带符号图中的群值电位差和流

IF 1.1 3区 数学 Q3 MATHEMATICS, APPLIED Discrete Applied Mathematics Pub Date : 2025-05-15 Epub Date: 2025-01-27 DOI:10.1016/j.dam.2025.01.035
Xiangyu Ren , Jianguo Qian
{"title":"带符号图中的群值电位差和流","authors":"Xiangyu Ren ,&nbsp;Jianguo Qian","doi":"10.1016/j.dam.2025.01.035","DOIUrl":null,"url":null,"abstract":"<div><div>A signed graph <span><math><mrow><mi>Σ</mi><mo>=</mo><mrow><mo>(</mo><mi>G</mi><mo>,</mo><mi>σ</mi><mo>)</mo></mrow></mrow></math></span> is a graph associated with a signature <span><math><mi>σ</mi></math></span> on each edge (positive or negative). Let <span><math><mi>Γ</mi></math></span> be an additive abelian group and <span><math><mi>τ</mi></math></span> be an orientation of <span><math><mi>Σ</mi></math></span>. Let <span><math><mrow><mi>f</mi><mo>:</mo><mi>E</mi><mo>→</mo><mi>Γ</mi></mrow></math></span> be a mapping. Then <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-flow if for each vertex <span><math><mrow><munder><mrow><mo>∑</mo></mrow><mrow><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mo>∈</mo><mi>E</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow></mrow></munder><mi>τ</mi><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mi>f</mi><mrow><mo>(</mo><mi>e</mi><mo>)</mo></mrow><mo>=</mo><mn>0</mn><mo>,</mo></mrow></math></span>\n <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-tension if for every signed circuit <span><math><mrow><mi>C</mi><mo>=</mo><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>2</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>⋯</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub></mrow></math></span>, <span><math><mrow><munderover><mrow><mo>∑</mo></mrow><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>k</mi></mrow></munderover><mfenced><mrow><mo>−</mo><mi>τ</mi><mrow><mo>(</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>,</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><munderover><mrow><mo>∏</mo></mrow><mrow><mi>j</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>i</mi><mo>−</mo><mn>1</mn></mrow></munderover><mi>σ</mi><mrow><mo>(</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>j</mi></mrow></msub><mo>)</mo></mrow></mrow></mfenced><mi>f</mi><mrow><mo>(</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mo>=</mo><mn>0</mn><mo>,</mo></mrow></math></span>\n and <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-potential difference if <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-tension such that for every closed walk <span><math><mrow><mi>W</mi><mo>=</mo><mrow><mo>(</mo><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>2</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>⋯</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow></mrow></math></span> around an unbalanced circuit, <span><math><mrow><munderover><mrow><mo>∑</mo></mrow><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>k</mi></mrow></munderover><mi>f</mi><mrow><mo>(</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mo>∈</mo><mrow><mo>{</mo><mn>2</mn><mi>x</mi><mo>:</mo><mi>x</mi><mo>∈</mo><mi>Γ</mi><mo>}</mo></mrow><mo>.</mo></mrow></math></span>\n We say a mapping <span><math><mrow><mi>f</mi><mo>:</mo><mi>E</mi><mo>⋃</mo><mi>V</mi><mo>→</mo><mi>Γ</mi></mrow></math></span> is a mixed <span><math><mi>Γ</mi></math></span>-flow if for each vertex <span><math><mi>v</mi></math></span>, <span><math><mrow><munder><mrow><mo>∑</mo></mrow><mrow><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mo>∈</mo><mi>E</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow></mrow></munder><mi>τ</mi><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mi>f</mi><mrow><mo>(</mo><mi>e</mi><mo>)</mo></mrow><mo>=</mo><mi>f</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mo>.</mo></mrow></math></span>\n Denote by <span><math><msub><mrow><mi>F</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span>, <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span> and <span><math><msub><mrow><mi>B</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span> the sets of <span><math><mi>Γ</mi></math></span>-flows, <span><math><mi>Γ</mi></math></span>-potential differences, and mixed <span><math><mi>Γ</mi></math></span>-flows of <span><math><mi>Σ</mi></math></span> respectively.</div><div>In this paper, we use a new method to determine the values of <span><math><mrow><mo>|</mo><msub><mrow><mi>F</mi></mrow><mrow><mi>Σ</mi></mrow></msub><mo>|</mo></mrow></math></span> and <span><math><mrow><mo>|</mo><msub><mrow><mi>P</mi></mrow><mrow><mi>Σ</mi></mrow></msub><mo>|</mo></mrow></math></span>. Furthermore, we show that <span><math><mrow><msub><mrow><mi>B</mi></mrow><mrow><mi>Σ</mi></mrow></msub><mo>/</mo><msub><mrow><mi>F</mi></mrow><mrow><mi>Σ</mi></mrow></msub></mrow></math></span> is isomorphic to <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span> by a new decomposition of <span><math><mi>Γ</mi></math></span>-potential difference.