A NNALES DE L ’I. H. P., SECTION B
M ICHEL T ALAGRAND
Approximating a helix in finitely many dimensions
Annales de l’I. H. P., section B, tome 28, n
o3 (1992), p. 355-363
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355-
Approximating
ahelix in finitely many dimensions
Michel TALAGRAND
Équipe
d’Analyse, Tour 46, U.A. au C.N.R.S. n° 754, Universite Paris-VI, 75230 Paris Cedex 05, FranceVol. 28, n° 3, 1992, p. 363. Probabilités et Statistiques
ABSTRACT. - Consider
a e ]0, 1[.
We prove that there exists a constantK (a), depending
on aonly,
such that forp >_ 1,
there exists a map F from R to RP such that for we haveRESUME. - Pour
ae]0,1[,
il existe une constanteK (a), dependant
de aseulement,
telle que pour/?~1,
il existe uneapplication
F de R dans RPtelle que, pour tous reels s, t on ait
A.M.S. 1980 classification numbers primary 461320, 60617.
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques - 0246-0203
356 M. TALAGRAND
1. INTRODUCTION
A helix is a map h from R to a Hilbert space H such that
I for
s, t e R. Withinisometries,
a helix is determin- edby
the functionIt is a theorem of I. J.
Shoenberg
that thefunctions 03C8(t) given by (1)
areexactly
the functions ofnegative type.
In this note, we are interested in thecase I h (t) II
for a certainae]0,1[.
The casea =1 /2 corresponds
to Wilson’s
helix,
that is realizedby
Brownian motion.P. Assouad and L. A.
Shepp
raised thequestion
whether the helixcorresponding
toII h (t) II = t 11/2 (Wilson’s helix)
can beapproximated
inthe
p-dimensional
euclidean space. This was settledby
J. P. Kahane[2]
who obtained the
following
result.(Throughout
the paper,II
denotesthe euclidean
norm.)
THEOREM 1
(J.
P.Kahane). -
There exists a universal constant K suchthat for
p >_ 1,
there exists a map F from R to RP such thatOn the other
hand,
P. Assouad[1] proved
that for allae]0,1],
there exists a map F from R to f~p such that
where K
depends
on aonly.
The estimate of(2)
does notimprove
whenp - ~. The purpose of the present note is to
improve
upon(2).
THEOREM 2. - Given a
e]0, 1[,
there exists a constant K(a), depending
on a
only,
such thatfor p >__ 1,
there exists a .map Ffrom ~
to IRP thatsatisfies
In the case
a = 1 /2,
thisgives
an error inK/ Jp,
andunfortunately
doesnot recover the error
K/p
of Kahane’s Theorem 1. It is not difficult to seethat this error
K/p
is ofoptimal
order in Kahane’stheorem;
but when1 /2,
we do not have a nontrivial lower bound for the error in(3).
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques
2. THE APPROACH
We fix
ae]0, 1[,
and/~1.
Forconvenience,
we assume that p is amultiple
of 4(so that p >_ 4).
We set, for~0,
For
0 q __ 2" + 1 _ 2,
we setThus For
nl, 0~~~2~~-2,
we findl(q)(=ln(q))
such that
In,q
c When0~2"~~-2,
andwhen q
is even, thereare two
possible
choices. We make anarbitrary choice;
the construction willactually
notdepend
on that choice.Consider a map t - x
(t)
from R to a Hilbert space H that satisfies We first construct affine maps from H to RPthat
satisfy
,We
proceed
to this easyconstruction, by
induction over n. A basicobservation is that
Dn
nIn, q
hasp + 1 points.
The affine span of thesepoints
is isometric toRP;
thus foreach n, q,
one can find an affine map~n, q
from H to RP that satisfiesWe take the maps have been
constructed,
for a certain n and for all
~2"’~-2,
we takewhere U is an
isometry
of RP such thatU(~+i ~(x(~)))=8~
~q~(x (t))
forBy isometry
we mean]
forThe existence of U follows from the
following elementary fact,
that will be usedrepeatedly:
if S is a map from a subset A of RP to RP suchthat
for x,y e A,
then we can find anisometry
Uof RP such that U
(x)
= S(x)
for x E A.For the
simplicity
ofnotation,
we will write xn, q, t =(x (t)).
The ideaof the
preceding
construction is that thepoints xn, q, t, t
eDn
riIn, q
havethe correct
position
with respect to each other.Also,
a certaindegree
ofconsistency
is obtainedthrough (5).
One would like to haveF (t) = xn, q,
tfor t e Dn n In, q-
Theproblem
is that it is notpossible
to insure that To solve thatdifficulty,
fort e
!~
~, we will construct anisometry Rn, q, of
IRP . Werequire
thefollowing
358 M. TALAGRAND
properties.
(8)
For s, t eIn,
q, x, y eRP,
we have(There,
as in thesequel,
K is a constantdepending
on (xonly,
that isnot
necessarily
the same at each occurence; on the otherhand, Kl, K2, ...
denote
specific
constantsdepending
on (xonly).
(10)
For t in[(~+1)2--B (~+2)2--~
theisometry
rdoes not
depend
on t.~ ~ ~
The construction of these isometries will be done in section
3; but, before,
weprovide
motivationby proving
Theorem 2.Givne n, there are two consecutive values
of q
for whicht e In,
~; if follows from(6)
that the value ofF (t)
does notdepend
on which valueof q
we use.
Also,
it follows from(7)
that the value of F(t)
does notdepend
on which value of n we consider.
Thus, (11) actually
definesF (t)
fortED= U D~.
n~O
Consider now
u,veDn
suchthat
Thusu,veIn,q
forsome q. Let
03C4=(q+1)2-n-1.
