A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
M ARCO B RUNELLA
On the discrete Godbillon-Vey invariant and Dehn surgery on geodesic flows
Annales de la faculté des sciences de Toulouse 6
esérie, tome 3, n
o3 (1994), p. 335-344
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- 335 -
On the discrete Godbillon-Vey invariant
and
Dehn surgery
ongeodesic flows
MARCO
BRUNELLA(1)
Annales de la Faculté des Sciences de Toulouse Vol. III,
n°3,
1994RÉSUMÉ. - On donne une methode pour construire des surfaces sec-
tionnelles pour le flot géodésique d’une surface fermee a courbure nega- tive, et dont l’application de premier retour est semi-conjuguee a un dif- féomorphisme torique Anosov . Cette construction est utilisée pour mon- trer que l’i.nvariant discret de Godbillon-Vey
[GS]
n’est pas un invarianttopologique, même quand on le restreint a
PL+ (S1).
Une variation de cette construction permet de construire des exemples de flots d’Anosov transitif lies a(BL~.
.ABSTRACT. - We give a method to construct surfaces of section for the geodisic flow on a negatively curved closed surface, with first return map semiconjugate to a toral Anosov diffeomorphism. This construction is used to prove that the discrete Godbillon - Vey invariant
[GS]
is not a topological invariant, even when restricted to A variation onthat construction produces examples of transitive Anosow flows related to
[BL].
Introduction
Let be the group of orientation
preserving piecewise
linearhomeomorphisms
of the circleS1
= The discreteGodbillon-Vey
class[GS]
is the class GV EH2(PL+(Sl), !R) represented by
the2-cocycle
~ * ~ Reçu le 21 o ct obre 1993
~ ) Dipartimento di Matematica, Piazza di Porta S. Donato 5, Bologna
where,
if h E denotes theright (left)
derivativeof h at the
point
x ESl.
.If ~ : G --; is a
representation
of a group G into we can setwhere
+* :
:IR)
--~H*(G, IR)
is the map inducedby
+. Inparticular,
if G is the fundamental group of a closed oriented surfaceEg
ofpositive
genus g, then we canidentify GV(+)
with the real number obtained from the canonicalisomorphisms HZ (~9) , IR) ^_~ H2 (E9, IR)
^_~ IR. Thisreal number is the discrete
Godbillon-Vey
invariant of therepresentation
+ --;
Let A E
IR+
and let be thesubgroup of PL+(Sl) composed by homeomorphisms
h such that E E7L~
at every differentiablepoint.
The discreteGodbillon-Vey
invariant of arepresentation + :
--~ is then an
integral multiple
of(1/2) (log a) 2.
In[Ghy]
(see
also[Ha2], [HM]),
E.Ghys
constructs tworepresentations
which are
topologically conjugate
but which have differentGodbillon-Vey invariant;
theproof
of this secondproperty
is based on the fact thatÀi
andÀ2
are different so that -The aim of this note is to prove that even restricted to the discrete
Godbillon-Vey
invariant is not atopological invariant,
at least forsome À.
THEOREM . - There ezist À E
IR+
and tworepresentations
which are
topologically conjugate
and which havedifferent
discrete Godbil-lon-Vey
invariant.The
proof
of this result isstrongly inspired
from~Ghy~ :
ourrepresenta-
tions03A6j
aretopologically conjugate
to therepresentation (into Diff~+ (S1))
corresponding
to the stable foliation of thegeodesic
flow onF409
w.r. to anhyperbolic
metric. The mainstep
is the observation that thegeodesic
flowon an
hyperbolic
surfaceE9, g > 2,
admits twoessentially
different surfaces of section of genus one: the one introducedby
BirkhofF([Fri], [Ghy])
andanother one which we describe in Section 2. We
give
adescription
of thesesurfaces of section which is a little different from that
explained
in[Fri];
this will lead to the
digression
of Section3,
where we construct transitiveAnosov flows which admit a transverse torus which is not a
global
crosssection
(compare [BL]
for otherexamples).
1. The surface of section of Birkhoff
Let
Eg
denote a closed oriented surface ofgenus g 2:
2equipped
withany
hyperbolic
metric.Let 03C6t : T103A3g
~T103A3g
denote the(Anosov) geodesic
flow on the
unitary tangent
bundle of~9.
