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Forcing faces in plane bipartite graphs

机译:在平面二部图中强制面

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Let Ω denote the class of connected plane bipartite graphs with no pendant edges. A finite face s of a graph GΩ is said to be a forcing face of G if the subgraph of G obtained by deleting all vertices of s together with their incident edges has exactly one perfect matching. This is a natural generalization of the concept of forcing hexagons in a hexagonal system introduced in Che and Chen [Forcing hexagons in hexagonal systems, MATCH Commun. Math. Comput. Chem. 56 (3) (2006) 649–668]. We prove that any connected plane bipartite graph with a forcing face is elementary. We also show that for any integers n and k with n4 and nk0, there exists a plane elementary bipartite graph such that exactly k of the n finite faces of G are forcing. We then give a shorter proof for a recent result that a connected cubic plane bipartite graph G has at least two disjoint M-resonant faces for any perfect matching M of G, which is a main theorem in the paper [S. Bau, M.A. Henning, Matching transformation graphs of cubic bipartite plane graphs, Discrete Math. 262 (2003) 27–36]. As a corollary, any connected cubic plane bipartite graph has no forcing faces. Using the tool of Z-transformation graphs developed by Zhang et al. [Z-transformation graphs of perfect matchings of hexagonal systems, Discrete Math. 72 (1988) 405–415; Plane elementary bipartite graphs, Discrete Appl. Math. 105 (2000) 291–311], we characterize the plane elementary bipartite graphs whose finite faces are all forcing. We also obtain a necessary and sufficient condition for a finite face in a plane elementary bipartite graph to be forcing, which enables us to investigate the relationship between the existence of a forcing edge and the existence of a forcing face in a plane elementary bipartite graph, and find out that the former implies the latter but not vice versa. Moreover, we characterize the plane bipartite graphs that can be turned to have all finite faces forcing by subdivisions.
机译:令Ω表示没有垂线边缘的连通平面二部图的类别。如果通过删除s的所有顶点及其入射边缘而获得的G的子图具有一个完全匹配,则图GΩ的有限面s称为G的强制面。这是在Che和Chen中引入的在六边形系统中强制六边形的概念的自然概括[在MATCH Commun中,在六边形系统中强制六边形。数学。计算化学56(3)(2006)649–668]。我们证明任何具有强迫面的连通平面二部图都是基本的。我们还表明,对于任何具有n4和nk0的整数n和k,都存在一个平面基本二部图,使得G的n个有限面中的k个正好受到强迫。然后,对于最近的结果,我们给出一个简短的证明,即对于任何G的完美匹配,连通的立方平面二部图G至少具有两个不相交的M共振面,这是本文的主要定理[S. Bau,M.A. Henning,立方二分平面图的匹配变换图,离散数学。 262(2003)27-36]。因此,任何连通的立方平面二部图都没有强制面。使用Zhang等人开发的Z变换图工具。 [六边形系统的完美匹配的Z变换图,离散数学。 72(1988)405-415;平面基本二部图,离散应用。数学。 105(2000)291–311],我们描述了有限面都受力的平面基本二部图。我们还获得了平面基本二部图中强制面的一个充要条件,这使我们能够研究平面基本二部图中强制边的存在与强制面的存在之间的关系,并发现前者暗含后者,反之则不然。此外,我们描述了平面二部图的特征,该二部图可以被细分为具有所有有限面的力。

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