The Hausdor¤ dimension of deformed self-similar sets
Tae Hee Kim, Sung Pyo Hong and Hung Hwan Lee
(Received October 12, 1999) (Revised June 12, 2001)
Abstract. We define deformed self-similar sets which are generated by a sequence of similar contraction mappingsffs:sASgonRd,fshaving its contraction ratiors, and calculate thier Hausdor¤ dimension.
1. Introduction
Hutchinson [4] proved that there exists a unique compact set FHRd such that F¼6n
i¼1fiðFÞ for any given finite set ffigi¼1n of similarities in Rd with ratio ri, 1aian. He also showed that dimHF ¼dimBF ¼dimpF¼s andPn
i¼1ris¼1 if ffigi¼1n satisfies the open set condition, that is, there exists a bounded non-empty open setOsuch that6n
i¼1fiðOÞHOandfiðOÞVfjðOÞ ¼j if i0j.
Recently, S. Ikeda [5] defined the loosely self-similar set F which is gen- erated by a sequence of mappingsffi1i2...ikg ðijAf1;2;. . .;ngÞ,fi1i2...ik having its contraction ratio rik, and showed that dimHF ¼s andPn
i¼1ris¼1 if ffi1i2...ikg satisfies the disjoint condition.
In this paper, we will generalize loosely self-similar sets [5] and perturbed Cantor sets [1]. The construction is as follows.
Fix mb2, write Sk ¼ f1;2;. . .;mgk and S¼6y
k¼1Sk. Consider a se- quence of similar contraction mappingsffs:sASgonRd. Suppose that each fshas a contraction ratiors, that is,jfsðxÞ fsðyÞj ¼rsjxyjfor anyx;yARd, where j j is the Euclidean norm. We further assume there exists 0<a;b<1 such thata<rs<b for anysASand there exists a bounded open set VHRd such that
(1) fsðVÞHV for any sAS
(2) fi1i2...ik1ikðVÞVfi1i2...ik1ik0ðVÞ ¼j, ik0i0k.
It is obvious that there exists a non-empty compact set XHV such that the properties (1) and (2) are satisfied when V is replaced by X.
2000 Mathematics Subject Classification. 28A78, 28A80.
Key words and phrases. Deformed self-similar set, Hausdor¤ measure, Hausdor¤ dimension.
The first author was supported by KOSEF and the second author was supported by Com2MaC- KOSEF. The third author was supported by TGRC and Korean Research Foundation 1998-015- D00019.
For brevity, we write
Fs1fi1fi1i2 fi1i2...ik
Rs1ri1ri1i2. . .ri1i2...ik
for anys¼i1i2. . .ik ASk. Then using a compact setXgiven above we obtain a unique compact set K,
K¼ 7
y
k¼1
6
sASk
FsðXÞ:
We call this K a deformed self-similar set. If we take rs¼rik for any s¼
i1i2. . .ik, the obtained set K becomes a loosely self-similar set in S. Ikeda’s
sense. Moreover, if we takefi1i2...ik¼fik for all k, the obtained setKis a self- similar set in Hutchinson’s sense.
2. Preliminaries and main theorem
We begin to recall the well-known s-dimensional Hausdor¤ measure and dimension: Let E be a bounded subset of Rd and sb0. For every d>0 we define
HdsðEÞ ¼inf Xy
i¼1
jUijs:EH 6
iUi;jUijad
( )
;
where jAj denotes the diameter of A. Then we obtain the s-dimensional Hausdor¤ measure of E by
HsðEÞ ¼lim
d!0 HdsðEÞ:
The Hausdor¤ dimension of E is defined by
dimH E¼supfsb0:HsðEÞ ¼yg:
Then we see that
dimHE¼inffsb0:HsðEÞ ¼0g:
To calculate the Hausdor¤ dimension ofK we recall a measure on subsets of K due to Rogers [7]. For any sb0, nAN and EHK, let
MnsðEÞ ¼inf X
jFsðXÞjs:EH 6
sFsðXÞ;sA 6
kbn
Sk
( )
:
Then we get a measure of Hausdor¤ type on subsets of K by letting MsðEÞ ¼ lim
n!yMnsðEÞ:
We note that if MtðEÞ>0 then MsðEÞ ¼y for all s<t. Therefore we see that
supfsb0:MsðEÞ ¼yg ¼inffsb0:MsðEÞ ¼0g:
Now we are ready to show a method to get the Hausdor¤ dimension of a deformed self-similar set.
