Editing Operator topologies (section)

== Topology to use ==

The most commonly used topologies are the norm, strong, and weak operator topologies. 
The weak operator topology is useful for compactness arguments, because the unit ball is compact by the [[Banach–Alaoglu theorem]]. 
The norm topology is fundamental because it makes {{math|B(''H'')}} into a Banach space, but it is too strong for many purposes; for example, {{math|B(''H'')}} is not separable in this topology. 
The strong operator topology could be the most commonly used.

The ultraweak and ultrastrong topologies are better-behaved than the weak and strong operator topologies, but their definitions are more complicated, so they are usually not used unless their better properties are really needed. 
For example, the dual space of {{math|B(''H'')}} in the weak or strong operator topology is too small to have much analytic content.

The adjoint map is not continuous in the strong operator and ultrastrong topologies, while the strong* and ultrastrong* topologies are modifications so that the adjoint becomes continuous. They are not used very often.

The Arens–Mackey topology and the weak Banach space topology are relatively rarely used.

To summarize, the three essential topologies on {{math|B(''H'')}} are the norm, ultrastrong, and ultraweak topologies. 
The weak and strong operator topologies are widely used as convenient approximations to the ultraweak and ultrastrong topologies. The other topologies are relatively obscure.