Mathematical Structures: Semilattices

[Home]Semilattices

HomePage | RecentChanges | Login

Difference (from prior major revision) (no other diffs)

Changed: 81,82c81
$\left\langle \mathbb{N},+\right\rangle $, the natural numbers, with additition.

$\left\langle \mathcal{P}_\omega(X)-\{\emptyset\},\cup\right\rangle $, the set of finite nonempty subsets of a set $X$, with union, is the free join-semilattice with singleton subsets of $X$ as generators.

http://mathcs.chapman.edu/structuresold/files/Semilattices.pdf
%%run pdflatex

%


\documentclass[12pt]{amsart}
\usepackage[pdfpagemode=Fullscreen,pdfstartview=FitBH]{hyperref}
\parindent=0pt
\parskip=5pt
\addtolength{\oddsidemargin}{-.5in}
\addtolength{\evensidemargin}{-.5in}
\addtolength{\textwidth}{1in}
\theoremstyle{definition}
\newtheorem{definition}{Definition}
\newtheorem*{morphisms}{Morphisms}
\newtheorem*{basic_results}{Basic Results}
\newtheorem*{examples}{Examples}
\newtheorem{example}{}
\newtheorem*{properties}{Properties}
\newtheorem*{finite_members}{Finite Members}
\newtheorem*{subclasses}{Subclasses}
\newtheorem*{superclasses}{Superclasses}
\newcommand{\abbreviation}[1]{\textbf{Abbreviation: #1}}
\pagestyle{myheadings}\thispagestyle{myheadings}
\markboth{\today}{math.chapman.edu/structures}

\begin{document}
\textbf{\Large Semilattices}
\quad\href{http://math.chapman.edu/cgi-bin/structures?action=edit;id=Semilattices}{edit}

\abbreviation{Slat}
\begin{definition}
A \emph{semilattice} is a structure $\mathbf{S}=\left\langle S,\cdot
\right\rangle $, where $\cdot $ is an infix binary operation, called the 
\emph{semilattice operation}, such that


$\cdot $ is associative:  $(xy)z=x(yz)$


$\cdot $ is commutative:  $xy=yx$


$\cdot $ is idempotent:  $xx=x$


Remark: 
This definition shows that semilattices form a variety.


\end{definition}
\begin{definition}
A \emph{join-semilattice} is a structure $\mathbf{S}=\left\langle S,\vee
\right\rangle $, where $\vee $ is an infix binary operation, called the $\emph{join}$, such that


$\leq $ is a partial order, where $x\leq y\Longleftrightarrow x\vee y=y$


$x\vee y$ is the least upper bound of $\{x,y\}$.
\end{definition}
\begin{definition}
A \emph{meet-semilattice} is a structure $\mathbf{S}=\left\langle S,\wedge
\right\rangle $, where $\wedge $ is an infix binary operation, called the $\emph{meet}$, such that


$\leq $ is a partial order, where $x\leq y\Longleftrightarrow x\wedge y=x$


$x\wedge y$ is the greatest lower bound of $\{x,y\}$.
\end{definition}
\begin{morphisms}
Let $\mathbf{S}$ and $\mathbf{T}$ be semilattices. A morphism from $\mathbf{S}$ to $\mathbf{T}$ is a function $h:S\rightarrow T$ that is a homomorphism: 

$h(xy)=h(x)h(y)$

\end{morphisms}
\begin{basic_results}
\end{basic_results}
\begin{examples}
\begin{example}
$\left\langle \mathcal{P}_\omega(X)-\{\emptyset\},\cup\right\rangle $, the set of finite nonempty subsets of a set $X$, with union, is the free join-semilattice with singleton subsets of $X$ as generators.
\end{example}
\end{examples}
\begin{table}[h]
\begin{properties} (\href{http://math.chapman.edu/cgi-bin/structures?Properties}{description})

\begin{tabular}{|ll|}\hline
Classtype & variety\\\hline
Equational theory & decidable in polynomial time\\\hline
Quasiequational theory & decidable\\\hline
First-order theory & undecidable\\\hline
Locally finite & yes\\\hline
Residual size & 2\\\hline
Congruence distributive & no\\\hline
Congruence modular & no\\\hline
Congruence meet-semidistributive & yes\\\hline
Congruence n-permutable & no\\\hline
Congruence regular & no\\\hline
Congruence uniform & no\\\hline
Congruence extension property & \\\hline
Definable principal congruences & \\\hline
Equationally def. pr. cong. & \\\hline
Amalgamation property & yes\\\hline
Strong amalgamation property & yes\\\hline
Epimorphisms are surjective & yes\\\hline
\end{tabular}
\end{properties}
\end{table}\begin{finite_members} $f(n)=$ number of members of size $n$.

$\begin{array}{lr}
f(1)= &1\\
f(2)= &1\\
f(3)= &2\\
f(4)= &5\\
f(5)= &15\\
f(6)= &53\\
f(7)= &222\\
f(8)= &1078\\
f(9)= &5994\\
f(10)= &37622\\
f(11)= &262776\\
f(12)= &2018305\\
f(13)= &16873364\\
f(14)= &152233518\\
f(15)= &1471613387\\
f(16)= &15150569446\\
f(17)= &165269824761\\
\end{array}$

These results follow from the paper below and the observation that semilattices with $n$ elements 
are in 1-1 correspondence to lattices with $n+1$ elements.

Jobst Heitzig,J\"urgen Reinhold,\emph{Counting finite lattices},
Algebra Universalis,
\textbf{48}2002,43--53\href{http://www.ams.org/mathscinet-getitem?mr=1 930 032}{MRreview}

\href{Search_for_finite_semilattices.pdf}{Search for finite semilattices}
\end{finite_members}
\hyperbaseurl{http://math.chapman.edu/structures/files/}
\parskip0pt
\begin{subclasses}\ 

\href{One-element_algebras.pdf}{One-element algebras} 

\href{Semilattices_with_zero.pdf}{Semilattices with zero} 

\href{Semilattices_with_identity.pdf}{Semilattices with identity} 

\end{subclasses}
\begin{superclasses}\ 

\href{Commutative_semigroups.pdf}{Commutative semigroups} 

\href{Partial_semilattices.pdf}{Partial semilattices} 

\end{superclasses}

\begin{thebibliography}{10}

\bibitem{Ln19xx}

\end{thebibliography}

\end{document}
%


HomePage | RecentChanges | Login
This page is read-only | View other revisions
Last edited September 4, 2008 7:50 pm by Jipsen (diff)
Search: