Title Local inverses of shift maps along orbits of ... - Osaka University
Title Local inverses of shift maps along orbits of ... - Osaka University
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<strong>Title</strong><strong>Local</strong> <strong>inverses</strong> <strong>of</strong> <strong>shift</strong> <strong>maps</strong> <strong>along</strong><br />
Author(s) Maksymenko, Sergiy<br />
Citation <strong>Osaka</strong> Journal <strong>of</strong> Mathematics. 48(2)<br />
Issue 2011-06<br />
Date<br />
Text Version<br />
publisher<br />
URL<br />
http://hdl.handle.net/11094/10155<br />
DOI<br />
Rights<br />
<strong>Osaka</strong> <strong>University</strong>
416 S. MAKSYMENKO<br />
denote by Sh(F) its image ³(C½ (V ,Ê)) in C½ (M, M). Then the following inclusions<br />
hold true:<br />
1 Sh(F)E id (F)½¡¡¡E id (F) E id (F) 0 .<br />
The idea <strong>of</strong> replacing the time in a flow map with a function was extensively used<br />
e.g. in [8, 3, 31, 12, 27, 10] for reparametrizations <strong>of</strong> measure preserving flows and investigations<br />
<strong>of</strong> their mixing properties, see also [19, §1]. Smooth <strong>shift</strong>s functions were<br />
applied in [13, 15, 16, 14, 17] for study <strong>of</strong> homotopical properties <strong>of</strong> certain infinite<br />
dimensional groups <strong>of</strong> diffeomorphisms and their actions on spaces <strong>of</strong> smooth <strong>maps</strong>.<br />
Also in [19, 18] some applications to parameter rigidity <strong>of</strong> vector fields are given.<br />
Suppose F is linearizable at each z ¾ F, see e.g. [29, 30, 32, 2, 11]. In [13]<br />
the author in particular claimed that if in addition M is compact, then D id (F) 0 and<br />
E id (F) 0 are either contractible or homotopy equivalent to the circle S 1 when endowed<br />
with W½ -topologies. Unfortunately, it turned out that in such a generality this statement<br />
fails and it is necessary to put additional restrictions on the behavior <strong>of</strong> regular<br />
<strong>orbits</strong> <strong>of</strong> F. In fact it was shown that Sh(F)E id (F) 0 and the mistakes appeared in<br />
estimations <strong>of</strong> continuity <strong>of</strong> local <strong>inverses</strong> <strong>of</strong> ³, see [13, Definition 15, Theorem 17,<br />
Lemma 32] and also Remarks 7.4 and 8.1 for detailed discussion.<br />
Furthermore, the above description <strong>of</strong> D id (F) 0 was essentially used in another author’s<br />
paper [15] concerning calculations <strong>of</strong> the homotopy types <strong>of</strong> stabilizers and <strong>orbits</strong><br />
<strong>of</strong> Morse functions on surfaces.<br />
The aim <strong>of</strong> the present paper is to repair incorrect formulations and pro<strong>of</strong>s <strong>of</strong> [13]<br />
and using [14, 19, 17] extend the classes <strong>of</strong> vector fields for which the homotopy types<br />
<strong>of</strong> E id (F) r and D id (F) r can be described (Theorem 3.5). In particular it will be shown<br />
that the results <strong>of</strong> [13] used in [15] remain true (Theorem 3.7).<br />
1.1. Structure <strong>of</strong> the paper. For the convenience <strong>of</strong> the reader and due to the<br />
length <strong>of</strong> the paper we will now briefly describe its contents.<br />
In §2 we recall the notion <strong>of</strong> <strong>shift</strong> map and review (correct) results obtained in<br />
[13]. Also notice that if a flow F <strong>of</strong> a vector field F is not global, then we can find<br />
a smooth function Ï M (0,½) such that the flow F¼<br />
generated by vector field<br />
F¼ F is global, e.g. [6, Corollary 2]. Moreover, F and F¼ have the same orbit<br />
structure, whence E(F)E(F¼ ) and D(F)D(F¼ ). Thus it could always be assumed<br />
that F is global. Nevertheless, in §10 and §11 we will consider restriction FW <strong>of</strong><br />
F to open subsets W M and compare <strong>shift</strong> <strong>maps</strong> <strong>of</strong> F and FW . The latter vector<br />
field usually generates non-global flow, therefore in this paper it is chosen to work with<br />
local flows from the beginning. In particular, the domain <strong>of</strong> <strong>shift</strong> map ³ <strong>of</strong> F changes<br />
to certain open and convex subset func(F)C½ (M,Ê).<br />
In §3 we introduce a certain class <strong>of</strong> vector fields F(M) on M and formulate the principal<br />
result <strong>of</strong> the paper: for every F¾F(M) its <strong>shift</strong> map³ is a local homeomorphism <strong>of</strong><br />
func(F) onto its image Sh(F) with respect to S½ -topologies (Theorem 3.5). It follows that
LOCAL INVERSES OF SHIFT MAPS 417<br />
Sh(F) is either contractible or homotopy equivalent to the circle, and so is the subspace <strong>of</strong><br />
Sh(F) consisting <strong>of</strong> diffeomorphisms. On the other hand, in [18] it is considered a class <strong>of</strong><br />
vector fields F¼ (M) which contains F(M) and such that for every F ¾ F¼ (M) the image<br />
<strong>of</strong> its <strong>shift</strong> map Sh(F) coincides with either E id (F) 1 or E id (F) 0 for each F ¾ F(M). Thus<br />
we obtain that E id (F) r (D id (F) r ) coincide with each other at least for all r 1 and these<br />
spaces are either contractible or have homotopy type <strong>of</strong> S 1 . As an application we prove<br />
Theorem 3.7 which extends [15, Theorem 1.3]. The rest <strong>of</strong> the paper is devoted to the<br />
pro<strong>of</strong> <strong>of</strong> Theorem 3.5.<br />
The assumptions <strong>of</strong> Theorem 3.5 imply that ³ is locally injective, therefore in<br />
order to prove this theorem it suffices to show that ³ is open with respect to S½ topologies.<br />
In §4 we present a characterization <strong>of</strong> S r,s -openness <strong>of</strong> ³ for some r, s <br />
0, (Theorem 4.2). First we describe local <strong>inverses</strong> <strong>of</strong> ³V as certain crossed homomorphisms<br />
and then show that like for homomorphisms <strong>of</strong> groups S r,s -openness <strong>of</strong> the<br />
whole map ³ is equivalent to S s,r -continuity <strong>of</strong> its local inverse defined only on arbitrary<br />
small S s -neighbourhood <strong>of</strong> the identity map id M .<br />
Further in §5 we recall notorious examples <strong>of</strong> irrational flows on the torus and<br />
some modifications <strong>of</strong> them. It is shown that <strong>shift</strong> <strong>maps</strong> <strong>of</strong> these flows are not local<br />
homeomorphisms onto their images. This provides counterexamples to [13, Theorem 1]<br />
and illustrates certain properties prohibited by Theorem 3.5.<br />
In §6 we repair [13, Lemma 28] by giving sufficient conditions for S r,s -openness<br />
<strong>of</strong> ³ to be inherited by regular extensions <strong>of</strong> vector fields.<br />
§7 summarizes the formulas for local <strong>inverses</strong> <strong>of</strong> <strong>shift</strong> <strong>maps</strong> <strong>of</strong> linear flows obtained<br />
in [13] and “reduced” Hamiltonian flows <strong>of</strong> homogeneous polynomials in two<br />
variables obtained in [19, 14]. Estimations <strong>of</strong> continuity <strong>of</strong> these formulas for linear<br />
flows were based on incorrect “division lemma” [13, Lemma 32], see Remark 7.4. We<br />
will show how to avoid referring to this lemma.<br />
§8 provides a correct version <strong>of</strong> [13, Theorem 17], see Theorem 8.2. It reduces<br />
verification <strong>of</strong> openness <strong>of</strong> ³ to openness <strong>of</strong> a family ³V i <strong>of</strong> “local <strong>shift</strong> <strong>maps</strong>” corresponding<br />
to any locally finite cover V i <strong>of</strong> M e.g. by arbitrary small smooth closed<br />
disks. The essentially new additional object here is a finite subset ¿¼¿ which appears<br />
due to the construction (8.3) <strong>of</strong> S½ -open set N and by existence <strong>of</strong> singularities<br />
for which “local <strong>shift</strong> map” is S½,½ -open but not S r,d(r) -open for some function<br />
dÏÆÆ. Without finiteness <strong>of</strong> ¿¼ the <strong>shift</strong> map ³ is open if its image is endowed<br />
with the so-called very-strong topology, [9]. This effect appears <strong>of</strong> course only on noncompact<br />
manifolds.<br />
§9 splits the “global analytical problem” <strong>of</strong> verification <strong>of</strong> openness <strong>of</strong> local <strong>shift</strong><br />
map ³V into the following two problems<br />
(i) openness <strong>of</strong> local <strong>shift</strong> map³W ,V corresponding to the restriction FW to arbitrary<br />
open neighbourhood W <strong>of</strong> V , and<br />
(ii) openness <strong>of</strong> the image Sh(F W , V ) in Sh(F, V ).<br />
Due to Theorem 8.2 the set V can also be taken arbitrary small. Hence to solve (i)<br />
it suffices to consider vector fields in Ên . Thus (i) is a “local analytical” problem. Its
418 S. MAKSYMENKO<br />
Fig. 1. D-submanifolds V and W .<br />
solutions for certain vector fields are given in §7.<br />
§10 and §11 present sufficient conditions for resolving (ii) at regular and singular<br />
points respectively (Theorem 10.1 and Lemma 11.2). In both cases the assumptions on<br />
F are formulated in the terms <strong>of</strong> dynamical systems theory, and so the problem (ii)<br />
can be regarded as a “global topological” one. In the regular case these conditions are<br />
also necessary. Moreover, in the singular case they are relevant with the notion <strong>of</strong> an<br />
isolated block introduced by C. Conley and R. Easton in [4], see Lemma 11.5.<br />
Finally in §12 we prove Theorem 3.5.<br />
1.2. Preliminaries. Put Æ0Æ0 and Æ0Æ0,½.<br />
Let M be a smooth manifold <strong>of</strong> dimension m. Glue to M a collar M¢ [0, 1) by<br />
the identity map M¢ 0 M and denote the obtained manifold by M¼ . If Mû,<br />
then M¼M. Evidently, M¼ has a smooth structure in which it is diffeomorphic with<br />
the interior Int M. Moreover M is a closed subset <strong>of</strong> M¼ and M¼û. We will call<br />
M¼ a collaring <strong>of</strong> M, see Fig. 1.<br />
DEFINITION 1.3.<br />
A closed subset V M will be called a D-submanifold if there<br />
exists an m-dimensional submanifold V¼ M¼ possibly with boundary and such that<br />
V M V¼ and the intersection MV¼ is transversal, see Fig. 1.<br />
Denote by Int V the interior <strong>of</strong> V in M. Then Int V VÒV¼ . We will also say<br />
that V is a D-neighbourhood <strong>of</strong> every point z¾ Int V .<br />
Let V M be a D-submanifold. If V M û, then V is a manifold with<br />
boundary, otherwise, V is a manifold with corners in which MV¼ is set <strong>of</strong> corners.<br />
Evidently, M is a D-submanifold <strong>of</strong> itself, and each z¾ Int M has arbitrary small<br />
D-neighbourhoods each diffeomorphic to a closed m-disk.<br />
Let N be another smooth manifold, N¼ be its collaring, and fÏ V N be a map.<br />
We say that f is <strong>of</strong> class C r , r ¾Æ0, (embedding, immersion, etc.) if it extends to a<br />
C r<br />
map (embedding, immersion, etc.) U N¼ from some open neighbourhood U <strong>of</strong><br />
V in M¼ into the collaring N¼ <strong>of</strong> N.<br />
M is C r<br />
Then it is well-known that f is C r if, and only if, the restriction fInt VÒ<br />
and all its derivatives have continuous limits when x tends to some point y¾V¼ , see<br />
e.g. [33, 28, 24, 5] for manifolds with boundary and e.g. [22, Proposition 2.1.10] for<br />
manifolds with corners.
LOCAL INVERSES OF SHIFT MAPS 419<br />
Denote by C r (V , N), r ¾Æ0, the space <strong>of</strong> all C r <strong>maps</strong> V N. Then similarly<br />
to [7] this space can be endowed with weak W r - and strong S r -topologies. If V is<br />
compact then W r and S r coincide for all r¾Æ0. For a subset X C r (V , N) denote by<br />
(X ) r W (resp. (X )r S ) the set X with the induced Wr -topology (resp. S r -topology), r¾Æ0.<br />
DEFINITION 1.4. A homotopy HÏ V¢ I N will be called an r-homotopy, (r¾<br />
Æ0), if for every t¾I the map H t H(¡, t)Ï V N is C r and all its partial derivatives<br />
in x ¾ V up to order r are continuous in (x, t). In other words, H is an r-homotopy<br />
if and only if it yields a continuous path I C r (V , N) from the standard topology <strong>of</strong><br />
I to the W r -topology <strong>of</strong> C r (V , N).<br />
Hence for every f ¾ X its path connected component in (X ) r W<br />
consists <strong>of</strong> all g¾<br />
X which are r-homotopic to f in X .<br />
Now let V 1 , V 2 be D-submanifolds <strong>of</strong> some smooth manifolds, N 1 , N 2 be two smooth<br />
manifolds, X C½ (V1 , N 1 ) and Y C½ (V2 , N 2 ) be two subsets, and FÏ X Y be<br />
a map.<br />
DEFINITION 1.5.<br />
We say that F is W r,s -continuous (-open, etc.) for some r, s¾<br />
(Y) s W .<br />
Æ0 if it is continuous (open, etc.) as a map FÏ (X ) r W<br />
<br />
Similarly we can define S r,s -continuous (-open, etc.) <strong>maps</strong> with respect to strong<br />
topologies.<br />
Notice that the statement that F is W½,½ -continuous at some x ¾ X means that<br />
for every s 0 and a W s -open neighbourhood V F(x)Y <strong>of</strong> F(x) there exist r 0 and<br />
a W r -neighbourhood U x X <strong>of</strong> x both depending on s and V F(x) such that F(U x )<br />
V F(x) . But in general such a map can be not W r,s -continuous for any r, s, see e.g. [23,<br />
p. 93 Equation (2)], and [25].<br />
2. Shift map<br />
M such that o x (0)x and<br />
is the maximal interval on which a map with the<br />
previous two properties can be defined. By standard theorems in ODE the following<br />
subset <strong>of</strong> M¢Ê<br />
dom(F) x¢ (a x , b x ),<br />
Let F be a vector field on M tangent to M. Then for every x ¾ M its orbit<br />
with respect to F is a unique mapping o xÏÊ(a x , b x )<br />
(ddt)o x F(o x ), where (a x , b x )Ê<br />
x¾M<br />
is an open, connected neighbourhood <strong>of</strong> M¢ 0 in M¢Ê. Then the local flow <strong>of</strong> F is<br />
the following map<br />
FÏ M¢Êdom(F) M, F(x, t)o x (t).
