Periodicity invariant of finitely generated algebraic structures

IF 0.4 Q4 MATHEMATICS Journal of Mathematical Extension Pub Date : 2020-09-08 DOI:10.30495/JME.V0I0.1266
Behnam Azizi, H. Doostie
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引用次数: 0

Abstract

In this paper‎, ‎we discuss the periodicity problems in the finitely generated algebraic structures and exhibit their natural‎ ‎sources in the theory of invariants of finite groups and it forms an interesting and relatively self-contained nook in the‎ ‎imposing edifice of group theory‎. ‎One of the deepest and important results of the related theory of finite‎ ‎groups is a complete classification of all periodic groups‎, ‎that is‎, ‎the finite groups with periodic properties‎. ‎If an integer‎ ‎be $k\geq 2$‎, ‎let $S$ will be a finite $k$-generated as well as non-associative algebraic structure $S= $‎, ‎where‎ ‎$A=\lbrace a_{1}‎, ‎a_{2},\dots‎, ‎a_{k}\rbrace$‎, ‎and the sequence‎ ‎$$x_{i}=\left\{‎ ‎\begin{array}{ll}‎ ‎a_{i}‎, ‎& 1\leq i\leq k‎, ‎\\‎ ‎x_{i-k}(x_{i-k+1}(\ldots(x_{i-3}(x_{i-2}x_{i-1}))\ldots))‎, ‎& i>k‎, ‎\end{array}‎ ‎\right‎. ‎$$‎ ‎is called the $k$-nacci sequence of $S$ with respect to the generating set $A$‎, ‎as denoted in $k_{A}(S)$‎. ‎When $k_{A}(S)$ is periodic‎, ‎we will use the length of the period of the periodicity length of $S$ proportional to $A$ in $LEN_{A}(S)$‎ ‎and the minimum of the positive integers of $LEN_A(S)$ will be mentioned as periodicity invariant of $S$‎, ‎denoted in $\lambda_k(S)$‎. ‎However‎, ‎this invariant has‎ ‎been studied for groups and semigroups during the years as well as the associative property of $S$ where above sequence was reduced to‎ ‎$x_i=x_{i-k}x_{i-k+1}\dots x_{i-3}x_{i-2}x_{i-1}$‎, ‎for every $i\geq k+1$‎. ‎Thus‎, ‎we attempt to give explicit upper‎ ‎bounds for the periodicity invariant of two infinite classes of‎ ‎finite non-associative $3$-generated algebraic structures‎. ‎Moreover‎, ‎two classes of non-isomorphic Moufang loops of the same periodicity length were obtained in the study‎.
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有限生成代数结构的周期不变量
在本文中,我们讨论了有限生成代数结构中的周期性问题,并展示了它们在有限群不变量理论中的自然来源,它在群论的宏伟大厦中形成了一个有趣而相对独立的角落。有限群相关理论中最深刻和最重要的结果之一是所有周期群的完全分类,即具有周期性质的有限群。如果是整数,则为 $k\geq 2$_, _让 $S$ 将是有限的 $k$-生成以及非结合代数结构 $S= $在哪里$A=\lbrace a_{1}‎, ‎a_{2},\dots‎, ‎a_{k}\rbrace$,和序列$$x_{i}=\left\{‎ ‎\begin{array}{ll}‎ ‎a_{i}‎, ‎& 1\leq i\leq k‎, ‎\\‎ ‎x_{i-k}(x_{i-k+1}(\ldots(x_{i-3}(x_{i-2}x_{i-1}))\ldots))‎, ‎& i>k‎, ‎\end{array}‎ ‎\right‎. ‎$$“”被称为“” $k$-nacci序列 $S$ 相对于发电机组 $A$,如中所示 $k_{A}(S)$…当 $k_{A}(S)$ 是周期的,我们会用周期的长度表示周期的长度 $S$ 成正比于 $A$ 在 $LEN_{A}(S)$的正整数的最小值 $LEN_A(S)$ 会被称为的周期性不变量吗 $S$以…表示 $\lambda_k(S)$…然而,这个不变量多年来已经被研究用于群和半群,以及的结合性 $S$ 上面的顺序在哪里被简化为“_”$x_i=x_{i-k}x_{i-k+1}\dots x_{i-3}x_{i-2}x_{i-1}$为每一个 $i\geq k+1$…因此,我们试图给出两个无限类有限非结合律的周期不变量的显式上界 $3$生成的代数结构。此外,还得到了两类具有相同周期长度的非同构牟方环。
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审稿时长
24 weeks
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