279. [2] Charles Ehresmann, "Les connexions infinitesimales dans un espace ... Bruxelles, 1950, 29-55 (Georges Thone, Liege; Masson, Paris;. 1951).
BULL. AUSTRAL. MATH. SOC. VOL. 25 ( 1 9 8 2 ) ,
I8FI5,
58AI5
357-386.
DIFFERENTIAL FORMS WITH VALUES IN GROUPS ANDERS KOCK
In the context of synthetic differential geometry, we present a notion of differential form with values in a group object, typically a Lie group or the group of all diffeomorphisms of a manifold.
Natural geometric examples of such forms and the role
of their exterior differentiation is given.
The main result is a
comparison with the classical theory of Lie algebra valued forms.
In synthetic differential geometry, one encounters formal manifolds, and in these it makes sense to talk about two points being neighbours [JO]. In terms of this neighbour notion, it makes sense to talk about differential forms with values in a group
G . This is equivalent to a
classically considered notion of Lie algebra valued differential form (namely with values in the Lie algebra of
G ) , and the comparison between
these two notions is the main result presented here. definition of coboundary of
0-
and
However, the
1-forms with values in
G
is, both
from the analytic and geometric viewpoint, more natural than the classical Lie algebra valued notions. group
G
Thus, the Maurer-Cartan form
appears as the coboundary of the identity map of
zero-form).
In particular, it is closed,
Q G
for a Lie (which is a
dQ. = 0 , and this can be
reinterpreted as the Maurer-Cartan formula. Also, the two well known lemmas (cf. , for example, [6] or [4]) Received 12 November 1981. This research was partially supported by the Australian Research Grants Committee. A preliminary report on some of the results is printed in Cahiers Topologie Geom. Diffeventielle 22 (1981), 11*1-11(8. 357
358
Anders Kock
concerning maps from connected and simply connected manifolds into a Lie group-become just the statements that where H
H
H (M, G) = G
denotes "deRham cohomology with values in
(which can be expressed:
"closed
(z, x) • u>{y, z) • m(x, y) ,
(1.2) where
• denotes the multiplication of the value group.
(We choose the
ordering in (1.2) rather than the more forward-looking w(x, y) • u(y, z) • u(z, x) , because we want the value groups to be transformation groups which act from the left.)
The element (1.2) is denoted
du>(x, y, s) .
In fact,
du> is a
2-form with values in the group in question, and its vanishing (that is, having
e
as its only value) means precisely that integrating
any triangle (l.l) gives
w
around
e .
If we can perform the passage from infinitesimal to finite (nullhomotopic) closed curves, alluded to above, we have
(1.3)
w depends only on the end points of k ^k
(in simply connected domains
M ) and by the standard procedure, this in
turn leads to the construction of a function
f(y) • f(x)~
(l.M namely letting
f(z) =
/ : M -*• G
such that
= w(x, y) for x ~ y
w , where
a
is a point chosen once and for
>k(a,z) all, and
k{a, s)
is any curve starting in
(l.l») can be expressed
a
dw = 0 =» a) = df . As an example of how one may arrive at a
group
F
z . How
df = w , so that (1.3) says
(*)
on
and ending in
M
Oiff(F) x
F
of all bijective maps
1-form with values in the
F •+ F , consider a distribution
transverse to the fibers of the projection to
are formal manifolds;
this means that around each
M , where
M
(x, u) € M x F ,
V and
Differential
there is given a subset maps bijectively to is a unique
u'
forms
V(x, u) c M (x, u)
36 1
which by
M (x) . Thus, if u € F , and x ~ y
with
1-form on M
with values in
Diff(F)
M
in M , there
(y, u') (. M(x, u) . Thus, the pair
an automorphism of F , u *—*• u' , which we denote a
proj : M * F
x, y
defines
w(x, y) . Thus
w
is
(which is a very big group - not
a formal manifold). Heuristically, the "line" connecting u ) to the "line" connecting V(x, u) , and thus
V
curve integration of u dui(x, y, z) = e , where
(x, u)
to
x
to y
(y, u') , and this "line" lies in
defines an infinitesimal path-lifting. amounts to lifting of finite paths. (x, y, z)
M, means that (for any initial value
that of
V
To say
u € F ) , the triangle lifts to a To say u> = df
for some
(locally) can by a little combinatorics be seen to imply
arises from a foliation, the leaf through
y >—>• f(y)f(x)~
(u) ; "din = 0 =* w = df"
about integrability of distributions. condition
The finite
is an infinitesimal triangle (l.l) in
closed triangle ("no infinitesimal holonomy"). f : M -*• Diff(F)
lifts (for the given
dbs = 0
(x, u)
being the graph
in this case expresses a theorem
In §8 we will demonstrate that the
"is" the usual analytic condition in Frobenius' Theorem
about distributions. Now,
Diff(F)
does not "admit integration over finite intervals" in
the sense to be explained in §6, whence we cannot really derive (*), unless we can assert that the form in question takes values in a subgroup of Diff(F)
that does admit integration, or alternatively, if M
enough.