420 S. MAKSYMENKO<br />
Fig. 2. Domain dom(F) <strong>of</strong> the flow F <strong>of</strong> the vector field F(x)<br />
x 2 ddx.<br />
If M is compact, then dom(F) M¢Ê, e.g. [26].<br />
Notice that if x¾M is either fixed or periodic for F, then x¢Êdom(F).<br />
EXAMPLE 2.1. Let F(x)x 2 ddx be a vector field on Ê1 . Then it is easy to<br />
see that it generates the following local flow F(x, t) x(1 xt). Hence F is defined<br />
on the subset dom(F)Ê2 bounded by the hyperbola xt 1, see Fig. 2.<br />
Let V M be either an open subset or a D-submanifold and i VÏ V M be<br />
the identity inclusion. Denote by E(F, V ) the subset <strong>of</strong> C½ (V , M) consisting <strong>of</strong> <strong>maps</strong><br />
fÏ V M such that (i) f (oV )o for every orbit o <strong>of</strong> F, and (ii) f is an embedding<br />
at every singular point z¾VF. Let also D(F, V )E(F, V ) be the subset<br />
consisting <strong>of</strong> immersions V M.<br />
Let E id (F, V ) r and D id (F, V ) r be the path-components <strong>of</strong> i V in the spaces E(F, V )<br />
and D(F, V ) respectively endowed with the corresponding topologies W r .<br />
Denote by func(F, V ) the subset <strong>of</strong> C½ (V ,Ê) consisting <strong>of</strong> functions « whose<br />
graph¼«(x,«(x))Ï x¾ V is contained in dom(F). Then we can define the following<br />
map<br />
³VÏ C½ (V ,Ê)func(F, V )C½ (V , M)<br />
by³V («)(x)F(x,«(x)). We will call³V the (local) <strong>shift</strong> map <strong>of</strong> F on V and denote<br />
its image in C½ (M, M) by Sh(F, V ). Put<br />
¼V «¾ func(F, V )Ï d«(F)(x) 1, x¾ V,<br />
where d«(F) is a Lie derivative <strong>of</strong> « <strong>along</strong> F. Since func(F, V ) is an S 0 -open and<br />
convex subset <strong>of</strong> C½ (V ,Ê) and the map<br />
L FÏ C½ (V ,Ê)C½ (V ,Ê),<br />
L F («)d«(F)<br />
is evidently linear and S 1,0 continuous, we see that¼V is convex and S1 -open inC½ (V ,Ê).
LOCAL INVERSES OF SHIFT MAPS 421<br />
It also follows from [13, Lemma 20 and Corollary 21] that<br />
(2.1) ¼V ³<br />
1<br />
V (D id(F, V ) 1 ), Sh(F, V )E(F, V ).<br />
Lemma 2.2 ([17]).<br />
³V (¼V<br />
The following inclusions hold true:<br />
)D id(F, V )½¡¡¡D id (F, V ) r ¡¡¡D<br />
Sh(F, V )E id (F, V )½¡¡¡E id (F, V ) r ¡¡¡E<br />
If Sh(F, V )E id (F, V ) r , then ³V (¼V )D id(F, V ) r .<br />
The set ker(³V ) ³ def 1<br />
V (i V ) will be called the kernel <strong>of</strong> ³V .<br />
id (F, V ) 0 ,<br />
id (F, V ) 0 .<br />
Lemma 2.3. The following properties <strong>of</strong> <strong>shift</strong> map hold true:<br />
(1) ³V is W r,r - and S r,r -continuous for all r 0, [13, Lemma 2].<br />
(2) d(F)0 for every ¾ker(³V ), [13, Lemma 7].<br />
(3) Let«,¬¾ func(F, V ). Then, [13, Lemma 7], the following conditions are equivalent:<br />
(a) ³V («)³V (¬)<br />
(b) « ¬¾ func(F, V ) and ³V (« ¬)i V , i.e.« ¬¾ ker(³V ).<br />
(4) ³V is locally injective with respect to each <strong>of</strong> W r - or S r -topologies <strong>of</strong> func(F, V )<br />
if and only if F V is nowhere dense in V , [13, Proposition 14].<br />
(5) Suppose that V is connected and that VF is nowhere dense in V . Then, [13,<br />
Theorem 12 (2)],<br />
(a) either ker(³V )0 and thus ³V is injective. This case holds if V contains<br />
either a non-periodic point <strong>of</strong> F or a fixed point z¾VF such that the tangent<br />
linear flow T z F t on the tangent space T z M is the identity;<br />
(b) or ker(³V )nn¾ for some smooth Ï V (0,½). In this case V¢Ê<br />
dom(F), so func(F, V )C½ (V ,Ê).<br />
3. Main result<br />
Let M be a smooth manifold <strong>of</strong> dimension m. We will introduce a class F(M)<br />
<strong>of</strong> smooth vector fields F on M satisfying certain topological conditions on regular<br />
points and certain analytical conditions on singular points. The main result describes<br />
the homotopy types <strong>of</strong> the identity path components <strong>of</strong> E(F) and D(F). First we give<br />
some definitions.<br />
Recurrent points. Let F be a vector field on M and z¾M be a regular point<br />
<strong>of</strong> F, i.e. F(z)0. Then z is called recurrent if there exists a sequence t ii¾Æ <strong>of</strong><br />
real numbers such that lim i½t i½ and lim i½ F(z, t i )z. In particular, every<br />
periodic point is recurrent.
422 S. MAKSYMENKO<br />
First recurrence map. Let z be a periodic point <strong>of</strong> F, o z be its orbit, and B<br />
M be an open (m 1)-disk passing through z and transversal to o z . Then we can<br />
define a germ at z <strong>of</strong> the so-called first return (or Poincaré) map RÏ (B, z)(B, z)<br />
associating to every x¾B the first point R(x) at which the orbit o x <strong>of</strong> x first returns<br />
to B. It is well-known that R is a diffeomorphism at z, e.g. [26].<br />
Reduced Hamiltonian vector fields. Let gÏÊ2 Ê be a homogeneous polynomial<br />
<strong>of</strong> degree p2, so we can write<br />
(3.1) gL l 1<br />
1<br />
¡¡¡ L l a<br />
a ¡ Q q 1<br />
1<br />
¡¡¡ Q q b<br />
b ,<br />
1, L iL i¼ const for i i¼ , and Q jQ j¼ const for j j¼ . Denote<br />
where L i is a non-zero linear function, Q j is an irreducible overÊ(definite) quadratic<br />
form, l i , q j <br />
DL l 1 1<br />
1<br />
¡¡¡ L l a 1<br />
a ¡ Q q 1 1<br />
1<br />
¡¡¡ Q q b 1<br />
b<br />
.<br />
Then gL 1¡¡¡L a¡Q 1¡¡¡ Q b¡D and D is the greatest common divisor <strong>of</strong> the partial<br />
derivatives g¼x and g ¼y . The following vector field on Ê2 :<br />
F(x, y) g ¼y<br />
D<br />
<br />
x<br />
g ¼x<br />
D<br />
will be called the reduced Hamiltonian vector field <strong>of</strong> g. In particular, if g has no<br />
multiple factors, i.e. l i q j 1 for all i, j, then D 1 and F is the usual Hamiltonian<br />
vector field <strong>of</strong> g.<br />
Notice that dg(F) 0 and the coordinate functions <strong>of</strong> F are homogeneous<br />
polynomials <strong>of</strong> degree deg F a 2b 1 being relatively prime in the ring <strong>of</strong> polynomials<br />
Ê[x, y].<br />
“Elementary” singularities. Let F be a vector field onÊk . It can be regarded as<br />
a map FÏÊkÊk . Define the following types (Z), (L), and (H) <strong>of</strong> such vector fields.<br />
Type (Z). F(x)0.<br />
Type (L). F(x)«(x)¡ Ax, where A is a non-zero (k¢ k)-matrix, and «ÏÊn<br />
(0,½) is a C½ strictly positive function. Let 1,,k be all the eigen values <strong>of</strong><br />
A taken with their multiplicities. We can also assume that A has a real Jordan normal<br />
form. Then we will distinguish the following particular cases.<br />
(L1) ( j)0 for some j 1,, k;<br />
(L2) The real Jordan normal form has a block<br />
<br />
<br />
0 1<br />
0 1<br />
¡¡¡ ¡¡¡<br />
0 1<br />
0<br />
<br />
n,<br />
y<br />
n 2Á
LOCAL INVERSES OF SHIFT MAPS 423<br />
(L3) The real Jordan normal form has a block<br />
<br />
0 b 1 0<br />
b 0 0 1<br />
¡¡¡ ¡¡¡ ¡¡¡<br />
0 b<br />
b 0<br />
1 0<br />
0 1<br />
0 b<br />
b 0<br />
<br />
<br />
2n,<br />
n 2, b0.<br />
In all other cases A is similar to the matrix:<br />
<br />
0 b 1<br />
b 1 0<br />
¡¡¡<br />
0 b n<br />
b n 0<br />
0<br />
¡¡¡<br />
0<br />
, n 1, b j 0, j 1,, n.<br />
<br />
Then we will also distinguish the following two cases:<br />
(L4) there exists 0 such that b j ¾ for all j;<br />
(L5) such a number as in (L4) does not exist.<br />
Type (H). F(x, y)«(x, y)¡( g¼yD, g¼xD) for some strictly positive<br />
tion«ÏÊ2<br />
C½ func-<br />
(0,½), and a homogeneous polynomial (3.1) such that a 2b 12,<br />
so F is not <strong>of</strong> type (L). Again we separate the following cases:<br />
(HE) a 0 and b2, i.e. g is a product <strong>of</strong> at least two distinct definite quadratic<br />
forms and has no linear multiples. In this case 0¾Ê2 is a degenerate global extreme<br />
<strong>of</strong> g;<br />
(HS) a 1 and a 2b3, so g has linear multiples. In this case 0¾Ê2 is a degenerate<br />
saddle critical point for g.<br />
REMARK 3.1. The types (L), (H), (HE), and (HS) coincide with the ones considered<br />
in [18].<br />
Also notice that in the case (L4) almost all <strong>orbits</strong> <strong>of</strong> F are periodic, while in the<br />
case (L5) almost all <strong>orbits</strong> are non-periodic and recurrent.<br />
Regular extensions and products <strong>of</strong> vector fields. Let M, N be manifolds,<br />
GÏ M T M be a vector field on M, and F be a vector field on M¢N. Then F can<br />
be regarded as a map FÏ M¢N T M¢ T N. We say that F is a regular extension<br />
<strong>of</strong> G if<br />
F(x, y)(G(x), H(x, y)),<br />
(x, y)¾ M¢N,
424 S. MAKSYMENKO<br />
for some smooth map HÏ M¢N T N, so G is the “first” coordinate function <strong>of</strong><br />
F and does not depend on y, see e.g. [1, 32]. If H does not depend on x, so it is a<br />
vector field on N, then<br />
F(x, y)(G(x), H(y))<br />
will be called the product <strong>of</strong> G and H. Moreover, if H 0, i.e.<br />
F(x, y)(G(y), 0),<br />
then F is said to be a trivial extension <strong>of</strong> G.<br />
In the case N Ên we will also say that F is a (regular or trivial) n-extension.<br />
Evidently, a regular (trivial) m-extension <strong>of</strong> a regular (trivial) n-extension is a regular<br />
(trivial) (m n)-extension, see e.g. [32, 13]. The following simple statement is left for<br />
the reader:<br />
Lemma 3.2. (a) A trivial extension is the same as a product with zero vector field;<br />
(b) a product <strong>of</strong> vector fields is a regular extension <strong>of</strong> each <strong>of</strong> them;<br />
(c) every non-zero linear vector field is a regular extension <strong>of</strong> a linear vector field<br />
defined by one <strong>of</strong> the following matrices: a, a b , (b0), or<br />
0 1<br />
<br />
b a<br />
0 0.<br />
DEFINITION 3.3. Let z¾F and (T) denotes one <strong>of</strong> the types (Z), (L), (L1), etc.,<br />
defined above. We will say that the germ <strong>of</strong> F at z is <strong>of</strong> type (T)¼<br />
if the germ <strong>of</strong> F<br />
at z is equivalent to a regular extension <strong>of</strong> some vector field <strong>of</strong> type (T). By (T) and<br />
(T)¼<br />
we will denote the set <strong>of</strong> singular points <strong>of</strong> F or types (T) and (T)¼<br />
respectively.<br />
Evidently, a singular point can belong to distinct types.<br />
We will say that a C½ vector field F on a C ½ manifold M<br />
DEFINITION 3.4.<br />
belongs to class F(M) if it satisfies the following conditions:<br />
(a) F is tangent to M and F is nowhere dense in M;<br />
(b) every non-periodic regular point <strong>of</strong> F is non-recurrent;<br />
(c) for every periodic point z <strong>of</strong> F the germ at z <strong>of</strong> its first recurrence map RÏ (D, z)<br />
(D, z) is either periodic or the tangent map T z RÏ T z DT z D has eigen valuesuch that<br />
1;<br />
(d) for every z¾F the germ <strong>of</strong> F at z is either<br />
(£) a product <strong>of</strong> finitely many vector fields each <strong>of</strong> which is <strong>of</strong> type (L) or (H),<br />
or<br />
(££) belongs to one <strong>of</strong> the types (L1)¼ , (L2)<br />
¼ , (L3)<br />
¼ , or (H)<br />
¼ , but z is an isolated<br />
singular point <strong>of</strong> F.<br />
Thus if the germ <strong>of</strong> F at z is a regular extension <strong>of</strong> an (L4)-vector field, then F<br />
must in fact be a product <strong>of</strong> such a vector field with vector fields <strong>of</strong> types (L) or (H)
LOCAL INVERSES OF SHIFT MAPS 425<br />
only. Also notice that singularities <strong>of</strong> type (L5) are not allowed at all since they have<br />
recurrent <strong>orbits</strong>. Moreover, we will present examples <strong>of</strong> vector fields with singularities<br />
<strong>of</strong> type (L5) for which the statement <strong>of</strong> our main result fails, see the end <strong>of</strong> §5.<br />
The following theorem summarizes the results obtained in [18] and in this paper.<br />
Theorem 3.5 (cf. [13, Theorem 1] and [18]). Let F¾F(M),³ be the <strong>shift</strong> map<br />
<strong>of</strong> F, and ¼«¾ func(F)Ï d«(F)(x) 1, x¾M. Then<br />
Sh(F)E id (F) 1 , ³(¼ )D id (F) 1 .<br />
If (L)¼(HS)¼<br />
, then Sh(F)E id (F) 0 and ³(¼ )D id (F) 0 .<br />
Suppose that the closure Ò ((L1)¼(L2)¼<br />
) is compact (this is always true for<br />
compact M). Then both <strong>maps</strong><br />
³Ï func(F)E id (F) 1 , ³¼Ï¼ D id (F) 1<br />
are either homeomorphisms or -covering <strong>maps</strong> with respect to S½ -topologies. If M<br />
is compact, then the inclusion D id (F) 1 E id (F) 1 is a homotopy equivalence and both<br />
spaces are either contractible or homotopy equivalent to the circle. If F has at least<br />
one non-closed orbit, or a singular point at which the linear part (i.e. 1-jet) <strong>of</strong> F vanishes,<br />
then D id (F) 1 and E id (F) 1 are contractible.<br />
The first statement about the image <strong>of</strong> <strong>shift</strong> <strong>maps</strong> is established in [18] under more<br />
general assumptions on F. Therefore we will be proving the second part <strong>of</strong> Theorem 3.5,<br />
see §12. Notice that in comparison with [13, Theorem 1] two additional assumptions are<br />
added: “non-ergodicity” condition (like absence <strong>of</strong> recurrent <strong>orbits</strong>) and compactness <strong>of</strong><br />
certain subset <strong>of</strong> singular points. On the other hand the classes <strong>of</strong> admissible singularities<br />
for F are extended due to results <strong>of</strong> [14, 19, 20].<br />
3.6. Functions on surfaces. As an application <strong>of</strong> Theorem 3.5 we will now<br />
show that [15, Theorem 1.3] which used incorrect results <strong>of</strong> [13] remains true. Moreover,<br />
we extend the latter theorem to a large class <strong>of</strong> functions on surfaces with degenerate<br />
homogeneous singularities satisfying certain “secondary” non-degeneracy conditions.<br />
Let M be a compact surface, P be either the real line Ê or the circle S 1 . For a<br />
smooth map fÏ MP denote by f the set <strong>of</strong> its critical points. Let also S( f )h¾<br />
D(M)Ï fÆh f be the stabilizer <strong>of</strong> f with respect to the action <strong>of</strong> D(M) on C½ (M, P)<br />
and S id ( f ) be the identity component <strong>of</strong> S( f ) with respect to the W½ -topology.<br />
Theorem 3.7 (cf. [15, Theorem 1.3]). Let f ¾ C½ (M, P). Suppose that<br />
(i) f takes constant values on connected components <strong>of</strong> M and has no critical points<br />
on M;
426 S. MAKSYMENKO<br />
(ii) for every z¾ f the map f is C½ equivalent near z to a homogeneous polynomial<br />
g z without multiple factors such that deg g z 2.<br />
If M is orientable and f consists <strong>of</strong> non-degenerate local extremes only, i.e. f<br />
is a Morse map without critical points <strong>of</strong> index 1, then S id ( f ) is homotopy equivalent<br />
to the circle. In all other cases S id ( f ) is contractible as well.<br />
Sketch <strong>of</strong> pro<strong>of</strong>. It suffices to assume that M is orientable. A non-orientable case<br />
will follow from an orientable one by arguments <strong>of</strong> [15, §4.7].<br />
Similarly to [15, Lemma 5.1] using (i) and (ii) it is possible to construct a vector<br />
field F on M with the following properties:<br />
(A) d f (F)0, in particular F is tangent to M;<br />
(B) F(z)0 if and only if z¾M is a critical point <strong>of</strong> F, i.e.F f ;<br />
(C) for every critical point z¾ f there exists a local presentation fÏÊ2Ê <strong>of</strong> f<br />
in which z 0, f is a homogeneous polynomial <strong>of</strong> degree 2 and without multiple<br />
factors, and F(x, y)( f¼y , f ¼x ) is a Hamiltonian vector field <strong>of</strong> f .<br />
Then it follows from (A), (B), and arguments <strong>of</strong> [15, Lemma 3.5] that S id ( f )D id (F)½ .<br />
Notice that F belongs to class F(M). Indeed, conditions (a) and (b) are evident.<br />
Moreover, for each periodic point <strong>of</strong> F its first recurrent map is the identity, which<br />
implies (c).<br />
Finally by (C) each non-degenerate saddle <strong>of</strong> f is <strong>of</strong> type (L1), each non-degenerate<br />
local extreme <strong>of</strong> f is <strong>of</strong> type (L4), while all degenerate critical points <strong>of</strong> f are <strong>of</strong> types<br />
(H). This implies (d).<br />
Hence S id ( f )D id (F)½ is either contractible or homotopy equivalent to S 1 . If M<br />
is orientable and f<br />
consists <strong>of</strong> non-degenerate local extremes only, then f is Morse<br />
and belongs to one <strong>of</strong> the types (A)–(D) <strong>of</strong> [15, Theorem 1.9]. In this case the corresponding<br />
<strong>shift</strong> map is not injective, whence S id ( f ) is homotopy equivalent to S 1 .<br />
In all other cases ³ is injective and so S id ( f ) is contractible. Indeed, if f has a<br />
saddle critical point then F has a on-closed orbit, while if f has a degenerate local<br />
extreme z then j 1 F(z)0.<br />
4. Openness <strong>of</strong> ³<br />
Let V M be a D-submanifold. Our aim is to find sufficient conditions for the<br />
<strong>shift</strong> map ³VÏ func(F, V )Sh(F, V ) to be a local homeomorphism with respect to<br />
S½ -topologies. Since ³V is S r,r -continuous for all r¾Æ0, this is equivalent to S½,½ -<br />
openness <strong>of</strong>³V . Moreover, as³V<br />
is locally injective, we can also require that its local<br />
<strong>inverses</strong> are S½,½ -continuous and defined on S<br />
½ -open subsets <strong>of</strong> Sh(F, V ).<br />
In this section we show that S r,s -openness <strong>of</strong>³V for some r, s¾Æ0 is equivalent to<br />
S s,r -continuity <strong>of</strong> its local inverse defined only on some neighbourhood <strong>of</strong> the identity<br />
inclusion i VÏ V M in Sh(F, V ).
