C AHIERS DE
TOPOLOGIE ET GÉOMÉTRIE DIFFÉRENTIELLE CATÉGORIQUES
P ING C HENG Y UEN
Higher order frames and linear connections
Cahiers de topologie et géométrie différentielle catégoriques, tome 12, n
o3 (1971), p. 333-371
<http://www.numdam.org/item?id=CTGDC_1971__12_3_333_0>
© Andrée C. Ehresmann et les auteurs, 1971, tous droits réservés.
L’accès aux archives de la revue « Cahiers de topologie et géométrie différentielle catégoriques » implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
HIGHER ORDER FRAMES AND LINEAR CONNECTIONS by
YUENPing Cheng
CAHIERS DE TOPOLOGIE ET GEOMETRIE DIFFERENTIELLE
Vol. XII, 3
Introduction.
In the first part of this paper we
develop
someelementary
proper- ties of semi-holonomic k-framesparallel
to those of holonomic k-frames.Our definition of a semi-holonomic k-frame is
essentially equivalent
to theone
originally given by Ehresmann £ 1b] ;
ourformulation, however,
leadsus
easily
to define a canonical 1-formok
on theprincipal
fibre bundleHk( Vn) of
semi-holonomic k-frames on a differentiable manifoldVn .
If werestrict
8k
to theprincipal
sub-bundleHk ( Vn )
of holonomic k-frames onVn,
we obtain the canonical 1-formgiven by Kobayashi. [3].
Our main re-sult is the
«Holonomy Theorem"
where wegive
ageometrical interpretation
of the
holonomy
conditions in terms of the canonical 1-form. This result will be useful forstudying
theintegrability
ofhigher
order G-structures.These
preliminary
results servedoriginally
as anintroductory
part to aforthcoming
paper which deals with the structure tensors ofhigher
orderregular
G-structures andhigher
ordergqometric
structures.The second part of this paper deals with the
higher
order linear con-nections. Let
Vn
be a differentiable manifold. A linear connection of order kon n
is an infinitesimal connection on theprincipal
fibre bundleHk( n) .
Its torsion form is defined to be the exterior covariant derivative of
6k
There is a one-to-one
correspondence
between the set of linear connections of order k(resp. quasi-holonomic
linear connections of order k withouttorsion)
onn
and the set of invariant sections of the canonicalprojection
Hk+ 1 (Vn) - H1 (Vn).
We show further that a linear connection of order kon
V n
islocally
flat if andonly
if it can be obtainedby
successive pro-longations
of a first order linear connection without torsion and curvature.Some of these results have been summarized in
161
and areprepublished
in
French,
in the first part of the author’s thesis171 -
Ifn
is a differen-tiable
manifold,
T( V )
is the tangent vector space of V at x.Part I
HIGHER ORDER FRAMES
1. Semi-holonomic frames.
Let n
be an n-dimensionalCoo -differentiable
manifold. Afirst
or-der
frame ( or
a1-frame)
ofn at
thepoint
x is an invertible1-jet
ofRn
into
V
with source 0 ERn
and target x EV .
The manifold of all 1-frames ofV ,
denotedby H1 (V n ),
forms aprincipal
fibre bundle overn
with na-tural
projection TTl0
whichassigns
to each1- j et
its target, the structure groupbeing L1n=GL (n,R).
The trivial bundleH1 ( Rn)= Rn X Lln
can beidentified with the group of all affine transformations on
Rn .
There is adistinguished
element inH1 (Rn) , namely
the1-frame el
ofRn
definedby
the1- j et
of theidentity mapping
ofRn
ontoR"
with source 0 .Let
b : H1( Rn ) - H 1 (Vn)
be a localisomorphism.
It induces a localdiffeomorphism f
ofRn
inton
withf o TT10=TT10o,b (pseudo-products );
wewill denote all natural
projections by
the samesymbol 77
with indices. Wesay that h is 1-admissible if the domain of h
contains e1
andb ( e1) = j10 f
(Here j10 f
denotes the1-j et
off
with source0) .
The manifold of
1-jets jlel b,
where b is a 1-admissible local iso-morphism
ofH1 ( Rn)
intoH1 (Vn) ,
will be denotedby H2 (Vn) .
There aretwo natural bundle structures
on H2 ( Vn) :
i)H2 ( Vn)
forms aprincipal
fibre bundleover H 1 ( Vn)
with naturalprojection TT21
and structure groupM2n consisting
of all1- j ets
of 1- admi s-sible local
isomorphisms
ofH1 (Rn)
into H1 ( Rn )
with source and targete 1.
The structure groupM2n
actson H2(Vn)
on theright by
thecomposi-
tion of
ets.
MoreoverTT21 (j1e1 b)=b (e1)=j10f
ii) H2( Vn)
forms aprincipal
fibre bundle overn
withprojection TT20 = TT10o TT21
and structure groupL2n.
HereL2n
is the fibre ofH2(Rn)
over theorigin 0 E Rn .
