共查询到17条相似文献,搜索用时 62 毫秒
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在不分明化拓扑空间中,从pre-开集出发引入了强紧性的概念,并且给出了它的一些性质.这些概念的结合有助于我们对不分明化拓扑的研究. 相似文献
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给出了一般的L-不分明拓扑空间的Alexandorff紧化,并且对弱诱导空间证明了该紧化是弱诱导紧化类中唯一最小的紧化。 相似文献
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本文给王国俊先生发现的良紧性定义了一个分明拓扑模型,利用此模型较为简洁地证明了关于良紧性的吉洪诺夫定理。然后,仿照良紧性的定义方式定义了J——紧性。最后,利用彭育威先生对良紧性作出的几何刻划证明了良紧性与一般的J——紧性之间的一个重要关系。总之,本文的结果对认识模糊拓扑与分明拓扑之间的联系有一定的意义。 相似文献
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Pre—Separation Axioms in Fuzzifying Topology 总被引:1,自引:0,他引:1
K.M.AbdEl-Hakeim F.M.Zeyada 《模糊系统与数学》2003,17(1):28-36
1 IntroductionYing[5,6 ] introduced and elementally developed so called fuzzifying topology with the semanticmethod of continuous valued L ogic.Shen[7] introduced and studied T0 -,T1-,T2 (Hausdorff) -,T3(regularity) -,T4 (normality) -separation axioms in fuzzifying topology.In [3 ]the concepts of thefamily of fuzzifying pre-open sets,fuzzifying pre-neighbourhood structure of a point and fuzzifyingpre-closure are introduced and studied.It is worth to mention that pre-separation axioms are … 相似文献
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通过应用完全剩余格值逻辑语义的方法把不分明化一致空间和不分明化一致拓扑推广为L-不分明化一致空间和L-不分明化一致拓扑。并且讨论了L-不分明化一致空间和L-不分明化一致拓扑的一些基本性质。 相似文献
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拓扑系统的紧性和分离性 总被引:1,自引:0,他引:1
考察拓扑系统的两种紧性——空间式紧和locale式紧,给出紧性的若干刻画,讨论了两种紧性的相互关系,证明了拓扑系统的两种紧性都是拓扑空间紧性的良好推广,说明了紧拓扑系统的闭子拓扑系统、有限和系统以及积系统仍是紧拓扑系统。最后在拓扑系统中考察了紧性加强分离性的问题,得到了紧,(强)T2拓扑系统为(强)T3,(强)T4拓扑系统等结论,并用理想收敛刻画了拓扑系统的强T2分离性。 相似文献
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拓扑分子格的S紧性和S次紧性 总被引:2,自引:0,他引:2
利用半开元等半拓扑概念在拓扑分子格中引入S紧性与S次紧性,给出了它们的刻画,推广了文[1]中的紧性与次紧性,证明了拓扑分子格的S紧性,S次紧性,STi分离性(i=-1,0,1,2)与STi^*分离性(i=0,1,2)为半拓扑性质。 相似文献
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Dirk Hachenberger 《Discrete Mathematics》2010,310(22):3246-3250
The present paper is a continuation of the author’s work (Hachenberger (2001) [3]) on primitivity and complete normality. For certain 2-power extensions E over a Galois field Fq, we are going to establish the existence of a primitive element which simultaneously generates a normal basis over every intermediate field of E/Fq. The main result is as follows: Letq≡3mod4and letm(q)≥3be the largest integer such that2m(q)dividesq2−1; ifE=Fq2l, wherel≥m(q)+3, then there exists a primitive element inEthat is completely normal overFq.Our method not only shows existence but also gives a fairly large lower bound on the number of primitive completely normal elements. In the above case this number is at least 4⋅(q−1)2l−2. We are further going to discuss lower bounds on the number of such elements in r-power extensions, where r=2 and q≡1mod4, or where r is an odd prime, or where r is equal to the characteristic of the underlying field. 相似文献