We discuss this in §8.
is small
2. Some infinitesimal arithmetic We assume satisfy Axiom
R W 1
to be of line type in the strong sense of [9], or of ['?].
As usual, we define
D(n) = { ( d l 5 . . . , dn) € FT I di • d. = 0 V i , o) c if1 . Mote that
D(2n) cz D(n) x D(n) .
An intermediate object i s
362
Anders Kock
..., dn), (6X, .... 6 J | [di
D(2n) =
&j + d..
6^
0)
A [di • ^. = 0) A (6i • 8j = 0) Vi, j} . We write Note also
d for (d , ..., d)
. Note
M (v) = u + D(n)
for u €fl".
0 ~ d ~ 6 ~ 0 if and only if (d, 6) € 0(2n) . Since
invertible in i? , we have furthermore (d, 6) t D(2n)
2 is
d. • 6. = 0 for any
and i = 1, ..., n . We have
PROPOSITION
2.1. Any map
D(n) •* if
with
0 «—> 0 is the
restriction of a unique linear map R -*• R . (For
n = 1 , this is the "basic ("Kock-Lawvere") axiom.) 2.2. Any map
PROPOSITION
(d, 0) i—> 0 j for all map
D{n) x D{n) •* if with
(0, d) i—• 0 and
d € D(n) , is the restriction of a unique bilinear
if1 x if1 ^ if . PROPOSITION
2.3. Any map
(d, 0) i—>• 0 j for all skew symmetric map
n
f : D{2n) •+ if
(0, d) •—* 0 and
x if -*- if .
We give the proof for the last one only. case
with
d € D(n) , is the restriction of a unique bilinear
m = 1 . The Weil algebra defining
It suffices to consider the
D(2n) is
*[*!• .-., * n , y i> •••• ^ / J where
k
is the ground field (assumed to be of characteristic not equal to
2 ) , and J is the ideal generated by all
X. • X., Y. ' Y. , and •&•
'•
3
0
X. ' Y . + X. • Y. . A k-linear basis for this Weil algebra i s given by i0 3 ithe classes (mod J) of the polynomials 1 , X . , , . . . , X , Y , . . . , Y , v[X. - Y. - X. ' 1 n' 1' ' n' i j j
' Y.) . . ^-'^ w e
C , and associates
e
of the simplex are equal.
Such forms have, in another context, been considered by Bkouche and Joyal who use them (with (unpublished).
G = R ) to define deRham cohomology
We shall be interested mainly in non-commutative groups
G , and therefore only in low dimensions A
0-form on
coboundary,
M
with values in
df , is the
G
k = 0, 1, 2 . is just a map
1-form given by
df(x, y) = fly) - f(x)-1 If
a) is a
f : M -*• G . Its
for x ~ y .
1-form, we define dirt(x, y, z) = ui(z, x) ' w(z/, 2 ) • w(x, y)
for
x ~ y ~ z ~ x ; under suitable assumptions on
G , du
will be a
364
Anders Kock
2-form on the
M , of. Proposition U.I. We denote (for
?c-form whose only value is
g : M -*• M'
e . Clearly
k = 0, 1, 2 ) by
0
d(df) = 0 . Since any map
between formal manifolds preserves the property of being
neighbours:
x ~ y =* g(x) ~ g(y) , a
k-form
Clearly,
u) on
M'
immediately gives rise to a fe-form g*(w)
on
A/ .
g*(du) = d{g*u) .
If the value group identity map
G
i : G "*• G
Maurer-Cartan form
^
itself is a formal manifold, we have the
as a
on
0-form on
G . Its coboundary
di- is the
G :
tt(x, y) = di{x, y) = y • x~X
for
x ~ y .