Themultiplication
inL 2
isgiven by:
ifg1 = j1e1 h 1 E L 2
and
g2 = je 1 b2 E L2n,
then thepseudo-product b1 o b2
is a 1-admissible lo- calisomorphism
andg1.g2=j1e1 ( b1 o b2) depends only
onj1e1 b1
andj1e1 h 2 .
Notice there isagain
adistinguished
element innamely
the elemente2
definedby
the7-jet
of theidentity mapping
ofH1( Rn)
ontoH1( Rn)
with sourceel .
An elementz E H2(Vn)
will be cal-led a semi-holonomic
2- frame
ofn
at thepoint x =TT20(z) .
We define
by
recurrence theprincipal
fibre bundleHk( Vn)
of semi-holonomic k-frames of
Vn .
Let us assume that we have defined theprinci- pal
fibrebundle fik-l (Vn)
of semi-holonomic(k -1) -frames
ofn , with
base space
V ,
structure groupL and proj ection TTk-1 k-2
onHk-2 (Vn).
A local
isomorphism u : H-k-1 ( Rn ) - Hk-1 (Vn) is said ( k -1)- admissible if : i) v
is( k -2)-admissible,
where v is the localisomorphism
ofHk-2( Rn ) into Hk-2( Vn)
inducedby u , such that vo TTj-1 k-2 =TTk-1 k-2 o u
, where
ek -1 (resp. ek-2)
is thedistingui-
shed element in
Hk-1 ( Rn) ( resp. Hk-2 (Rn)),
The set
Hk(Vn)
of1-jets
of the formje
u, where uis a (k -1)-
admissible localisomorphism of Hk-1 ( Rn) into Hk-1 (Vn),
forms aprin-
cipal
fibre bundle overn
with structure groupL n ;
th eunderlying
set ofLkn
isjust
the fibre ofHk(Rn)
over 0 E Rn . The spaceHk(Vn)
can alsobe
regarded
as aprincipal
fibre bundle overHk-1 ( Vn)
with structure groupMkn
= Ker( Lk n - Lk-1 n) .
An element z ofHk (V n)
will be called a semi-holo- nomick-frame
ofn
at thepoint
x, where x is theprojection
of z intoVn.
For m
k ,
the naturalprojection TTk m
ofNk( n )
ontoHm(Vn)
iscompatible
with thesurjective homomorphism
ofLkn
ontoLr;:.
The distin-guished element ek
inHk( Rn ) = Rn X Lkn
is definedby
the7-jet
of the i-dentity mapping
ofHk-1 ( Rn) with
sourceek
-1.2. Canonical form
onHk (Vn).
An element
u E Hk(n)
can be written asu = j1ek-1
b, where b is a( k -1 ) -admissible
localisomorphism
ofHk-1 (Rn)
intoHk-1 ( Vn);
it de-termines a linear
isomorphism 9
of ontowe have a canonical
decomposition Ek-1=RnOLk-1 n,
whereLk-1 n
is theLie
algebra
ofL k-1 n.
From now on, we willidentify
Rn with a vector sub-space
of Ëk-l given by
the canonicaldecomposition.
Since f1 is a linearisomorphism, u (Rn)
is an n-dimen sional vectorsubspace
oftransversal to the
fibres,
called the horizontaln-plane
associated to the k-frame u .Let v be the
projection
of u underTTkm .
Thefollowing diagram
is
commutative,
where v’ is theprojection
of v underTTm m-1
and where thevertical arrows are the natural
projections.
Consider a vector
Z E Tu ( Hk (Vn)) .
Itsimage
under the
tangential
mapT7T k
is tangentto Hk-1 (Vn)
at thepoint
The
Ek-1 -valued
differentialI-form 8k
definedby
will be called the canonical
fo rm
onHk( Vn).
For mk ,
we have the fol-lowing
commutativediagram
where the vertical arrows are the natural
projections.
The Lie group
Ln
actsnaturally
onEk-1
on theleft.
Each ele-ment g of
Ln
defines a lineari somorphi sm g of Ek-1
onto 7The
right
translationR-1g’ = RlJ’ ).-1
determines a li-near
isomorphism
T ) onto . If we putwe obtain a linear
representation
p ofLkn
on the vector spaceis a commutative
diagram,
where the vertical arrows are the natural pro-jections.
PROPOSITION I.1. The canonical
form ’9k
is apseudo-tensorial 1- form
on3. Holonomic Frames.
A
diffeomorphism f : Vn - V’n
induces aprincipal
fibre bundle iso-morphism f (k)
ofHk(Vn)
ontoHk( V’n) .
Thisisomorphism f (k) posses-
ses the
following properties :
ii) I( k)
iscompatible
with the canonicalforms,
i.e.wh ere
8k ( resp. 8k )
is the canonical form onHk (Vn) ( resp. Hk (V’n)).
THEOREM 1.2.
Let 4J
be a localdiffeomorphism of Hk( n)
intoHk (V’n).
