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Firstly, the dynamic characteristics of two high\u2010order memristor hyperchaotic systems with uncertain parameters are analyzed. Then, an adaptive multi\u2010switching controller is designed to realize the multi\u2010switching synchronization of the two high\u2010order hyperchaotic systems, and the unknown parameters of the systems are identified to their true values. Furthermore, numerical simulation results testify the effectiveness of the proposed strategy. Finally, the proposed algorithm applied in secure communication of masking encryption and image encryption is validated by statistical analysis.<\/jats:p>","DOI":"10.1155\/2019\/3827201","type":"journal-article","created":{"date-parts":[[2019,12,19]],"date-time":"2019-12-19T23:30:44Z","timestamp":1576798244000},"update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":13,"title":["Adaptive Multi\u2010Switching Synchronization of High\u2010Order Memristor\u2010Based Hyperchaotic System with Unknown Parameters and Its Application in Secure Communication"],"prefix":"10.1155","volume":"2019","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-2533-5187","authenticated-orcid":false,"given":"Zhili","family":"Xiong","sequence":"first","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0002-4874-4186","authenticated-orcid":false,"given":"Shaocheng","family":"Qu","sequence":"additional","affiliation":[]},{"given":"Jing","family":"Luo","sequence":"additional","affiliation":[]}],"member":"311","published-online":{"date-parts":[[2019,12,19]]},"reference":[{"key":"e_1_2_9_1_2","doi-asserted-by":"publisher","DOI":"10.1016\/B978-012396840-1\/50040-0"},{"key":"e_1_2_9_2_2","doi-asserted-by":"publisher","DOI":"10.1063\/1.4794794"},{"key":"e_1_2_9_3_2","doi-asserted-by":"publisher","DOI":"10.1631\/jzus.c1100085"},{"key":"e_1_2_9_4_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.amc.2018.11.017"},{"key":"e_1_2_9_5_2","doi-asserted-by":"publisher","DOI":"10.1142\/s0219477504001653"},{"key":"e_1_2_9_6_2","doi-asserted-by":"publisher","DOI":"10.1177\/1077546317713532"},{"key":"e_1_2_9_7_2","doi-asserted-by":"publisher","DOI":"10.1007\/s11071-016-2747-8"},{"key":"e_1_2_9_8_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.cjph.2018.12.020"},{"key":"e_1_2_9_9_2","doi-asserted-by":"publisher","DOI":"10.1063\/1.1899823"},{"key":"e_1_2_9_10_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.physleta.2013.05.046"},{"key":"e_1_2_9_11_2","doi-asserted-by":"publisher","DOI":"10.1109\/tcad.2018.2834436"},{"key":"e_1_2_9_12_2","doi-asserted-by":"publisher","DOI":"10.1007\/s40435-017-0320-z"},{"key":"e_1_2_9_13_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.physleta.2012.08.021"},{"key":"e_1_2_9_14_2","doi-asserted-by":"publisher","DOI":"10.1007\/s11071-018-4524-3"},{"key":"e_1_2_9_15_2","doi-asserted-by":"publisher","DOI":"10.1103\/physrevlett.76.1232"},{"key":"e_1_2_9_16_2","doi-asserted-by":"publisher","DOI":"10.1007\/s11071-010-9880-6"},{"key":"e_1_2_9_17_2","doi-asserted-by":"publisher","DOI":"10.1103\/physreve.75.067201"},{"key":"e_1_2_9_18_2","doi-asserted-by":"publisher","DOI":"10.1007\/s11071-013-0749-3"},{"key":"e_1_2_9_19_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.chaos.2006.11.041"},{"key":"e_1_2_9_20_2","doi-asserted-by":"publisher","DOI":"10.1007\/s11071-010-9822-3"},{"key":"e_1_2_9_21_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.cjph.2018.03.011"},{"key":"e_1_2_9_22_2","doi-asserted-by":"crossref","unstructured":"WenY. 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