Clearly
(3.D
dn = o ;
we shall see in §5 that this is really the Maurer-Cartan formula. Also, for any
f :M + G ,
(3.2)
df = d(/*i) = f*(di) = f*Sl . 4.
If
w is a
Certain infinitesimal curve integrals
C-valued
1-form on a formal manifold
M , we want t o
consider (U.I)
w(j/, a;) • w(x, j/)
for
x ~ j/
for
x ~ y ~ s ~ x .
and (U.2)
i»)(3, x) • u(!/, z) If
M = K
• u{x, y)
(or any etale subobject thereof), these can also be
written (U.3)
w(x+d, x) • o)(x, x+d)
for
d € 0(w)
and (U.U)
w(x+6, x) • w(x+d, x+6) • u(x, x+d)
These are to be thought of as infinitesimal !:
forth
and infinitesimal
l:
for
(d, 6) € 5(2n) .
"curve integral back and
curve integral around a triangle11, respectively.
Differential
forms
365
We also want to consider the infinitesimal curve integral around a parallelogram: (U.5) w(x+6, a:) • w(x+d+6, x+6) • w(x+d, x+d+6) • m(x, x+d) for PROPOSITION
4.1.
bijeotive maps
Let
G
be a subgroup of the group Diff(F)
F •* F , where F
1-form with values in such
is a formal manifold. If
e , for all
(it.5) gives e Proof. u
of all
is a
x ~ y , (expressing
is alternating); and
(ii) (k.h) gives e , for all
fixed
w
G , we have:
(i) the value of (U.1) is that u
(d, 6) € D(n) x D(n) .
for all
(d, 6) € D(n) , if and only if (d, 6) € D{n) * DM
.
For all of the five expressions, we consider their effect on a
£ F . We choose a frame around
local, we may as well assume we also choose a frame around respectively; For fixed
FcB
u
and since the question is
(etale subset);
x , reducing them to C+.3) and (i*.it)
in particular, we assume
M c R
(etale subset).
y €M , u £F , w(j/, -)(u) is a map
M A y ) •+ M A u ) ,
thus, by Proposition 2.1, given by a unique affine part we denote
for (U.l) and (U.2)
R
•*• FT
whose linear
A(y, u, -) , in other words co(x, x+d)(u) = u + A(x, u, d) .
Let us note that u(a;+d, x){u) = u + A(x+d, u, -d) = u + A(x, u, -d) + DxA{x, u, -d)(d) , where
DA
variable.
denotes partial Jacobian of Since
D A(x, u, s)(t)
A
with respect to its first
is bilinear in
S
and
t , and
d € D(n) , the last term vanishes, so that we have tu(x+d, x)(u) = u + A{x, u, -d) = u - A{x, u, d) . How let us calculate the effect of (1».3) on
u :
366
Anders
w(x+d, x) • w(x,
Kock
x+d)(u) = w(x+d,
x)[u+A(x,
u, d ) )
= u + 4 ( x , w, d ) - A(x,
U+A{X,
U, d ) , d)
= u + 4 ( x , w, d ) - 4 ( x , w, d) - DJi{x,
(where
u, d)A(x,
u, d)
D.A is partial Jacobian with respect to the second variable). The
last term here equals bilinear
0 because it again is from S(d, d) for some
B . So the effect of (It.3) on u is u . This proves (i).
To prove (ii) , we calculate {k.k) and (k.5) by the same technique; we get, after cancelling all S(d, d) and B(6, &) for B bilinear, that (k.h) - u = DxA{x, u, 6)(d) + D2(x, u, &){A(x, U, d)) , (d, 6) e D(2n) . Similarly, we get (U.6)
(U.5) - u = ^ ( x , u, 6)(d) - D±A(x, u, d)(6) + D2A(x, u, 6)[A(x, U, d)) - D2A(x, u, d)[A(x, u, • N
into
[t >—*• cp o t] . This is well-known; PROPOSITION arbitrary
5.2. Let M
x €M
3
and
F
be formal manifolds.
linear maps
taking
T M •+ Vect(F)
x
to
[that is,
id j T. (Diff(f)) ) , '
i*'
where
Vect(F)
id
is the vector space o/ aZZ- vector fields on
passage from (l) to (2) is given by sending *
There is, for
a natural bijective correspondenae between
M A x ) -*• Diff(F)
(1) maps (2)
see, for example, [JO], Remark 6.1.
cp : M
F . T?ze
-»• Diff(F)
to
: T M •*• Vect(F) , where
*(t)(w, d) = constructed is
u € F . i?-linear.
