A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
J EAN E CALLE
B RUNO V ALLET
Intertwined mappings
Annales de la faculté des sciences de Toulouse 6
esérie, tome 13, n
o3 (2004), p. 291-376
<http://www.numdam.org/item?id=AFST_2004_6_13_3_291_0>
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- 291 -
Intertwined mappings(*)
JEAN ECALLE
(1),
BRUNO VALLET (2)ABSTRACT. - We show that, contrary to expectations, there exist pairs
of formal and even analytic, non-commuting and non-elementary
(neither
algebraic noralgebraic-differential)
mapping germs inDiff(C,0)
that are‘entwined’ in a group relation
W(f, g)
= id. In the case of identity-tangent mappings, ’twins’ exhibit, rather than analyticity, generic divergence , butof a particularly interesting sort: resurgent, accelero-summable, and with simple alien derivatives.
RÉSUMÉ. - Nous montrons que, contrairement à une attente assez parta- gée, il existe dans
Diff(C, 0)
des paires( f, g)
de difféos locaux jumelés, qui engendrent des groupes « intéressants », i. e. ni libres ni trop élémentaires(ils
ne sont pas abéliens et ne se réduisent pas, même après éclatement, àdes groupes
d’homographies).
De tels groupes sont dits liés. Nous ébau- chons une classification des relationsW ( f, g),
nécessairement très spo-radiques, qui les définissent. Dans le cas de difféos tangents à l’identité, les générateurs jumelés f, g sont génériquement divergents, mais résurgents, accéléro-sommables, et ils possèdent des dérivées étrangères remarquables.
Annales de la Faculté des Sciences de Toulouse Vol. XIII, n° 3, 2004 pp. 291-376
Contents
1 Introduction. Intertwined
mappings
and boundgroups293
1.1 Interwined
mappings
and bound groups ... 293 1.2 Motivations ... 294 1.3 Reminders about local diffeos of C ... 295(*) Reçu le 29 août 2003, accepté le 14 janvier 2004
(1) CNRS et Univ. Paris-Sud, Dépt. de Math, Bât. 425 Univ. Paris-Sud, 91405 Orsay Cedex, France.
E-mail: [email protected]
(2) Univ. Paris Sud, Mathématiques, 91405 Orsay, France.
E-mail: [email protected]
1.4 Free groups and
algebras
... 2971.5
Campbell-Hausdorff type
formulae ... 2981.6 General notations ... 299
1.7 Outline of the paper ... 299
2 Some group
theory.
Alternators and word factorisation. Periodicautomorphisms
... 3002.1 Filtrations and
gradations
on Gr and Lie... 3002.2 Finite criteria for alternance
(dl, d2)
... 3032.3
Low-complexity
alternators. Measures of word com-plexity
... 3042.4 Periodic
automorphisms
of Gr ... 3053
Identity-tangent
twins:twenty typical examples
.... 3073.1
Collapsors
and divisors ... 3073.2 Normal-conormal form of twins. Connectors ... 309
3.3 Main
types
oftwin-begetting
relatorsW(A, B)
... 3113.4 Basic
examples
... 3113.5
Examples
with built-insymmetries
... 3223.6 Further
examples
... 3314 Some Lie
theory. Active/passive subalgebras.
Divisors and universal kernels ... 3344.1 The
active/passive
filtration ofLie[a, b]
... 3344.2 Dimensions ... 338
4.3 Universal constraints ... 340
4.4
Lagrangian
constraints ... 3414.5 Power constraints ... 343
4.6 Proofs ... 344
5
Generic, low-complexity identity-tangent
twins .... 3465.1 Finite co-dimension. The
general picture
... 3465.2 Fixed ratio
p/q
and no continuousparameter
... 3475.3 Fixed ratio
p/q
and one continuousparameter
.... 3485.4 Free ratio
p/q
and one continuousparameter
... 3496 Non
identity-tangent
twins ... 3516.1 Twins
of tangency (0, q)
... 3516.2
Simple examples
... 3526.3 Twins of
tangency (0, 0)
... 3546.4
Simple examples
... 3546.5
Pre-identity-tangent
’twins’:type (0*,0*)
... 3546.6
Simple examples
... 3556.7
Siblings
... 3556.8
Simple examples
... 3577
Analytic
nature of twins ... 3587.1
Multiplier lai i-
1: convergence ... 358- 293 -
7.2
Multiplier lai
= 1:divergence
... 360 7.3Pre-identity-tangent
’twins’: convergence ... 360 7.4Identity-tangent
twins: thegeneral picture
... 3617.5
Identity-tangent
twins: autonomous differential-difference
equations
and double resurgence ... 362 7.6Identity-tangent
twins: canonical accelero-summability
... 366 7.7Identity-tangent
twins: ’shadow twins’ and obstruc-tions to
analyticity
... 366 8 Transserial twins ... 3678.1 Reminders about transseries ... 367 8.2 Transserial twins of
exponential
ortransexponential
type
... 369 8.3 Van der Hoeven’s intermediate value theorem ... 370 8.4 Canonical resummation of transserial twins ... 370 8.5 Theordering
of free or bound groups. Natural andexotic orders.
