{"title":"分析复杂性与信号编码","authors":"V.K. Beloshapka","doi":"10.1134/S106192084010035","DOIUrl":null,"url":null,"abstract":"<p> There are two ways to describe a geometric object <span>\\(L\\)</span>: the object as an image of a mapping and the object as a preimage. Every method has its own advantages and shortcomings; together, they give a complete picture. In order to compare these descriptions by complexity, one can use Kolmogorov’s approach: i.e., after the clarification of the system of basic operations, the complexity of a description is the minimum length of the defining text. Accordingly, we obtain two Kolmogorov complexities: in the first case, <span>\\(K^{+}(L)\\)</span>, and in the other, <span>\\(K^{-}(L)\\)</span>. Let <span>\\(Cl^n\\)</span> be the class of functions of two variables that can be represented by analytic functions of one variable and by the addition of the depth not exceeding <span>\\(n\\)</span>, and let <span>\\(K^{+}(Cl^n)\\)</span> and <span>\\(K^{-}(Cl^n)\\)</span> be their corresponding Kolmogorov complexities. There are arguments in favor of the fact that, for <span>\\(n \\geq 2\\)</span>, the value of <span>\\(K^{-}(Cl^n)\\)</span> is very large, and the task of constructing a description of <span>\\(Cl^n\\)</span> in the form of a preimage (by defining relations) even for <span>\\(n=2\\)</span> is computationally unrealizable. Based on this observation, a signal encoding-decoding scheme is proposed, and arguments are given in favor of the fact that the decoding of a signal encoded using such a scheme is inaccessible to a quantum computer. </p><p> <b> DOI</b> 10.1134/S106192084010035 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"44 - 49"},"PeriodicalIF":1.7000,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Analytical Complexity and Signal Coding\",\"authors\":\"V.K. Beloshapka\",\"doi\":\"10.1134/S106192084010035\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p> There are two ways to describe a geometric object <span>\\\\(L\\\\)</span>: the object as an image of a mapping and the object as a preimage. Every method has its own advantages and shortcomings; together, they give a complete picture. In order to compare these descriptions by complexity, one can use Kolmogorov’s approach: i.e., after the clarification of the system of basic operations, the complexity of a description is the minimum length of the defining text. Accordingly, we obtain two Kolmogorov complexities: in the first case, <span>\\\\(K^{+}(L)\\\\)</span>, and in the other, <span>\\\\(K^{-}(L)\\\\)</span>. Let <span>\\\\(Cl^n\\\\)</span> be the class of functions of two variables that can be represented by analytic functions of one variable and by the addition of the depth not exceeding <span>\\\\(n\\\\)</span>, and let <span>\\\\(K^{+}(Cl^n)\\\\)</span> and <span>\\\\(K^{-}(Cl^n)\\\\)</span> be their corresponding Kolmogorov complexities. There are arguments in favor of the fact that, for <span>\\\\(n \\\\geq 2\\\\)</span>, the value of <span>\\\\(K^{-}(Cl^n)\\\\)</span> is very large, and the task of constructing a description of <span>\\\\(Cl^n\\\\)</span> in the form of a preimage (by defining relations) even for <span>\\\\(n=2\\\\)</span> is computationally unrealizable. Based on this observation, a signal encoding-decoding scheme is proposed, and arguments are given in favor of the fact that the decoding of a signal encoded using such a scheme is inaccessible to a quantum computer. </p><p> <b> DOI</b> 10.1134/S106192084010035 </p>\",\"PeriodicalId\":763,\"journal\":{\"name\":\"Russian Journal of Mathematical Physics\",\"volume\":\"31 1\",\"pages\":\"44 - 49\"},\"PeriodicalIF\":1.7000,\"publicationDate\":\"2024-03-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Russian Journal of Mathematical Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S106192084010035\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, MATHEMATICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Russian Journal of Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S106192084010035","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
There are two ways to describe a geometric object \(L\): the object as an image of a mapping and the object as a preimage. Every method has its own advantages and shortcomings; together, they give a complete picture. In order to compare these descriptions by complexity, one can use Kolmogorov’s approach: i.e., after the clarification of the system of basic operations, the complexity of a description is the minimum length of the defining text. Accordingly, we obtain two Kolmogorov complexities: in the first case, \(K^{+}(L)\), and in the other, \(K^{-}(L)\). Let \(Cl^n\) be the class of functions of two variables that can be represented by analytic functions of one variable and by the addition of the depth not exceeding \(n\), and let \(K^{+}(Cl^n)\) and \(K^{-}(Cl^n)\) be their corresponding Kolmogorov complexities. There are arguments in favor of the fact that, for \(n \geq 2\), the value of \(K^{-}(Cl^n)\) is very large, and the task of constructing a description of \(Cl^n\) in the form of a preimage (by defining relations) even for \(n=2\) is computationally unrealizable. Based on this observation, a signal encoding-decoding scheme is proposed, and arguments are given in favor of the fact that the decoding of a signal encoded using such a scheme is inaccessible to a quantum computer.
期刊介绍:
Russian Journal of Mathematical Physics is a peer-reviewed periodical that deals with the full range of topics subsumed by that discipline, which lies at the foundation of much of contemporary science. Thus, in addition to mathematical physics per se, the journal coverage includes, but is not limited to, functional analysis, linear and nonlinear partial differential equations, algebras, quantization, quantum field theory, modern differential and algebraic geometry and topology, representations of Lie groups, calculus of variations, asymptotic methods, random process theory, dynamical systems, and control theory.