It is
easily seen to be homogeneous (that is commute with multiplication by scalars from is an
R ). But because
F
is infinitesimally linear,
V = Vect(F)
/?-module for which Proposition 1.10.2 of [/)] can be applied, to give
the linearity.
We next produce the passage from (2) to (l). We choose a
frame around
x 6 M , identifying
TM
. Let there be given a linear
with
K
M (x) with
D{n)
(n = dim M) , and
T M = if1 -£+ Vect(F) . cc Let *.
$. = $(e.) where
e.
is a vector field on
is the
ith
F . We define
canonical basis vector of cp : D(n) •*• Diff(F)
FT ;
by putting
If
(for
u i F , and
d = [d±, .. . , d)
£ D(n) )
cp(d, u) = * 1 ( d 1 , * 2 (d 2 , .-., \{dn, where
#.
is identified with a map
u)) ...) ,
D x F -*• F .
To see that the processes are mutually inverse, first note that the process
cp •—*• $
described in the proposition in coordinates can be
described as follows;
it suffices to describe
*. : 7s
368
Anders Kock *.(
N
which take (x, z) and (y, x) to u , and (2) bilinear skew symmetric maps T M x T M —-* T N U
XX
(the codomain is Vect(F) , if u = e € Diff(F) ) . Proof. Here we have to do the whole work in coordinates, by choosing frames, and then prove independence of the choice. Let us do the case N = Diff(F) . So identify M A x ) with D(2n) . For fixed u € F we have, by choosing a frame around
u and working with coordinates there,
cp(d, 6)(u) = u + Ajd, 6) , where A : D(2n) •+ FT (k = dim F) takes Now A
extends uniquely to a skew bilinear
(d, 0) and (0, 6) to zero. R
x
n •*• FT , by Proposition
2.3. Thus the information contained in cp is: to each bilinear
H
X FT -»• R
u , a skew
, which is also the information in (2). We omit the
details about independence of choice of frames, and so on. From Proposition 5.3 follows that we have a bijective correspondence between
2-forms
9 on M with values in G , and ordinary "linear"
2-forms
B on M with values in LG for any G which is either a formal
manifold, or Diff(F) with
F a formal manifold.
If we let at denote exterior differentiation of ordinary linear differential forms, we may ask what is the relationship between
So and
3J3 ? The answer involves the Lie bracket structure on LG (calculated via right invariant vector fields on G ). THEOREM
5.4. Let G be a group which is a formal manifold, or
Diff(F) for F a formal manifold.
Let M be a formal manifold, and w
370 a
Anders Kock
1-form on M with values
(5.1)
in
G.
(dii){wx, w2) = h&i{wv
Then, for
w , w €TM,
w2) + [5(uj , w(u2
Equivalently (5-2)
S
[u, Proof.
6](M, y) := [5>{tO,
Since the former case is easily reduced to the latter, we
shall only do the Diff(F) notation as in §U. For
case. We may do it in coordinates. We use
(d, 6) € 3(2n) , we calculated, in (U.7),
du(x, x+d, x+S)(u) = u + %C
(d, 6)
with
(5 3)
"
°x,u^l' W 2^ = D1A(X> "' W 2 )( W J " V ^ X ' "• W lH w 2 ) + D24(x, M , W2)(4(ar, u, w^^)) - ^ ( x , M , W ^ ^ a : , u, V*2))
for all
(w , W ) €fl"x Rn . Thus the skew bilinear
the coordinate information of dw at x two terms in (5-3) involving
DA
I?1 x F?1 ->• R
and u
is %C ( - , - ) . The x ,u will be shown to be 3w (w W )(M) ,
i
and the two terms involving [w (w ) , w (w )J(M)
x
j.
if
C> 4 will be shown to be
. Now the first is rather clear, since the vector
space structure on Vect(F) separately.
giving
Keeping
u
is calculated in T F
for each fixed
u € F
fixed and omitting it from notation, the
expression
is the standard expression for the exterior differential of the 1-form given by A . We now turn to calculating the tangent vector at u bracket.
Let us, for
[d , d)
€D x D
involving the Lie
arbitrary, calculate
Differential
^ K ) («> d±) = u + ^ t * .
M,