Then
locally o = f(k) for
some localdi f feomorphism f o f n
intoV n,
i f
andonl y if o
iscompatibl e
with the canonicalforms, i. e. o*0’k=0k .
It remains to show that the condition is sufficient. For this we will
proceed by
induction on k .LEMMA 1.3.
L et o
be a localdiffeomorphism o f H 1 (Vn)
intoH1 (V’n)
with
o* 0’1 = 01.
Then we canlocall y
writeo = f (1) for
some localdi f feo- morphism f o f n
inton’.
Consider a tangent vector
Z ET u ( H 1 (Vn))
withTTT10 ( Z ) = 0 .
Thecondition
o*0’1=01 implies
thatT TT10 (T0 (Z))=0. Thus 4J
sends a tan-gent space to the fibre of
H1(Vn)
onto a tangent space to the fibre ofHI ( V’n) .
This means thatlocally o
is a fibre map and induces a mapf
ofn
intoV’n satisfying f o TT10 =TT10oO
We want to showthat O = f (1).
Thus we want to show that for any u with
TT10 (u) = x
wehave O ( u ) =
j1xfou. Let E E Rn.
Choose avector Z E T u ( H1 (Vn)) with TTT10(Z)=
O (u) = jlxfou
holdsproving
the lemma.To prove the theorem for k we may assume that it has been establi- shed for k-l. Let
Z E Tu( Hk(n))
withT TTk k-1 (Z)=0.
The conditionO* 0’k = 0k implies ( T TTk k-1o T O) (Z)=0 . Thus O
is a local fibre map with respect to the fibrationsThere exists a local
diffeomorphism Y
of . suchfor all is
surj ective,
we deducethat Y * 0’k-1 = 0k-1 . By
the inductionhypothesis,
there exists a localdiffeomorphism f
ofV
intoV’
such thatlocally Y=f (k-1).
We have thus1T1-10 rp locally.
Now we aregoing
to show thatlocally
ment u E
Hk ( Vn)
determines a linearisomorphism
iwith
u’= TTk k-1 (u) .
Two elements u and vof Hk (Vn)
are identical if andonly
if u = v . It suffices therefore to show that for all Choose a tangent ve.ctor ) withOn the other
hand,
It follows that for allWe have
therefore O = f (k) locally
and our theorem isproved.
COROLLARY
I.4. Let O
bea principal fibre
bundleisomorphism of Hk( n)
onto
Hk(V’n).
L etf
be th ediffeomorphism o f n
ontoV
inducedby O .
Then
O = f (k) if and only if O* 0’k = 0k.
Consider a
local diffeomorphism f
of an openneighbourhood
of0 E Rn
onto an open set ofV .
It induces a( k -1 ) -admissible
local iso-morphism f (k-1) : Hk-1 ( Rn) -Hk-1 (Vn) ,
It follows thatu = j1e
k -1f(k-1)
is an element of
Hk (Vn).
We say thatuE Hk (Vn)
i s ahol onomic k- f ram e
of
n
if u can be written asu = jle k-1 f (k-1) for
some local diffeomor-phism f
ofRn
intoVn .
A k-frame uof n
is holonomic if andonly
if onecan find a
representative
for ucompatible
with the canonical forms. Theset of
holonomic k-frames
ofV
forms aprincipal
fibre subbundleHk (Vn)
of
Hk(Vn).
Its structure group is thesubgroup Lkn
ofLkn consisting
ofholonomic elements. Notice there is a group
isomorphism
betweenLkn
andthe group of all invertible
k-jets
ofRn
intoRn
with source and target 0.The
space Hk(V n)
can also beregarded
as aprincipal
fibre bundle overHk-1 (Vn)
with structure groupMkn = Mfkn n Lkn ,
kernel of thesurjective
ho-momorphism Lk -LK-1 .
n n
4. Relations between
Let W and Y be two
COO -
-differentiable manifolds. We will denoteby Jk(W, Y)
the differentiable manifold of semi-holonomick-jets
of W intoY . For the definition of semi-holonomic
jets,
see the works of Ehresmann.For m
k ,
letPk
be the canonicalprojection
ofJk ( W,Y)
ontoJm ( W, Y) .
A
jet X E J k ( W, Y )
is invertible if andonly
ifpk 1 (X)
is invertible. LetIT k( W, Y)
denote the set of invertiblejets
inJk(W, Y) .
This set is thenthe inverse
image of fî 1 ( W. Y) by
the submersionp7. Since 111( W, Y )
is an open submanifold of
J1 (W. Y) ~J1 ( W , Y),
it followsthat fik(W, Y)
is an open submanifold of
Jk( W, Y). Moreover, pkm : TTk( W, y)- Hm (
W,y)
is a submersion.
A semi-holonomic k-frame
(resp.
holonomick-frame)
ofn
in thesense of Ehresmann is an invertible semi-holonomic
k-jet ( resp.
invertibleholonomic
k-jet)
ofRn
into V with source 0 ERn .