Ultraexponential
arbitration ... 372 9 Conclusion: settledpoints,
openquestions
... 373References ... 375
1. Introduction. Intertwined
mappings
and bound groups 1.1. Interwinedmappings
and bound groupsThe
mappings
we shall be concerned with aremainly
the localdiff eo- morphisms (or "diffeos"
forshort)
of C(with
either x = 0 or z = 00 asfixed
point)
as well as theirformal counterparts.
More to thepoint,
we shallbe
looking
for "intertwinedmappings",
i.e. forpairs (f,g)
of diffeos(or
"twins")
thatgenerate
a ’bound’ groupG{f,g}, by
which we mean a groupthat is
(i) non-free,
i.e notisomorphic
to thetwo-generator
free group(ii)
non-abelian(iii) non-elementary,
i.e. notconjugate
to a group ofhomographies.
The last
requirement
is there to rule outuninteresting
situations. Itmeans that no local
change
ofvariable,
whetheranalytic
orformal,
unrami- fied(x
~ cx + ···; z ~a z +···)
or ramified(x
~c xn +···;
z ~a zn +···)
should turn
f and g simultaneously
into apair
of"homographies"
or"möbius
maps"
x Hax(1
+bx)-l (near
x =0)
or, if the fixedpoint
bez = oo, into a
pair
of "similitudes" z H a z + b.In order to
generate
a bound group in the above sense,f and g
must ofcourse
verify
somecomposition
relation :The
point, however,
is that most relations W forcef and g
to commute or"nearly-commute" ,
i.e. to besimultaneously conjugate
tohomographies.
Infact,
as we shall see,only finely
honed andfairly
intricate relations W canlead to suitable solutions
(f,g)
andgive
rise to bound groupsG{f,g}.
1.2. Motivations
(i) Originally,
thequestion
as to the existence of bound groups(specif- ically,
foranalytic, identity-tangent
localself-mappings of C)
wasraised in the
early
90sby
D.Cerveau,
R. Moussu and others in con-nection with the classification of local
analytic
foliations onC2
and theholonomy
of local differentialequations (see [Ce]).
Theexpecta- tion,
it seems, was that such groups didn’t exist. In1995, however,
one of us came up with a first series of
examples, namely
those listed in themid-part
of§3 (mainly §3.3).
But then thesubject
wasprovi- sionally
laid torest,
andonly recently
taken up anew forsystematic investigation.
(ii)
Another way oflooking
at the samequestion ([Ce])
isby trying
to extend the so-called Tits alternative. In its classical
formulation,
the Tits alternative
applies
tosubgroups
GC Gl (n, C)
of the linear group, and it states that- either G is
virtually solvable,
i.e. it contains a finite solvable sub- group of finite index- or it contains a free
2-generator subgroup,
which is Zariski dense.So a natural and
important question
is: does a similar alternative hold forDiff(C, 0)
and its formalcounterpart?
For thelatter,
we shall showthat the answer is no. For the former
also,
the answer is no, but theidentity-tangent
sub-case is still open.(iii) Actually,
bound groups ofmappings
are basic and naturalobjects
intheir own
right
and theirstudy requires
no elaborateapology. Indeed,
in the
one-operation-only
context of grouptheory, "being
intertwined"is for a
pair
ofmappings ( f , g)
the closestequivalent
one could think- 295 -
of to
"algebraic dependence"
for apair
of irrational numbers(a, b).
Moreover,
since twins(f,g)
are so scarce, sothinly spread
out inthe
landscape,
theirprecise shape
andproperties
are a matter oflegitimate curiosity.
(iv)
The search for twins(and
moregenerally
forsiblings,
ie "overrelated"systems
ofdiffeomorphisms;
see§6.7-8)
isclosely
bound up with thetopic
of infinite-dimensional grouprepresentations ("into")
and re-alisations
("onto").
Whereas finite-dimensionalrepresentations
andrealisations are
quite adequate
for finite groups, infinite groups(es- pecially
solvableones)
often call for infinite-dimensionalrepresenta- tions,
and inparticuliar
for realisations asspecial
groups ofmappings (local
orglobal).
