Chaos and Statistical Methods: Proceedings of the Sixth by K. Tomita (auth.), Professor Dr. Yoshiki Kuramoto (eds.)

By K. Tomita (auth.), Professor Dr. Yoshiki Kuramoto (eds.)

Show description

Read Online or Download Chaos and Statistical Methods: Proceedings of the Sixth Kyoto Summer Institute, Kyoto, Japan September 12–15, 1983 PDF

Similar japan books

Hiroshima: The Autobiography of Barefoot Gen (Asian Voices)

This compelling autobiography tells the existence tale of famed manga artist Nakazawa Keiji. Born in Hiroshima in 1939, Nakazawa was once six years previous while on August 6, 1945, the USA dropped the atomic bomb. His gritty and wonderful account of the bad aftermath is powerfully informed in the course of the eyes of a kid who misplaced so much of his kinfolk and acquaintances.

The Broken Bridge: Fiction from Expatriates in Literary Japan

An insightful anthology of 36 brief tales written through non-Japanese who've known as Japan their domestic. "Judging from the robust writing during this quantity . . . the combo of eastern reserve and the distant fantastic thing about the country's artwork and panorama has intensified those writers' powers of observation," says Publishers Weekly.

The Scars of War: Tokyo during World War II: Writings of Takeyama Michio

Takeyama Michio, the writer of Harp of Burma, used to be thirty-seven in 1941, the 12 months of the japanese assault on Pearl Harbor. Husband, father of youngsters born in the course of the struggle, and instructor at Japan's elite tuition of upper schooling in Tokyo, he skilled the conflict on its domestic entrance. His essays offer us with a private list of the bombing of Tokyo, the lack of foodstuff, the lack to get actual information regarding the battle, the frictions among civilians and army and among his elite scholars and different civilians, the mobilization of scholars into manufacturing unit jobs and the army, and the relocation of civilians out of the Tokyo quarter.

The Making of China’s War with Japan: Zhou Enlai and Zhang Xueliang

This innovative examine examines the profession of chinese language baby-kisser and diplomat Zhou Enlai (1898–1976) and assesses his management function within the Communist social gathering of China’s (CPC) process opposed to the japanese invasion of China which tested the root for post-World battle II Sino-Japanese family members.

Additional info for Chaos and Statistical Methods: Proceedings of the Sixth Kyoto Summer Institute, Kyoto, Japan September 12–15, 1983

Sample text

Recently, KOHMOTO et al. (2) and OSTLUND et al. (3) showed that the transfer matrices of a special almost periodic Schrodinger equation obey the following recursion relation: (1) where M~ is a 2 x 2 real matrix with unit determinant. The purpose of this article is to review the derivation of this dynamical system and also to give a more general class of the equations than reported previously. 2. ,V(t+l) 52 z V(t), and w is an irrational number. It is traditional to introduce a transfer matrix in one-dimensional problems: ~n+l where ~n = M(nw}~n' = [ Wn ] and (3) M is the transfer matrix given by M(t} Wn-l The matrix satisfies M(t+l} matrices are also defined, = M(t} and detM(t} 1.

It is clear that as A-I, D - 2, hence ~ -1, and that chaos is approached without bifurcation. The facts are perhaps easier to visualize in terms of the parameter Po = 1/A and the variable u = 1/z. This change of variable does not change IF*. For I Pol <1, there is one limit point at u = O. As Po crosses 1, this limit point bifurcates into two limit points that coexist in a chaotic situation. 7. Third Path Beyond the Great Wave. The Siegel Scenario Figure 5 represents the IF* set for a value of A within the atom I A-I /2 I < 1/2, but very close to a point on boundary, namely AS = 1/2+(1/2) exp(2'ITiy), where y is the irrational number «1) whose continued fraction expansion is (4,1,1,1, ...

In both the Henon map and the rotor map (R) there is seen a special saddle periodic orbit whose collision with the chaotic attractor, as the parameter on the nonlinear term is increased, marks the destruction of the attractor. The stable manifold of this orbit delineates the boundary of the chaotic 27 Fig. 6 The attractor of map (R) very near destruction. A=1/2. 1986n. The two-piece chaotic attractor is shown relative to the unstable orbit of period' six (arrows). As the map is iterated the point cycles Pl+P2 ...

Download PDF sample

Rated 4.02 of 5 – based on 32 votes