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http://eprints.org/relation/isVersionOf https://pure.iiasa.ac.at/id/document/51357 http://eprints.org/relation/isVolatileVersionOf https://pure.iiasa.ac.at/id/document/51357 http://eprints.org/relation/issmallThumbnailVersionOf https://pure.iiasa.ac.at/id/document/51357 51362 1 138779 document 51362 indexcodes.txt text/x-c++ f4677809a1ed0e4cd01d3a754f17d922 MD5 4624 2016-04-25 07:45:31 https://pure.iiasa.ac.at/id/eprint/12838/6/indexcodes.txt 12838 6 6 text/x-c++ other Generate index codes conversion from text to indexcodes en public

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http://eprints.org/relation/isVersionOf https://pure.iiasa.ac.at/id/document/51357 http://eprints.org/relation/isVolatileVersionOf https://pure.iiasa.ac.at/id/document/51357 http://eprints.org/relation/isIndexCodesVersionOf https://pure.iiasa.ac.at/id/document/51357 archive 5 disk0/00/01/28/38 2016-04-21 07:21:33 2021-08-27 17:40:45 2016-04-21 07:21:33 article show Binder P.-M. AL1650 pub prog_sds Cellular automata (CA) dynamics are ordered in terms of two global parameters, computable a priori from the description of rules. While one of them (activity) has been used before, the second one is new; it estimates the average sensitivity of rules to small configurational changes. For two-well-known families of rules, the Wolfram complexity classes cluster satisfactorily. The observed simultaneous occurrence of sharp and smooth transitions from ordered to disordered dynamics in CA can be explained with the two-parameter diagram. 1994 published American Physical Society 10.1103/PhysRevE.49.2023 2683 public Physical Review E 49 3 2023-2025 TRUE 1063-651X FALSE info:eu-repo/semantics/article