(v)
Twinsprovide
astriking
illustration of theubiquity
of resurgence and the usefulness of acceleration.Indeed,
as we shallshow, although identity-tangent
twins aregenerically (and probably always)
diver-gent, they
arealways resurgent (in
a suitablechart)
and even biresur-gent,
i.e.resurgent
withrespect
to two distinct "critical times". There-fore,
to resumthem,
we must resort notonly
to the usual Borel-Laplace scheme,
but also to oneintermediary
accelerationtransform.
1.3. Reminders about local diffeos of C
Rather than
working directly
with local diffeosf :
we shall
give precedence
to the associated substitutionoperators F,
denotedby
the sameletters,
butcapitalised :
The reason is that
operators
affordgreater flexibility :
instead of onesingle operation
for diffeos(namely
thecomposition product o), operators
canbe
subjected
to fouroperations: addition; multiplication;
thetaking
of thelogarithm (or
infinitesimalgenerator)
and the Liebracketing
of infinitésimalgenerators.
But one should be mindful of the order reversal: theoperator product
FGcorresponds
to thecomposition product g
of.
Diffeos
(1.2)
with a"multiplier’
a = 1 are said to beidentity-tangent.
When a is
~
1 but a unitroot, f
is said to bepre-identity tangent (since
asuitable iterate is
identity tangent).
When neither is the case,f
is declarednon-identity tangent.
If
f
isidentity-tangent,
the substitutionoperator
F istriangular
withrespect
to the natural basis{xn} of C[[x]]. Moreover,
F -1 istriangular
witha
zero-diagonal,
and so isF*
:=log F,
but whereas F is anautomorphism
of the
algebra C[[x]]:
its
logarithm F*
is a derivation and thus of the form:The
tangency
order p( 2)
of anidentity-tangent
diffeof
is the index of the first non zero coefficient an in(1.2)
or a*n in(1.5),
which amounts tothe same, since the
leading
coefficients coincide in both series(ap
=a*p).
If
f
hastangency
order p, then under some(formal, unramified) change
of coordinate it can be
brought
to the normal form:with a well-defined iteration residue ce,, E C. As a consequence, a further
(ramified) change
of coordinate :will turn
f
into theplain
unitshif t z
~ z + 1 with the fixedpoint moving
from x = 0 to z = ~.If
f
ispre-identity-tangent,
itsmultiplier
is aprimitive
unit root a =exp(27ri p** p*)
of some order p*. So the iteratefP*
isidentity-tangent,
andf
itself can be normalised to:
with a well-defined iteration residue 03B1*, a
tangency order p
divisibleby
p* , and with Rdenoting
the rotationoperator
ofangle
-203C0 p** p*:- 297 -
Lastly,
iff
isnon-identity-tangent,
it can belinearised,
at leastformally,
i.e. normalised to
f nor (x) =
a x.Throughout
the first half of thisinvestigation (right through §5),
weshall be concerned with
f ormal twins,
without anygrowth
restriction on the coefficients an in(1.2). Only
in the second half shall we look foranalytic
twins or,
failing that,
forresurgent
ones. Butright
now, we mustbriefly
mention how
analyticity
affects the main constructspertaining
to diffeos.For
non-identity-tangent analytic
diffeosf,
thenormalising (i.e.
linearis-ing) change
of coordinate(unique
up to a linear map x ~c x)
isalways analytic, except
if themultiplier
a off
is of module 1 andLiouvillian,
which in this context means that it violates A.D.
Bryuno’s diophantine
condition. In that case, the
normalising
map isgenerically divergent
andnon-resummable.
For
identity-tangent (or pre-identity-tangent) analytic diffeos,
on theother
hand,
both thenormalising change
of coordinate and the infinitesimalgenerator f *
are(generically) divergent
but(always) resurgent (with
criticaltime z =
x-P)
andBorel-Laplace
resummable. Suchdiffeos,
ontop
of theirtwo formal invariants
(the tangency
order p and the iteration residueQ*)
possess a countable
infinity
ofindependent analytic invariants,
each of whichdepends holomorphically on f (see [E2]).
All these results carry over, with
only slight changes,
to the context ofhigher-dimensional
local diffeos(i.e.
diffeos ofC03BD0),
but there is onerespect
in which one-dimensional diffeos stand out: for
them,
the set of all iteratesf w
ofcomplex
order walways
coincides with the centraliser off,
thatis,
with the set of all
diffeos g
that commute withf.
