{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2022,4,4]],"date-time":"2022-04-04T22:32:27Z","timestamp":1649111547457},"reference-count":9,"publisher":"World Scientific Pub Co Pte Lt","issue":"01","content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Int. J. Neur. Syst."],"published-print":{"date-parts":[[2001,2]]},"abstract":"<jats:p> Many real-world systems such as irregular ECG signal, volatility of currency exchange rate and heated fluid reaction exhibit higly complex nonlinear characteristic known as chaos. These chaotic systems cannot be retreated satisfactorily using linear system theory due to its high dimensionality and irregularity. This research focuses on prediction and modelling of chaotic FIR (Far InfraRed) laser system for which the underlying equations are not given. This paper proposed a method for prediction and modelling a chaotic FIR laser time series using rational function neural network. Three network architectures, TDNN (Time Delayed Neural Network), RBF (radial basis function) network and the RF (rational function) network, are also presented. Comparisons between these networks performance show the improvements introduced by the RF network in terms of a decrement in network complexity and better ability of predictability. <\/jats:p>","DOI":"10.1142\/s0129065701000527","type":"journal-article","created":{"date-parts":[[2003,4,22]],"date-time":"2003-04-22T07:45:54Z","timestamp":1050997554000},"page":"89-99","source":"Crossref","is-referenced-by-count":1,"title":["MODELLING AND PREDICTION FOR CHAOTIC FIR LASER ATTRACTOR USING RATIONAL FUNCTION NEURAL NETWORK"],"prefix":"10.1142","volume":"11","author":[{"given":"Seongyun","family":"Cho","sequence":"first","affiliation":[{"name":"Intelligent Systems Laboratory, School of Engineering, Cardiff University, PO Box 688 Cardiff CF24 3TE, UK"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"219","published-online":{"date-parts":[[2011,11,21]]},"reference":[{"key":"p_1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.55.2571"},{"key":"p_2","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.57.2804"},{"key":"p_3","doi-asserted-by":"publisher","DOI":"10.1016\/0375-9601(86)90210-0"},{"key":"p_4","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.38.3017"},{"key":"p_6","first-page":"104","volume":"7","author":"Hbner U.","year":"1994","journal-title":"Gershenfeld N."},{"key":"p_15","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.65.1331"},{"key":"p_16","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevA.45.3403"},{"key":"p_17","doi-asserted-by":"publisher","DOI":"10.1145\/355744.355745"},{"key":"p_18","doi-asserted-by":"publisher","DOI":"10.1007\/BF01759061"}],"container-title":["International Journal of Neural Systems"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/www.worldscientific.com\/doi\/pdf\/10.1142\/S0129065701000527","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2019,8,7]],"date-time":"2019-08-07T12:31:52Z","timestamp":1565181112000},"score":1,"resource":{"primary":{"URL":"https:\/\/www.worldscientific.com\/doi\/abs\/10.1142\/S0129065701000527"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2001,2]]},"references-count":9,"journal-issue":{"issue":"01","published-online":{"date-parts":[[2011,11,21]]},"published-print":{"date-parts":[[2001,2]]}},"alternative-id":["10.1142\/S0129065701000527"],"URL":"https:\/\/doi.org\/10.1142\/s0129065701000527","relation":{},"ISSN":["0129-0657","1793-6462"],"issn-type":[{"value":"0129-0657","type":"print"},{"value":"1793-6462","type":"electronic"}],"subject":[],"published":{"date-parts":[[2001,2]]}}}