# Difference between revisions of "Complete lattice"

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− | A [[ | + | {{TEX|done}}{{MSC|06B23}} |

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+ | A [[partially ordered set]] in which any subset $A$ has a least upper bound and a greatest lower bound. These are usually called the join and the meet of $A$ and are denoted by $\wedge_{a \in A} a$ and and $\vee_{a \in A} a$ or simply by $\vee A$ and $\wedge A$ (respectively). If a partially ordered set has a largest element and each non-empty subset of it has a greatest lower bound, then it is a complete lattice. A lattice $L$ is complete if and only if any isotone mapping $\phi$ of the lattice into itself has a fixed point, i.e. an element $a \in L$ such that $a \phi = a$. If $\mathcal{P}(M)$ is the set of subsets of a set $M$ ordered by inclusion and $\phi$ is a [[Closure relation|closure operation]] on $\mathcal{P}(M)$, then the set of all $\phi$-closed subsets is a complete lattice. | ||

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+ | Any partially ordered set $P$ can be isomorphically imbedded in a complete lattice, which in that case is called a completion of $P$. For example, the map | ||

+ | $$ | ||

+ | x \mapsto \{x\}^\nabla = \{ y \in X : y \le x \} | ||

+ | $$ | ||

+ | maps $P$ into the complete lattice $\mathcal{P}(P)$, and hence defines a completion $\mathcal{O}(P)$ of $P$. However this has this disadvantage that if $P$ is already a complete lattice, and hence a completion of itself, then the completion $\mathcal{O}(P)$ is larger than $P$ itself. The [[Completion, MacNeille (of a partially ordered set)|Dedkind–MacNeille completion]] is the least of all completions of a given partially ordered set. | ||

+ | |||

+ | Complete lattices are formed by the set of all subalgebras in a universal algebra, by the set of all congruences in a universal algebra, and by the set of all closed subsets in a topological space (note that while the meet of a family of closed sets is their set-theoretic intersection, the join of a family of closed sets is the closure of their set-theoretic union). | ||

====References==== | ====References==== | ||

<table> | <table> | ||

− | <TR><TD valign="top">[1]</TD> <TD valign="top"> G. Birkhoff, "Lattice theory" , ''Colloq. Publ.'' , '''25''' , Amer. Math. Soc. ( | + | <TR><TD valign="top">[1]</TD> <TD valign="top"> G. Birkhoff, "Lattice theory", 3rd ed. ''Colloq. Publ.'' , '''25''' , Amer. Math. Soc. (1967) {{ZBL|0153.02501}}</TD></TR> |

− | <TR><TD valign="top">[2]</TD> <TD valign="top"> L.A. Skornyakov, "Elements of lattice theory" , | + | <TR><TD valign="top">[2]</TD> <TD valign="top"> L.A. Skornyakov, "Elements of lattice theory" , Hindustan Publ. Comp. (1977) (Translated from Russian) ISBN 0852743319 {{ZBL|0222.06002}}</TD></TR> |

</table> | </table> | ||

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<table> | <table> | ||

− | <TR><TD valign="top">[a1]</TD> <TD valign="top"> B. A. Davey, H. A. Priestley, ''Introduction to lattices and order'', 2nd ed. Cambridge University Press (2002) ISBN 978-0-521-78451-1</TD></TR> | + | <TR><TD valign="top">[a1]</TD> <TD valign="top"> B. A. Davey, H. A. Priestley, ''Introduction to lattices and order'', 2nd ed. Cambridge University Press (2002) ISBN 978-0-521-78451-1 {{ZBL|1002.06001}}</TD></TR> |

+ | <TR><TD valign="top">[a2]</TD> <TD valign="top"> G. Gierz, K.H. Hofmann, K. Keimel, J.D. Lawson, M.V. Mislove, D.S. Scott, "A compendium of continuous lattices" , Springer (1980) ISBN 3-540-10111-X {{MR|0614752}} {{ZBL|0452.06001}} </TD></TR> | ||

</table> | </table> |

## Latest revision as of 17:39, 9 December 2017

2010 Mathematics Subject Classification: *Primary:* 06B23 [MSN][ZBL]

A partially ordered set in which any subset $A$ has a least upper bound and a greatest lower bound. These are usually called the join and the meet of $A$ and are denoted by $\wedge_{a \in A} a$ and and $\vee_{a \in A} a$ or simply by $\vee A$ and $\wedge A$ (respectively). If a partially ordered set has a largest element and each non-empty subset of it has a greatest lower bound, then it is a complete lattice. A lattice $L$ is complete if and only if any isotone mapping $\phi$ of the lattice into itself has a fixed point, i.e. an element $a \in L$ such that $a \phi = a$. If $\mathcal{P}(M)$ is the set of subsets of a set $M$ ordered by inclusion and $\phi$ is a closure operation on $\mathcal{P}(M)$, then the set of all $\phi$-closed subsets is a complete lattice.

Any partially ordered set $P$ can be isomorphically imbedded in a complete lattice, which in that case is called a completion of $P$. For example, the map $$ x \mapsto \{x\}^\nabla = \{ y \in X : y \le x \} $$ maps $P$ into the complete lattice $\mathcal{P}(P)$, and hence defines a completion $\mathcal{O}(P)$ of $P$. However this has this disadvantage that if $P$ is already a complete lattice, and hence a completion of itself, then the completion $\mathcal{O}(P)$ is larger than $P$ itself. The Dedkind–MacNeille completion is the least of all completions of a given partially ordered set.

Complete lattices are formed by the set of all subalgebras in a universal algebra, by the set of all congruences in a universal algebra, and by the set of all closed subsets in a topological space (note that while the meet of a family of closed sets is their set-theoretic intersection, the join of a family of closed sets is the closure of their set-theoretic union).

#### References

[1] | G. Birkhoff, "Lattice theory", 3rd ed. Colloq. Publ. , 25 , Amer. Math. Soc. (1967) Zbl 0153.02501 |

[2] | L.A. Skornyakov, "Elements of lattice theory" , Hindustan Publ. Comp. (1977) (Translated from Russian) ISBN 0852743319 Zbl 0222.06002 |

[a1] | B. A. Davey, H. A. Priestley, Introduction to lattices and order, 2nd ed. Cambridge University Press (2002) ISBN 978-0-521-78451-1 Zbl 1002.06001 |

[a2] | G. Gierz, K.H. Hofmann, K. Keimel, J.D. Lawson, M.V. Mislove, D.S. Scott, "A compendium of continuous lattices" , Springer (1980) ISBN 3-540-10111-X MR0614752 Zbl 0452.06001 |

**How to Cite This Entry:**

Complete lattice.

*Encyclopedia of Mathematics.*URL: http://encyclopediaofmath.org/index.php?title=Complete_lattice&oldid=33805