It follows from(4),
since is an iso- metry, thatThus, by (9),
used for and for we haveIt follows in
particular
thatAnnales de l’Institut Henri Poincaré - Probabilités et Statistiques
LEMMA. -
Proof. -
Consider thelargest n
suchthat ~-~~2’",
so thatWe observe
that, given se[O, 1],
we can find suchthat
We thus construct sequences(uk), (vk) k> n,
such that
Thus
We can and do assume that vk = t for k
large enough.
ThenBy ( 13),
thisimplies
thatThe lemma
implies
inparticular
that F can be extendedby continuity
to the closure of
D,
i. e. to[0,1],
and thatfor s,
t E [o,1 ] .
Consider now
s, t E [o,1 ]
and thelargest
n suchthat
so that
2 -" __ 4 ~
s - Consider q such that s, t eIn,
q. Thus we can find u, v e nDn
suchthat s - u _- 2 - n/p, ~ t - v 2 - n/p. By ( 1 4),
we haveThus
From
( 12),
we haveThus, since ~ 2014 ~ ~ 2 " ~,
we haveWe have
Using
that forI x I 5 4,
we get thatThus,
we have constructed a map F from[0,1] to
(~p such that360 M. TALAGRAND
There is no loss of
generality
to assumeF (1 /2) = 0.
Consider an ultra-filter 4Y on and define
The limit exists
since,
from( 14)
andF( - B2/ )=0, we have
Moreover it is immediate to check
that, for s, teR,
we have Thiscompletes
theproof
of Theorem 2.The reader has observed that conditions
(8)
and(10)
have not beenused. Condition
(8)
is usedduring
the construction as apreliminary
step for conditions(9).
Condition(10) helps
tokeep
control of the situation asthe induction continues.
3. CONSTRUCTION
The construction
proceeds by
induction on n. Fort E [0,1],
we setRo, o, t - Identity.
We nowperform
the induction step from n -1 to n.Consider q, - I ~~2" ~-2,
and setFor t e I,
we construct isometriesTn, q, t’ Sn, q, of RP,
such that thefollowing
holds
(where
we set/(- 1)=0)
(22)
Fort E I,
theisometry T-1n,q,t°Sn,q+1,t does
notdepend
on t.Annales de l’Institut Henri Poincaré - Probabilités et Statistiques
Before we
proceed
to the construction of the isometriesTn, q, t, Sn,
we show how to construct the isometries
Rn, q,
t for0 _ q _ 2" 1 _ 2.
(~+2)2’"’~],
we setRn, q, t = Tn, q, t.
Condition(17)
ensures that~ so that is well defined. It is
simple
to see thatconditions
(6) to (10)
follow from conditions( 18)
to(22) respectively.
We now construct the isometries
Sn, q,
t. Setl = l (q), I’ = I(q + 1).
Thus,
we either have /’==/ or l’ = l + 1.I
For~e[(/+l)2-~ (/+2)2 "L
wehave
by
inductionhypothesis
and(10) that,
if /’=1+1,
If
/’=/,
the above alsoholds,
forV = identity.
We set forsimplicity thus, by (23),
weGiven we have
This is obvious if
/’=/;
if/’=/+1,
this follows from(6). Remembering
that we
get
It then follows from
(5)
thatSince
A,
B areisometries,
it follows from(4)
thatThus, there exists an
isometry
U of RP such thatSince card I n
Dn =p/2
+ 1 p, we can assume that det U =1(by
compos-ing
if necessary Uby
a reflectionthrough
ahyperplane containing
thepoints A (xn, q, t), tel
nDn.)
It is then clear that we can find asemi-group U (t)
of isometries ofRP,
withU ( 1 ) = U,
such that(actually
one can takeK3
=2 ~).
For
t e l,
we setwhere
q)(~)=2~(~-T).
Thus(p(r)=0,
cp(-r’)
=1. Thus( 17)
holds.It remains to prove
(18)
to(22).
362 M. TALAGRAND
Proof 01(18). -
It follows from(25) that,
for nI,
we haveso that
and,
combined with(27)
and the definitionof Tn, q, t,
thisimplies ( 18).
Proof of (19). -
We consideronly
the case of and leave the other case to the reader.By (24), (25),
we have~ ’
so have
for all s e R. Thus which
implies
i the result.Proof of (20). -
We prove thisinequality
for the constantwhere
K3
occurs in(26)
and weagain
consideronly
the case ofTn, q,
t.We have
’ ’
where
for Since A and
U
(cp (s))
areisometries,
wehave ~
x’ -y’ ~= ( x -
We observe that(8)
holds with the same value
K = Kl
of the constant K than(20); thus, by
induction
hypothesis,
we haveSince ° A 1 is an
isometry,
we haveThus
Annales de l’Institut Henri Poincaré - Probabilités et Statistiques
Prool 01 (21). -
We prove(21)
forK2 = 2°‘ K 1 (1-2’~’~)’~
andagain
we consider
only
the case of T. Weproceed by induction, observing
that
(9)
holds with the same constantK2.
We find v in with!M-~!2’"’’~.
We havewhere
We recall that
by (24), (25)
so
that, by
definition ofTn, q,
tand, by
inductionhypothesis,
If we recall that
(20)
holds for the constantKl
we haveSince, by (4),
we have Thus
and this does not
depend
on t.The
proof
iscomplete.
[1] P. ASSOUAD, Plongements Lipschitziens dans Rn, Bull. Soc. Math. Fr., Vol. 111, 1983, pp. 429-448.
[2] J. P. KAHANE, Hélices et quasi-hélices, Adv. Math., Vol. 7 B, 1981, pp. 417-422.
(Manuscript received February 13, 1991.) REFERENCES