LOCAL INVERSES OF SHIFT MAPS 427<br />
DEFINITION 4.1. Let A be a group and S be a semigroup with unit e. Then<br />
the right action <strong>of</strong> S on A is a map £Ï A¢ S A such that «£ e « and «£<br />
( f g)(«£ f )£g for all «¾ A and f , g¾S. A map Ï S A is called a crossed<br />
homomorphism if<br />
( f g)( ( f )£ g) (g).<br />
Suppose for the moment that F generates a global flow F. Put S Sh(F) and<br />
Afunc(F)C½ (M,Ê). Then A is an abelian group and by [13, Equation (8)] S is<br />
a subsemigroup <strong>of</strong> C½ (M, M) acting from the right on A as follows:<br />
«Æ sÏ s M M<br />
«Ê, «¾ A, s¾S.<br />
Suppose also that the <strong>shift</strong> map ³ <strong>of</strong> F is injective, i.e., ³Ï C½ (M,Ê)Sh(F) is a<br />
bijection. Then it follows from [13, Equation (8)] that the inverse map<br />
³ 1Ï Sh(F)C½ (M,Ê)<br />
is a crossed homomorphism, i.e.<br />
( f Æ g) ( f )Æg (g),<br />
f , g¾S.<br />
If ³ is not injective, then the local inverse <strong>of</strong> ³ near id M is a “local crossed homomorphism”.<br />
Moreover, if F is not a global flow, then func(F) is an open subset <strong>of</strong><br />
C½ (M,Ê) containing the zero function, i.e. a “local group”.<br />
Notice that if Sh(F) were a group and³ 1 were a homomorphism, then continuity<br />
<strong>of</strong> ³ 1 would be equivalent to its continuity at the unit element id M only, which <strong>of</strong><br />
course is a simpler problem. In our case Sh(F) is just a semigroup, ³ 1 is a local<br />
crossed homomorphism, and func(F, V ) is in general a local group. Nevertheless we<br />
will now show that continuity <strong>of</strong> local <strong>inverses</strong> <strong>of</strong> ³ is equivalent to continuity <strong>of</strong> the<br />
local inverse <strong>of</strong> ³ at i VÏ V M.<br />
Theorem 4.2. Let V M be a D-submanifold and r, s¾Æ0. Then the following<br />
conditions are equivalent:<br />
(1) The <strong>shift</strong> map ³VÏ func(F, V )Sh(F, V ) is S r,s -open;<br />
(2) For every «¾ func(F, V ) there exists an S s -neighbourhood N f <strong>of</strong> f ³V («) in<br />
Sh(F, V ) and an S s,r -continuous section <strong>of</strong> ³V , i.e. a map<br />
Ï N f C½ (V ,Ê),<br />
such that ( f )« and ³V Æ<br />
for all g¾ N f and x¾ V .<br />
id(N f ). In other words<br />
f (x)F(x, ( f )(x)),
428 S. MAKSYMENKO<br />
(3) Property (2) holds for the zero function « 0Ï V Ê and the identity inclusion<br />
f ³V (0)i VÏ V M.<br />
Pro<strong>of</strong>. (1)µ(2). Suppose that³VÏ func(F, V )Sh(F, V ) is S r,s -open. Since<br />
³V is locally injective with respect to the S 0 -topology, condition (1) means that for every<br />
«¾ func(F, V ) there exists an S r -open neighbourhood M« in func(F, V ) such that<br />
a) the restriction ³VM«Ï M«³V (M«) is a bijection,<br />
b) ³V (M«) is S s -open in Sh(F, V ), so ³V (M«)Sh(F, V )N f , for some S s -open<br />
N f<br />
1<br />
V<br />
neighbourhood <strong>of</strong> f ³V («) in C½ (V , M),<br />
ϳV (M«)M« is S s,r -continuous.<br />
c) the inverse map V ³<br />
def<br />
Then N f ³V (M«)Sh(F, V )N f and V satisfy condition (2).<br />
The implication (2)µ(3) is evident.<br />
(3) µ (1). It suffices to show that for every « ¾ func(F, V ) there exists an<br />
S r -open neighbourhood M« in func(F, V ) satisfying conditions a)–c) above. Condition<br />
(3) means that such a neighbourhood M 0 exists for the zero function 0.<br />
For every «¾ C½ (V ,Ê) define the following subset <strong>of</strong> C½ (V , M)<br />
U«f ¾ C½ (V , M)Ï ( f (x),«(x))¾dom(F),x¾ V<br />
and consider a map q«Ï U« C½ (V , M) defined by<br />
q«( f )(x)F( f (x),«(x)), f ¾ U«, x¾ V .<br />
It is easy to see that U« is S 0 -open in C½ (V , M). Also notice that, q « is S r,r -continuous<br />
for all r ¾Æ0 and that i V ¾ U« if and only if«¾ func(F, V ).<br />
Lemma 4.3. The image <strong>of</strong> q« coincides with U « and q « is its inverse, i.e.,<br />
1<br />
q « q « Ï U « U«. Thus q« is an S r,r -homeomorphism (r ¾Æ0) between the<br />
S 0 -open sets U« and U «.<br />
Pro<strong>of</strong>.<br />
Let f ¾ U«, i.e. ( f (x),«(x))¾dom(F) for all x¾ V . Then<br />
(q«( f )(x), «(x))(F( f (x),«(x)), «(x))¾dom(F),<br />
q «Æ q«( f )(x)F(F( f (x),«(x)), «(x))F( f (x),«(x) «(x)) f (x).<br />
Hence q«(U«)U « and q «Æq« id U« . Interchanging« and « will give the result.<br />
Now we turn to the pro<strong>of</strong> <strong>of</strong> Theorem 4.2. For every «¾ func(F, V ) set<br />
M«<br />
def<br />
(M 0³<br />
1<br />
Then M« is S r -open in func(F, V ).<br />
V (U «)«)func(F, V ).
0¾³<br />
1<br />
V (i V )³<br />
1<br />
V (U) and thus «¾ M «.<br />
Moreover «¾ M«. Indeed, since «¾ func(F, V ), we have that i V ¾<br />
We will show that M« satisfies the conditions a)–c) above.<br />
a) The restriction <strong>of</strong> ³V to M« is 1-1, since so is ³VM 0<br />
.<br />
Conditions b) and c) are implied by the following lemma:<br />
U«, whence<br />
LOCAL INVERSES OF SHIFT MAPS 429<br />
Lemma 4.4.<br />
in Sh(F, V ).<br />
Let M¼« M« be any S r -open subset. Then ³V (M¼«<br />
) is Ss -open<br />
Pro<strong>of</strong>. Denote M¼0M¼« «. Then M¼0M 0³<br />
1<br />
V (U «) and by the condition b)<br />
for M 0 there exists an S s -open subset N¼ <strong>of</strong> C½ (V , M) such that<br />
³V (M¼0 )Sh(F, V )N ¼ .<br />
Define the following S r,r -homeomorphism<br />
a«Ï C½ (V ,Ê)C½ (V ,Ê),<br />
Then we obtain the following commutative diagram:<br />
(4.1)<br />
M¼0<br />
³V<br />
Ã<br />
M¼«<br />
³V<br />
a«Ã<br />
a«(¬)«¬.<br />
³V (M¼0<br />
¼U«<br />
)Sh(F,<br />
q«<br />
V )N<br />
à Sh(F, V )q«(N¼U«)<br />
Ã<br />
simply meaning that F(x,¬(x)«(x))F(F(x,¬(x)),«(x)) for all¬¾M 0 and x¾ V .<br />
We claim that<br />
³V (M¼« )Sh(F, V )q «(N¼U«).<br />
Indeed, by (4.1), ³V (M¼« )Sh(F, V )q «(N¼U«).<br />
Conversely, let g ¾ Sh(F, V )q«(N¼ U«), i.e., there exist ¬ ¾ func(F, V ) and<br />
f ¾ N¼U« such that<br />
(4.2) g(x)F(x,¬(x))F( f (x),«(x)), x¾ V .<br />
Then f (x)F(x,¬(x) «(x)), i.e. f ¾ Sh(F, V ) and therefore<br />
f ³V (¬ «)¾Sh(F, V )N¼U«³V (M¼0 ).<br />
Thus there exists ¾ ¬ M¼0<br />
( , possibly distinct from «, such that f ³V ). Denote<br />
¬¼ «. Then ¬¼¾ M¼« and<br />
g(x)F( f (x),«(x))F(F(x, (x)),«(x))F(x,¬¼ (x)).
430 S. MAKSYMENKO<br />
In other words, g³V (¬¼ )¾³V (M¼« ). Lemma 4.4 and Theorem 4.2 are completed.<br />
5. Examples when <strong>shift</strong> map is not open<br />
In this section we discuss four examples <strong>of</strong> well-known flows whose <strong>shift</strong> <strong>maps</strong> turn<br />
out not to be homeomorphisms onto their images. They have similar nature, but are<br />
given on different types <strong>of</strong> manifolds. These examples also provide counterexamples to<br />
[13, Theorem 1]. All manifolds in this section are compact, therefore we will not distinguish<br />
weak and strong topologies. In all the examples below our vector fields will<br />
satisfy the assumptions <strong>of</strong> the following simple lemma:<br />
Lemma 5.1. Let F be a vector field on a compact manifold M tangent to M.<br />
Suppose that the <strong>shift</strong> map³ <strong>of</strong> F is injective and for every r¾Æ0, a W r -neighbourhood<br />
N <strong>of</strong> id M , and arbitrary large T 0 there exists t ¾Ê, regarded as a constant function<br />
tÏ M Ê, such that tT and F t ³(t)¾N . Then ³ is not W r,s -open for<br />
any r, s¾Æ0. In particular, ³ is not a homeomorphism onto its image with respect to<br />
W½ -topologies <strong>of</strong> C ½ (M,Ê) and Sh(F).<br />
Pro<strong>of</strong>.<br />
Consider the following W 0 -neighbourhood <strong>of</strong> the zero function:<br />
M 0«¾ C½ (M,Ê)Ï«(x)1.<br />
Suppose that there exists a W r -neighbourhood N <strong>of</strong> id M<br />
assumption there exists a constant function t 1 such that³(t)¾N . Since³ is injective,<br />
and tM 0 , we obtain that³(t)³(M 0 ), whence Nê³(M 0 ). This contradiction<br />
such that N ³(M 0 ). By<br />
implies that ³ is not W r,s -open for any r, s¾Æ0.<br />
Irrational flow. For simplicity we will consider the irrational flow on T 2 . Let<br />
¾Ê be an irrational number and F be the irrational flow on the 2-torus T 2Ê22<br />
given by F(x, y, t)(x t, y t).<br />
Lemma 5.2.<br />
for any r, s¾Æ0.<br />
The <strong>shift</strong> map ³Ï C½ (T 2 ,Ê)C½<br />
(T 2 , T 2 ) <strong>of</strong> F is not W r,s -open<br />
Pro<strong>of</strong>. Notice that every orbit <strong>of</strong> F is non-closed and everywhere dense, so ³ is<br />
injective. First we give convenient formulas for the metrics generating W r -topologies<br />
on C½ (T 2 , T 2 ). Let fÏ T 2T 2 be a C½ map. Then f lifts to some 2 -equivariant<br />
map f É (É f1 , f2 É 2 )ÏÊ2Ê2 . Let I [0, 1]¢[0, 1]Ê2 be the fundamental domain<br />
. Define the r-th norm <strong>of</strong> f by<br />
for the covering map pÏÊ2T 2<br />
fr<br />
<br />
sup min(É f j, 1 É f<br />
(x, y)¾I<br />
j) <br />
2<br />
j1,2<br />
1i 1i 2r<br />
sup<br />
(x, y)¾I 2¬<br />
i 1i 2 f É j<br />
x 1 i y i 2<br />
¬ ,
LOCAL INVERSES OF SHIFT MAPS 431<br />
be a base W r -neighbourhood<br />
<strong>of</strong> id T 2 ³(0)¾C½ (T 2 , T 2 ) for some0. We will show that there exists arbitrary<br />
large (by absolute value) n ¾ such that ³(n)F n ¾ N r . Then our lemma will<br />
where t is the fractional part <strong>of</strong> the absolute value <strong>of</strong> t¾Ê.<br />
Let r 0 and N f ¾C½ (T 2 , T )Ï 2 f id T 2r<br />
follow from Lemma 5.1.<br />
Notice that F n(x, y)(xn, yn)(xn, y) for all n¾, i.e., F n is just<br />
a “rotation <strong>along</strong> the first coordinate”. Since this map is defined by adding constants to<br />
coordinates, it follows from formula for fr that for each r¾Æ0 the distance between<br />
id T 2 and F n with respect to the W r -topology is equal to<br />
F n id T 2r<br />
<br />
min(n, 1 n)<br />
and therefore does not depend on r.<br />
Sinceis irrational, the set Tmin(n, 1 n)n¾ is everywhere dense<br />
in S 1<br />
Ê. Hence there are arbitrary large (by absolute value) n ¾ such that<br />
F n id T 2r<br />
, i.e. F n¾ r N .<br />
be the unit disk<br />
Irrational flows on a solid torus. Let D z¾Ïz1 2<br />
in the complex plane, T S 1¢D2 be the solid torus, and be an irrational number.<br />
Define the following flow on T by F(, z, t)( 2t t mod 1, e z). Then by<br />
the arguments similar to Lemma 5.2 is can be shown that F satisfies assumptions <strong>of</strong><br />
Lemma 5.1.<br />
The main feature <strong>of</strong> this example is that F has periodic orbit 1¢ S 0 and all<br />
other ones are recurrent. Let B 1¢ D 2 be and RÏ BB be the first recurrence map<br />
<strong>of</strong> 2 defined by R(z)e z, i.e. it is the rotation by 2. Then R is not periodic,<br />
eigen values <strong>of</strong> its tangent map T 0 R at 0¾ B have modulus 1, and the iterations <strong>of</strong> R<br />
can be arbitrary close to id B . Thus F satisfies all assumptions but (b) <strong>of</strong> Definition 3.4<br />
<strong>of</strong> class F(T 2 ).<br />
Periodic linear flows.<br />
Ê2nn by<br />
Given 1,,n¾Ê define the following linear flow on<br />
(5.1) F(z 1 ,, z n , t)(e i1t z 1 ,, e int z n ).<br />
Evidently, the closed 2n-disk D r <strong>of</strong> radius r and centered at the origin is invariant with<br />
respect to F.<br />
Lemma 5.3.<br />
The following conditions are equivalent:<br />
(1) F idn for some 0, i.e. j ¾ for all j 1,, n;<br />
(2) every z¾n is either fixed or periodic with respect to F;<br />
(3) at least one point z (z 1 ,,<br />
z n ) with all non-zero coordinates is periodic.<br />
A flow satisfying one <strong>of</strong> these conditions will be called periodic.