The setPk(Vn) (resp.
pk(Vn))
of semi-holonomic k-frames( resp.
holonomick-frames)
ofn
inthe sense of Ehresmann has a
principal
fibre bundle structure overVn’
the structure group
being
the group of all invertible semi-holonomick-jets (resp.
holonomick- jets)
ofRn
intokn
with source and target0 E Rn .
An elementu E pk( Vn)
can then be written asu = j10f, where f
is a differen-tiable
mapping
ofRn
intopk-J ( Vn) satisfying
the condition:Here we have also denoted
by pk;2
the canonicalprojection
ofpk-1 (Vn)
onto
Pk-2(Vn ).
TH E O R E M I. 5. There exists a canonical
di f feomorphism vk 01 Hk(Vn)
onto
Pk(Vn) satisfying
theproperties:
(1) vk is a fibre map,i.e. pk0o vk =TTk0;
(2) for
mk,
is a commutative
diagram;
(3) vk,
restricted toHk(Vn), is a diffeomorphism of Hk(Vn)
ontoPk(Vn).
We prove the theorem
by
induction on k . Fork = 1, H1 (Vn)
i s i-dentical with
pI (Vn)
andvI
isjust the identity map,Let u = j1e1 b
be anarbitrary
elementin H2( Vn) .
IfN1
denotes the «zerosection t of H1 ( Rn)
the
mapping u -v2 (u) = j10 ( v1 o b o n1)
defines adiffeomorphism of fi2 (Vn)
onto
P2(Vn),
because thecomposition
ofjets
is a differentiable map. Letus assume there exists
vk-1
suchthat,
for allzEHk-1 (Vn), vk-1 (z)=
where and
nk-2
is the «zero sec-tion) of the trivial bundle
Hk-2( Rn) =
Rn XLk-2 n.
Consider then an arbi-trary element
y = j e k-1
g inHk( Vn) .
Ifnk-1
i s the « zero section» of defines a localdiffeomorphism
of . Since the
1-jet jog,
which*)
corresponding toRn
Xtel,
where e is the unit element.is
independent
of the choiceof g
for y, is an element inP k (Vn).
Themapping y-vk (y)=j10g’
defines adiffeomorphism Vk of Hk(Vn)
ontoPk (Vn).
It is easy to check thatvk
has the desiredproperties.
Consider the case where
n
=Rn .
Let us recall that theunderlying
set of
L"
isjust
the fibre ofHk ( R n)
over theorigin
0 . Since the multi-plication
inLkn
isgiven by
thecomposition
ofjets,
the restriction ofvk
to
L"
defines a groupisomorphism
ofLkn
onto the group of all invertiblesemi-holonomic
k-jets
ofRn
intoRn
with source and target 0. It is easyto see that the
diffeomorphism vk
of the above theorem iscompatible
withthis group
isomorphism.
We have therefore thefollowing corollary:
COROLLARY 1.6. The
principal fibre
bundleHk(Vn) (resp. Hk(Vn))
iscanonically isomorphic
toPk(Vn) ( resp. Pk (Vn)).
Let E be a
locally
trivial fibre bundle overVn .
We will denoteby Jk E
the differentiable manifold ofk-jets
of local sections of E. Letj2 E
=J1 ( Jl E) .
The k- th non-holonomicprolongation
of E is definedby
induction :We define also the semi-holonomic
prolongation Ïk
Eby restricting
oursel-ves to those local sections such
that,
for all 0 mk,
the local sectiono- of
n into JmE
satisfies the condition:j1x (TTmm -1°o)=o (x),
where7TM
is the naturalprojection
ofJm E on to Jm-1E.
We haveTHEOREM I. 7. There exists a canonical
di f feomorphism fLk of Hk (Vn)
onto
J k-l (H1 (Vn)) satisfying
thefollowing properties:
(1) for k
= 1,u1 is just
theidentity map of H1 (V n );
(2) fLk
is afibre map;
moreexplicitly
is a commutative
diagram,-
(3) for
0 m k, thefollowing diagram
commutes.
We prove the theorem
by
induction on k . For k = 1,JO ( HI (Vn))=
HI ( n ) by
definition andf.L 1
isjust
theidentity
mapof H1 (Vn).
Letu = j1e1 b
be anarbitrary
element ofH2(Vn) .
Consider the local diffeomor-phism f
of Rn inton
definedby
the condition:TT10b=fo TT10.
IfTJI
isthe zero sections of
H1 (Rn) = Rn x L1n,
themapping
defines a local section a of
n into H1 (Vn).
If we putu2 (u) = j1x o
with
x = TT1 0 (u) ,
themapping u -u2(u)
defines aninj ection of H2 (Vn)
into
J1 ( H1 (Vn)) .
This differentiablemapping fL 2
issurjective.
In factlet cr be a local section of
n
intoH1 (Vn)
withj1x o E J1 (H1 (Vn)) .
