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Algebraic Representation Of Mappings Between Submodule Lattices

机译:子模块格之间的映射的代数表示

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We show that under certain weak conditions on the module _RM, every mapping f : £(_RM) → £(_SN) between the submodule lattices which preserves arbitrary joins and "disjointness" has a unique representation of the form f(u) = for all u ∈£(_RM), where _SB_R is some bimodule and h is an R-balanced mapping. Furthermore, f is a lattice homomorphism if and only if Br is flat and the induced S-module homomorphism h : _SB_⊕ _RM → _SN is monic. If _SN also satisfies the same weak conditions, then f is a lattice isomorphism if and only if Br is a finitely generated projective generator, S ≌ End(B_R) canonically, and h : _SB_⊕ _RM → _SN is an S-module isomorphism, i.e., every lattice isomorphism is induced by a Morita equivalence between R and S and a module isomorphism.
机译:我们表明,在模块_RM上的某些弱条件下,子模块晶格之间的每个映射f:£(_RM)→£(_SN)保留了任意连接,并且“不相交”具有形式f(u)= <对于所有u∈£(_RM),h [_SB_R×_RU]>,其中_SB_R是某个双模数,h是R平衡映射。此外,当且仅当Br是平坦的并且诱导的S模同质性h:_SB_⊕_RM→_SN是一元的时,f是晶格同质性。如果_SN也满足相同的弱条件,则且仅当Br是有限生成的射影生成器且S≌End(B_R)典范且h:_SB_⊕_RM→_SN是S模同构时,f才是晶格同构,也就是说,每个晶格同构都是由R和S之间的Morita等价物和模块同构引起的。

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