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It is time to face the elephant in the room. Beautiful though they are, the gauge bosons of the weak interactions are massless and cannot be the mediators of the weak interactions. They do not reproduce Fermi’s interaction at low energy. They make the weak interactions long range while they are most definitely not.
We summarize some basics on quantum mechanics and relativity theory as needed in order to understand the physical content and context of the theory of causal fermion systems.
Strong interactions are, well, strong. You have hadrons interacting and breaking up into a huge number of other hadrons. It is hard to understand what is going on. Physicists stumbled along during the 1960s trying out many ideas (the key words here are current algebra, analytic S-matrix, Regge trajectories and string theory) without much real understanding.
Surface layer integrals are introduced as an adaptation of surface integrals to causal fermion systems and causal variational principles. Conservation laws are derived and formulated in terms of surface layer integrals.
The Lagrangian for the charge and neutral currents of the Standard Model contains fermion fields, what we call matter – leptons and quarks – and their interaction with spin-1 fields. These spin-1 fields are the W-, Z- and γ-bosons. As will become clear as I proceed, these fields are at the very center of the definition of the Standard Model as a gauge theory.
“Marvelous is the working of our world!” N. Gogol, Nevsky Prospect, 1835 Should this have been the first chapter? Where to start from in teaching the Standard Model? The data painfully collected by experiments are the basis of everything – but they would be mute were it not for our models and theories. On the other hand, it seems that our brain is not very good at working all by itself. It needs the gentle prodding of experimental data, of finding out how (real) things are. Without external inputs, our mind is easily led astray, going round in circles (often of narrower and narrower radius).
Fourier methods for the analysis are developed and used for the analysis of the kernel of Green’s operators, the causal fundamental solution and the kernel of the fermionic projector.