Relationships Between The Axioms
The T0 axiom is special in that it can be not only added to a property (so that completely regular plus T0 is Tychonoff) but also subtracted from a property (so that Hausdorff minus T0 is R1), in a fairly precise sense; see Kolmogorov quotient for more information. When applied to the separation axioms, this leads to the relationships in the table below:
T0 version | Non-T0 version |
---|---|
T0 | (No requirement) |
T1 | R0 |
Hausdorff (T2) | R1 |
T2½ | (No special name) |
Completely Hausdorff | (No special name) |
Regular Hausdorff (T3) | Regular |
Tychonoff (T3½) | Completely regular |
Normal T0 | Normal |
Normal Hausdorff (T4) | Normal regular |
Completely normal T0 | Completely normal |
Completely normal Hausdorff (T5) | Completely normal regular |
Perfectly normal T0 | Perfectly normal |
Perfectly normal Hausdorff (T6) | Perfectly normal regular |
In this table, you go from the right side to the left side by adding the requirement of T0, and you go from the left side to the right side by removing that requirement, using the Kolmogorov quotient operation. (The names in parentheses given on the left side of this table are generally ambiguous or at least less well known; but they are used in the diagram below.)
Other than the inclusion or exclusion of T0, the relationships between the separation axioms are indicated in the following diagram:
In this diagram, the non-T0 version of a condition is on the left side of the slash, and the T0 version is on the right side. Letters are used for abbreviation as follows: "P" = "perfectly", "C" = "completely", "N" = "normal", and "R" (without a subscript) = "regular". A bullet indicates that there is no special name for a space at that spot. The dash at the bottom indicates no condition.
You can combine two properties using this diagram by following the diagram upwards until both branches meet. For example, if a space is both completely normal ("CN") and completely Hausdorff ("CT2"), then following both branches up, you find the spot "•/T5". Since completely Hausdorff spaces are T0 (even though completely normal spaces may not be), you take the T0 side of the slash, so a completely normal completely Hausdorff space is the same as a T5 space (less ambiguously known as a completely normal Hausdorff space, as you can see in the table above).
As you can see from the diagram, normal and R0 together imply a host of other properties, since combining the two properties leads you to follow a path through the many nodes on the rightside branch. Since regularity is the most well known of these, spaces that are both normal and R0 are typically called "normal regular spaces". In a somewhat similar fashion, spaces that are both normal and T1 are often called "normal Hausdorff spaces" by people that wish to avoid the ambiguous "T" notation. These conventions can be generalised to other regular spaces and Hausdorff spaces.
Read more about this topic: Separation Axiom
Famous quotes containing the word axioms:
“I tell you the solemn truth that the doctrine of the Trinity is not so difficult to accept for a working proposition as any one of the axioms of physics.”
—Henry Brooks Adams (18381918)