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Lipschitz continuous points of functions on an interval 区间上函数的Lipschitz连续点
Pub Date : 2025-07-13 DOI: 10.1016/j.exco.2025.100194
Zhekai Shen
In this paper, we address the problem of finding functions with predetermined Lipschitz continuous points. More precisely, given A[0,1], we are interested in the existence of function f:[0,1]R which is Lipschitz continuous exactly on A. Our result is related to Liouville numbers.
在本文中,我们讨论了寻找具有预定的Lipschitz连续点的函数的问题。更确切地说,给定A的[0,1],我们关注函数f:[0,1]→R在A上恰好是Lipschitz连续的存在性。我们的结果与Liouville数有关。
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引用次数: 0
Cauchy’s stress theorem and its influence on the first elasticity tensor 柯西应力定理及其对第一弹性张量的影响
Pub Date : 2025-07-11 DOI: 10.1016/j.exco.2025.100190
Stefan Buchen
The well-known Clausius–Planck inequality for solids is derived from the second law of thermodynamics and provides the important relation between stress and strain tensors according to the Coleman–Noll procedure. For the detailed derivation of this inequality, mass continuity equation, the equation of motion and the first law of thermodynamics in local form are required. The transfer of integral to local formulation can be calculated using Cauchy’s stress theorem and the divergence theorem. In the literature, however, there are two definitions for both, the Cauchy’s stress theorem and the divergence theorem for second-order tensors. The aim of this article is to show the resulting differences in the first principles for polar solids up to the first elasticity tensor for hyperelastic materials.
众所周知的固体克劳修斯-普朗克不等式是由热力学第二定律推导出来的,并根据Coleman-Noll过程提供了应力张量和应变张量之间的重要关系。为了详细推导该不等式,需要质量连续性方程、运动方程和局部形式的热力学第一定律。利用柯西应力定理和散度定理可以计算积分到局部公式的转换。然而,在文献中,这两者都有两种定义,柯西应力定理和二阶张量的散度定理。本文的目的是显示极性固体的第一原理到超弹性材料的第一弹性张量的差异。
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引用次数: 0
The third axiom of filling properties 填充性质的第三个公理
Pub Date : 2025-06-30 DOI: 10.1016/j.exco.2025.100192
Ridwan Pandiya
Since its first appearance in 1983, the filled function method, which was initiated to solve global optimization problems, has developed very rapidly. From the results conducted by many scholars, the ideal filled function has at least two properties: parameter-free and continuously differentiable. Several researchers have attempted to provide filled functions with such properties that meet the three axioms (filling properties) required by the filled function definition. The third axiom specifically states that the filled function has a minimum point in the region of attraction. This paper examines the fact that the currently available continuously differentiable parameter-free filled functions do not fulfil the third axiom of the filling properties by providing several counterexamples.
自1983年首次出现以来,填充函数法作为解决全局优化问题的一种方法得到了迅速的发展。从许多学者的研究结果来看,理想填充函数至少具有无参数和连续可微两个性质。一些研究者试图提供具有满足填充函数定义所要求的三个公理(填充属性)的性质的填充函数。第三个公理明确指出,填充函数在引力区域有一个最小点。本文通过几个反例,证明了现有的无参数连续可微填充函数不满足填充性质的第三公理。
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引用次数: 0
A family of polynomials that defy general convergence in three methods 用三种方法都不能普遍收敛的多项式族
Pub Date : 2025-06-14 DOI: 10.1016/j.exco.2025.100191
Jared Collins , Grant Hunter
We consider the root-finding algorithms of Newton’s method, Halley’s method and Schröder’s method. These methods are known to have polynomials for which the method produces extraneous attracting cycles, i.e. the method is not generally convergent for these polynomials. We produce a family of polynomials that have an extraneous attracting cycle in all three methods. By doing so we show that mixing methods is not beneficial to overcoming the issues of general convergence. We also address a more specific result for the degree three case.
我们考虑了牛顿法、哈雷法和Schröder法的寻根算法。已知这些方法具有多项式,该方法对其产生多余的吸引循环,即该方法对这些多项式通常不收敛。在所有三种方法中,我们都得到了一个具有外部吸引循环的多项式族。通过这样做,我们表明混合方法不利于克服一般收敛问题。我们还处理了一个更具体的结果为度三的情况。
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引用次数: 0
Jensen-type generalized quadratic fractional integral inequalities jensen型广义二次分数积分不等式
Pub Date : 2025-06-01 DOI: 10.1016/j.exco.2025.100189
McSylvester Ejighikeme Omaba
This work introduces a generalized quadratic (double) fractional integral operator and derives a two-dimensional extension of Jensen’s inequality for functions integrable on rectangular domains in R2. To illustrate and validate our findings, some examples are provided. Many established results in the literature are derived as special cases of our results.