Thetopological equivalence
classof
~t
does notdepend
on the chosenhyperbolic
metric.Let the collection of
simple
closed orientedgeodesics
on:Eg
shown in the
following picture:
Fig. 1
The
geodesics ~ ~y3 } 2g i 2 (~-y~
=’Y~, -’y~
=’y3
with reversed orienta-tion)
lift toT1Eg
to4g -~ 4
closed orbits of the flow which we will denoteby ~~~ ~2912 projects
onto~y~).
These closed orbits areboundary
of a
surface of
section 6’ for ’S’ is an embedded surface in with 8S = transverse to~t
and every orbit of~t
intersects 5 in auniformly
bounded time. This surface 5~ can be described in two ways.Description 1 ( ~~i~ ~. composed by
fourTake two of these
(2g
+2)-gons,
such that their closures intersectonly
incorrespondence
of theirvertices,
and fill them with two foliationsby strictly
convex circles with a
centre-type singularity.
Then S is the closure of theset of
unitary tangent
vectors which aretangent
to these convex circles. Itis easy to see that S is a torus with
4g ~- 4
holes.Description
2. - Each y3 has a naturalcoorientation,
inducedby
theorientations of
Eg
and y~. Forevery j
=1,
...,2g
+ 2 letCj
be the setof
unitary tangent
vectors atpoints of yj
which arenon-negative
w.r. tothe coorientation
of Ij.
EachCj
is a closedcylinder,
boundedby I‘3
andrj;
it intersects andalong segments
and does not intersectthe other
Ci’S; J Cj
is transverse to A surgeryalong Cj
n asdescribed in
[Fri], produces
an embedded surfaceS’,
boundedby
diffeomorphic
to the torus with4g -f- 4
holes. ThisS’
is a surface of section for~t .
The two surfaces S and
S’
areisotopic rel( boundary),
theisotopy being
realized be the
flow 03C6t
itself. The flow03C6t
induces on S(or S’)
a first returnmap
f,
which issemiconjugate
to anhyperbolic
toralautomorphism ([Ghy], [Hal]).
Theconjugacy
class of theautomorphism
has been calculatedby
N.Hashiguchi (see
also[Chr]
for aparticular
case and[Ghy]
for thecomputation
of thetrace).
PROPOSITION 1
([Hal]).2014
Thefirst
return mapf defined by ~t
on thesurface of
section S istopologically semiconjugate
to thehyperbolic
toralautomorphism defined by
Let ~s be the stable foliation of
~t.
It is transverse to the fibres ofTl ~9
-->E9
and hence itcorresponds
to arepresentation
Let
a9
E(1,
be thelargest eigenvalue
ofAg.
The aboveproposition,
or more
simply
thecomputation
of.19
done in[Ghy],
has thefollowing
consequence.
COROLLARY 1 - The
representation 03A8g
istopologically conjugate
to arepresentation
The
explicit
form of~9
can be found in[Ha2].
2. Another surface of section
Let be the collection of
simple
closed orientedgeodesics
onEg
shown in the
following picture.
Fig. 2
(We
havereplaced
yl and y2 with asingle geodesic freely homotopic
to the
product
of yl andy2.~
Let
{M±j}2g+1j=1
be the closed orbitsof 03C6t corresponding
to{± j}2g+1j=1
.Then
M[ is
theboundary
of a surface of section T forwhich,
asbefore,
can be constructed in two ways.Description
1. . -Eg ~~2g+1 ~c
iscomposed by
two(2g+ 1)-gons
and one(4g + 2)-gon.
The closures of the two intersectonly
atvertices,
and the closure of the
(4g
+2)-gon
has selfintersections incorrespondence
of its vertices. We may
repeat
the construction of Section 1starting
eitherfrom foliations
by
convex circles on the two(2g + 1 )-gons,
or from a foliationon the
single (4g
+2)-gon.
Description
~ - Same construction of Section1, using cylinders
overgeodesics
.These two constructions
produce
surfaces of section which areisotopic rel(boundary )
and which arediffeomorphic
to a torus with4g
+ 2 holes.Working
as in[Hal] (see
also[Chr], [Ghy])
one obtains thefollowing
analogue
ofProposition
1. .PROPOSITION 1’. - The
first
return map hdefined by ~t
on thesurface
on section T is
topologically semiconjugate
to thehyperbolic
toral automor-phism defined by
Let vg E
~1,
be thelargest eigenvalue
ofBg.
