1/1 1.3 D-branes
We saw that string theory has two expansion parameters:lₛ(or rather the dimension-less lₛ/r,with r a curvature radius),and eф,which when constant is also called gₛ.
In(1.1.21),we wrote the expansion as a power series,but we wondered whether this
really captures the whole dependence.Recall that a function is called (real) analytic
if it coincides with its Taylor series around every point. A famous nonanalytic
function is
f(g)=e⁻¹/g². (1.3.1)
Both f and all its derivatives vanish at g=0,so its Taylor series vanishes identically,but f(g) ≠ 0. In physics,we call an effect with such a dependence on the coupling nonperturbαtiνe.In attempts at describing nonperturbative aspects of field theory,
two types of objects often come up:solitons, which are large and stable field
configurations,localized in space;and instantons,which occur in the Euclidean path
integral and are localized in time as well. In string theory,the most prominent objects
that play these roles are D-brαnes;this section is devoted to them.
1.3.1 Solitons and instantons
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