</div></div>","PeriodicalId":50573,"journal":{"name":"Discrete Applied Mathematics","volume":"366 ","pages":"Pages 185-192"},"PeriodicalIF":1.1000,"publicationDate":"2025-05-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"On group-valued potential differences and flows in a signed graph\",\"authors\":\"Xiangyu Ren ,&nbsp;Jianguo Qian\",\"doi\":\"10.1016/j.dam.2025.01.035\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>A signed graph <span><math><mrow><mi>Σ</mi><mo>=</mo><mrow><mo>(</mo><mi>G</mi><mo>,</mo><mi>σ</mi><mo>)</mo></mrow></mrow></math></span> is a graph associated with a signature <span><math><mi>σ</mi></math></span> on each edge (positive or negative). Let <span><math><mi>Γ</mi></math></span> be an additive abelian group and <span><math><mi>τ</mi></math></span> be an orientation of <span><math><mi>Σ</mi></math></span>. Let <span><math><mrow><mi>f</mi><mo>:</mo><mi>E</mi><mo>→</mo><mi>Γ</mi></mrow></math></span> be a mapping. Then <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-flow if for each vertex <span><math><mrow><munder><mrow><mo>∑</mo></mrow><mrow><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mo>∈</mo><mi>E</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow></mrow></munder><mi>τ</mi><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mi>f</mi><mrow><mo>(</mo><mi>e</mi><mo>)</mo></mrow><mo>=</mo><mn>0</mn><mo>,</mo></mrow></math></span>\\n <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-tension if for every signed circuit <span><math><mrow><mi>C</mi><mo>=</mo><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>2</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>⋯</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub></mrow></math></span>, <span><math><mrow><munderover><mrow><mo>∑</mo></mrow><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>k</mi></mrow></munderover><mfenced><mrow><mo>−</mo><mi>τ</mi><mrow><mo>(</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>,</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><munderover><mrow><mo>∏</mo></mrow><mrow><mi>j</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>i</mi><mo>−</mo><mn>1</mn></mrow></munderover><mi>σ</mi><mrow><mo>(</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>j</mi></mrow></msub><mo>)</mo></mrow></mrow></mfenced><mi>f</mi><mrow><mo>(</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mo>=</mo><mn>0</mn><mo>,</mo></mrow></math></span>\\n and <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-potential difference if <span><math><mi>f</mi></math></span> is a <span><math><mi>Γ</mi></math></span>-tension such that for every closed walk <span><math><mrow><mi>W</mi><mo>=</mo><mrow><mo>(</mo><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>1</mn></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>2</mn></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>⋯</mo><msub><mrow><mi>v</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>e</mi></mrow><mrow><mi>k</mi></mrow></msub><msub><mrow><mi>v</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow></mrow></math></span> around an unbalanced circuit, <span><math><mrow><munderover><mrow><mo>∑</mo></mrow><mrow><mi>i</mi><mo>=</mo><mn>1</mn></mrow><mrow><mi>k</mi></mrow></munderover><mi>f</mi><mrow><mo>(</mo><msub><mrow><mi>e</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>)</mo></mrow><mo>∈</mo><mrow><mo>{</mo><mn>2</mn><mi>x</mi><mo>:</mo><mi>x</mi><mo>∈</mo><mi>Γ</mi><mo>}</mo></mrow><mo>.</mo></mrow></math></span>\\n We say a mapping <span><math><mrow><mi>f</mi><mo>:</mo><mi>E</mi><mo>⋃</mo><mi>V</mi><mo>→</mo><mi>Γ</mi></mrow></math></span> is a mixed <span><math><mi>Γ</mi></math></span>-flow if for each vertex <span><math><mi>v</mi></math></span>, <span><math><mrow><munder><mrow><mo>∑</mo></mrow><mrow><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mo>∈</mo><mi>E</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow></mrow></munder><mi>τ</mi><mrow><mo>(</mo><mi>v</mi><mo>,</mo><mi>e</mi><mo>)</mo></mrow><mi>f</mi><mrow><mo>(</mo><mi>e</mi><mo>)</mo></mrow><mo>=</mo><mi>f</mi><mrow><mo>(</mo><mi>v</mi><mo>)</mo></mrow><mo>.