本文引入了广义二次(二重)分数阶积分算子,推导了R2中矩形域上可积函数的Jensen不等式的二维推广。为了说明和验证我们的发现,提供了一些例子。文献中许多已确定的结果都是作为我们结果的特殊情况推导出来的。
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引用次数: 0
Meta-analytic functions with derivative not in a Hardy space 非Hardy空间中导数的元解析函数
Pub Date : 2025-05-14 DOI: 10.1016/j.exco.2025.100187
William L. Blair
We show there exist solutions to higher-order Vekua equations that, along with their z̄-derivatives, have finite Hardy space norm, but their z-derivatives do not.
我们证明了高阶Vekua方程的解及其z导数具有有限Hardy空间范数,但它们的z导数没有。
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引用次数: 0
An upper bound for the largest singular value of extended mixed graphs 扩展混合图的最大奇异值的上界
Pub Date : 2025-05-14 DOI: 10.1016/j.exco.2025.100188
Zoran Stanić
An extended mixed graph contains edges declared to be either positive, or negative, or oriented from one end to the other. They unify concepts of mixed graphs, signed graphs, oriented graphs and ordinary graphs. We demonstrate a method that establishes an upper bound for the largest singular value of the corresponding adjacency matrix in a bit general setting allowing the existence of loops at vertices. An upper bound for the largest singular value of the Laplacian matrix is extracted. The obtained bounds remain valid for the largest modulus of the corresponding eigenvalues, and cover the aforementioned particular structures.
扩展混合图包含声明为正或负的边,或从一端指向另一端的边。它们统一了混合图、符号图、有向图和普通图的概念。我们证明了一种方法,建立了一个上限的最大奇异值的相应邻接矩阵在比特一般设置允许在顶点上的循环存在。给出了拉普拉斯矩阵最大奇异值的上界。所得的边界对于相应特征值的最大模量仍然有效,并且覆盖了上述特定结构。
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引用次数: 0
G-Tseng’s extragradient method for approximating G-variational inequality problem in Hilbert space endowed with graph 在具有图的Hilbert空间中,G-Tseng近似g变分不等式问题的提取方法
Pub Date : 2025-04-28 DOI: 10.1016/j.exco.2025.100185
Monika Swami , M.R. Jadeja
In this article, we introduce the G-Tseng’s extragradient method, inspired by the extragradient method defined by Korpelevich, for solving G-variational inequality problems in Hilbert space. We also address a fixed point problem in a Hilbert space endowed with a graph using the proposed G-Tseng’s extragradient method. In the context of Hilbert space, we establish weak and strong convergence theorems for the algorithm. Additionally, we provide numerical examples to support our findings.
在本文中,我们从Korpelevich定义的extragradent方法中得到启发,引入了求解Hilbert空间中g -变分不等式问题的G-Tseng的extragradent方法。我们还利用所提出的G-Tseng的外聚方法解决了具有图的Hilbert空间中的不动点问题。在Hilbert空间中,我们建立了算法的弱收敛定理和强收敛定理。此外,我们提供了数值例子来支持我们的发现。
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引用次数: 0
A family of asymptotically bad wild towers of function fields 函数域的渐近野塔族
Pub Date : 2025-04-25 DOI: 10.1016/j.exco.2025.100186
M. Chara , R. Toledano
In Chara and Toledano (2015) general conditions were given to prove the infiniteness of the genus of certain towers of function fields over a perfect field. It was shown that many examples where particular cases of those general results. In this paper the genus of a family of wild towers of function fields will be considered together with a result with less restrictive sufficient conditions for a wild tower to have infinite genus.
