physics, mathematical physics, philosophy of physics
theory (physics), model (physics)
experiment, measurement, computable physics
Axiomatizations
Tools
Structural phenomena
Types of quantum field thories
The SVG figures are still not displaying completely properly. The text labels seem to be almost all left aligned, while some of them should be right or center aligned. In particular, the (?) in the last figure should be centered. –Igor
These aim of these notes is to summarize the various mathematical structures and constructions employed in physics to build models of classical and quantum field theories. To avoid the (yet non-existent) rigorous construction of non-linear (interacting) field theories, non-linearities are treated as formal perturbations. Theories with gauge invariance (first class constraints) are treated within the BV-BRST formalism.
There are multiple operations on classical and quantum field theories that produce new ones. I roughly classify them into three kinds. These terms are not meant to be rigorously defined or taken literally. They mostly reflect how these operations are viewed in the physics literature.
The relevant examples that will appear in these notes are the following. A solid arrow represents a reduction, while a dashed arrow represents the inverse deformation or resolution, in the senses described above.
The transition to the classical limit corresponds to taking the limit $\hbar\to0$, which is a parameter explicitly appearing in all physically relevant quantum systems. The inverse operation is quantization, which corresponds to the mathematical field technically called deformation quantization.
Explicit solutions or other kinds of information is readily available for linear field theories. Thus, often, the first step to understanding a non-linear field theory is to consider its linearization. The inverse operation of deforming the linear theory with a non-linear perturbation is often very difficult and thus considered in the physics literature mostly at the level of formal power series in the perturbation parameter.
Many physical theories are difficult to describe without introducing extra/non-physical/redundant so-called gauge degrees of freedom and at the same time so-called gauge symmetry acting on them. However, given such a description, the physical theory must be recovered from the quotient by gauge transformations. The description involving gauge degrees of freedom is highly non-unique, but a particularly convenient (though still not unique) one is provided by the BV-BRST resolution.
The operations described above can be used as the axes of a three-dimensional space, inhabited by what can be called the resolution-deformation-reduction cube of quantization. Note that gauge fixing can be considered as one of the (non-uniquely defined) steps of the BV-BRST construction.
One corner of the cube corresponds to some classical, non-linear, physical theory. The goal of quantization is to jump to the corner with the quantum version of this theory. This is difficult to do directly because of the non-linearity and when gauge degrees of freedom are present. The usual procedure is then to construct the remaining auxiliary vertices of the cube and to take the indirect path, indicated in pale blue. The meaning of the solid and dashed lines is the same as above.