1.4. Free groups and
algebras
Let
Al(a, b) (resp. Lie(a, b)
denote the associative(resp. Lie) alge-
bra
freely generated by
twonon-commuting symbols
a andb,
with thenatural immersion
Lie (a, b)
CAl (a, b). Further,
letGr (A, B)
be thefree non-abelian group
generated by
A and B.By substituting (ea, eb)
for(A,B),
we mayregard Gr(A, B)
as amultiplicative
subset ofAl(a, b)
and
log(Gr(A, B))
as a subset ofLie(a, b),
where Al and Lie denote the naturalcompletion
of Al and Lie obtainedby allowing
infinite sums.A
polynomial function
onGr (A, B)
is a(scalar-valued)
function P ofthe form:
with
polynomial dependence
on the variables mi and ni and the natura connection condition:A subset H of
Gr(A, B)
is said to be of(polynomial)
codimension d if it is the zero locus of dindependent polynomial
functions onGr (A, B) :
If,
for each monomial c = a03BC1 b03BD1 ··· aJ-Ls b03BDs inAl (a, b)
and each ele mentW(A, B) -
Am1 Bn1 ··· Ams Bns inGr(A, B),
we definePc(W
as the
(rational)
coefficient of c in the naturalexpansion
ofW(ea, eb)
the]the
aggregate
of all thesePc clearly
constitutes acomplete
butnon-free
seof
polynomial
functions onGr ( A, B).
But if welet,
runthrough
somebasis
(eg Lyndon basis)
ofLie (a, b)
and defineP*03B3(W)
as the coefficien oflog(W(ea, eb)) along
the basis vector 03B3, then thesePi yield
a set opolynomial
functions onGr(A, B)
that is stillcomplete
butfree
as well.1.5.
Campbell-Hausdorff type
formulae We shall make constant use of the notations:We shall also
require
theCampbell-Hausdorff
formula :along
with these two variants:- 299 -
where the first term in the
sum E (corresponding to j = 1)
has to beinterpreted
as ar ... a3 al a2 al or,equivalently,
as 2013r ··· a3âi
a2.1.6. Général notations
Boldface symbols
shall be reserved almostexclusively
forfree
structures(groups,
associativealgebras,
Liealgebras)
and their elements. Plain sym- bols shall be used for boundstructures,
such as thegroup 9 (resp. 9)
ofall formal
(resp. analytic)
localdiffeomorphisms
of C. As arule,
the twid-dle N shall
signal formalness (as opposed
toanalyticity)
inseries, diffeos,
differential
equations
etc. But inpractice,
to avoid unnecessaryclumsiness,
the twiddle will mark
only
sets(such
asg)
and seldom their elements( f ,
g
etc.), except
whenstrictly indispensible,
for instance whenever we mustcarefully distinguish
between adivergent
formal powerséries
and its(not necessarily unique)
sums ~ obtainedby
various resummationprocedures.
As
already pointed out, diffeomorphisms
shall be denotedby
small lettersf,
g,etc,
while thecorresponding
substitutionoperators F, G, etc,
shallalways
becapitalised.
Forexpediency,
both willusually
be referred to as"diffeos".
1.7. Outline of the paper
The
paper’s
first half is devoted to the construction off ormal
twins. Af-ter some
group-theoretic
reminders(§2),
we gothrough
a series ofeasy-to-
construct
examples (§3)
illustrative of the maintypes
of(identity-tangent)
twins.
Then,
after a Lie-theoretic excursion with some novel material(§4),
we
attempt
a reasonablesystematisation (§§5, 6),
asopposed
to an exhaus-tive one
which,
as we shall see, iscompletely
out of reach. For each of theleading
twintypes,
wecarefully
indicate thesimplest defining
relationsW,
i.e. those with lowest
(polynomial)
codimension or with other low "com-plexity
indices". We then sketch a naturalgeneralisation:
bound groups with more than twogenerators ("siblings".)1
(1) A section devoted to yet another generalisation - bound groups consisting of higher-
dimensional diffeos - was scrapped for lack of space.
In the next section
(§7)
weinvestigate
theanalytic
nature of the twins constructed thus far. Since the solutions(F, G)
of anyequation W(F, G)
= 1are defined
upto
a simultaneousconjugacy:
the
pertinent question
isnot,
of course, whether thegeneral
solution con-verges, but rather: how
simple
can thepair (F, G)
be made in a suitablechart? Or
again:
howsimple
does F(resp. G)
become after its twin G(resp. F)
has been normalised? Fornon-identity tangent twins,
it is rathereasy
(by applying
thetheory
of the so-called "sandwichequation" )
to showthe
generic analyticity
of well-chosenrepresentatives (F, G).
Foridentity- tangent twins,
theposition
isexactly
the reverse: we establish theirgeneric divergence
and resurgence. It would even seem thatidentity-tangent
twinsare
always divergent
andalways resurgent,
but aregular proof (especially
of the
former)
appears to be along
way off.The
last,
verysketchy
section(§8)
discusses twins in thelarger setting
of transseries and
analysable
functions(as opposed
to power series andanalytic
orresurgent germs)
and broaches a number ofside-issues,
such asthe
ordering
of freegroups. 2
2. Some group
theory.