432 S. MAKSYMENKO<br />
Pro<strong>of</strong>.<br />
i The implications (1)µ(2)µ(3) are evident. (3)µ(1) Let z¾n be a<br />
periodic point with all non-zero coordinates and be the period <strong>of</strong> z with respect to<br />
F. Then e j z j z j 0 for all j 1,, n, whence j¡2 ¾.<br />
Lemma 5.4.<br />
W r,s -open for any r, s¾Æ0.<br />
If F is not periodic then its <strong>shift</strong> map ³ is injective and is not<br />
Pro<strong>of</strong>. By Lemma 5.3 every point z¾n with all non-zero coordinates is nonperiodic<br />
and it is easy to see that its orbit is dense on some open subset <strong>of</strong> the sphere<br />
S 2n 1<br />
x Dx <strong>of</strong> radius x. In particular, this orbit is non-closed, whence the <strong>shift</strong><br />
map <strong>of</strong> F is injective. Then similarly to Lemma 5.2, we can find arbitrary large t¾Ê<br />
such that F t is arbitrary close to idÊ2n in any <strong>of</strong> W r -topologies.<br />
Flow on S 2n , n2. We will now extend the last result for the construction <strong>of</strong> a<br />
flow on the sphere S 2n with two fixed points at which this flow is linear.<br />
Let Ê2n<br />
1<br />
and Ê2n<br />
2<br />
be two copies <strong>of</strong> Ê2n n . Define a diffeomorphism ÏÊ2n<br />
1<br />
Ò<br />
0Ê2n<br />
2<br />
Ò0 by(z)zz2 , wherez is the usual Euclidean norm inÊ2n . Then<br />
<strong>maps</strong> every sphere <strong>of</strong> radius r centered at 0 to the sphere <strong>of</strong> radius 1r. Gluing Ê2n<br />
1<br />
and Ê2n<br />
2<br />
via we obtain a 2n-sphere.<br />
Notice that Equation (5.1) defines the flows on Ê2n<br />
1<br />
and Ê2n<br />
2<br />
so that the following<br />
diagram is commutative:<br />
Ê2n<br />
1<br />
Ò0<br />
F tÃ<br />
Ê2n<br />
1<br />
Ò0<br />
Ã<br />
<br />
ÃÊ2n<br />
Ê2n<br />
2<br />
Ò0<br />
F t<br />
Ã<br />
2<br />
Ò0.<br />
Hence these flows determine a unique flow F¼<br />
on S 2n with two fixed points. Moreover,<br />
F¼<br />
is linear on the charts Ê2n<br />
1<br />
and Ê2n<br />
2<br />
at these points.<br />
Now suppose that F is not periodic. Then we can find arbitrary large t ¾Ê such<br />
that F t is arbitrary close to idÊ2n in any <strong>of</strong> W r -topologies. This implies that F¼<br />
satisfies<br />
assumptions <strong>of</strong> Lemma 5.1.<br />
6. Regular and trivial extensions<br />
The results <strong>of</strong> this section will allow to estimate continuity <strong>of</strong> <strong>shift</strong> <strong>maps</strong> for vector<br />
fields <strong>of</strong> types (L) and (H).<br />
Let M, N be two manifolds, G be a vector field on M, F be some regular extension,<br />
and Æ G be the trivial extension <strong>of</strong> G on M¢N. Thus<br />
F(x, y)(G(x), H(x, y)), Æ G(x, y)(G(x), 0),
LOCAL INVERSES OF SHIFT MAPS 433<br />
for some smooth map HÏ M¢N T N. By F, Æ G, and G we will denote the corresponding<br />
local flows, and by ³, Æ, and the corresponding <strong>shift</strong> <strong>maps</strong> <strong>of</strong> F, Æ G, and<br />
G. It is easy to see that<br />
(6.1) dom(F)dom(Æ G)dom(G)¢ N.<br />
Moreover,<br />
(6.2) F(x, y, t)(G(x, t), H(x, y, t)), Æ G(x, y, t)(G(x, t), y),<br />
for some smooth map HÏ dom(Æ G) N.<br />
Let V M¢N be a connected compact D-submanifold. Then it follows from (6.1)<br />
that func(F, V ) is W 0 -open in func(Æ G, V ). Define the map<br />
PÏ Sh(F, V )Sh(Æ G, V )<br />
by the rule: if f ¾ Sh(F, V ), and f (x, y) (A(x, y), g(x, y)), then P( f )(x, y) <br />
(A(x, y), y). It follows from (6.2) that P is well defined and is W r,r -continuous for<br />
every r ¾Æ0. Moreover, we have the following commutative diagram:<br />
(6.3)<br />
Theorem 6.1.<br />
³V<br />
func(F, V ) Ã Sh(F, V )<br />
ÆV<br />
P<br />
ÆV<br />
func(Æ G, V ) Ã Sh(Æ G, V ).<br />
¸ Ã<br />
Ã<br />
Ã<br />
Suppose thatG is nowhere dense in M and that ÆV is W r,s -open<br />
for some r, s¾Æ0.<br />
(1) If ÆV is injective, then ³V is W r,s -open as well.<br />
(2) If ³V is W r,s -open, then P is locally injective with respect to the W s -topology<br />
<strong>of</strong> Sh(F, V ).<br />
Suppose in addition that ÆV is also W s,t -open for some t¾Æ0.<br />
(3) If P is locally injective with respect to the W s -topology <strong>of</strong> Sh(F, V ), then ³V is<br />
W r,t -open.<br />
(4) If both ÆV and³V are not injective, then P is locally injective with respect to the<br />
W 0 -topology <strong>of</strong> Sh(F, V ), whence, by (3), ³V is W r,t -open.<br />
Pro<strong>of</strong>. (1) If ÆVÏ func(Æ G, V )Sh(Æ G, V ) is a bijection, it follows from (6.3)<br />
that so is ³V . Let Mfunc(F, V ) be a W r -open subset. Then<br />
³V (M) P<br />
1Æ ÆV (M)<br />
is W s -open in Sh(F, V ) due to W r,s -openness <strong>of</strong> ÆV and W s,s -continuity <strong>of</strong> P.
434 S. MAKSYMENKO<br />
(2) Let «¾ func(F, V ) and f ³V («). We will find a W s -neighbourhood <strong>of</strong> f<br />
such that PN is 1-1.<br />
Since both³V and ÆV are W r,s -open and locally injective with respect to W 0 -topologies<br />
<strong>of</strong> func(F, V ) and func(Æ G, V ) respectively, there exists a W r -neighbourhood M <strong>of</strong>« in<br />
func(F, V ) such thatN ³V (M) is a W s -neighbourhood <strong>of</strong> f in Sh(F, V ) and the restrictions<br />
<strong>of</strong>³V and ÆV to M are 1-1. Then it follows from (6.3) that PN is 1-1 as well.<br />
(3) Let Mfunc(F, V ) be a W r -open subset and«¾M. We will show that there<br />
exists a W s -neighbourhood M¼ M <strong>of</strong> « such that ³V (M¼ ) is W t -open in Sh(F, V ).<br />
Since«¾ M is arbitrary, we will obtain that³V (M) is W t -open in Sh(F, V ).<br />
It follows from W r,s -openness <strong>of</strong> ÆVM and W s,s -continuity <strong>of</strong> P that the set P 1Æ<br />
ÆV (M) is a W s -open neighbourhood <strong>of</strong>³V («) in Sh(F, V ). Moreover, since P is locally<br />
injective with respect to the W s -topology <strong>of</strong> Sh(F, V ), there exists a W s -neighbourhood<br />
N P 1Æ ÆV (M) <strong>of</strong>³V («) such that the restriction PNÏ N Sh(Æ G, V ) is injective.<br />
1<br />
Denote M¼ M³<br />
V<br />
(N ). We claim that<br />
³V (M¼ ) P<br />
1Æ ÆV (M¼ )N ,<br />
whence ³V (M¼ ) will be W t -open in Sh(F, V ). Indeed,<br />
P<br />
1Æ ÆV (M¼ )N (6.3)<br />
injectivity <strong>of</strong> PN<br />
P<br />
1Æ PƳV (M¼ )N ³V (M¼ ).<br />
(4) Suppose that both ÆV and ³V are not injective. We will show that for some<br />
m 0 there exists a free P-equivariant action <strong>of</strong> the group m on Sh(F, V ) such that<br />
P( f ) P(g) if and only if f , g belongs to the same m-orbit. This will give us<br />
a decomposition<br />
PÏ Sh(F, V ) q Sh(F, V )m Sh(Æ G, V )<br />
in which q is a covering map, and is a bijection with the image P(Sh(F, V )) <br />
Sh(Æ G, V ). Then q will be locally injective with respect to the W 0 -topology since m<br />
is a finite group. Hence so will be P.<br />
By Lemma 2.3 (5b) func(Æ G, V )func(F, V )C½ (V ,Ê), ker(ÆV )nÆn¾, and<br />
ker(³V )nn¾ for some smooth functions Æ,Ï M¢N (0,½) such that<br />
ÆG(x, y, tÆ(x, y)) Æ G(x, y, t),<br />
F(x, y, t(x, y))F(x, y, t).<br />
In other words<br />
(6.4)<br />
(G(x, tÆ), y)(G(x, t), y),<br />
(G(x, t), H(x, y, t))(G(x, t), H(x, y, t)).<br />
It follows that Æ G(x, y, t)(G(x, t), y)(G(x, t), y) Æ G(x, y, t), whence<br />
¾ker(ÆV ), i.e.mÆ for some m¾.
LOCAL INVERSES OF SHIFT MAPS 435<br />
In particular, by (2) <strong>of</strong> Lemma 2.3, Æ is constant <strong>along</strong> <strong>orbits</strong> <strong>of</strong> F. Since for every<br />
«¾ func(F, V ) the map ³V («) preserves every orbit <strong>of</strong> F, we have that ÆƳV («)Æ,<br />
whence<br />
[13, Equation (8)]<br />
³V (Æ)ƳV («) ³V («ÆƳV («))³V («Æ).<br />
Then we can define an action £ <strong>of</strong> the group m on Sh(F, V ) by<br />
k£ f ³V (kÆ)Æ f , k¾m, f ¾ Sh(F, V ).<br />
Evidently this action is free and by (6.4) is equivariant with respect to P.<br />
Moreover, let f ³V («), g ³V<br />
(¬) for some «,¬ ¾ func(F, V ) and suppose<br />
that P( f ) P(g), i.e. ÆV («) ÆV (¬). Then it follows from (3) <strong>of</strong> Lemma 2.3 that<br />
« ¬ kÆ for some k ¾, whence f ³V (kÆ)Æg. Moreover, since mÆ, we<br />
may take k modulo m. In other words, P( f ) P(g) if and only if f k£ g for some<br />
k¾m.<br />
7. Vector fields <strong>of</strong> types (L) and (H)<br />
The following lemma shows that property <strong>of</strong> openness <strong>of</strong> <strong>shift</strong> <strong>maps</strong> near singular<br />
points is invariant under reparametrizations.<br />
Lemma 7.1 (cf. [20].). Let F be a C½ vector field on M, Ï M (0,½) a<br />
C½ strictly positive function, and G F. Let also V M be a D-submanifold and<br />
³V andV be <strong>shift</strong> <strong>maps</strong> for F and G respectively. Then Sh(F, V )Sh(G, V ). Moreover,<br />
³V is S r,s -open iff so is V .<br />
Pro<strong>of</strong>.<br />
Define the functions «Ï dom(F)Ê and ¬Ï dom(G)Ê by<br />
¬(x, s) s<br />
0 0<br />
(G(x,)) d, «(x, s) s<br />
d<br />
(F(x,)) .<br />
Then it is well-known that for each f ¾ func(F, V ) and g¾ func(G, V ), see e.g. [20],<br />
G(x, g(x))F(x,¬(x, g(x))),<br />
F(x, f (x))G(x,«(x, f (x))),<br />
for all x¾ V . Define the following map<br />
Ï func(G, V )func(F, V ), (g)(x)¬(x, g(x)).<br />
Then is a homeomorphism with respect to topologies W r for all r, and its inverse is<br />
given by 1 ( f )(x)«(x, f (x)). Moreover V ³V Æ . Hence ³V is S r,s -open iff<br />
so is V .
