19 - The extended objects of string theory

Summary

After the general introduction to extended objects of the preceding chapter, in this one we are going to study specifically the extended objects that appear in string theory. The existence of these objects is implied by our previous knowledge of existing objects (strings and D_p-branes) combined with duality. This path will be followed in Section 19.1, in which we will arrive at the diagrams in Figures 19.4.1 and 19.4.1 that represent, respectively, more- and less-conventional extended string/M-theory objects and their duality relations. The duality relations can be used to find the masses of all these objects compactified on tori (Tables 19.1–19.3) using as input the mass of a string wound once on a circle (i.e. the mass of a winding mode). To obtain consistent results (in particular for electric–magnetic dual branes to coexist satisfying the Dirac quantization condition), the ten-dimensional Newton constant has to have a specific value in terms of the string coupling constant and the string length that we will determine.

The next step (Section 19.2) will be to identify which are, among the general solutions of the p-brane a-model, those that represent the long-range fields of the basic extended objects of string and M theory that we found before. We will first identify families of solutions and then we will study one by one the most important solutions. In Section 19.3 we will check the values of the integration constants of those solutions against the masses and charges of the extended objects that we determined using duality arguments. Then, the duality relations between the solutions will be checked in Section 19.4.