Theorem 2.1. Let K be a deformed self-similar set as defined in the intro- duction. Puta¼supfsb0jMsðKÞ ¼yg. Then we have0<HaðKÞ<yand
dimH K¼a:
Proof. By the definition ofa;MsðKÞ<y for anys>a. Thus, for such an s, HdsðKÞaMnsðKÞaMsðKÞ if dbbn, where b is an upper bound of con- traction ratios rs. Letting d!0, we have
HsðKÞaMsðKÞ<y fors>a;
which implies dimHKaa.
To prove that dimHKba, we claim thatsadimH K, for alls<a. For 0<s<a,MsðKÞ ¼yby the definition ofa. Then there exists a compact subset FHK and a constant b>0 such that 0<MsðFÞ<y and MsðFVFsðXÞÞa bRss for all sAS. (See Proposition 3.1 [3].) Define a Borel measure m by
mðAÞ ¼MsðFVAÞ forAHK:
Then 0<mðKÞ<y and mðFsðXÞÞabRss for all sAS.
Let Vbe the open set given in the introduction and letUHRd satisfy 0<
jUjajVj. Set
Q¼ fsAS:jFsðVÞj<jUjandjFsj ðjsj1ÞðVÞjbjUjg;
where sjl¼i1i2. . .il fors¼i1i2. . .ik andlak. We see that ajUj<jFsðVÞj<
jUj for sAQ. Then Qo¼ fsAQ:UVFsðVÞ0 jg has at most some finite mo elements which is independent of U sincefFsðVÞ jsAQog is disjoint. (See Lemma 9.2 [2].)
Hence
mðUÞa X
sAQo
mðFsðXÞÞ
ab X
sAQo
Rss
abmojVjsjUjs
which, by Mass distribution principle 4.2 [2], implies thatHsðKÞ>0. That is, dimHKbs for any s<a. Therefore dimH Kba. r
Remark(cf. [3]). LetKbe a non-empty compact set generated by relaxing equality (3) to inclusion, that is,
KH 7
y
k¼1
6FsðKÞ:
Then it can be proved that
dimHK¼supfsb0:MsðKÞ ¼yg by the same proof as in Theorem 2.1.
Corollary2.2 (I. S. Baek [1]). Put X ¼ ½0;1. Define a sequence of con- traction maps ffi1i2...ikg on X for i1i2. . .ik Af1;2gk, k¼1;2;. . .; such that
fi1i2...ikðxÞ ¼ rðkÞ1 x; if ik ¼1 rðkÞ2 xþ ð1rðkÞ2 Þ; if ik ¼2 8<
:
and there exist 0<a;b<1 such that
a<rðkÞi <b; and a<1X2
i¼1
rðkÞi <b for all k. Put
K¼ 7
y
k¼1
6
sASk
FsðXÞ:
Then K is a perturbed Cantor set and dimH K¼supfsb0:MsðKÞ ¼yg
¼sup sb0:lim inf
n!y
X
i1i2...inAf1;2gn
ðrð1Þi1 rð2Þi2 . . .rðnÞin Þs¼y 8<
:
9=
;: Proof. Let
b¼sup sb0:lim inf
n!y
X
i1i2...inAf1;2gn
ðrð1Þi1 rð2Þi
2 . . .rðnÞin Þs¼y 8<
:
9=
;
¼sup sb0:lim inf
n!y
X
sAf1;2gn
jFsðXÞjs¼y 8<
:
9=
;:
To show that dimH Kab, suppose that 0<s<dimHK. Then lim
n!yMnsðKÞ ¼ y, that is, for givenL, there existsnosuch thatMnsðKÞbLfornbno. Hence
P
sAf1;2gn
jFsðXÞjs>L for nbno. Therefore lim inf
n!y
P
sAf1;2gnjFsðXÞjs¼y, so sab. Now supposes<b. Then lim inf
n!y
P
sAf1;2gn
