By Ryu Murakami
Coin Locker infants is Ryu Murakami's cult cyperpunk novel
'A cyber-Bildungsroman of playful breadth and unsure depth' Publishers Weekly
'A interesting peek into the weirdness of latest Japan' Oliver Stone
Two infants are left in a Tokyo station coin locker and live to tell the tale opposed to the percentages, yet their lives are endlessly tainted via this inauspicious start.
As they develop up, they subscribe to the ranks of Toxitown: a district of addicts, freaks and prostitutes. One turns into a bisexual rock famous person and appears for his mom, whereas the opposite one, an athlete, seeks revenge. This savage and lovely tale unfolds in a surrealistic whirl of violence.
Ryu Murakami is the enfant bad of up to date eastern literature. offered the distinguished Akutagawa Prize in 1976 for his first ebook, a singular a few crew of children drowned in intercourse and medicine, he has long gone directly to discover with cinematic depth the subjects of violence and expertise in modern eastern society. His novels contain Coin Locker infants, Sixty-Nine, renowned Hits of the Showa period, Audition, within the Miso Soup and From the place of origin, with Love.
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Example text
Let us define a NXM-dimensional column vector o~( t) = (Oli l (t ) I , o~2 (t )I , ••• , o~M (t )I o~(t) as (18) ) I and a (NXM)x(NxM) matrix P as L Pl J' -P12 -P2l . = P .. , the matrix Q=P-I is symmetric and hence its eigenvalues a~e aiI real. The solution lir,li~"",li~ is stable if and only if the eigenvalues are all negative. A sufficient condition for asymptotic stability is that p(x) is * * ... ,wM' *) zero for all ~ on every boundary Bij= Bij (* lil'~2, In fact, from the definition (17), P ij = 0 for all i and for all j#i, and hence all the eigenvalues are equal to -1.
J' r----~ . ' ,{ , , • " ~.. u . -=-C_ _ _ . . 'j ,; ; - ~ '" ,~ . ' • . ~ ,'# ',~ " • y '<' w": • • 'i • • 'f' Four-Cluster Pattern Distribution Used in the Simulation Experiment s . ~~----~~' " I; ,; (a) .... , ...... w, w, /' I' I I; A NUMERICAL EXAMPLE AND A RECOGNITION EXPERIMENT Several other aspects must be investigated before the nonlinear algorithm derived in Section III can be applied to numerical calculations or physical experiments. For example, one must have the means of computing the error covariance K at each stage of the n learning process. In addition, a proper selection of the threshold e is also important for a desirable learning performance. The interested reader is referred to [3J for further discussions on 24 CHIEN these subjects.