In mathematics, in the field of potential theory, the fine topology is a natural topology for setting the study of subharmonic functions. In the earliest studies of subharmonic functions, namely those for which
\Deltau\ge0,
\Delta
\Rn
The fine topology was introduced in 1940 by Henri Cartan to aid in the study of thin sets and was initially considered to be somewhat pathological due to the absence of a number of properties such as local compactness which are so frequently useful in analysis. Subsequent work has shown that the lack of such properties is to a certain extent compensated for by the presence of other slightly less strong properties such as the quasi-Lindelöf property.
In one dimension, that is, on the real line, the fine topology coincides with the usual topology since in that case the subharmonic functions are precisely the convex functions which are already continuous in the usual (Euclidean) topology. Thus, the fine topology is of most interest in
\Rn
n\geq2
Cartan observed in correspondence with Marcel Brelot that it is equally possible to develop the theory of the fine topology by using the concept of 'thinness'. In this development, a set
U
\zeta
v
\zeta
v(\zeta)>\limsupz\to\zeta,v(z).
Then, a set
U
\zeta
U
\zeta
The fine topology is in some ways much less tractable than the usual topology in euclidean space, as is evidenced by the following (taking
n\ge2
F
\Rn
F
\Rn
\Rn
The fine topology does at least have a few 'nicer' properties:
\Rn
The fine topology does not possess the Lindelöf property but it does have the slightly weaker quasi-Lindelöf property:
\Rn