Thetarget
o (x)
can be writtenas o(x) = j10 f
for some localdiffeomorphism I
of Rn intoVn.
Let h be the localisomorphism
ofH1 (Rn)
intoH1 (n)
defined
by
the conditions:It is easy to check that h is I - admi s sibl e
and j1x o =u2 (j1e1 b) .
The map-ping J.L2 gives
then adiffeomorphism of H2(Vn) onto J1 (’/Y ( n ))
withthe desired
properties. Now,
let us assume there existsuk-1
andJ.Lk-2
such
that,
for all u Eilk-l ( n ),
we havewith
u’ =TT k-1 k-2 (u), w =TTk1 (u)
and wherenk-2 is the
«zero section» of1 h
be anarbitrary
element ofHk( Vn) .
Let
f
be the localdiffeomorphism of
R n inton
inducedby
h . If we de-note
by nk-1
the «zero sections ofdefines a local section of
n
intoJ k-2( H1 (Vn))
andjx h’
determinesan element
uk (z)
ofJk-1 ( H1 (Vn)) independent
of the choice of the re-presentative h
for z . It is easy toverify
thatz -uk (z)
defines a diffeo-morphism ILk of Hk(Vn)
ontoJk-1 ( H1 (Vn)) satisfying
therequired
con-ditions of the theorem.
COROLLARY 1.8
[4c] pk(Vn) and Jk-i(H1( Vn)) are canonically dif- feomorphic.
5.
Local coordinate systems in Hk( Vn) .
Let { x1 , x2 , .... , xn )
be the natural coordinate system inRn .
Let U be a coordinateneighbourhood
inn
with a local coordinate system{ y1, y2,
.... ,yn) .
Con sider an elementu E H1 (Vn)
withproj ection
The 1-frame u is
completely
determinedby
the linearisomorphism
In terms of local
coordinates,
M can beexpressed by
The 7-frame u is therefore
completely
determinedby
the set of local co-ordinates
(yi, yjk)
withdet (yjk) #0.
Thus we cantake {yin, yjk}
as a’lo-cal coordinate system in
(TT10-1 (U) C H1 (Vn). Similarly,
we have aglo-
bal coordinate
system {xi, xjk} in H1 ( Rn),
with respect to which thedistinguished element
isgiven by e1d=(0, djk).
The
n +n2
vectors form a basi sx a
for
El=T el (H1 (Rn)),
and then + n2
local vector fieldsare
linearly independent.
Onceagain,
any 2-frame v iscompletely
determi-ned
by
the linearisomorphism v
associated to v . In terms of local coordi- nates, we havewhere and Tu is the
tangential
map of u, ubeing
considered as a differentiable map. Thus v iscompletely
determinedby
the set of local coordinates( yt, yij, Y;k)
withdet( yij) # 0 .
By
iteration we have a coordinateneighbourhood (TTk0) -1 (U)
inHk (Vn)
with a local coordinate system{yi, yij,..., yij }
withThe natural
projection
ofgiven by
If u
=( ai, ai ,
... ,ai ...jk) E Hk( Vn),
the associated linearisomorphism
j1
j1... jk i7
can beexpressed by
where
and
u’ = TTkk-1 (u).
The localcoordinates ai
. aresymmetrical
withrespect to the lower indices if and
only
if u is a holonomic k-frameof V n [1c] .
6. Holonomy Theorem.
Consider an
arbitrary
element u inHk (Vn).
In thisparagraph
wegive
a necessary and sufficient condition for u to be a holonomic k- frame.Let us recall that the horizontal
n-plane
definedby u
isjust
theimage
ofthe
Rn-component of Ek-1 = RnOLk-1 n
under the linearisomorphism
ü. Itis tangent to
Hk-1 ( Vn ) at
thepoint u’ = TTk k-1 (u) ,
if u is holonomic . For k = 1, there is no distinction between semi-holonomic frames and holonomic frames. Fork > 2 , Hk (Vn) C Hk (Vn).
PROPOSITION 1.9. An element u
of H2 (Vn) is a
bolonomic2- frame if and
only i f
the2-fonn d01
vanishes on tbe horizontaln-plane
associated to u.Let
r1 ,
r2, ... , rn be a basis for Rn. The canonical form01
on111 (Vn)
can beexpressed
as follows:In terms of a local coordinate
system {yi}, yij}
inH 1 (Vn) ,
the compo-nents
0i
of81
aregiven by
where
( zij)
is the inverse matrix of( y)..9y
exteriordifferentiation,
weget -
Let
u=( ai, aij, aijk) E H2( Vn ) .
i jk n The horizontalrz-pane Qu
u asso-ciated to 11 is
generated by
the n vectorswith
u’ =TT2(u) =( ai , aij).
1 i The 2-formd01
vanishes onQ
u if andonly
ifis zero for all
1 i , j , k n .