Alternators and word factorisation.Periodic
automorphisms
In this
section,
Gr and Lie will stand forGr(A, B)
andLie(a, b),
i.e.will denote the
two-generator
free group resp. Liealgebra.
2.1. Filtrations and
gradations
on Gr and LieThe
algebra
Lie has anelementary gradation
intohomogeneous
compo- nentswith
Lie[d] (resp. Lie[d1,d2]) spanned by
multicommutators ofglobal degree
d
(resp.
ofdegree dl
andd2
in a andb).
Thecorresponding
dimensions are (2) Another such side-issue, originally meant for inclusion in this paper, has been removed for lack of space and redirected to[EV2].
It asks: what is the "proper" andmost "comprehensive" notion of analyticity on free algebras
(Lie
orassociative)?
We rephrase the question so as to give it a clear-cut meaning. Then we solve it and come up with a startling, quite counter-intuitive answer.-301-
given by
classical formulas:03BC(2022) being
the classical Môbiusfunction.3 Going
with thatgraduation
whave the filtration:
with the obvious commutation inclusions.
As far as the
algebra
Lie isconcerned,
thegradation
is theprimary
notion and the filtration rather derivative. But with the group Gr the po- sition is
exactly
the reverse.Moreover,
we seem to have the choice between twoalternative, a priori non-equivalent
definitions for the filtration on Gr.According
to thefirst definition, Gr Idj (resp. Gr{d1,d2})
issimply
the setof all
W(A, B)
in Gr whose natural Lieimage
lies in
Lie{d} (resp. Lie{d1,d2}).
This defines afiltration,
i.ebecause the
Campbell-Hausdorff
formula(1.19)
for bracketsinvolves,
on itsright-hand side, only
terms ofdegree
1 in a and b.Then we have a second definition
(provisionnally distinguished by
dou-ble
braces) according
to whichGr{{d}} (resp. Gr{{d1,d2}})
is thesubgroup generated by
all multicommutators ofalternance
d(resp. (di, d2)).
Wespeak
here of "alternance" rather than"degree"
topreclude
any confusion with the"degree"
of a wordW(A, B).
A multicommutator of alternance d is of course one withexactly
darguments (which
we may take to beA±1
(3) Recall that
03BC(n) = (-1)s (resp 0)
if n is quadrat-frei and a product of s distinct primes(resp otherwise).
or
B±1)
and a multicommutator of alternance(dl, d2)
is one withexactly dl arguments
Ami(or A±1)
andd2 arguments
Bn2(or B-1:1).
The reasonwhy
we may assume allexponents
mi and ni to be ±1 is thatby repeated
use of the Witt-Hall identities:
we may break up any multicommutator into a
product
of multicommutators withequal (or greater) alternance,
but witharguments
of the formA±1
orB±1.
Clearly,
theGr{{d}}
andGr{{d1,d2}}
define a new filtration onGr,
i.e.the inclusions
(2.7)
extend to the double-bracedGr{{···}}.
But in fact:PROPOSITION 2.1. - The two natural
filtrations
on Gr coincide:COROLLARY 2.2. - The
quotients:
make sense
(since
the groupsright of
the slash aredistinguished subgroups of
those
left of the slash)
anddefine
abelian groupsGr[d]
andGr[d1,
d2] that areisomorphic to Lie[d]
andLie[d1,d2] (or
rather to their additive submodulesspanned by multicommutators).
Proof.
- The inclusionsGr{···} ~ Gr{{···}}
aretrivial,
since formula(1.20)
carries on itsright-hand
sideonly
multicommutators ofdegree
1 ineach of the variables ai. The reverse
inclusions, however,
areby
no meansobvious. The one
involving
the"global" filtration, namely Gr{d}
CGr{{d}},
is a classical result
by
P. Hall(see [L.S]),which
involves much more thandabbling
with the Witt-Hall identities(2.8), (2.9), (2.10). Fortunately,
it isbut a short
step
from this inclusion to the moreprecise
inclusionGr{d1,d2}
CGr{{d1,d2}}.