436 S. MAKSYMENKO<br />
Thus for the study <strong>of</strong> vector fields <strong>of</strong> types (L) and (H) is suffices to consider<br />
linear and reduced Hamiltonian vector fields only.<br />
Lemma 7.2 ([19, 14]). Let gÏÊ2Ê be a homogeneous polynomial, G be its<br />
reduced Hamiltonian vector field, F be a trivial n-extension <strong>of</strong> G on Ên¢Ê2 , and V<br />
<strong>of</strong> F is W½,½ -open. If<br />
be a D-neighbourhood <strong>of</strong> 0¾Ên2 . Then the <strong>shift</strong> map ³V<br />
deg G 2, i.e. G is <strong>of</strong> type (H), then for every regular n-extension <strong>of</strong> G its <strong>shift</strong> map<br />
is W½,½ -open as well.<br />
Pro<strong>of</strong>. It follows from [19, 14] that the <strong>shift</strong> map ÆV <strong>of</strong> G Æ has a W<br />
½,½ -continuous<br />
local section on some neighbourhood <strong>of</strong> the identity inclusion i VÏ V Ên2 , see also<br />
[19, Theorem 11.1]. By Theorem 4.2 this implies W½,½ -openness <strong>of</strong>V .<br />
Moreover, if deg G 2, i.e. the linear part <strong>of</strong> F at 0 vanishes, then by Lemma 2.3<br />
³V is injective. Hence by (1) <strong>of</strong> Theorem 6.1 the <strong>shift</strong> map <strong>of</strong> G is W½,½ -open as well.<br />
Lemma 7.3.<br />
Let B be a non-zero (k¢k)-matrix, G(y) By be the corresponding<br />
linear vector field on Êk , G(y, t)e Bt y be its flow, and F be a vector field on Ênk<br />
being a regular (possibly trivial) n-extension <strong>of</strong> G with respect to the origins <strong>of</strong> Ênk<br />
and Êk as indicated in the third column <strong>of</strong> the table below. Let also V Ênk be a<br />
D-neighbourhood <strong>of</strong> the origin 0¾Ênk . Then the <strong>shift</strong> map³V <strong>of</strong> F is W r,s -open for<br />
the values r, s described in the following table.<br />
type B F openness <strong>of</strong> ³V<br />
1 (L1) Ba, a 0, regular W r,r1 , r 0<br />
2 (L1) B a b , a, b0 regular W<br />
b a<br />
r,r2 , r 0<br />
3 (L2) B 0 1<br />
0 0, regular W r,r1 , r 0<br />
4 (L3) B 0 b 1 0<br />
b 0 0 1<br />
5 (L4) B 0 b<br />
6 B <br />
6a<br />
(L4)<br />
<br />
, b0 regular W½,½<br />
0 0 0 b<br />
0 0 b 0<br />
, b0 trivial W½,½<br />
b 0<br />
0 b 1<br />
b 1 0<br />
<br />
, l 2<br />
. ..<br />
0 b l<br />
b l 0<br />
(a) b j¾ for some 0 and all<br />
j 1,, l (periodic case)<br />
trivial<br />
W½,½<br />
6b (L5) (b) otherwise (non-periodic case) — —
LOCAL INVERSES OF SHIFT MAPS 437<br />
Pro<strong>of</strong>. In Cases 1–3 we will first suppose that F is a trivial n-extension <strong>of</strong> G.<br />
Then F is linear and is generated by the following matrix 0 n 0, where 0<br />
0 B<br />
n is the<br />
zero (n¢ n)-matrix. Let denote the coordinates in Ên .<br />
CASE 1. In this case F(, x) axx, (a 0), F generates the following<br />
global flow F(, x, t)(, xe at ) on Ên1 , ³V is injective (because F has non-closed<br />
<strong>orbits</strong>), its image Sh(F, V ) consists <strong>of</strong> <strong>maps</strong> f ( f 1 , f 2 )¾C½ (V ,Ên¢Ê) satisfying<br />
the following conditions:<br />
f 1, f 2<br />
f 2 (, 0)<br />
(, 0)0, 0, x f 2 (, x)0 (x 0),<br />
x<br />
Ï Sh(F, V )C½ (V ,Ê) is given by<br />
and the inverse mapping ³<br />
1<br />
V<br />
(7.1) ³<br />
1<br />
V ( f )(, x) 1 a ln f 2(, x)<br />
x<br />
1 a ln 1<br />
0<br />
f 2 (, tx)<br />
x<br />
1<br />
see [13, Equation (23) and (27)]. Hence³<br />
V<br />
is Wr1,r -continuous for all r 0, whence<br />
³V is W r,r1 -open.<br />
CASE 2. We will regard Ên2 as Ên¢. Since a 0, we have that F has nonclosed<br />
<strong>orbits</strong>, whence again its <strong>shift</strong> map ³V is injective but now the image Sh(F, V )<br />
Æ f2<br />
can not be described so simply as in the previous cases. Let «¾ C½ (V ,Ê) and f <br />
( f 1 , f 2 )³V («)¾C½ (V ,Ên¢). Then f 1. Notice that we can define complex<br />
and its partial derivatives f2z Æ and f2Æz Æ in z and Æz in a usual way.<br />
conjugate<br />
Then it follows from [13, Equation (29) and Lemma 34] that<br />
«(, z) Im( 1<br />
2a ln f 2 d f2 Æ (Æ))<br />
1<br />
Im(zÆ)<br />
dt,<br />
Im(¡ 2¡ ((<br />
2a<br />
f2z)( Æ Æ ln f<br />
2 f2Æz)Æ))<br />
y(a b 2 )<br />
and that the numerator <strong>of</strong> the last fraction is equal to zero, when y 0. It follows<br />
from this formula and the Hadamard lemma that the expression <strong>of</strong> « via f contains<br />
1<br />
partial derivatives <strong>of</strong> f up to order 2. Hence ³<br />
V<br />
is W r2,r -continuous for all r 0.<br />
CASE 3. Now F(, x, y) yx for (, x, y)¾Ên2 and it generates the following<br />
flow F(, x, y, t)(, x yt, y). Then³V is again injective (since F has non-closed<br />
<strong>orbits</strong>), its image Sh(F, V ) consists <strong>of</strong> mappings f ( f 1 , f 2 , f 3 )¾C½ (V ,Ên¢Ê¢Ê)<br />
such that<br />
and the inverse map ³<br />
1<br />
V<br />
Ï Sh(F, V )C½ (V ,Ê) is given by<br />
f 1, f 2 (, x, 0)0, f 3y,<br />
(7.2) ³<br />
1<br />
V ( f ) f 2(, x, y) x<br />
y<br />
1<br />
0<br />
f 2 (, x, ty)<br />
dt,<br />
y<br />
see [13, Equation (26)]. Hence ³<br />
1<br />
V<br />
is W r1,r -continuous for all r 0.
438 S. MAKSYMENKO<br />
Since in Cases 1–3 ³V is injective, it follows from (1) <strong>of</strong> Theorem 6.1 that the<br />
1<br />
same estimations <strong>of</strong> continuity <strong>of</strong> ³<br />
V<br />
hold for regular extensions <strong>of</strong> G.<br />
Notice that in the remaining Cases 4–6 F is a regular n-extension <strong>of</strong> the linear<br />
vector field G 5 byx bx y defined by the matrix B 5 0 b<br />
. In fact, it<br />
b 0<br />
is easy to see that this vector field is the Hamiltonian vector field <strong>of</strong> the homogeneous<br />
polynomial g(x, y)(b2)(x 2y2 ). Also notice that the <strong>shift</strong> map ³V <strong>of</strong> any trivial<br />
extension F <strong>of</strong> G 5 is not injective and its kernel ker(³V ) consists <strong>of</strong> integer multiples<br />
<strong>of</strong> constant function 2b.<br />
CASE 5. It follows from Lemma 7.2 that local <strong>inverses</strong> <strong>of</strong>³V are W½,½ -continuous.<br />
An independent pro<strong>of</strong> <strong>of</strong> W½,½ -continuity <strong>of</strong>³V for this case is also given in [21] under<br />
more general settings. Notice that in this case we claim nothing about openness <strong>of</strong> <strong>shift</strong><br />
<strong>maps</strong> <strong>of</strong> regular extensions F <strong>of</strong> G 5 , since due to Theorem 6.1 it is necessary to have<br />
additional information about F.<br />
CASE 4. We will regardÊ4 as2 . Suppose at first that F is a trivial n-extension<br />
<strong>of</strong> G. Since G is a regular 2-extension <strong>of</strong> G 5 , we see that F is a regular (n 2)-<br />
extension <strong>of</strong> G 5 . Let also Æ G be a trivial (n 2)-extension <strong>of</strong> G 5 . Thus F and Æ G are<br />
defined on Ên¢¢ and generate the following global flows:<br />
F(, z 1 , z 2 , t)(, e ibt (z 1 tz 2 ), e ibt z 2 ), Æ G(, z 1 , z 2 , t)(, z 1 , e ibt z 2 ).<br />
Denote 2b and let V Ên¢2 be a D-neighbourhood <strong>of</strong> 0¾Ên¢2 . For<br />
every «¾ C½ (V ,Ê) put<br />
f(«)(, z 1 , z 2 )e ib«(,z 1 ,z 2 ) z 1 , g(«)(, z 1 , z 2 )e ib«(,z 1 ,z 2 ) z 2 ,<br />
Then the <strong>shift</strong> <strong>maps</strong> ³V and ÆV <strong>of</strong> F and G respectively are given by<br />
(7.3) ³V («)(, f(«)«¡ g(«), g(«)), ÆV («)(, z 1 , g(«)).<br />
Similarly to (6.3) define PÏ Sh(F, V )Sh(Æ G, V ) by the following rule: if h <br />
(, f , g)¾Sh(F, V )C½ (V ,Ên<br />
¢¢), then P(h)(, z 1 , z 2 )(, z 1 , g(z 1 , z 2 )).<br />
Evidently, ÆV PƳV .<br />
By Case 5 the <strong>shift</strong> map ÆVÏ C½ (V ,Ê)Sh(Æ G, V ) is W<br />
½,½ -open. We claim<br />
that so is ³VÏ C½ (V ,Ê)Sh(F, V ). Since G has non-closed <strong>orbits</strong>, ÆV is always<br />
injective, whence it will follow from (1) <strong>of</strong> Theorem 6.1 that the <strong>shift</strong> map <strong>of</strong> any<br />
regular extension <strong>of</strong> G is W½,½ -open as well.<br />
By (3) <strong>of</strong> Theorem 6.1 it suffices to show that P is locally injective with respect<br />
to the W 1 1<br />
-topology. Evidently, <br />
V<br />
ÆV («)«nn¾, whence we obtain from<br />
(7.3) that<br />
P<br />
1Æ ÆV («)³V («)(0,n¡ g(«), 0)n¾.
LOCAL INVERSES OF SHIFT MAPS 439<br />
Now, define the following CW 1 -neighbourhood <strong>of</strong> ³V («) in Sh(F, V ):<br />
<br />
.<br />
N f ¾ Sh(F, V )<br />
We claim that the restriction PN is 1-1.<br />
and ³V (¬n)<br />
Then<br />
f ³V («)1<br />
V <br />
<br />
4<br />
Since³V is injective map, it suffices to establish that n 0, whenever both³V (¬)<br />
belong to N for some ¬¾ ib¬ C½ (V ,Ê). Notice that<br />
g(¬)1<br />
V g(¬)¼z 2(z 1 ,z 2 )0e (ibz2¬¼z 2 1)(z 1 ,z 2 )0 1.<br />
³V (¬) ³V (¬n)1<br />
V ³V (¬) ³V («)1<br />
V ³V (¬n) ³V<br />
<br />
2 .<br />
On the other hand,<br />
³V (¬) ³V (¬n)1<br />
V (0,ng(¬), 0)1<br />
V n.<br />
(«)1<br />
V<br />
Hence n 0.<br />
CASE 6a. In this case F is a regular extension <strong>of</strong> G 5 . Since the flow F is periodic,<br />
we have that the <strong>shift</strong> <strong>maps</strong> <strong>of</strong> F and G 5 are not injective and by Case 5 the<br />
<strong>shift</strong> map <strong>of</strong> G 5 is W½,½ -open. Then by (4) <strong>of</strong> Theorem 6.1 so is the <strong>shift</strong> map <strong>of</strong> F.<br />
CASE 6b. In this case³V is injective, but as it is shown in Lemma 5.4 its inverse<br />
map is not even W½,½ -continuous.<br />
Lemma 7.3 is completed.<br />
REMARK 7.4. Incorrect estimations <strong>of</strong> continuity <strong>of</strong> local <strong>inverses</strong> <strong>of</strong>³V given in<br />
[13, pp. 199–200] were bases on at the following “division lemma”, which was wrongly<br />
formulated 1 in [13].<br />
Lemma 7.5 (cf. [13, Lemma 32]). Let be either Ê or , V be a D-<br />
submanifold, and ZÏ C½ (V ,)C½ (V ,) be a map defined by the formula: Z(«)(x)<br />
x¡«(x). IfÊ then the inverse map Z 1Ï im Z C½ (V ,) is W r1,r -continuous<br />
for all r 0. If, then Z 1 is only W½,½ -continuous.<br />
The caseÊ easily follows from the Hadamard lemma, see also [25]. The case<br />
is more complicated and can be established by methods <strong>of</strong> [19, 14] but during<br />
the pro<strong>of</strong> <strong>of</strong> Lemma 7.3 we avoided referring to it.<br />
1 In [13, Lemma 32] it was claimed that Z 1 is W r,r -continuous for all r ¾Æ0. But the latter<br />
inequality in the pro<strong>of</strong> <strong>of</strong> [13, Lemma 32] actually shows W r,r -continuity <strong>of</strong> Z but not <strong>of</strong> its inverse.