Since(zij) = (yij)-1,
we have the relationj j
zip ypk = dik) . By differentiation,
we getwhere I . It follows that
Since
det ( bij) # 0 ,
we con clude that det( Xj, Xk ) =0
for all 1i, j, k n
if and
only
if theatk
aresymmetrical
with respect to theirlower
indices..
Thu s our
propo sition
i sproved.
For the
general
case where k >2 ,
we have thefollowing
« Holono-my Theorem»:
THEOREM I.lo.
An
element u EHk( Vn)
is a holonomick-frame if
and on-ly i f
thefollowing
conditions aresatis fied :
i)
the horizontaln-plane Qu
associated to u istangent
to thesubmanifold Hk-1 ( V ) of Hk-1 (V n);
ii)
the2-form d 0k-1
vanishes onQu .
Let us assume that u is a holonomic k-frame. We can then write
u =
i eL, - 1 f( k-1 )
for some localdiffeomorphism f
ofRn
intoVn.
If0k-1
and
ek-1
arerespectively
the canonical form onwe have It follows that
Now,
the 2-formd0k-1
vanishes on theRn-component of I
As a consequence,
d dk-1
vanisheson Qu.
The first condition is obvious-ly
necessary.It remains to show that the conditions are sufficient. The first con-
dition
implies
thatu’=IIkk-1 (u)
is a holonomic( k -1) -frame,
and thatwe can find a local coordinate
system {yi, yijl,...yijl ...yijl...jk}
inHk (Vn)
such that
u = ( 0 , ai jl,..., aij...jk) where aijl...jm are symmetrical
with respect to their lower indices for2 m k -1
and ai j l ...jk . issymmetrical
with respect to the
first
k -1 lower indices.By
achange
of local co-ordinate systems, we can even suppose that
aij=dij
andaijl...jm
= 0 forbe the natural coordinate system in
Rn . By iteration,
we define aglobal
coordinate systemThe vectors
form a basis
for Ek-2
and we can writeAn element defines a linear
isomorphism
In termsof local coordinate
systems, v
isgiven by
where 1 The
matrix
A = ( A03B2a)
is of the formwhere J
is the matrixcorresponding
to the linearisomorphism
ve therefore
be the inverse matrix of A
=(,A,8) .
The componentsexpressed by
By
exteriordifferentiation,
we getSince we obtain
by
differentiationhence
and let
Qu
be the horizontaln-plane
ofi
as soci ated to u .
Qu
isgen erated by
the n vectorswhere an d
The
nullity
ofimplies
that c for all lwith Since
det ( Ba03B2( u’ ))~ 0 ,
we obtainIt follows that
the aijl...jk
aresymmetrical
with respect to their lower indices and thus u is a holonomic k-frame.Let us call
uE Hk (Vn)
aquasi-holonomic k- frame
if the horizon-tal
n-plane Qu
ofHk-1 ( n )
associated to u is tangent to the submanifoldHk-1 (Vn) .
We will denoteby Hk( Vn)
the set ofquasi-holonomic
k-frames.We have
obviously Hk (Vn) C Hk (Vn) C Hk (Vn).
From the above theorema
quasi-holonomic
k-frame u is a holonomic one if andonly
ifd 8k-l
va-nishes on the horizontal
n-plane Qu
associated to u .7. Some remarks
onH k ( Rn) .
In the
preceding paragraphs, Rn X Ln
has been identified withHk( Rn) .
In thisidentification,
acouple ( x, g ) E Rn X Ln
is identifiedwith the element
tx(k)(g) E Hk (Rn), where tx
denotes the translation inRn sending
theorigin
0 to thepoint
x. The tangent spaceEk
toiTk( Rn)
at the
distinguished
elementek
has a canonical Liealgebra
structure. Letus say a few words on this Lie
algebra
structure. Let u= ( x, g ) E Hk( Rn) .
The
translation tx
inRn
induces anautomorphism t(k)x
offik( Rn)
whichcommutes with the
right
translations ofL k on Hk( Rn ),
i. e.for all
b E L kn.
Inparticul ar, t (k) xo R g =R go t (k)x gives
adiffeomorphism
of iik( Rn)
onto itself that we will denoteby tu .
We call a vector fieldon lik( Rn)
invariant if it is invariant with respect to alldiffeomorphisms
of the
form tu,
where u is anarbitrary
element ofHk( Rn) .
There is aone-to-one
correspondence
betweenËk
and the set of invariant vectorfields on
iik( Rn).
IfX,
Y are two invariant vector fields onHk(Rn),
sois the
bracket [X, Y].
The vectorspace Ek,
endowed with thismultipli- cation,
becomes a Liealgebra
over the field of real numbers. The Lie al-gebra flf
ofn
is a Liesubalgebra of Ek = Rn OLkn.
To every differentiable map
f
of a differentiable manifold W intoHk(Rn),
we can associate a differential1-form cef = f-1df
with values in the Liealgebra Ek
definedby
for al l X inTx( W) .