Infact,
all it takes isproving
thefollowing:
- 303 -
LEMMA 2.3
(WORD FACTORISATION). -
For eachW (A, B)
inGr{d}
(d 1)
and eachpair (d1(2022), d2(2022)) of ’complementary’ permutations of {1,...,
d -11 (i. e. permutations
such thatd1(i)
+d2 (i)
~d),
there exists a(non-unique) factorisation:
The
argument being
much the same for allpermutations,
let us checkthis for
dl (i)
= i. Due to the inclusionGr Idj
CGr{{d}}
andby repeated
useof the Witt-Hall
identities,
we canproduce
a factorisation W =VI V2 ... Vs
with
elementary
factorsVy
of alternance(d’j,d"j)
in(A, B) with d’j + d"j
d. Set l5 ==
inf dj
and write W =P Q Vj R,
with P -V1 V2 ... Vj1
regrouping
all factorsVj (if any)
with alternance l5 in A andalready
infront
position;
withVj1 denoting
the first factor(if any)
with A-alternance l5 but not in frontposition;
and withQ regrouping
allremaining
factors.This leads to a new factorisation:
with a
factor {Vj1, Q-1}Q
which in turn may be broken up intoelementary
factors
vj
of A-alternance > 2 J.By repeating
the process for theremaining
factors
V j1’ Vj2,
etc.(i f therebesuch)o f A -
alternance03B4 inQ,
we can moveall these factors into front
position;
and the all factors with A-alternance03B4 + 1, 03B4 + 2,
etc.This proves the
lemma,
which we may nowapply
to wordsW ( A, B)
inGr{d1,d2},
in which case thedecomposition (2.15)
will reduce toonly
onenon-trivial
factor,
thatsingle
factorbeing
inGr{{d1,d2}}. So Gr{d1,d2}
CGr{{d1,d2}},
whichcompletes
theproof
ofProposition
2.1. Thecorollary
about the structure of
Gr[d]
andGr[dl,d2]
is then an easy consequence. D2.2. Finite criteria for alternance
(dl, d2)
Each
subgroup Gr Idl
hasfinite
codimension in Gr(see §1.4).
Infact,
itscodimension is
exactly lie(2)+···+lie(d-1). But,
save for(di, d2) = (1,1),
each
subgroup Gr{d1,d2}
hasinfinite
codimension.Indeed,
if we goby
the(first)
definition ofGr{d1,d2}, checking
that agiven
wordW (A, B)
is inGr{d1,d2} implies checking infinitely
many"polynomial"
identitiesP(W) =
0 of type (1.12).
Fortunately,
there exist criteriainvolving
a finite number ofsteps. First,
observe that any
W ( A, B)
inGr{1,1}
may be written in aunique
way as finiteproducts
of factorsAn :=
Bn A B-n orBm :=
A"2 B A-’:LEMMA 2.4. -
W(A, B)
is inGr{d1,d2} ((d1, d2)
>(1, 1)) if
and onlif :
The
symbol
0 means that theright-hand
sides are of totaldegree di (or d2)
in the an2(or bmj) regarded
as freeindependent
variables. The lemmadirectly
follows from the fact that within thealgebra
Lie{a, b}
(i.e.
in the ’closure’ derived from Lie{a, b} by allowing
infinitesums),
thesubalgebras
Lie{an1, ans1}
or Lie{bm1, ..., bms2} finitely generated by
afinite
number of distinct elements an orbm:
are themselves
free. So, checking
thatW (A, B)
has alternance(dl, d2)
involves
only
a finite number ofsteps which, however, steeply
increaseswith 81 and 82.
2.3.
Low-complexity
alternators. Measures of wordcomplexity
Let us
apply
the above criterion to words of the form:with
indices j regarded
as elements ofZr
:= Z/
r Z. For r =3,
we find thatW (A, B)
hasalternance (1, 3)
iff:and alternance
(2, 3)
iff A = 1- 305 -
Similarly,
for r =4,
the wordW (A, B)
hasalternance (1, 4)
iff:and alternance
(2,4)
iff T = -1. In the case r ==3,À = 1,
we may take:(n1, n2, n3) = (n’2, n’3, n’1)
=(-1, -1, 2)
in which case the(2, 3)-alternator W(A, B)
has afairly simple
commutator factorisation:but otherwise the
simplest
words with alternance(dl, d2)
tend to be muchsimpler
than theirsimplest expressions
in terms of multicommutators(of
the same
alternance).
There exist of course many ways of
measuring
the"complexity"
of aword
W (A, B) - 03A0(Ami Bn2),
but we shall useonly
thefollowing
fourcomplexity
indices:(i)
thelength, global
orpartial:
(ii)
the numberof alternatzng
monomials Am2 or Bmi(iii)
the variancevar(W) (resp. varA(W)
orvarB(W)),
defined as thenumber of distinct
pairs (mi, ni) (resp.
as the number of distinct values assumedseparately by mi
orni ) whereby mj
:= m1 +··· mjand nj : = n1 + ··· nj
(iii)
the alternancealt(W) (resp. (altA(W), altB(W)))
defined as thesmallest d
(resp. (di, d2))
such that W be inGr{d} (resp. Gr{d1,d2}).