440 S. MAKSYMENKO<br />
8. Fragmentation<br />
The aim <strong>of</strong> this section is to repair [13, Theorem 17] by giving a sufficient condition<br />
for the <strong>shift</strong> map³Ï func(F)Sh(F) to be either a homeomorphism or an infinite<br />
cyclic covering map with respect to S½ -topologies, see Theorem 8.2.<br />
REMARK 8.1. The error occurred in the third paragraph <strong>of</strong> [13, Theorem 17],<br />
where it was claimed that “. . . the image N i ³U i (M¼i ) is a Cr W<br />
-neighbourhood <strong>of</strong><br />
fU i<br />
in C½ (Ui , M) for all r ¾Æ0.” First <strong>of</strong> all this phrase contains a misprint: instead<br />
<strong>of</strong> C½ (Ui , M) the author supposed to be written im³U i<br />
. But nevertheless the<br />
statement that N i is CW r -open in im³U i<br />
does not follow from the assumptions <strong>of</strong> [13,<br />
Theorem 17] and must be included into the formulation <strong>of</strong> “section” property (S) 0 <strong>of</strong><br />
[13, Definition 15]. This is the point which was missed.<br />
Theorem 8.2 (cf. [13, Theorem 17]).<br />
Let F be a vector field on M such that<br />
F is nowhere dense. Suppose that there exists a¾Æ0, a function dÏÆ0Æ0, a locally<br />
finite coverV ii¾¿ <strong>of</strong> M by D-submanifolds, and a finite (possibly empty) subset<br />
¿¼¿ such that Int V ii¾¿ is also a cover <strong>of</strong> M, and the local <strong>shift</strong> map<br />
³V iÏ<br />
func(F, V i )Sh(F, V i )<br />
is S½,½ -open if i¾¿¼ and S r,d(r) -open for all r a if i¾¿Ò¿¼ . Then the <strong>shift</strong> map<br />
³Ï func(F)Sh(F)<br />
is S½,½ -open. Moreover, if ¿¼û, then ³ is S r,d(r) -open for every r a.<br />
Hence if³Ï func(F)Sh(F) is injective, then it is a homeomorphism with respect<br />
to S½ -topologies. Otherwise, ³ is a -covering map.<br />
Pro<strong>of</strong>. The pro<strong>of</strong> follows the line <strong>of</strong> [13, Theorem 17]. Since F is nowhere<br />
dense, there exists a continuous function ÆÏ M (0,½) such that for every periodic<br />
point x <strong>of</strong> period x we have that Æ(x)3x, see [13, Proposition 14].<br />
Let«¾ func(F), r a, d r be a metric on the manifold J r (M,Ê) <strong>of</strong> r-jets,Ï M<br />
(0, 1) be a strictly positive continuous function such that Æ, and<br />
M¬¾ def<br />
func(F)d r ( j r«(x), j x¾M<br />
r¬(x))(x),<br />
be a base S r -neighbourhood <strong>of</strong> «, where j r¬(x) denotes the r-jet <strong>of</strong> ¬ at x. Then the<br />
restriction <strong>of</strong> ³ to M is injective, [13, Proposition 14]. We will show that ³(M) is<br />
S½ -open in Sh(F) and if ¿¼û, then ³(M) is even S d(r) -open in Sh(F). This will<br />
complete Theorem 8.2.<br />
For every i¾¿ let<br />
def<br />
(8.1) M i ¬¾ func(F, V i )Ï d r ( j r«(x), j x¾ r¬(x))(x), V i
p iÃ<br />
LOCAL INVERSES OF SHIFT MAPS 441<br />
in func(F, V i ). It follows from assumption about open-<br />
be an S r -neighbourhood <strong>of</strong>«V i<br />
ness <strong>of</strong> ³V i<br />
that<br />
³V i<br />
(M i )Sh(F, V i )N i ,<br />
where N i is S½ -open in C ½ (Vi , M) for i¾¿¼ and S d(r) -open for i¾¿Ò¿¼ . Moreover,<br />
the restriction <strong>of</strong> ³V i<br />
to M i is one-to-one.<br />
Let p iÏ C½ (M,Ê)C½ (Vi ,Ê) and q iÏ C½ (M, M)C½ (Vi , M) be the “restriction<br />
to V i ” <strong>maps</strong>. Then we have the following commutative diagram<br />
³<br />
func(F) Ã Sh(F)<br />
(8.2)<br />
q i<br />
func(F, V i )<br />
³V i<br />
Ã<br />
Sh(F, V i ).<br />
Ã<br />
By definition ³ and ³V i<br />
as surjective. It also follows from definitions <strong>of</strong> func(F) and<br />
func(F, V i ) and assumption that V i is a D-submanifold, that every ¾ C½ (V ,Ê) extends<br />
to some Æ ¾ C½ (M,Ê). Moreover, if ¾ func(F, V i ), we can assume that Æ ¾<br />
func(F), whence p i (func(F))func(F, V i ). Therefore q i is surjective as well. It follows<br />
from definition that<br />
M i¾¿ <br />
p 1<br />
i (M i ).<br />
Put<br />
(8.3) N def<br />
i¾¿ <br />
q 1<br />
i (N i ).<br />
SinceV ii¾¿ is a locally finite cover and¿¼ is finite 2 , it follows from [13, Lemma 18]<br />
that N is S½ -open in C ½ (M, M) and even S d(r) -open if¿¼û. We will now show that<br />
(8.4) ³(M)Sh(F)N .<br />
This will complete our theorem.<br />
It follows from (8.2) and (8.3) that³(M)Sh(F)N . Conversely, let g¾ Sh(F)<br />
N . Then gV i<br />
q i (g)¾Sh(F, V i )N i³V i<br />
(M i ) for all i¾¿ and<br />
¬¼¾C½ g³(¬¼ ) for some<br />
(M,Ê). We have to find (possibly another) function¬¾M such that g³(¬).<br />
Since the restriction <strong>of</strong> ³V i<br />
to M i is injective, gV i<br />
³V i<br />
(¬i) for a unique ¬i ¾ M i .<br />
It remains to show that ¬i ¬ j on V i V j for all i, j¾¿. Since Int V ii¾¿ is a<br />
cover <strong>of</strong> M as well, the family <strong>of</strong> functions ¬ii¾¿ will define a unique smooth function<br />
¬¾Ëi¾¿ p 1<br />
i<br />
(M i )M such that ¬V i<br />
¬i and ³(¬)g. This will prove (8.4)<br />
and complete our theorem.<br />
If¿¼ 2 were infinite, then N would be open in the so-called very-strong topology, see [9]
442 S. MAKSYMENKO<br />
Let x¾ Int V i Int V j for some i, j¾¿. Then g(x)F(x,¬i(x))F(x,¬ j(x)).<br />
If x is a non-periodic regular point, then ¬i(x)¬ j(x).<br />
If x is periodic <strong>of</strong> periodx, then¬i(x) ¬ j(x)bx for some b¾. But¬i(x)<br />
¬ j(x)«(x) ¬i(x)«(x) ¬ j(x)2Æ(x)x, whence b0.<br />
Thus ¬i ¬ j on (Int V i Int V j )ÒF. Since F is nowhere dense, we see that<br />
¬i ¬i<br />
on all <strong>of</strong> V i V j as well.<br />
9. Replacing M with an open subset<br />
Theorem 8.2 reduces the verification <strong>of</strong> openness <strong>of</strong> the <strong>shift</strong> map to openness <strong>of</strong> a<br />
family <strong>of</strong> <strong>shift</strong> <strong>maps</strong>³V i, whereV i is any locally finite cover <strong>of</strong> M by D-submanifolds.<br />
Our next aim is to “localize” the verification an openness <strong>of</strong>³V by replacing all the manifold<br />
M with an open neighbourhood W <strong>of</strong> V .<br />
Let F be a vector field on M, W M be a connected, open subset, and F WÏ W¢<br />
Êdom(F W ) W be the local flow generated by the restriction FW <strong>of</strong> F to W . Then<br />
dom(F W )dom(F)(W¢Ê)<br />
and FF W on dom(F W ). Let V W be a D-submanifold. Then func(F W , V ) is an<br />
S 0 -open subset <strong>of</strong> func(F, V ), and the corresponding <strong>shift</strong> map ³W ,V <strong>of</strong> F W coincides<br />
with ³V on func(F W , V ), i.e.<br />
(9.1) ³W ,V ³Vfunc(F W ,V )Ï func(F W , V )Sh(F W , V )Sh(F, V ).<br />
The following statement characterizes openness <strong>of</strong> ³V via openness <strong>of</strong> ³W ,V .<br />
Theorem 9.1.<br />
conditions (A)–(C) are equivalent:<br />
(A) The <strong>shift</strong> map ³V is S r,s -open;<br />
Let V W be a D-submanifold, and r, s¾Æ0. Then the following<br />
(B) The <strong>shift</strong> map ³W ,V is S r,s -open and its image Sh(F W , V ) is S s -open in Sh(F, V ),<br />
i.e. there exists an S s -open subset N C½ (V , W ) such that<br />
(C) The <strong>shift</strong> map ³W ,V<br />
Sh(F, V )N Sh(F W , V ).<br />
is S r,s -open and there exists an S s -neighbourhood N <strong>of</strong> the<br />
identity inclusion i VÏ V M in C½ (V , M) such that<br />
Sh(F, V )N Sh(F W , V ).<br />
Pro<strong>of</strong>. (A)µ(B). Since func(F W , V ) is an S 0 -open subset <strong>of</strong> func(F, V ) and³V<br />
is an S r,s -open map, it follows that the restriction<br />
³Vfunc(F W ,V )³W ,V
LOCAL INVERSES OF SHIFT MAPS 443<br />
is an S r,s -open map and its image Sh(F W , V ) is S s -open in Sh(F, V ).<br />
The implication (B)µ(C) is evident.<br />
(C)µ(A). Suppose that ³W ,V is S r,s -open. Then by (2) <strong>of</strong> Theorem 4.2 there<br />
exists an S s -neighbourhood U <strong>of</strong> the identity inclusion i VÏ V W in C½ (V , W ) and<br />
an S s,r -continuous section <strong>of</strong> ³W ,V defined on U¼ U Sh(F W , V ):<br />
Ï Sh(F, V )Sh(F W , V )U¼ func(F W , V )func(F, V ),<br />
i.e., ³W ,V Æ id U¼.<br />
Since Sh(F, V )N Sh(F W , V ) and C½ (V , W ) is an S 0 -open subset <strong>of</strong> C½ (V , M),<br />
we obtain that U¼¼ U¼ N is an S s -neighbourhood <strong>of</strong> i VÏ V M in C½ (V , M).<br />
Moreover, ³V coincides with ³W ,V on func(F W , V ). Therefore is also a section <strong>of</strong><br />
³V defined on U¼¼ . Then by (2) <strong>of</strong> Theorem 4.2 ³V is S r,s -open.<br />
Emphasize that in this theorem W is an arbitrary open neighbourhood <strong>of</strong> V .<br />
10. Openness <strong>of</strong> Sh(F W , V) in Sh(F): Regular case<br />
Let z be a regular point <strong>of</strong> F, i.e. F(z)0. In this section we present necessary<br />
and sufficient conditions for W r,r -openness <strong>of</strong> local <strong>shift</strong> map ³V , where V is arbitrary<br />
small D-neighbourhood <strong>of</strong> z, see Theorem 10.2. As a consequence we will obtain<br />
the following<br />
Theorem 10.1. Suppose that z is a regular point <strong>of</strong> F having one <strong>of</strong> the following<br />
properties:<br />
(a) z is non-periodic and non-recurrent;<br />
(b) z is periodic and the germ at z <strong>of</strong> its first recurrence map RÏ (B, z)(B, z) is<br />
periodic;<br />
(c) z is periodic and the tangent map T z RÏ T z B T z B has at least one eigen value<br />
such that 1.<br />
Then for any sufficiently small connected D-neighbourhood V <strong>of</strong> z the corresponding<br />
<strong>shift</strong> map ³V <strong>of</strong> F is W r,r -open for all r 1. Moreover, if z satisfies either (a) or (b),<br />
then ³V is W 0,0 -open as well.<br />
The pro<strong>of</strong> will be given in §10.8.<br />
Since z is a regular point <strong>of</strong> F, there exist 0, a neighbourhood W¼ <strong>of</strong> z, and<br />
a diffeomorphism<br />
Ï W¼Ên 1¢ ( 4, 4)<br />
such that in the coordinates (y, s) on W¼ induced by we have that<br />
F((y, s), t)(y, s t),
444 S. MAKSYMENKO<br />
Fig. 3. Flow box.<br />
whenever s, s t ¾ ( 4, 4). We will call W¼ a 4-flow-box at z, see Fig. 3. Let also<br />
W 1 (Êm 1¢( ,))W¼ be the “central”-flow-box at z. For every D-submanifold<br />
V W denote<br />
(10.1) U V «¾<br />
func(F, V )ϳV («)(V )W.<br />
Then func(F W , V )U V<br />
and<br />
(10.2) ³V (U V )Sh(F, V )C½ (V , W )<br />
is a W 0 -open neighbourhood <strong>of</strong> i V in Sh(F, V ).<br />
Let p 1Ï W¼ Êm 1 and p 2Ï W¼ ( 4, 4) be the standard projections. Then<br />
we can define two <strong>maps</strong> P 1Ï U V C½ (V ,Êm 1 ) and P 2Ï U V C½ (V , ( ,)) by<br />
³V<br />
P 1 («) p 1ƳV («)Ï V<br />
(«) W Êm 1¢ ( ,) p 1Êm 1 ,<br />
³V<br />
P 2 («) p 2ƳV («)Ï V<br />
(«) W Êm 1¢ ( ,)<br />
2 p ( ,),<br />
for «¾ U V . Thus ³V («)(P 1 («), P 2 («)).<br />
Theorem 10.2.<br />
Ê be the zero function.<br />
(1) Then the map P 1 is locally constant with respect to the W 0 -topology <strong>of</strong> U V and its<br />
image P 1 (U V )C½ (V ,Êm 1 ) is at most countable.<br />
Let V W be a connected compact D-submanifold, and 0Ï V <br />
(2) The <strong>shift</strong> map ³VÏ func(F, V )Sh(F, V ) is W r,r -open if and only if P 1 (0) is an<br />
isolated point <strong>of</strong> P 1 (U V ) in C½ (V ,Êm 1 ) with respect to the W r -topology.<br />
Pro<strong>of</strong>. (1) We need the following lemma:<br />
Lemma 10.3.<br />
(i) «(x) ¬(x)2 for all x¾ V ,<br />
(ii) «(x) ¬(x)6 for all x¾ V ,<br />
(iii) ¬(x) «(x)6 for all x¾ V .<br />
Moreover, condition (i) implies that<br />
(iv) P 1 (¬) P 1 («) and P 2 (¬) P 2 («)¬<br />
Let «,¬¾ U V . Then one <strong>of</strong> the following conditions holds true:<br />
«.
LOCAL INVERSES OF SHIFT MAPS 445<br />
Pro<strong>of</strong>. Define the following three open, mutually disjoint subsets <strong>of</strong> V :<br />
K 1x¾ VÏ«(x) ¬(x)2,<br />
K 2x¾ VÏ«(x) ¬(x)6,<br />
K 3x¾ VϬ(x) «(x)6.<br />
Let x ¾ V and suppose that ¬(x) «(x)2, i.e. x K 1 . Since W is the central<br />
-flow-box <strong>of</strong> a 4-flow-box, and<br />
³V («)(V )³V (¬)(V )W ,<br />
we see that ¬(x) «(x)6, i.e. x¾K 2K 3 . Thus V K 1K 2K 3 . Since V is<br />
connected and K i are open and disjoint, we obtain that V coincides with one <strong>of</strong> them.<br />
(i)µ(iv). Denote f ³V («), g³V (¬), and (x)¬(x) «(x). Then<br />
(10.3) g(x)F(x,¬(x))F(F(x,«(x)),¬(x) «(x))F( f (x),(x))<br />
for all x ¾ V . Suppose that 2 on all <strong>of</strong> V . Recall that F(y, sÁ t)(y, s t)<br />
whenever s, t, s t ¾ ( 4, 4) and y¾Êm 1 . Since P 2 («),P 2 (¬), we obtain<br />
that P 2 («)3<br />
and<br />
(P 1 (¬), P 2 (¬))g (10.3)<br />
F(P 1 («), P 2 («)Á)(P 1 («), P 2 («)).<br />
P 2 («)¬ «.<br />
Hence P 1 (¬) P 1 («) and P 2 (¬)<br />
Corollary 10.4. Define the following equivalence relation on U V by<br />
«¬ if and only if « ¬2.<br />
Then every class is W 0 -open and by (iv) <strong>of</strong> Lemma 10.3 the map P 1 is defined on the<br />
equivalence classes, whence P 1 is locally constant.<br />
Moreover, there is a well-defined strict order on the equivalence classes <strong>of</strong> : if<br />
A and B are two distinct classes <strong>of</strong> then<br />
A B if and only if « ¬ 6<br />
on V for some «¾ A and ¬¾B. Hence there are at most countable many classes <strong>of</strong><br />
, and therefore the image <strong>of</strong> P 1 is at most countable.<br />
Pro<strong>of</strong>.<br />
We have only to show that the definition <strong>of</strong> “” does not depend on a<br />
particular choice <strong>of</strong> « and ¬. Let «¼¾ A and ¬¼¾B be another functions. Then<br />
«¼ ¬¼ («¼ «)(« ¬)(¬ ¬¼ ) 2 6 2 2.<br />
Hence by Lemma 10.3, «¼ ¬¼ 6 as well.
