Madhur Mangalam, Aaron D Likens, Damian G Kelty-Stephen
{"title":"多分形非线性作为乘法级联动态的稳健估算器","authors":"Madhur Mangalam, Aaron D Likens, Damian G Kelty-Stephen","doi":"arxiv-2312.05653","DOIUrl":null,"url":null,"abstract":"Multifractal formalisms provide an apt framework to study random cascades in\nwhich multifractal spectrum width $\\Delta\\alpha$ fluctuates depending on the\nnumber of estimable power-law relationships. Then again, multifractality\nwithout surrogate comparison can be ambiguous: the original measurement series'\nmultifractal spectrum width $\\Delta\\alpha_\\mathrm{Orig}$ can be sensitive to\nthe series length, ergodicity-breaking linear temporal correlations (e.g.,\nfractional Gaussian noise, $fGn$), or additive cascade dynamics. To test these\nthreats, we built a suite of random cascades that differ by the length, type of\nnoise (i.e., additive white Gaussian noise, $awGn$, or $fGn$), and mixtures of\n$awGn$ or $fGn$ across generations (progressively more $awGn$, progressively\nmore $fGn$, and a random sampling by generation), and operations applying noise\n(i.e., addition vs. multiplication). The so-called ``multifractal\nnonlinearity'' $t_\\mathrm{MF}$ (i.e., a $t$-statistic comparing\n$\\Delta\\alpha_\\mathrm{Orig}$ and multifractal spectra width for\nphase-randomized linear surrogates $\\Delta\\alpha_\\mathrm{Surr}$) is a robust\nindicator of random multiplicative rather than random additive cascade\nprocesses irrespective of the series length or type of noise. $t_\\mathrm{MF}$\nis more sensitive to the number of generations than the series length.\nFurthermore, the random additive cascades exhibited much stronger ergodicity\nbreaking than all multiplicative analogs. Instead, ergodicity breaking in\nrandom multiplicative cascades more closely followed the ergodicity-breaking of\nthe constituent noise types -- breaking ergodicity much less when arising from\nergodic $awGn$ and more so for noise incorporating relatively more correlated\n$fGn$. Hence, $t_\\mathrm{MF}$ is a robust multifractal indicator of\nmultiplicative cascade processes and not spuriously sensitive to ergodicity\nbreaking.","PeriodicalId":501305,"journal":{"name":"arXiv - PHYS - Adaptation and Self-Organizing Systems","volume":"1 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-12-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Multifractal nonlinearity as a robust estimator of multiplicative cascade dynamics\",\"authors\":\"Madhur Mangalam, Aaron D Likens, Damian G Kelty-Stephen\",\"doi\":\"arxiv-2312.05653\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Multifractal formalisms provide an apt framework to study random cascades in\\nwhich multifractal spectrum width $\\\\Delta\\\\alpha$ fluctuates depending on the\\nnumber of estimable power-law relationships. Then again, multifractality\\nwithout surrogate comparison can be ambiguous: the original measurement series'\\nmultifractal spectrum width $\\\\Delta\\\\alpha_\\\\mathrm{Orig}$ can be sensitive to\\nthe series length, ergodicity-breaking linear temporal correlations (e.g.,\\nfractional Gaussian noise, $fGn$), or additive cascade dynamics. To test these\\nthreats, we built a suite of random cascades that differ by the length, type of\\nnoise (i.e., additive white Gaussian noise, $awGn$, or $fGn$), and mixtures of\\n$awGn$ or $fGn$ across generations (progressively more $awGn$, progressively\\nmore $fGn$, and a random sampling by generation), and operations applying noise\\n(i.e., addition vs. multiplication). The so-called ``multifractal\\nnonlinearity'' $t_\\\\mathrm{MF}$ (i.e., a $t$-statistic comparing\\n$\\\\Delta\\\\alpha_\\\\mathrm{Orig}$ and multifractal spectra width for\\nphase-randomized linear surrogates $\\\\Delta\\\\alpha_\\\\mathrm{Surr}$) is a robust\\nindicator of random multiplicative rather than random additive cascade\\nprocesses irrespective of the series length or type of noise. $t_\\\\mathrm{MF}$\\nis more sensitive to the number of generations than the series length.\\nFurthermore, the random additive cascades exhibited much stronger ergodicity\\nbreaking than all multiplicative analogs. Instead, ergodicity breaking in\\nrandom multiplicative cascades more closely followed the ergodicity-breaking of\\nthe constituent noise types -- breaking ergodicity much less when arising from\\nergodic $awGn$ and more so for noise incorporating relatively more correlated\\n$fGn$. Hence, $t_\\\\mathrm{MF}$ is a robust multifractal indicator of\\nmultiplicative cascade processes and not spuriously sensitive to ergodicity\\nbreaking.\",\"PeriodicalId\":501305,\"journal\":{\"name\":\"arXiv - PHYS - Adaptation and Self-Organizing Systems\",\"volume\":\"1 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-12-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Adaptation and Self-Organizing Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2312.05653\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Adaptation and Self-Organizing Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2312.05653","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Multifractal nonlinearity as a robust estimator of multiplicative cascade dynamics
Multifractal formalisms provide an apt framework to study random cascades in
which multifractal spectrum width $\Delta\alpha$ fluctuates depending on the
number of estimable power-law relationships. Then again, multifractality
without surrogate comparison can be ambiguous: the original measurement series'
multifractal spectrum width $\Delta\alpha_\mathrm{Orig}$ can be sensitive to
the series length, ergodicity-breaking linear temporal correlations (e.g.,
fractional Gaussian noise, $fGn$), or additive cascade dynamics. To test these
threats, we built a suite of random cascades that differ by the length, type of
noise (i.e., additive white Gaussian noise, $awGn$, or $fGn$), and mixtures of
$awGn$ or $fGn$ across generations (progressively more $awGn$, progressively
more $fGn$, and a random sampling by generation), and operations applying noise
(i.e., addition vs. multiplication). The so-called ``multifractal
nonlinearity'' $t_\mathrm{MF}$ (i.e., a $t$-statistic comparing
$\Delta\alpha_\mathrm{Orig}$ and multifractal spectra width for
phase-randomized linear surrogates $\Delta\alpha_\mathrm{Surr}$) is a robust
indicator of random multiplicative rather than random additive cascade
processes irrespective of the series length or type of noise. $t_\mathrm{MF}$
is more sensitive to the number of generations than the series length.
Furthermore, the random additive cascades exhibited much stronger ergodicity
breaking than all multiplicative analogs. Instead, ergodicity breaking in
random multiplicative cascades more closely followed the ergodicity-breaking of
the constituent noise types -- breaking ergodicity much less when arising from
ergodic $awGn$ and more so for noise incorporating relatively more correlated
$fGn$. Hence, $t_\mathrm{MF}$ is a robust multifractal indicator of
multiplicative cascade processes and not spuriously sensitive to ergodicity
breaking.