Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3392
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dc.contributor.authorYadav, Avinash Chanden_US
dc.contributor.authorRamaswamy, Ramakrishnaen_US
dc.contributor.authorDHAR, DEEPAKen_US
dc.date.accessioned2019-07-01T05:39:13Z
dc.date.available2019-07-01T05:39:13Z
dc.date.issued2017-08en_US
dc.identifier.citationPhysical Review E, 96(2), 022215.en_US
dc.identifier.issn1539-3755en_US
dc.identifier.issn1550-2376en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3392-
dc.identifier.urihttps://doi.org/10.1103/PhysRevE.96.022215en_US
dc.description.abstractWe consider the response of a memoryless nonlinear device that acts instantaneously, converting an input signal ξ(t) into an output η(t) at the same time t. For input Gaussian noise with power-spectrum 1/f α, the nonlinearity can modify the spectral index of the output to give a spectrum that varies as 1/f α′ with α′ ≠ α. We show that the value of α′ depends on the nonlinear transformation and can be tuned continuously. This provides a general mechanism for the ubiquitous 1/f noise found in nature.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectGeneral mechanismen_US
dc.subject1/f noiseen_US
dc.subjectMemoryless nonlinear deviceen_US
dc.subjectNonlinear transformationen_US
dc.subjectSpectral indexen_US
dc.subjectStochastic processesen_US
dc.subject2017en_US
dc.titleGeneral mechanism for the 1/f noiseen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Een_US
dc.publication.originofpublisherForeignen_US
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