COROLLARY 1’. - The
representation
istopologically conjugate
to arepresentation
3.
Digression:
Anosov flows with a transverse torus Let be a collection of closed oriented(hence cooriented) geodesics
onEg,
notnecessarily simple,
such that:(i) Uj r~~
has notriple point,
(ii)
every othergeodesic
onEg
intersectssome ~j
in thepositive
direction.For
example, ~r~~ }~
. can reduce to asingle "long"
closedgeodesic,
"welldistributed" in
Eg.
Then construction 2 of the
previous
two sections(construction
1 is notalways available) produces
a surface of section 0 for~t
withboundary
where
Nt
is the lift of~r~~.
It is not difficult to see that the stable foliation ~’s induces on 0 a
foliation ~
with2k*
semisaddles onN3 ,
wherek*
is the number ofpositive
intersections of with This
permits
thecomputation
of thehomeomorphism type
of0,
viaPoincare-Hopf
formula.In
particular, 0
has genus one and the first return map istopologically semiconjugate
to anhyperbolic
toralautomorphism
if andonly
forevery
j.
. This means thatevery ~j
issimple
and that(modulo reordering)
~j r1 ~i = Ø
for |j
-i|
>2, (~j-1)
intersects~j
inexactly
onepoint
andin
negative (positive)
direction.This,
inturn, implies
that~ r~~ ~
j coincideswith one of the collections or
previously
examinated(remark
that condition(ii) implies
that03A3g B ~j ~j
issimply connected).
For this reason, we don’t know how to construct other surfaces of section with first return map
semiconjugate
to ahyperbolic
toralautomorphism,
different from the two constructed above.
Because first return maps associated to surfaces of section are semi-
conjugate
topseudo
Anosovdiffeomorphism [Fri],
our constructiongives
very concrete
examples
of suchdiffeomorphisms.
Thegeodesics
which formthe
boundary
of the surface of section willcorrespond
to fixedpoints
ofthe
pseudo
Anosovdiffeomorphism,
and ageodesic
which intersects k times in thepositive
direction willcorrespond
to aperiodic point
of pe- riod k. Forinstance,
if j is asingle long
closedgeodesic,
then thecorresponding
first return map will besemiconjugate
to apseudo
Anosovdiffeomorphism
on a surface oflarge
genus whosesingular
set iscomposed by only
two(fixed) points.
A"generic"
choice of thegeodesic
will ensure thatsuch a
diffeomorphism
is not a branchedcovering
of a toralautomorphism.
Let now the collection
~ r~~ ~ ~
of closed orientedgeodesics satisfy:
(i) Uj r~3
is connected and has notriple point, (ii) J~~ = 1 for every j,
but doesn’t
satisfy
the condition that every othergeodesic
intersects somer~~
in thepositive
direction. Then a Dehn surgeryalong ~ r~~ ~ ~ 1 [Fri] , [Goo]
produces
a transitive Anosov ~ M which admits a transverse torus T but which is not thesuspension
of a toral Anosovautomorphism (compare [BL]).
Forexample,
. can be asingle
closedgeodesic
withexactly
onepoint
ofself-intersection,
or it can be a"piece"
of the collection of BirkhofF’s section(fig. 3).
Fig. 3
Remark
that,
ingeneral,
the maximalÇt-invariant
set in MB
T willbe
large,
i. e. not reduced to a finite collection of closed orbits(this
is adifference with
~BL~~.
In the secondexample above,
this maximal invariant set isisomorphic
to the set ofgeodesics (lifted
inTl
which arecompletely
contained in an handle of
Eg (the
handle to theright
in thepicture).
