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On a theorem of ndreanu and Tudor

机译:关于ndreanu和Tudor定理

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摘要

For an operator domain $mathbf{Sigma}$, which has exactly one binary operator symbol $sigma$, and a set $M$, c{T}u{a}ndu{a}reanu and Tudor have defined a homomorphism $f_{M}$ from the inf-semi-lattice $mathbf{Sub}(M)$, where $mathrm{Sub}(M)$, the underlying set of $mathbf{Sub}(M)$, is the set of all subsets of $M$, to the inf-semi-lattice $mathbf{Sub}_{mathbf{Sigma}}(mathbf{T}_{mathbf{Sigma}}(M))$, where $mathrm{Sub}_{mathbf{Sigma}}(mathbf{T}_{mathbf{Sigma}}(M))$, the underlying set of $mathbf{Sub}_{mathbf{Sigma}}(mathbf{T}_{mathbf{Sigma}}(M))$, is the set of all subalgebras of the free $mathbf{Sigma}$-algebra $mathbf{T}_{mathbf{Sigma}}(M)$ on $M$, by assigning to each $Xsubseteq M$ precisely $mathrm{T}_{mathbf{Sigma}}(X)$, the underlying set of the free $mathbf{Sigma}$-algebra $mathbf{T}_{mathbf{Sigma}}(X)$ on $X$, identified to $mathrm{Sg}_{mathbf{T}_{mathbf{Sigma}}(M)}(X)$, the subalgebra of $mathbf{T}_{mathbf{Sigma}}(M)$ generated by $X$. In this note we show, on the one hand, that the aforementioned homomorphisms between inf-semi-lattices are the components of a natural transformation between two suitable contravariant functors, and, on the other hand, that when the above mentioned homomorphisms are considered as order preserving mappings, they are the components of a natural transformation between two appropriate functors.
机译:对于一个运算符域$ mathbf { Sigma} $,它只有一个二进制运算符$ sigma $和一组$ M $, c {T} u {a} nd u {a} reanu和都铎(Tudor)从反半格$ mathbf {Sub}(M)$中定义了同态$ f_ {M} $,其中$ mathrm {Sub}(M)$是$ mathbf {Sub的基础集合}(M)$是$ M $的所有子集的集合,位于反半格$ mathbf {Sub} _ {{mathbf { Sigma}}}( mathbf {T} _ { mathbf { Sigma}}(M))$,其中$ mathrm {Sub} _ { mathbf { Sigma}}( mathbf {T} _ { mathbf { Sigma}}(M))$是基础集合$ mathbf {Sub} _ { mathbf { Sigma}}( mathbf {T} _ { mathbf { Sigma}}(M))$中的$是所有$ mathbf { Sigma} $-代数$ mathbf {T} _ { mathbf { Sigma}}(M)$在$ M $上,方法是将每个$ X subseteq M $精确地分配给$$ mathbf { Sigma}}(X)$,$ X $上的免费$ mathbf { Sigma} $-代数$ mathbf {T} _ { mathbf { Sigma}}(X)$的基础集合,标识为$ mathrm {Sg} _ { mathbf {T} _ { mathbf { Sigma}}(M)}(X)$,$ mathbf {T} _ { mathbf { Sigma }}(M)$由$ X $。在本说明中,我们表明,一方面,半小晶格之间的上述同态是两个合适的对变函子之间自然转换的组成部分;另一方面,当上述同态被视为为了保留顺序,它们是两个适当的函子之间自然转换的组成部分。

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