在Chara和Toledano(2015)中,给出了证明函数场的某些塔在一个完美场上的属的无穷性的一般条件。它表明,许多例子,其中的特殊情况,这些一般结果。本文考虑了函数域上野塔族的格,并给出了野塔具有无限格的不太严格的充分条件。
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引用次数: 0
Distance equienergetic graphs of diameter 4 直径为4的距离等能图
Pub Date : 2025-03-28 DOI: 10.1016/j.exco.2025.100184
B.J. Manjunatha , B.R. Rakshith , R.G. Veeresha
Let Γ1, Γ2 and Γ3 be graphs with pairwise disjoint vertex sets. The graph Θ(Γ1,Γ2,Γ3) is obtained from the graphs Γ1Γ3 (the corona product) and Γ2 by joining each vertices of Γ1 in Γ1Γ3 with every vertices in Γ2. Two connected graphs are called distance equienergetic graphs if their distance energies are the same. Several methods for constructing distance equienergetic graphs have been presented in the literature, most constructed distance equienergetic graphs have diameters of 2 or 3. So the problem of constructing distance equienergetic graphs of diameter greater than 3 would be interesting. Another interesting problem posed by Indulal (2020) is to construct a pair of graphs which are both adjacency equienergetic and distance equienergetic. Motivated by these two problems, in this paper, we obtain the distance spectrum of Θ(Γ1,Γ2,Γ3) when all these graphs are regular. As an application, we give a method to obtain distance equienergetic graphs of diameter 4. Also we construct a pair of graphs on 2n+1 vertices (n6) which are both adjacency equienergetic and distance equienergetic graphs.
设Γ1, Γ2, Γ3为顶点集不相交的图。图Θ(Γ1,Γ2Γ3)从图形获得Γ1∘Γ3(电晕产品)和Γ2通过加入Γ1中每个顶点Γ1∘Γ3Γ2中每个顶点。如果两个连通图的距离能相同,则称为距离等能图。文献中提出了几种构造距离等能图的方法,大多数构造的距离等能图的直径为2或3。所以构造直径大于3的距离等能图的问题会很有趣。Indulal(2020)提出的另一个有趣的问题是构造一对同时具有邻接等能和距离等能的图。在这两个问题的推动下,本文得到了Θ(Γ1,Γ2,Γ3)图均为正则时的距离谱。作为应用,给出了一种获取直径为4的距离等能图的方法。并在2n+1个顶点(n≥6)上构造了一对图,它们都是邻接等能图和距离等能图。
{"title":"Distance equienergetic graphs of diameter 4","authors":"B.J. Manjunatha ,&nbsp;B.R. Rakshith ,&nbsp;R.G. Veeresha","doi":"10.1016/j.exco.2025.100184","DOIUrl":"10.1016/j.exco.2025.100184","url":null,"abstract":"<div><div>Let <span><math><msub><mrow><mi>Γ</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>, <span><math><msub><mrow><mi>Γ</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> and <span><math><msub><mrow><mi>Γ</mi></mrow><mrow><mn>3</mn></mrow></msub></math></span> be graphs with pairwise disjoint vertex sets. The graph <span><math><mrow><mi>Θ</mi><mrow><mo>(</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>,</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>)</mo></mrow></mrow></math></span> is obtained from the graphs <span><math><mrow><msub><mrow><mi>Γ</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>∘</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math></span> (the corona product) and <span><math><msub><mrow><mi>Γ</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> by joining each vertices of <span><math><msub><mrow><mi>Γ</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> in <span><math><mrow><msub><mrow><mi>Γ</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>∘</mo><mspace></mspace><msub><mrow><mi>Γ</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math></span> with every vertices in <span><math><msub><mrow><mi>Γ</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>. Two connected graphs are called distance equienergetic graphs if their distance energies are the same. Several methods for constructing distance equienergetic graphs have been presented in the literature, most constructed distance equienergetic graphs have diameters of 2 or 3. So the problem of constructing distance equienergetic graphs of diameter greater than 3 would be interesting. Another interesting problem posed by Indulal (2020) is to construct a pair of graphs which are both adjacency equienergetic and distance equienergetic. Motivated by these two problems, in this paper, we obtain the distance spectrum of <span><math><mrow><mi>Θ</mi><mrow><mo>(</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>,</mo><msub><mrow><mi>Γ</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>)</mo></mrow></mrow></math></span> when all these graphs are regular. As an application, we give a method to obtain distance equienergetic graphs of diameter 4. Also we construct a pair of graphs on <span><math><mrow><mn>2</mn><mi>n</mi><mo>+</mo><mn>1</mn></mrow></math></span> vertices (<span><math><mrow><mi>n</mi><mo>≥</mo><mn>6</mn></mrow></math></span>) which are both adjacency equienergetic and distance equienergetic graphs.</div></div>","PeriodicalId":100517,"journal":{"name":"Examples and Counterexamples","volume":"7 ","pages":"Article 100184"},"PeriodicalIF":0.0,"publicationDate":"2025-03-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143739188","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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Examples and Counterexamples
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