jFsðXÞjs¼y. Define a finite Borel measure m on X such that
mðFsðXÞÞ ¼ jFsðXÞjs P
sAf1;2gn
jFsðXÞjs:
Then mðFsðXÞÞ ¼P2
i¼1
mðFsiðXÞÞ and this measure m is supported on K, thus, mðKÞ ¼1. Since s<b, it is easy to see that from the definition of b that
lim inf
n!y
jFi1i2...inðXÞjs
mðFi1i2...inðXÞÞ¼lim inf
n!y
X
sAf1;2gn
jFsðXÞjs¼y
for all xAK, where i1i2. . .in. . . is the uniquely obtained sequence such that x¼ lim
n!yFi1i2...inðXÞ. Hence there exists c>0 such that HsðKÞbc mðKÞinf
xAK lim inf
n!y
jFi1i2...inðXÞjs mðFi1i2...inðXÞÞ¼y: (See Theorem 2.1 [8] and Lemma 2.2 [6].)
Therefore MsðKÞbHsðKÞ ¼y. So, MsðKÞ ¼y, which implies ba
dimHK. r
Corollary 2.3 (S. Ikeda [5]). Let K be a deformed self-similar set such that ri1;...;ik ¼rik for alls¼i1. . .ikAS. Then K is a loosely self-similar set and
dimHK¼supfsb0:MsðKÞ ¼yg
¼d with Xm
i¼1
rid ¼1:
Proof. The proof is similar to that of Corollary 2.2. r Open question: Let K be a deformed self-similar set. We wonder if the packing dimension [8] of K is equal to
sup sb0: lim
n!y MnsðKÞ ¼y
n o
where MnsðKÞ ¼sup PjFsðXÞjs:FsðXÞVFs0ðXÞ ¼j;s0s0ands;s0A 6
kbn
Sk
( )
.
Acknowledgement. We wish to thank the referee for his helpful comments about the proof of Corollary 2.2 and Corollary 2.3.
References
[ 1 ] I. S. Baek, Dimensions of the perturbed Cantor set, Real Analysis Exchange 19 (1993/
1994), 269–273.
[ 2 ] K. J. Falconer, Fractal geometry-Mathematical foundations and applications, Wiley, 1990.
[ 3 ] K. J. Falconer, Sub-self-similar sets, Trans. Amer. Math. Soc. 347 (1995), 3121–3129.
[ 4 ] J. E. Hutchinson, Fractals and self-similarity, Indiana Univ. Math. J.30(1981), 713–747.
[ 5 ] S. Ikeda, On loosely self-similar sets, Hiroshima Math. J.25 (1995), 527–540.
[ 6 ] S. Ikeda and M. Nakamura, Dimensions of Measures on perturbed Cantor set, preprint.
[ 7 ] C. A. Rogers, Hausdor¤ measures, Cambridge Univ. Press, 1970.
[ 8 ] S. J. Taylor and C. Tricot, The packing measure and its evaluation for a Brownian path, Trans. Amer. Math. Soc. 288 (1985), 679–699.
Tae Hee Kim and Hung Hwan Lee Department of Mathematics Kyungpook National University
Taegu 702-701, Korea
E-mail: T. H. Kim: [email protected] E-mail: H. H. Lee: [email protected]
Sung Pyo Hong Department of Mathematics
Pohang University of Science and Technology Pohang 790-784, Korea
E-mail: [email protected]