446 S. MAKSYMENKO<br />
This corollary proves statement (1) <strong>of</strong> Theorem 10.2.<br />
(2) Let A 0 be the equivalence class <strong>of</strong>containing the zero function 0, i.e. A<br />
«¾ U VÏ«2. Then it is easy to see that<br />
0<br />
A 0 func(F W , V ), whence Sh(F W , V )³W ,V (A 0 )³V (A 0 ).<br />
Thus we obtain the following commutative diagram<br />
A 0 func(F W , V ) ¸ ÃU V ¸ Ã func(F, V )<br />
³W ,V³V ³V ³V<br />
¸ óV (U V )Sh(F, V )C½ (V , W ) ¸ à Sh(F, V )<br />
Ã<br />
³V (A 0 )Sh(F W , V )<br />
Ã<br />
Ã<br />
p£1<br />
à im P 1 .<br />
p£1Ã<br />
P 1 (A 0 )¸<br />
Ã<br />
Lemma 10.5. The image Sh(F W , V ) is W r -open in Sh(F, V ) for some r ¾ Æ0<br />
if and only if P 1 (0) P 1 (A 0 ) is an isolated point <strong>of</strong> the image im P 1 P 1 (U<br />
C½<br />
V<br />
(V ,Êm<br />
)<br />
1 ) with respect to the W r -topology.<br />
Pro<strong>of</strong>. Sufficiency. Suppose that P 1 (0) is an isolated point <strong>of</strong> im P 1 in the<br />
W r -topology, i.e. P 1 (0) is a W r -open subset <strong>of</strong> im P 1 . Since p£1 is Wr,r -continuous, we<br />
obtain that Sh(F W , V )³V (A 0 ) is W r -open in ³V (U V ) being W r -open in Sh(F, V ).<br />
Hence Sh(F W , V ) is W r -open in Sh(F, V ) as well.<br />
Necessity. Conversely, suppose that P 1 (0) is not isolated in im P 1 with the<br />
W r -topology. We will construct a sequence <strong>of</strong> functions ¬i such that<br />
(i) P 1 (¬i) P 1 (0),<br />
(ii) the sequence ³V (¬i) converges to i VÏ V M in the W r -topology.<br />
It will follow from (i) that ³V (¬i)Sh(F W , V )³V (A 0 ), and in particular ¬i A 0<br />
func(F W , V ) for all i¾Æ. Then from (ii) we will obtain that Sh(F W , V )³W ,V (A 0 ) is<br />
not a W r -neighbourhood <strong>of</strong> i V in Sh(F, V ), i.e. Sh(F W , V ) is not W r -open in Sh(F, V ).<br />
Since P 1 (0) is not isolated in im P 1 , there exists a sequence <strong>of</strong> classes A i distinct<br />
from A 0 such that their images P 1 (A i ) converge to P 1 (A 0 ) in the W r -topology.<br />
A i<br />
It is easy to see that for every i ¾Æ there exists a function ¬i ¾ such that<br />
P 2 (¬i)(x, s) P 2 (0)(x, s)s. Indeed, take any ¬¼i ¾ A i and set ¬i ¬¼i P 2 (¬¼i ).<br />
We claim that the sequence ¬ii¾Æ satisfies conditions (i) and (ii). Property (i)<br />
holds since P 1 (¬i) P 1 (A i ) P 1 (A 0 ) for all i¾Æ.<br />
Moreover, we have that P 2 (¬i) P 2 (0) p 2Æ i V and P 1 (¬i) C½ (V ,Êm 1 )<br />
converges to P 1 (0) p 1Æi V in W r -topology. Hence³V (¬i) converges to i V with respect<br />
to the W r -topology. This proves (ii).<br />
Lemma 10.6. The map ³W ,V is W r,r -open for all r 0.
LOCAL INVERSES OF SHIFT MAPS 447<br />
Pro<strong>of</strong>.<br />
Notice that<br />
func(F W , V )«¾ C½ (V ,Ê)Ï«(y, s), s«(y, s),<br />
and<br />
Hence<br />
³W ,V («)(y, s)(y,«(y, s)s).<br />
Sh(F W , V )f ¾ C½ (V , W )Ï p 1Æ f (y, s) y, p 2Æ f.<br />
1<br />
and the inverse map ³<br />
W ,VÏ Sh(F W , V )func(F W , V ) is given by<br />
1<br />
³ s) W ,V 2Æ ( f )(y, p f (y, s) s.<br />
Evidently, this map is W r,r -continuous for all r ¾Æ0, whence ³W ,V<br />
is W r,r -open.<br />
Now statement (2) <strong>of</strong> Theorem 10.2 follows from Lemmas 10.5, 10.6, and statement<br />
(B) <strong>of</strong> Theorem 9.1. Theorem 10.2 is completed.<br />
10.7. Periodic case. Let z be a periodic point <strong>of</strong> F. We will show that for a<br />
sufficiently small flow-box at z the images <strong>of</strong> -classes defined in Corollary 10.4 can<br />
be described in terms <strong>of</strong> that first recurrence map <strong>of</strong> orbit o z <strong>of</strong> z only, see (10.5).<br />
Let be the period <strong>of</strong> z, B be a codimension one open disk which transversally<br />
intersects the orbit o z at z, and RÏ (B, z)(B, z) be the first recurrence map. Let also<br />
5 and Ï W¼Êm 1¢ ( 4, 4) be a 4-flow-box at z. Decreasing W¼ we can<br />
assume, in addition, that<br />
(10.4) o z W¼ F(z¢ ( 4, 4)),<br />
B W , and B is transversal to all <strong>orbits</strong> <strong>of</strong> W¼ , so that the restriction p1BÏ W¼ <br />
BÊm 1 is a diffeomorphism. Put<br />
d (p 1B)<br />
1Æ p 1Ï V p 1Êm 1 (p 1B) 1 B.<br />
Then d preserves the first coordinate.<br />
Let W W¼ be the central -flow-box, V W be a connected D-neighbourhood<br />
<strong>of</strong> z, and A be the-class <strong>of</strong> U V . Then it follows from (10.4) that there exists a unique<br />
k¾ such that «(z) k for every «¾ A, and<br />
(10.5) P 1 (A) p 1Æ kÆ R dÏ d Rk V B B p 1Êm 1<br />
.
448 S. MAKSYMENKO<br />
10.8. Pro<strong>of</strong> <strong>of</strong> Theorem 10.1. Due to Theorem 10.2 it suffices to find a<br />
4-flow-box neighbourhood W¼ <strong>of</strong> z such that for every connected D-neighbourhood<br />
V <strong>of</strong> z, contained in the central -flow-box neighbourhood W , the image P 1 (0) is an<br />
isolated point <strong>of</strong> P 1 (U V ) in the W r -topology, where r 0 in the cases (a) and (b), and<br />
r 1 in the case (c).<br />
(a) Suppose that z is non-recurrent. Then there exist 0, and a 4-flow-box<br />
neighbourhood W¼ <strong>of</strong> z such that F(z, t)¾W¼ iff t4. Let W W¼ be the central<br />
-flow-box and V W be a connected D-neighbourhood. Then it follows from<br />
Lemma 10.3 that there exists only one equivalence class <strong>of</strong> . Hence im P 1 P 1 (0),<br />
and thus P 1 (0) is isolated in im P 1 in any <strong>of</strong> W r -topologies.<br />
Suppose that z is periodic. Let B be a codimension one open disk which transversally<br />
intersects the orbit o z at z, RÏ (B, z)(B, z) be the first recurrence map, and<br />
W¼ , W , and V be such as in §10.7.<br />
(b) If the germ <strong>of</strong> R at z is periodic <strong>of</strong> some period q, then we can assume that<br />
there exists an open neighbourhood E B <strong>of</strong> z such that R(E) E and d(V ) E.<br />
Then it follows from (10.5) that the image <strong>of</strong> P 1 is finite and consists <strong>of</strong> q points.<br />
Hence P 1 (0) is isolated in im P 1 in any <strong>of</strong> W r -topologies.<br />
(c) Suppose that the tangent map T z RÏ T z B T z B has at least one non-zero<br />
eigen vectorÚ¾T z B<br />
T z V with eigen valuesuch that1. Then T z R k (Ú)kÚ.<br />
Let T z p 1Ï T z B T 0Êm 1 be the tangent map <strong>of</strong> p 1 at z and uT z p 1 (Ú). Then for<br />
every class A corresponding to some k¾ we have that<br />
T z (P 1 (A)) (10.5)<br />
T z (p 1Æ kÆ R d)(Ú)k u.<br />
Since1, we see that P(0) is isolated in im P 1 in any <strong>of</strong> W r -topologies for r 1.<br />
11. Openness <strong>of</strong> Sh(F W , V) in Sh(F): Singular case<br />
Let W M be an open subset and V W be a D-submanifold.<br />
to (10.1) put<br />
Similarly<br />
(11.1) U V «¾<br />
func(F, V )ϳV («)(V )W.<br />
Then func(F W , V )U V<br />
and<br />
(11.2) ³V (U V )Sh(F, V )C½ (V , W )<br />
is a W 0 -open neighbourhood <strong>of</strong> i V in Sh(F, V ). We will now present a sufficient condition<br />
which guarantees that func(F W , V )U V . Due to (11.2) this will imply that<br />
(11.3) Sh(F W , V ) def<br />
³V (func(F, V ))³V (U V )Sh(F, V )C½ (V , W )
LOCAL INVERSES OF SHIFT MAPS 449<br />
a) b)<br />
Fig. 4.<br />
is W 0 -open in Sh(F, V ). In particular, we will prove (11.3) for vector fields <strong>of</strong> types<br />
(Z), (L), (H) and their products.<br />
DEFINITION 11.1.<br />
Let V W be a subset. We will say that a pair (W , V ) has<br />
proper boundary intersection property (p.b.i.) if for any x ¾ V , a ¾Ê, and T 1<br />
such that<br />
• F(x,a)¾W for ¾ [0, 1)T, but<br />
• F(x, a)¾Fr(W )WÒ W ,<br />
there exists ¼¾ (1, T ) such that F(x,¼ a)W , see Fig. 4 a).<br />
Roughly speaking, if the orbit o x <strong>of</strong> any x¾ V leaves W for a certain amount <strong>of</strong><br />
time and comes back into W , then during this time it must leave the closure W . In<br />
Fig. 4 b) the pair (W , V ) does not satisfy p.b.i. The following lemma is the crucial<br />
implication <strong>of</strong> p.b.i.:<br />
Lemma 11.2. Let z¾W , F(z)0, and V W be a connected D-neighbourhood<br />
<strong>of</strong> z such that (W , V ) has p.b.i. Then func(F W , V )U V .<br />
Pro<strong>of</strong>. Let « ¾ U V , so F(x,«(x)) ¾ W for all x ¾ W . We have to show that<br />
«¾ func(F W , V ). It suffices to verify that the following subset <strong>of</strong> V :<br />
K«x¾ VÏ F(x, s«(x))¾W for all s¾I [0, 1]<br />
coincides with all <strong>of</strong> V . Notice that z ¾ K«. Moreover, since W is open in M, it<br />
follows that K« is open in V . Therefore it suffices to show that VÒ K« is open in V<br />
as well. Since V is connected, we will get that K« V .<br />
Let x¾ VÒ K«. Then x F(x, 0¡«(x)) and F(x, 1¡«(x)) belong to W and there<br />
exists 0 ¾ (0, 1) such that F(x,«(x))¾W for all ¾ [0,0) while F(x,0«(x))¾<br />
Fr(W ). Now it follows from p.b.i. for the pair (W , V ) that there exists¼¾ (0, 1) such<br />
that F(x,¼«(x))W .<br />
Then there is an open neighbourhood V x <strong>of</strong> x in V such that<br />
F(y,¼«(y))W
450 S. MAKSYMENKO<br />
for all y¾V x . Hence V x <br />
VÒ K«, and thus VÒ K« is open in V .<br />
The following simple lemma is left for the reader.<br />
Lemma 11.3. (1) If (W , V ) has p.b.i., then for every subset V¼ V the pair<br />
(W , V¼ ) also has that property.<br />
(2) Let W¼ be an open neighbourhood <strong>of</strong> W . Then (W , V ) has property p.b.i. with<br />
respect to F if and only if it has this property with respect to the restriction FW¼. In<br />
other words, p.b.i. is determined by the behavior <strong>of</strong> F on arbitrary small neighbourhood<br />
<strong>of</strong> W only.<br />
(3) For every x¾ W denote by x the connected component <strong>of</strong> o x W containing x.<br />
Suppose that Fr(W ) is a smooth submanifold <strong>of</strong> M and for every x ¾ V its orbit o x<br />
is transversal to Fr(W ) at each y ¾x Fr(W ) whenever such a point exists. Then<br />
(W , V ) has p.b.i.<br />
11.4. Isolating blocks. Statement (3) <strong>of</strong> Lemma 11.3 is relevant with one <strong>of</strong> the<br />
principal results <strong>of</strong> [4]. An open subset U M is an isolating neighbourhood for the<br />
flow F if o x ê<br />
U for all x ¾ Fr(U)U Ò U. A closed F-invariant subset X M<br />
is isolated, if X is the maximal invariant subset <strong>of</strong> some isolating neighbourhood U<br />
<strong>of</strong> X.<br />
Let W be a compact D-submanifold <strong>of</strong> M and ÛW Ò Int W be its boundary.<br />
Denote<br />
Ûx¾ÛÏ0 with F(x¢ ( , 0)) W û,<br />
Û x¾ÛÏ0 with F(x¢ (0,)) W û,<br />
x¾ÛÏ F is tangent to Û.<br />
Then W is called an isolating block for F if ÛÛ and is a smooth submanifold<br />
<strong>of</strong> Û with codimension one. Thus Û and Û are submanifolds (possibly<br />
with corners if so is W ) <strong>of</strong>Ûwith common boundary. It follows that the interior <strong>of</strong><br />
an isolating block is an isolating neighbourhood. Moreover, from (3) <strong>of</strong> Lemma 11.3<br />
we obtain<br />
Lemma 11.5. If W is an isolating block, then for any subset V Int W the pair<br />
(Int W , V ) has p.b.i.<br />
Theorem 11.6 ([4]).<br />
Let X M be a closed isolated F invariant subset and<br />
U X be its isolating neighbourhood. Then there exists an isolating block W such<br />
that X Int W U.<br />
This result was established for the case when W is a manifold with boundary, but<br />
if M is F-invariant and X Mû, then the pro<strong>of</strong> easily extends to D-submanifolds.