Inparticular,
ifW = Hk(Rn)
and iff
is theidentity
map ofHk( Rn),
we get a differential 1-form ú) onHk( Rn)
with values inEk ,
called the invariant
form
onHk ( Rn) .
PROPOSITION 1.11. The invariant
form
ú) onHk( Rn) satisfies
the equa- tionWe recall that the
form [w,w]
is definedby [w,w] (X , Y)=
[w (X), w (Y)]
for all vector fieldsX, Y
onjfk( Rn ).
Since the mo- dule of vector fields onHk( Rn)
isgenerated by
the invariant vectorfields,
it suffices to prove theequation
for two invariant vector fields Xand Y . Behave
proving
theproposition.
REMARK: VIe have
adopted
thefollowing
convention for the exterior pro- duct :where the summation runs over all
permutations i1 ,
... ,i p , ip + 1, ... , i p + q of {1 , 2, ..., p+q}
and where 6 denotes thesignature
of the correspon-ding permutation.
With thisconvention,
we have thefollowing
formula: ifa, is a
p-form,
thenKumpera pointed
out to me that the above Liealgebra
structure onEk
comes from a canonical Lie group structure onHk(Rn).
Since( x , g )
E;
is identifiedwith t
denote the
underlying
set ofLkn
endowed with thefollowing multiplication:
g*b =b g
whereg*h
denotes theproduct
intLkn
andb g
denotes the pro- duct inL k.
With the identificationHk(Rn)=Rn x Lkn, Hk ( Rn)
becomesa Lie group isomorphic to
Rn XtLkn. Moreover,
ifu = ( x, g ) , u’= (x’,g’)
th en
where tu
is thediffeomorphism
defined in theopening paragraph
of thissection. In
fact, tu
is no other than the left translation definedby u
inthe Lie group
Hk ( Rn) .
The Liealgebra
structure ongk
defined above isprecisely
the Liealgebra
of the Lie group17k( Rn) .
The invariant form6d is
simply
the Maurer-Cartan form of the Liegroup Hk( Rn) .
Part II
HIGHER ORDER CONNECTIONS
1.
Linear
connections oforder
k .An infinitesimal connection
1-k
in theprincipal
fibre bundle of se-mi-holonomic
k-frames Hk( Vn)
over n will be called a linearconnection o f
order k ofVn. Let w
be its connection form. We will sometimes say thatcvk
is a linear connection of order k ofVn.
If D is the exterior co-variant differentiation relative to
wk ,
the tensorial 2-formOk = D 0k (resp.
Qk = D wk )
will be called the torsionform ( reps.
curvatureform)
oflk
or we havewhere p is th-e linear
representation
ofLkn on Tk-’
defined in Part I . IfY or Z is a vertical vector, then
(3 k ( Y, Z) = 0.
The linear
representation
p induces arepresentation
ofLk
on , we putwhere at= exp tA
is the1-parameter
group of transformations ofLkn
gene-rated
by
A . Inparticular, if f
isvertical,i.e. E E Lk-1 n
, we haveTHEOREM 11.1 1 ( s tru c tu re e qu a tio n s ) Let
wk
be a linear connectiono f
or-der k. Then
The first structure
equation
is well known. Let us show the secondstructure
equation:
for all vectors
X E u ( Hk (V n))
andYeT u (Hk (Vn)).
It is sufficient toverify
theequality
in thefollowing
threespecial
cases :i)
X and Y are horizontal. In this case,wk (X)=0, wk (Y) = 0
andthe
equation
reduces to the definition of(3 k .
ii)
X and Y are vertical. LetX = A*u
andY=B*u,
where A* and B*are the fundamental vector fields on
Hk (Vn) corresponding
toA = wk (X)
and
B = wk ( Y) respectively.
We haveand
The
equality
holds.iii)
X is vertical and Y is horizontal. LetX = A*u
with.A = wk (X) E
Lkn.
We can extend Y to an invariant horizontal vector field Yon i7k( V ) .
We have thenSince
6k ( A*)
is constant,Y 0k ( A*) =0 .
As Y is an invariant horizontalvector
field, [A*, Y] = 0 . Let at = exp
tAbe
theI-parameter
group of transformations ofL n generated by A E Lkn .
Now,
Theequali-
ty therefore holds.
The
proj ection TTkm
ofHk (Vn)
ontoHm(Vn ) being compatible
with the natural
surjection
ofLkn
ontoLmn ( m k),
any linear connectionwk ( of order k )
induces a linear connectionúJm
of order m ,given by
P R O P O SIT IO N II. 2
Any
linear connectionwk o f
order k induces canoni-cally a
linear connectionwm o f
order m kgiven by
We have the
relations:
Let us
verify only
the last formula. We know thatAs a consequence, From the second structure
equation,
we obtainCOROLLARY II. 3
1 f
the torsionform ( resp.
the curvatureform) o f úJk
va-nishes
identically
onT (Hk (Vn)),
theinduced connection úJ m (m k )
is without torsion
( resp.
withoutcurvature ) .
