2.3Order Topology
Chapter (PDF)If a set is totally ordered, then the ordering actually induces a canonical topology on called the order topology. We investigate its construction and behavior in this section.
First, considering open/closed/half-open intervals in , we may define them equivalently in an arbitrary totally ordered set, using its order in place of 's standard ordering. We name them equivalently, suggesting that open intervals in a totally ordered set should be open with respect to the order topology. This is true.
Suppose is a totally ordered set. Let be the collection of all sets of the following forms.
All open intervals , for every .
The half-open interval , for some minimum element (if any) and any .
The half-open interval , for any and some maximum element (if any) .
Then forms a basis for a topology on called the ordered topology.
We show is, indeed, a basis. First, note that every element of lies in one of the three prescribed sets: the smallest lies in the upper-open set, the largest lies in the lower-open set, and all other elements lie in an open interval—thus covers as promised. With a long argument by cases, it follows that the intersection of two basis elements can be locally refined.
Note the standard topology on is simply the topology induced by the standard order. Note the order topology on is simply the discrete topology, since every subset of falls into an interval (the singleton ).
If is a totally ordered set, an element determines four rays. They are .
The rays of form and are called open rays. Its name is accurate—this interval forms an open set with respect to the order topology. For a set whose maximum , ; if no maximum exists, then is simply the union of all basis elements for . Similar argumentation follows for .
Please note that, for a totally ordered set with maximum (resp. minimum) (resp. ), then (resp. ).
Suppose is a totally ordered set. Then the set
forms a subbasis for the order topology on .
It should follow immediately that every basis element can be generated by a finite intersection of one or two open rays.