LOCAL INVERSES OF SHIFT MAPS 451<br />
Corollary 11.7.<br />
Suppose z is an isolated singular point <strong>of</strong> F. Then there exist a<br />
base ¬W««¾A <strong>of</strong> open neighbourhoods <strong>of</strong> 0¾Êk such that for every W ¾¬ and<br />
any subset V W the pair (W , V ) has p.b.i.<br />
11.8. Semi-invariant sets. We say that W is negatively (positively) invariant with<br />
respect to F if for every x ¾ W and t 0 (t 0) such that (x, t)¾dom(F) we have<br />
F(x, t)¾ W . In this case we will also say that W is semi-invariant.<br />
Lemma 11.9. If W is semi-invariant with respect to F, then for any subset V <br />
W the pair (W , V ) has p.b.i.<br />
Pro<strong>of</strong>. Notice that if x, F(x, T a)¾W for some a¾Ê and T 1, then it follows<br />
from semi-invariance <strong>of</strong> W that F(x,a)¾W for all ¾ [0, T ]. Hence there are no<br />
x¾ V , a¾Ê and T 1 satisfying assumptions <strong>of</strong> Definition 11.1. Therefore (W , V )<br />
has p.b.i.<br />
11.10. Product <strong>of</strong> flows. For i 1, 2 let M i be a manifold, F i be a vector field<br />
on M i , W i M i be an open subset, and V i W i be a subset. Denote MM 1¢M 2<br />
and W W 1¢ W 2 . Consider the product <strong>of</strong> these vector fields F(x, y)(F 1 (x), F 2 (y))<br />
on M. It generates a local flow F(x, y, t)(F 1 (x, t), F 2 (y, t)).<br />
Lemma 11.11. Suppose that (W i , V i ) has p.b.i. with respect to F i , (i 1, 2), and<br />
let V V 1¢V 2 be a subset. Then (W , V ) has p.b.i. with respect to F.<br />
Pro<strong>of</strong>.<br />
Let x (x 1 , x 2 )¾V , a¾Ê, and T 1 be such that<br />
F(x,a)(F 1 (x 1 ,a), F 2 (x 2 ,a))¾W , ¾ [0, 1)T,<br />
F(x, a)(F 1 (x 1 , a), F 2 (x 2 , a))¾Fr(W )(Fr(W 1 )¢ W 2 )(W 1¢ Fr(W 2 )).<br />
In particular, F i (x i , a)¾Fr(W i ) for at least one index i 1, 2. For definiteness assume<br />
that F 1 (x 1 , a)¾Fr(W 1 ). Since x 1 ¾ V 1 , it follows from p.b.i. for (W 1 , V 1 ) that there<br />
exists ¼ ¾ (1, T ) such that F 1 (x 1 ,¼ a) W 1 . Then F(x,¼ a) W as well. Hence<br />
(W , V ) has p.b.i. with respect to F.<br />
Corollary 11.12. Let F be a product <strong>of</strong> vector fields <strong>of</strong> types (L) or (H) on Êm .<br />
Then there exist a base ¬W««¾A <strong>of</strong> open neighbourhoods <strong>of</strong> 0¾Êk such that for<br />
every W ¾¬ and any subset V W the pair (W , V ) has p.b.i. In particular, if V is<br />
a connected D-neighbourhood <strong>of</strong> 0, then func(F W , V )U V and thus by (11.2)<br />
is W 0 -open in Sh(F, V ).<br />
Sh(F W , V )Sh(F, V )C½ (V , W )
452 S. MAKSYMENKO<br />
Pro<strong>of</strong>. Due to Lemma 11.11 it suffices to assume that F is <strong>of</strong> type (L) or (H).<br />
If F is <strong>of</strong> type (HE), then 0 has an arbitrary small invariant neighbourhoods W and<br />
by Lemma 11.9 (W , V ) has p.b.i. for any subset V W . If F is <strong>of</strong> type (HS) then<br />
is an isolated invariant subset <strong>of</strong> any <strong>of</strong> its small neighbourhood, whence<br />
0 Ê2<br />
existence <strong>of</strong> W follows from Theorem 11.6, though it can easily be constructed without<br />
referring to this theorem.<br />
It remains to consider the case when F(x) Bx, where B is a Jordan cell corresponding<br />
either to some eigen value a¾Ê or to the pair <strong>of</strong> complex conjugate a¦ ib,<br />
(a, b¾Ê).<br />
1) If a 0 (a 0), then, e.g. [26], 0 has arbitrary small positively (negatively)<br />
F-invariant neighbourhoods W . Moreover, if B 0 b<br />
, then 0¾Ê2 has arbitrary<br />
b 0<br />
small F-invariant neighbourhoods W . Then again by Lemma 11.9 such neighbourhoods<br />
have desired properties.<br />
2) Suppose that B <br />
¡¡¡<br />
0 1<br />
0 1<br />
0<br />
given by the following formulas:<br />
F 1 (x, t)x 1x 2 t<br />
is nilpotent. Then the coordinate functions <strong>of</strong> F are<br />
t 2<br />
t<br />
x 3 x<br />
2!¡¡¡ m 1<br />
m<br />
(m 1)! , F i <br />
F i 1<br />
,<br />
t<br />
for i 2,, m. In particular, for each x ¾Êm these functions are polynomials in t<br />
<strong>of</strong> degree m 1. Hence for every Ær 0 there exists T 0 such that if x 0Ær and<br />
x 0 is not a fixed point <strong>of</strong> F, then F(x, t) strictly monotone increases when increases<br />
t T (decreases t T ).<br />
For every r 0 let V Êm r be the closed m-disk <strong>of</strong> radius r centered at the<br />
origin and W r Int(V r ) be its interior. Since F(0, t)0 for all t¾Ê, it follows that<br />
for every R 0 there exists rÆr such that F(V r¢ [ T , T ])W R , i.e.F(x, t) R<br />
for xr and tT . We claim that the pair (W R , V r ) has p.b.i.<br />
Suppose that for some x¾ V r and a¾Ê we have F(x,a)¾W R for¾ [0, 1) and<br />
F(x, a)¾Fr(W R )V<br />
R<br />
, i.e.F(x,a) R andF(x, a) R. ThenaT , whence<br />
F(x, t) strictly monotone increases when increases t. In particular, F(x,a) R<br />
for all 1, i.e. F(x,a)V R W R .<br />
3) Suppose that ib, (b0), is purely imagine but m 2k 4 for some k 2.<br />
Then regarding Êm as k we have that in complex coordinates A <br />
¡¡¡<br />
ib 1<br />
ib 1<br />
ib .<br />
Hence the coordinate functions <strong>of</strong> F are given by formulae similar to the case 2). Denote<br />
z (z 1 ,, z k ) and p(z, t)z 1 z 2 t z 3 t 22!¡¡¡z k t k 1(k 1)!. Then<br />
F 1 (z, t)e ib p(z), F i e ibF i 1<br />
, i 2,, k.<br />
t
LOCAL INVERSES OF SHIFT MAPS 453<br />
Since e ib1, it follows that F(x, t) satisfies monotonicity conditions analogous to<br />
the case 2). Then by the similar arguments we obtain that for every R 0 there exists<br />
r 0 such that the pair (W R , V r ) has property p.b.i.<br />
12. Pro<strong>of</strong> <strong>of</strong> Theorem 3.5<br />
Let F be a vector field <strong>of</strong> class F(M). It follows from results <strong>of</strong> [18] that Sh(F)<br />
E id (F) k , where k 1 if (L)¼(HS)¼<br />
and k 0 otherwise.<br />
Therefore we should prove that the map³Ï func(F)Sh(F) is a homeomorphism<br />
with respect to S½ -topologies. Actually we want to apply Theorem 8.2.<br />
Claim 12.1. Suppose that F belongs to class F(M).<br />
(1) If z¾, then for any sufficiently small connected compact D-neighbourhood V <strong>of</strong><br />
z the <strong>shift</strong> map ³VÏ func(F, V )Sh(F, V ) is<br />
(L2)¼<br />
W½,½ -open. Moreover, if<br />
, then ³V is even W<br />
z¾(L1)¼<br />
r,r2 -open for all r 0.<br />
(2) If z is a regular point <strong>of</strong> F, then for any sufficiently small connected compact D-<br />
neighbourhood V <strong>of</strong> z the <strong>shift</strong> mapping ³VÏ func(F, V )Sh(F, V ) is W r,r -open for<br />
all r 1.<br />
Pro<strong>of</strong>. By (C) Theorem 9.1 it suffices to find a neighbourhood W <strong>of</strong> z such that<br />
for every connected D-neighbourhood V W <strong>of</strong> z<br />
(i) the <strong>shift</strong> map³W ,VÏ func(F W , V )Sh(F W , V ) is W r,s -open for the corresponding<br />
values r, s, and<br />
(ii) its image Sh(F W , V ) is W k -open in Sh(F), where k 0 in the cases (1), and k 1<br />
in the case (2).<br />
(1) Let z¾F. Then by definition <strong>of</strong> class F(M) there exists a neighbourhood<br />
W <strong>of</strong> z on which in some local coordinates either<br />
(a)<br />
G n each <strong>of</strong> which belongs<br />
F is a product <strong>of</strong> finitely many vector fields G 1 ,,<br />
to one <strong>of</strong> the types (Z), (L), or (H), or<br />
(b) F belongs to one <strong>of</strong> the types (L1)¼ , (L2)<br />
¼ , (L3)<br />
¼ , (H)<br />
¼<br />
and z is an isolated singular<br />
point <strong>of</strong> F.<br />
Decreasing W we can also assume that Sh(F W , V ) is W 0 -open in Sh(F), i.e. condition<br />
(ii) is satisfied. In the case (a) this follows from Corollary 11.12, while in the<br />
case (b) from Corollary 11.7.<br />
Then (i) directly follows from Lemmas 7.1–7.3.<br />
(2) Suppose that z is a regular point for F. Since F belongs to F(M), it follows<br />
that the assumptions <strong>of</strong> Theorem 10.1 are satisfied, whence for any sufficiently small<br />
D-neighbourhood <strong>of</strong> z the <strong>shift</strong> map ³V is W r,r -open for all r 1.<br />
For every z ¾ M let V z be a neighbourhood guaranteed by Claim 12.1. By assumption<br />
<strong>of</strong> Theorem 3.5 the set Ò ((L1)¼(L2)¼<br />
) is compact.
454 S. MAKSYMENKO<br />
Therefore using paracompactness <strong>of</strong> M we can find a locally finite cover V ii¾¿<br />
<strong>of</strong> M by compact connected D-submanifolds and a finite subset ¿¼¿ such that the<br />
map ³V i<br />
is W½,½ -open for i¾¿¼ and W r,r2 -open for all r 0 whenever i¾¿Ò¿¼ .<br />
Hence by “fragmentation” Theorem 8.2 ³ is a local homeomorphism with respect to<br />
S½ -topologies. All other statements concerning homotopy types <strong>of</strong> Did (F) r and E id (F) r<br />
follow by the arguments <strong>of</strong> the pro<strong>of</strong> <strong>of</strong> [13, §9]. Theorem 3.5 is completed.<br />
ACKNOWLEDGEMENTS. I would like to thank V.V. Sharko, A. Prishlyak,<br />
I. Vlasenko, and I. Yurchuk for useful discussions. I am especially grateful to E. Polulyakh<br />
for very helpful conversations and pointing out to the irrational flow on T 2 which lead<br />
me to discovering mistakes <strong>of</strong> [13].<br />
References<br />
[1] D.L. Blackmore: On the local normalization <strong>of</strong> a vector field at a degenerate critical point, J.<br />
Differential Equations 14 (1973), 338–359.<br />
[2] A.D. Brjuno: Analytic form <strong>of</strong> differential equations, I, Trudy Moskov. Mat. Obšč. 25 (1971),<br />
119–262.<br />
[3] R.V. Chacon: Change <strong>of</strong> velocity in flows, J. Math. Mech. 16 (1966), 417–431.<br />
[4] C. Conley and R. Easton: Isolated invariant sets and isolating blocks, Trans. Amer. Math. Soc.<br />
158 (1971), 35–61.<br />
[5] L. Frerick: Extension operators for spaces <strong>of</strong> infinite differentiable Whitney jets, J. Reine Angew.<br />
Math. 602 (2007), 123–154.<br />
[6] D. Hart: On the smoothness <strong>of</strong> generators, Topology 22 (1983), 357–363.<br />
[7] M.W. Hirsch: Differential Topology, corrected reprint <strong>of</strong> the 1976 original, Graduate Texts in<br />
Mathematics 33, Springer, New York, 1994.<br />
[8] E. Hopf: Ergodentheorie, Chelsea Publishing Co., Berlin, 1937.<br />
[9] S. Illman: The very-strong C½ topology on C ½ (M, N) and K -equivariant <strong>maps</strong>, <strong>Osaka</strong> J. Math.<br />
40 (2003), 409–428.<br />
[10] A.V. Kočergin: Change <strong>of</strong> time in flows, and mixing, Izv. Akad. Nauk SSSR Ser. Mat. 37<br />
(1973), 1275–1298.<br />
[11] V.A. Kondrat¼ ev and V.S. Samovol: The linearization <strong>of</strong> an autonomous system in the neighborhood<br />
<strong>of</strong> a singular point <strong>of</strong> “knot” type, Mat. Zametki 14 (1973), 833–842.<br />
[12] M. Kowada: The orbit-preserving transformation groups associated with a measurable flow, J.<br />
Math. Soc. Japan 24 (1972), 355–373.<br />
[13] S. Maksymenko: Smooth <strong>shift</strong>s <strong>along</strong> trajectories <strong>of</strong> flows, Topology Appl. 130 (2003),<br />
183–204.<br />
[14] S. Maksymenko: Hamiltonian vector fields <strong>of</strong> homogeneous polynomials in two variables, Pr.<br />
Inst. Mat. Nats. Akad. Nauk Ukr. Mat. Zastos. 3 (2006), 269–308, arXiv:math/0709.2511.<br />
[15] S. Maksymenko: Homotopy types <strong>of</strong> stabilizers and <strong>orbits</strong> <strong>of</strong> Morse functions on surfaces, Ann.<br />
Global Anal. Geom. 29 (2006), 241–285.<br />
[16] S. Maksymenko: Stabilizers and <strong>orbits</strong> <strong>of</strong> smooth functions, Bull. Sci. Math. 130 (2006),<br />
279–311.<br />
[17] S. Maksymenko: Connected components <strong>of</strong> partition preserving diffeomorphisms, Methods Funct.<br />
Anal. Topology 15 (2009), 264–279.<br />
[18] S. Maksymenko: Image <strong>of</strong> a <strong>shift</strong> map <strong>along</strong> the <strong>orbits</strong> <strong>of</strong> a flow, to appear in Indiana Univ.<br />
Math. J.
LOCAL INVERSES OF SHIFT MAPS 455<br />
[19] S. Maksymenko: ½-jets <strong>of</strong> diffeomorphisms preserving <strong>orbits</strong> <strong>of</strong> vector fields, Cent. Eur. J.<br />
Math. 7 (2009), 272–298.<br />
[20] S. Maksymenko: Reparametrization <strong>of</strong> vector fields and their <strong>shift</strong> <strong>maps</strong>, Pr. Inst. Mat. Nats.<br />
Akad. Nauk Ukr. Mat. Zastos. 6 (2009), 489–498, arXiv:math/0907.0354.<br />
[21] S. Maksymenko: Symmetries <strong>of</strong> center singularities <strong>of</strong> plane vector fields, Nonlinear Oscilations<br />
13 (2010), 177–205.<br />
[22] J. Margalef Roig and E. Outerelo Domínguez: Differential Topology, North-Holland Mathematics<br />
Studies 173, North-Holland, Amsterdam, 1992.<br />
[23] J.N. Mather: Stability <strong>of</strong> C½ mappings, I, The division theorem, Ann. <strong>of</strong> Math. (2) 87 (1968),<br />
89–104.<br />
[24] B.S. Mitjagin: Approximate dimension and bases in nuclear spaces, Uspehi Mat. Nauk 16<br />
(1961), 63–132.<br />
[25] M.A. Mostow and S. Shnider: Joint continuity <strong>of</strong> division <strong>of</strong> smooth functions, I, Uniform<br />
Lojasiewicz estimates, Trans. Amer. Math. Soc. 292 (1985), 573–583.<br />
[26] J. Palis, Jr. and W. de Melo: Geometric Theory <strong>of</strong> Dynamical Systems, translated from the<br />
Portuguese by A.K. Manning, Springer, New York, 1982.<br />
[27] W. Parry: Cocycles and velocity changes, J. London Math. Soc. (2) 5 (1972), 511–516.<br />
[28] R.T. Seeley: Extension <strong>of</strong> C½ functions defined in a half space, Proc. Amer. Math. Soc. 15<br />
(1964), 625–626.<br />
[29] C.L. Siegel: Über die Normalform analytischer Differentialgleichungen in der Nähe einer<br />
Gleichgewichtslösung, Nachr. Akad. Wiss. Göttingen. Math.-Phys. Kl. Math.-Phys.-Chem. Abt.<br />
1952 (1952), 21–30.<br />
[30] S. Sternberg: <strong>Local</strong> contractions and a theorem <strong>of</strong> Poincaré, Amer. J. Math. 79 (1957),<br />
809–824.<br />
[31] H. Totoki: Time changes <strong>of</strong> flows, Mem. Fac. Sci. Kyushu Univ. Ser. A 20 (1966), 27–55.<br />
[32] R.J. Venti: Linear normal forms <strong>of</strong> differential equations, J. Differential Equations 2 (1966),<br />
182–194.<br />
[33] H. Whitney: Analytic extensions <strong>of</strong> differentiable functions defined in closed sets, Trans. Amer.<br />
Math. Soc. 36 (1934), 63–89.<br />
Topology dept.<br />
Institute <strong>of</strong> Mathematics <strong>of</strong> NAS <strong>of</strong> Ukraine<br />
Tereshchenkivs’ka st. 3, Kyiv, 01601<br />
Ukraine<br />
e-mail: maks@imath.kiev.ua