Quantum Field Theory (QFT) is one of the most powerful tools invented by physicists in the last 50 years. It provides, in essence, a way to think of - and, in many cases, to calculate properties of - interacting and or disordered physical systems in the "low-energy" regimes which are the most useful for experiments and practical applications.
The success of quantum field theory in particle physics has been well publicized in particular thanks to the successful CERN experiments that confirmed the existence of the Higgs boson. Quantum field theory is however also widely used in condensed matter or statistical physics. In this case, it can often happen that the formalism, well developed in the context of particle physics, has to be extended beyond a certain comfort zone. In particular, phase transitions occurring in a variety of disordered non-interacting electronic systems such as integer quantum Hall devices can only be tackled using quantum field theories that are not unitary. This technical term means that, after properly taking into account the disorder, one ends up having to deal with some formal processes for which probabilities are, in fact, negative! However unpleasant, the study of these processes still seems the best way to make progress on fundamental questions of current interest. Chief among these are the properties of the localization/delocalization transitions in topological insulators, which offer a wealth of potential technological applications via, in particular, the prospects of quantum computation.
The goal of this project was to build the technical apparatus necessary to handle complications arising from the loss of unitarity, and apply this apparatus to a better understanding of several types of physical systems, including the aforementioned phase transitions.
At the end of the project, a great deal has indeed being accomplished. The serious technical difficulties arising from non-unitarity in 1+1 conformal field theory have been surmounted, thanks to the development of new analytical and numerical techniques, and a systematic use of lattice regularizations combined with algebraic considerations. Some of the results obtained have deep mathematical consequences, but the rest of the project has been devoted rather to investigate applications to problems of physical interest. Another set of difficulties related with the non-compactness of the relevant field theories has been tackled in this context, and many aspects of the plateau transitions in classes A and C of quantum Hall effect have been elucidated. More results are expected in the near future.