In the usual
graphical representation
ofwords,
the first threecomplexity
indices are immediate to
detect,
but not so thealternance,
which doesn’t’meet the
eye’,
at least whendl
+d2
3.2.4. Periodic
automorphisms
of GrLet
Aut(Gr)
denote the group of allautomorphisms
of Gr. It is known(Nielsen’s theorem)
to begenerated by
threeelementary automorphisms:
For the
sequel,
we need toknow,
up toconjugacy,
all thefinite subgroups
of
Aut(Gr)
and inparticular
all itsperiodic (unipotent)
elements.LEMMA 2.5
(PERIODIC
AUTOMORPHISMS OFGr). - They necessarily
have order
1,2,3,4,
the numberof
distinctconjugacy
classesbeing
respec-tively 1,4,1,1.
Each involution(order 2)
isconjugate
either to(A, B) (B, A)
or(A, B) ~ (A-1, B) or (A, B) ~ (A-1, B-1)
or(A, B) ~
(B-1, A-1).
Eachautomorphism of
order 3 isconjugate
to(A, B)
(B-1, AB-1).
Eachautomorphism of
order 4 isconjugate
to(A, B) ~
(B-1, A).
For a
proof,
see[L.S.], prop.4.6, p25,
and the references thereafter.Now that we have the list of all
periodic automorphisms,
it is an easy matter to construct allnon-cyclic
finitesubgroups
ofAut(Gr).
There arefour of them
(upto conjugacy), namely
the two abelian groups of order 4:and the two non-abelian groups of order 6 and 8:
whose elements P are listed
below,
in terms of their action P : W ~Wpon
words:
Note that the
composition
law follows from the rule(W pl )p2
=W(P1P2)
(beware
of the properorder).
Thus:- 307 -
3.
Identity-tangent
twins:twenty typical examples
3.1.
Collapsors
and divisorsOur aim in this section is to
produce examples
ofidentity-tangent
twinsthat cover all the main
possible
situations andyet
remain easy to construct.But this ease of construction cornes at a
price:
itusually
entails severe com-plexity.
It also involveshighly non-generic
relationsW(F, G)
==1,
with thecorresponding
wordsW (A, B)
neverranging
over subsets of finite codi- mension inGr{A, B}.
Fortruly generic examples
and finitecodimensions,
we shall have to wait
for §5.
As in most of this paper, we shall have to work
simultaneously
in thefour structures:
go
is the group offormal, identity-tangent
diffeosf : x ~ x {1 + 03A3anxn},
usually
denotedby
thecorresponding
substitutionoperators
F.CO
is theLie
algebra
of0,
with its natural basis elements:The map F ~
F*
:=log F
fromgo
intoÊo
isone-to-one,
but the in-jective
mapW(A, B) ~ w(a, b)
=log W(ea, eb)
fromGr{A, B}
intoLie{ a, b}
is of course far fromsurjective. Among
the maps fromLie{a, b}
into
Êo, deserving
ofspecial
attention are thegraded morphisms (i.e.
whichrespect
the naturalgradation
of bothalgebras)
and arenecessarily
of theform:
Perhaps
thequickest
way toproduce
twins ingo
is to consider mul- ticommutatorsW(A, B) (with
alternance(dl, d2)
>(1, 1))
whose cornercomponent wo (a, b) (defined
as thehomogeneous component
ofw (a, b)
that lies in
Lie[d1,d2])
has thefollowing
threeproperties:
(i) wo (a, b) ~
0.(ii)
It is acollapsor,
i.e. itbelongs
to the kernel of some(or all) graded
morphisms
of Lieinto 0:
(iii)
Its divisor D is~
0 for all t in N*. The divisorD(t) - D(p,
q;t)
is apolynomial
in t characterised(for
all p, q such thatwo(lp, lq) = 0) by
the
identity:
which makes
good
sense, since theright-hand
of(3.5)
is apriori
ofthe form:
but
necessarily
vanishes when we take:Divisors owe their name to the fact
that,
whensolving
theequation W(F, G) =
1through
coefficientidentification,
one has to divideby D(t)
at the t-th inductive
step.
And thecollapse’ (3.4)
is necessary toget
the induction started.Now,
acheap (if wasteful)
way toget
words W with those three prop- erties is to take them of the form W ={U, V},
where U and V are them-selves multicommutators with
non-proportional
cornercomponents
uo, vo and with distinct(resp. identical)
alternance whichgenerally
leads to twinswith a fixed
(resp. free) tangency
ratioplq.
The actual
expression
of the divisors shall of course involve the structure constantsT.
of thealgebra Co:
which are
explicitely given by:
We shall also make
frequent
use of theidentity:
which
immediately
results fromapplying
the derivationad(lt)
to both sidesof (3.6).
