残差映射网格的原子

IF 0.3 Q4 MATHEMATICS
K. Kaarli, S´ándor Radeleczki
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引用次数: 0

摘要

给定一个晶格L,我们用Res(L)表示L上所有剩余映射的晶格。本文的主要目的是研究Res(L)上的原子,其中L是一个完全晶格。注意Res(L)的双原子描述很容易从Shmuely(1974)的早期结果中得到。首先考虑栅格L,其中Res(L)的所有原子都是具有2元范围的映射,并给出了一个充分条件。扩展这一结果,我们在Blyth和Janowitz(残差理论,1972)的意义上描述了Res(L)的这些弱正则残差映射的原子。在本文的其余部分,我们研究了Res(M)的原子,其中M是有限投影平面的晶格,特别是描述了Res(F)的原子,其中F是Fano平面的晶格。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Atoms of the lattices of residuated mappings
Given a lattice L, we denote by Res(L) the lattice of all residuated maps on L. The main objective of the paper is to study the atoms of Res(L) where L is a complete lattice. Note that the description of dual atoms of Res(L) easily follows from earlier results of Shmuely (1974). We first consider lattices L for which all atoms of Res(L) are mappings with 2-element range and give a sufficient condition for this. Extending this result, we characterize these atoms of Res(L) which are weakly regular residuated maps in the sense of Blyth and Janowitz (Residuation Theory, 1972). In the rest of the paper we investigate the atoms of Res(M) where M is the lattice of a finite projective plane, in particular, we describe the atoms of Res(F), where F is the lattice of the Fano plane.
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来源期刊
CiteScore
0.60
自引率
33.30%
发文量
11
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