By Jon Aaronson, Toshihiro Hamachi, Klaus Schmidt (auth.), Y. Takahashi (eds.)

In 1992 successive symposia have been held in Japan on algorithms, fractals and dynamical structures. the 1st one was once Hayashibara discussion board '92: foreign Symposium on New Bases for Engineering technological know-how, Algorithms, Dynamics and Fractals held at Fujisaki Institute of Hayashibara Biochemical Laboratories, Inc. in Okayama in the course of November 23-28 within which forty nine mathematicians together with 19 from overseas participated. They contain either natural and utilized mathematicians of different backgrounds and represented eleven coun attempts. The organizing committee consisted of the next household contributors and Mike KEANE from Delft: Masayosi HATA, Shunji ITO, Yuji ITO, Teturo KAMAE (chairman), Hitoshi NAKADA, Satoshi TAKAHASHI, Yoichiro TAKAHASHI, Masaya YAMAGUTI the second was once held on the examine Institute for Mathematical technological know-how at Kyoto collage from November 30 to December 2 with emphasis on natural mathematical aspect during which greater than eighty mathematicians participated. This quantity is a partial list of the stimulating alternate of rules and discussions which came about in those symposia.

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7, 1962, 299-301. 5. Schrnidt, Normalitiit beziiglich matrizen, J. fUr die Riene u. Angewandte Math. 2314/5, 1964, 227-260. A Montreal (Quebec) Canada H 3C 3A 7 Abstract. Bya stretch of imagination we shall identify spirals with systems of interacting particles. Mimicking the formalism of Statistical Mechanics we shall then discover that spirals go through a phase transition as the "temperature" increases. The inverse critical temperature coincides with the box dimension of the spiral. The article is a restatement of previous joint work [1].

2. It is enough to consider the case IIhll2 = 1. Take two real numbers K, L satisfying 0 < K < 1 < L. From Tchebycheff inequality we have On the other hand, from Cauchy-Schwartz inequality 1= { J{lhl>K} h2 + { i{lhl:5K} h2:s; (fh 4 )1/2(f-L{lhl > K})1/2 + K2; whence f-L{lhl> K} ~ (1- K2)2/C 4 • Now to have the conclusion of the lemma it is enough to choose c: > 0, put M = I/C4 - 2c:, then find K small enough to have (I-K2)2/C 4 > M+c: and finally select L sufficiently big to have (C 4 _I)(L2_I)-2 < c:.

P). 2. p. with Gp(D(cp)) = JR. This is an obvious modification of the previous construction. 2 E JR, with the sequences inn, i = 1,2. p). The group generated by dense in JR and the advertised condition is attained. 2 are ergodic, coalescent, and nonsquashable. §5 Ergodicity of smooth cylinder flows. Generic point of view Suppose that f: 1[' -+ JR is smooth. We shall prove that under certain assumptions, the set of those irrational translations for which the corresponding cylinder flow is ergodic is residual.