Ify C
Eg
is the unorientedgeodesic
whichseparates
this handle from theregion
ofEg containing ~j
~j and if CT103A3g
is itspreimage
inthen after the Dehn surgery
T.y
willcorrespond
to a torus S C M(disjoint
from
T)
with theproperties:
(a)
S contains two closed orbits yl and y2 of~t
and is transverse to~~
outside yl
u y2
;(b)
Sseparates
M in twopieces,
one of which is a"piece"
ofgeodesic
flow
(or
thegeodesic incomplete
flow on a holed torus withnegative
curvature and
geodesic boundary),
the other one isdiffeomorphic
tothe
complement
of a solid torus embedded in a torus bundle over thecircle
(more precisely,
the torus bundle whosemonodromy
isA2 )
anddisjoint
from a fiber( e.g. T)
of that bundle.Hence that
example
is a sort of connected sum between two classicalexamples
of Anosovflows,
or it is asuspension
of a toralautomorphism (A2 )
to which a handle(a piece
ofgeodesic flow)
has beenglued.
It wouldbe
interesting
to show the existence of anoperation
of"glueing
a handle"(glueing
apiece
ofgeodesic flow)
to any transitive Anosov flow.Finally,
let us remarkthat, taking ~r~3 ~
j such thatlJ~ r~~
has .~ connectedcomponents
insteadbeing connected,
we obtainexamples
of transitive Anosov flows with lpairwise
nonisotopic
transverse tori.4. Proof of the theorem
Recall that
Àg (resp. Vg)
is thelargest eigenvalue
ofA9 (resp. Bg).
. Adirect
computation
shows thata35
= v25, hence we setThe surface
~409
covers both~35
and~25.
Themultiplicity
of acovering
1~409 ~ ~35
is12,
whereas themultiplicity
of acovering ~409 ~ ~25
is 17.Let
~35 : ~ ~1 ~~35~ -~ PL+ (S1)
be therepresentation
ofcorollary
1 andits lift defined
by
t :03A3409
~03A335
.Clearly, 03A60
istopologically conjugate
to~ 409
.Let
~~ : : 7c1~~25~
--~ be therepresentation
ofcorollary
1’ andits lift defined
by j : ~409
--~~25. Also, ~o
istopologically conjugate
to~’4os
and hence to~o.
The discrete
Godbillon-Vey
invariant of+g
has been evaluatedby Hashiguchi [Ha2]:
It follows that
The discrete
Godbillon-Vey
invariant of~9
is anintegral multiple
of(1/2)(log vg~2,
and so _Because
(1728 2 ) ~ 17
is not aninteger,
wenecessarily
haveand this
completes
theproof.
,Remark. - The
geodesic
flow on~g
is obtained from thesuspension
of
Bg
:lf 2 --~ y2 through ( 1,1 )-Dehn surgeries along 4g
+ 2 closedorbits of
period 1;
the result ofHashiguchi (see
the comments at the end of the introduction of[Ha2]) suggests G’V ( ~9 ) _ - (4g
+ andconsequently GY ( ~o ) _
-1734(log À)2.
References
[BL]
BONATTI(C.)
and LANGEVIN(R.) .
2014 Un exemple de flot d’Anosov transitiftransverse à un tore et non conjugué à une suspension, Preprint
(1992).
[Chr]
CHRISTY(J.) .
2014 Intransitive Anosov flows, to appear on Memoirs AMS.[Fri]
FRIED(D.) .
2014 Transitive Anosov flows and pseudo-Anosov maps, Topology 22(1983),
pp. 299-303.- 344 -
[Ghy]
GHYS(E.) .
2014 Sur l’invariance topologique de la classe de Godbillon-Vey, Ann.Inst. Fourier 37, n° 4,
(1987),
pp. 59-76.[GH]
GHYS(E.)
and SERGIESCU(V.) .
2014 Sur un groupe remarquable de difféomor- phismes du cercle, Comm. Math. Helv. 62(1987),
pp. 185-239.[Goo]
GOODMAN(S.) .
2014 Dehn surgery on Anosov flows, Geometric Dynamics, SpringerLecture Notes 1007
(1981),
pp. 300-307.[Ha1]
HASHIGUCHI(N.) .
2014 On the Anosov diffeomorphisms corresponding to geodesicflows on negatively curved closed surfaces, J. Fac. Sci. Univ. Tokyo 37
(1990),
pp. 485-494.
[Ha2]
HASHIGUCHI(N.) .
2014 PL-representations of Anosov foliations, Ann. Inst. Fourier 42, n° 4(1992),
pp. 937-965.[HM]
HASHIGUCHI(N.)
and MINAKAWA(H.)
.2014 Continuous variation of the discreteGodbillon-Vey invariant, J. Fac. Sci. Univ. Tokyo 39