</mo></mrow></math></span>\\n Denote by <span><math><msub><mrow><mi>F</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span>, <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span> and <span><math><msub><mrow><mi>B</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span> the sets of <span><math><mi>Γ</mi></math></span>-flows, <span><math><mi>Γ</mi></math></span>-potential differences, and mixed <span><math><mi>Γ</mi></math></span>-flows of <span><math><mi>Σ</mi></math></span> respectively.</div><div>In this paper, we use a new method to determine the values of <span><math><mrow><mo>|</mo><msub><mrow><mi>F</mi></mrow><mrow><mi>Σ</mi></mrow></msub><mo>|</mo></mrow></math></span> and <span><math><mrow><mo>|</mo><msub><mrow><mi>P</mi></mrow><mrow><mi>Σ</mi></mrow></msub><mo>|</mo></mrow></math></span>. Furthermore, we show that <span><math><mrow><msub><mrow><mi>B</mi></mrow><mrow><mi>Σ</mi></mrow></msub><mo>/</mo><msub><mrow><mi>F</mi></mrow><mrow><mi>Σ</mi></mrow></msub></mrow></math></span> is isomorphic to <span><math><msub><mrow><mi>P</mi></mrow><mrow><mi>Σ</mi></mrow></msub></math></span> by a new decomposition of <span><math><mi>Γ</mi></math></span>-potential difference.</div></div>\",\"PeriodicalId\":50573,\"journal\":{\"name\":\"Discrete Applied Mathematics\",\"volume\":\"366 \",\"pages\":\"Pages 185-192\"},\"PeriodicalIF\":1.1000,\"publicationDate\":\"2025-05-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Discrete Applied Mathematics\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0166218X25000447\",\"RegionNum\":3,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2025/1/27 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q3\",\"JCRName\":\"MATHEMATICS, APPLIED\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Discrete Applied Mathematics","FirstCategoryId":"100","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0166218X25000447","RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/1/27 0:00:00","PubModel":"Epub","JCR":"Q3","JCRName":"MATHEMATICS, APPLIED","Score":null,"Total":0}
引用次数: 0

摘要

签名图Σ=(G, Σ)是在每条边(正或负)上都有一个签名Σ的图。设Γ为加性阿贝尔群,τ为Σ的一个取向。设f:E→Γ是一个映射。然后f是一个Γ-flow if,对于每个顶点∑(v,e)∈e (v)τ(v,e)f(e)=0, f是一个Γ-tension if,对于每个带符号电路C=v1e1v2e2⋯vkekv1,∑i=1k−τ(vi,ei)∏j=1i−1σ(ej)f(ei)=0, f是一个Γ-potential差分,如果f是一个Γ-tension,使得对于每一个围绕不平衡电路的闭合行走W=(v1e1v2e2⋯vkekv1),∑i=1kf(ei)∈{2x:x∈Γ}。我们说映射f:E∈V→Γ是一个混合Γ-flow,如果对于每个顶点V,∑(V, E)∈E(V)τ(V, E)f(E)=f(V)。分别用FΣ、PΣ和BΣ表示Σ的Γ-flows、Γ-potential的差异集和混合Γ-flows集。在本文中,我们使用了一种新的方法来确定|FΣ|和|PΣ|的值。进一步,我们通过对Γ-potential差分进行新的分解,证明BΣ/FΣ与PΣ是同构的。
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On group-valued potential differences and flows in a signed graph
A signed graph Σ=(G,σ) is a graph associated with a signature σ on each edge (positive or negative). Let Γ be an additive abelian group and τ be an orientation of Σ. Let f:EΓ be a mapping. Then f is a Γ-flow if for each vertex (v,e)E(v)τ(v,e)f(e)=0, f is a Γ-tension if for every signed circuit C=v1e1v2e2vkekv1, i=1kτ(vi,ei)j=1i1σ(ej)f(ei)=0, and f is a Γ-potential difference if f is a Γ-tension such that for every closed walk W=(v1e1v2e2vkekv1) around an unbalanced circuit, i=1kf(ei){2x:xΓ}. We say a mapping f:EVΓ is a mixed Γ-flow if for each vertex v, (v,e)E(v)τ(v,e)f(e)=f(v). Denote by FΣ, PΣ and BΣ the sets of Γ-flows, Γ-potential differences, and mixed Γ-flows of Σ respectively.
In this paper, we use a new method to determine the values of |FΣ| and |PΣ|. Furthermore, we show that BΣ/FΣ is isomorphic to PΣ by a new decomposition of Γ-potential difference.
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来源期刊
Discrete Applied Mathematics
Discrete Applied Mathematics 数学-应用数学
CiteScore
2.30
自引率
9.10%
发文量
422
审稿时长
4.5 months
期刊介绍: The aim of Discrete Applied Mathematics is to bring together research papers in different areas of algorithmic and applicable discrete mathematics as well as applications of combinatorial mathematics to informatics and various areas of science and technology. Contributions presented to the journal can be research papers, short notes, surveys, and possibly research problems. The "Communications" section will be devoted to the fastest possible publication of recent research results that are checked and recommended for publication by a member of the Editorial Board. The journal will also publish a limited number of book announcements as well as proceedings of conferences. These proceedings will be fully refereed and adhere to the normal standards of the journal. Potential authors are advised to view the journal and the open calls-for-papers of special issues before submitting their manuscripts. Only high-quality, original work that is within the scope of the journal or the targeted special issue will be considered.
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