- 309 -
3.2. Normal-conormal form of twins. Connectors
Since
knowing
apair
of twins(F, G)
is the same asknowing
their in-finitesimal
generators (F*, G*),
we shall often work with thelatter,
for thegreater fiexibility they
afford. And since thesepairs
are defined up to acommon
conjugacy,
we shallprivilege
"normal-conormalforms",
which nor-malise one of the twins to
F*nor (resp. G*nor)
while the other assumes arigidly
fixed conormal formG*conor (resp. F;onor). Actually,
forcomplete rigidity
we have to demand thatF*conor
andG*conor
should contain no termof the form
lp+q
ifF*
starts withlp
andG*
withlq.
In the most
typical examples,
thesenamely
withexactly
oneparameter
(other
than the ratiop/q,
which isdiscrete),
we shall find that:with a countable
infinity
of invariants:Another
object
of centralimportance,
on account both of its invariancand
(anti)symmetry
in(F, G),
is the connector Hnor =expH,,nO’r
whiclconjugates
the normal to the conormal forms:but which may also be constructed
directly
from any solution(F, G) by
setting:
The connector Hnor is
uniquely defined, provided
we normalise itby
im-posing
the absence inH*nor
of termslp
andlq.
In the mosttypical (one-
continuous
parameter) examples,
we shall see that the connector assumesthe form:
In this case, the
secondary
invariants{03B1(m,n)}
or{03B2(m,n)}
or{03B3(m,n)},
to-gether
with theprimary
invariants(03B1, 0)
and(03B1*, 03B2*)
and(p, q),
constitutea
complete
andfree
set ofjoint
invariants for thepair (F, G).
The three setsof
secondary
invariants areclearly equivalent.
Indeed for m + n 2:with the condition m + n 2
excluding
the terms:and
ensuring
that theleading
factors in(2.19), (2.20), (2.21) be i- 0, oo.
The invariants
(a, {3)
in the firstpair
ofprimary
invariants have a sepa- rate existenceonly
if we restrict ourselves toidentity-tangent conjugacies.
Ifwe
accept conjugacies
with amultiplier k’(0) ~ 1,
then there remainsonly
one
invariant, namely
the ratio:Similarly,
thetangency
orders(p, q)
lose their invariance if weaccept
rami-fied conjugacies
and thereonly
remains thepair (p*, q*)
ofcoprime
numbersproportional
to(p, q).
On the otherhand,
the thirdpair (03B1*, 03B2*),
as wellas all the
secondary
invariants{03B1(m,n)} {03B2(m,n)},
possessstrong invariance,
since
they
remain unaffected evenby non-identity-tangent
or ramified con-jugacies.
- 311 -
3.3. Main
types
oftwin-begetting
relatorsW(A, B)
Our first series of
examples (3.1 through 3.9)
illustrates two basic di- chotomies :- the twins
(F, G) verifying
agiven
relationW (F, G)
= 1 may have a fixedor free
tangency
ratiop/q
- or
again,
their continuousparameter
c(constructed
from theleading
co-efficients : see
(3.22))
may be fixed or free.The second series of
examples (3.10 through 3.20) imposes
additionalsymmetries
on twins. Moreprecisely,
for each of the 10 basic finite groupsAuti
ofautomorphisms
ofGr{A, B},
we construct relationsW(F, G) -
1whose set of non-trivial solutions
(F, G)
isglobally
invariant underAuti.
Our third series of
examples (3.21 through 3.23)
deals with more excep- tionalsituations,
e.g. with relationsW (F, G)
= 1 whosegeneral
solution(F, G) depends
on several continuousparameters
withfixed
or variable po- sitions(i.e. parameters making
their "firstappearance"
inside coefficientsof fixed
or variabledepth t). They
also illustrate relatedquestions
such asthe
glueing
orsplitting
of relators.3.4. Basic
examples
Example
3.1(Fixed
ratiop/q,
no continuousparameter)
- If we setthen for each s E
N*, W(F, G)
= 1 has aunique (upto conjugacy)
twinsolution
(F, G)
withtangency
orders(p,q) = (s, 2 s)
and fixed invariants c, 03B1*,03B2*.
Proof.
- Let us look for a solution(F, G)
withtangency
ordersp i-
q.We may write the infinitesimal
generators (F*, G*)
in the form:Then if we set:
we find
by
theCampbell-Hausdorff-like identity (1.20):
Moreover,
since U and V have as cornercomponents:
the series in
U* and V*
have initial coefficients:and current coefficients of the form:
with
In view of
(2.28); (2.29)
theidentity W (F, G)
= 1clearly implies
M =N,
which in turn
implies (p,q) = (s, 2 s).
It alsoimplies
thevanishing
of thefirst coefficient in
W* :
which