Let
wk
be a linear connection ofVn.
We say thatwk
isquasi-ho-
lonomic if the connection form
wk ,
restricted toT (H (Vn)),
defines aconnection in the
principal
fibre bundleHk( Vn) over Vn .
Ifwk
isquasi- holonomic,
all induced connectionsúJm ( m k )
arequasi-holonomic.
Th ec anonical connection in
Hk (Rn)=RnX Lkn
i squasi-holonomic.
2. Second order linear
connections.Let u be an element
of H2( Vn ) .
Consider a coordinateneighbour-
hood U of
a0 = TT20(u)
with a system of localcoordinates {x1,x2,...xn}.
The 2-frame u can be
represented by
a set of local coordinates(xi, xij,
xijk)
withdet ( xij) ~0 .
Let U’ be another coordinateneighbourhood
ofa0
with a system of localcoordinates {y1, y2,
... ,yn} .
The same u is re-presented by (yi, yij, yijk) .
Thechanges
of local coordinates aregiven by
An
elementg E L2n
can berepresented by u = ( aij, aj k)
withdet ( aij)~0. In
terms of these
coordinates,
themultiplication
inL2n
isgiven by
The action of
L2n on H2(Vn)
isgiven by
Let a be the
automorphism
ofL2n
definedby a(aij , aijk)= (aij , aikj).
It is evident that a leaves fixed every element in
L 2. Moreover, a 2
=identity.
We haveimmediately
P R O P O SIT IO N II. 4 There exists an involutive
automorphism
Cx,o f L2n
suchthat
L2n is
thesubgroup o f
all thef ixed points o f
a.T H E O R E M II. 5 The
homogeneous space L2n/L2n
isweakl y
reductive:there exists a vector
subspace
such thatwhere
?2 ( resp. F2)
is the Liealgebra of L 2 ( resp. L2n.
This result is an immediate consequence of the
following
lemmaproved
in[2] .
LEMMA 11.6 Let a be an involutive
automorphism of a
Liegroup
G. Theset
of fixed points of
aforms a
Liesubgroup
Gof
G. Moreover, the homo-geneous
space G/G
isweakly
reductive: there exists a vectorsubspace m of
the Liealgebra q of G
such thatwhere 9
is the Liealgebra of
G . The vectorspace m
can begiven by
Let ?
be the vectorsubspace
of22
definedby
the above lemma.showing
that We have therefore the follo-wing
result.COROLLARY II.7 The
homogeneous space E2 /L 2
is asymmetric space.
For the rest of this
section,
we fix once for all adecomposition where t
is the vectorsubspace
defined in the theoremII.5 .
We denoteby
i the canonicalinj ection of H2 ( Vn) into H2 (Vn) .
Let
éJ2
be a connection formin H2 (Vn).
We can writei*w2 = w2 + t,
whereÚ)2 ( resp. t )
is theL2n-component ( resp. m-component)
ofi*w2 .
Sincead (L2n)MCM, w2
defines a connection in theprincipal
fibrebundle
H2(Vn) over n
and t isa M-valued tensorial
1-form onH2(Vn)
called the
quasi-holonomic form
ofw2. Inversely,
thecouple (w2, t)
de-termines a connection
w2
inH2 (Vn).
Infact,
ifEETu (H2(Vn))
withuE (H2 (Vn),
we canwrite E =E’+E", where E’
is a horizontal vectorwith respect to the connection
Ú)2
andE"
is a vertical vector. Let us putw2(E)=t(E’)+u-1(E"). Now, if E E Tv(H2(Vn)) where v E H2(Vn) ,
there exist
u E H2(Vn)
andg E L2n
such that v = ugand E = TRg(E)
forsome
EE Tu(H2(Vn)).
It is easy to check thatw2(E)=ad(g-1)w2(E)
does not
depend
on the choice of u and g . Themapping E -w2 (E) gives
the
required
connection form onH2(Vn) . Besides, i*w2 = w2 + t .
We havethus established the
following
result.P R O P O SIT IO N II. 8 There is a one-to-one
correspondence
between the seto f
all second order connectionsw2 o f Vn
and the setof
allcoupl es (w2,
t),
whereÚ)2
is a connectionform
inH2(Vn)
and t is a’)IT-valued
tenso-rial
1- form on H2(Vn) ;
thecorrespondence
isgiven by
COROLLARY II.9 A linear connection
w2
isquasi-holonomic if
andonly if
its associatedquasi-holonomic form
t vanishesidentically
onH2( Vn) . Let O
be a tensorial form onfi2( Vn) .
From the structureequation
where
D 4J
is the exterior covariant derivativeof 4J
with respect toce 21
we deduce that
The induced
form i*O
is a tensorial formon H2(Vn).
If D is the exterior covariant differentiation with respect tow2
, we haveThus
Let Q2 ( resp. Q2)
be the curvature form ofw2 (resp. W2).
Fromthe structure
equation
we have