Please login to be able to save your searches and receive alerts for new content matching your search criteria.
The canonical quantization of midisuperspace gravitational models is a particular case of the quantization of fields. Typically, the requirement of symmetries other than homogeneity reduces the phase space of full General Relativity, but still leaves an infinite number of degrees of freedom, encoded in some fields which parametrize the metric components and are subject to constraints. Since the total Hamiltonian vanishes, and constraints are all that there is left, a peculiar situation occurs in the quantization of these models. On the one hand, it is tempting to solve at the classical level as many constraints as possible, e.g. by gauge fixing or other means. On the other hand, if all the constraints were to be solved, one would be left just with the infinite dimensional reduced phase space of the model, and no extra structure to guide us through the quantization process.
The following sections are included: