I'd however qualify that "Old Quantum Theory" is not really there anyore, and that's good. You can learn about it in a history-of-science study, which I strongly recommend to any serious student of physics since to fully understand the modern point of view of physics, particularly the development of the modern quite abstract quantum theory, it is very important to learn about how this modern view has developed from less comprehensive views, but it's not helpful for introducing you to modern physics. The same holds for what's called "Relativistic Quantum Mechanics", which is very cumbersome and problematic to understand, because it's "unnatural" to use it for relativistic particles to begin with. The reason is that "Relativistic Quantum Mechanics", which was the try to build a relativistic quantum theory in analogy to Schrödinger's wave mechanics, which deals with a fixed number of particles ("1st quantization formalism"). This works well in non-relativistic physics, but the very point of relativistic particle physics is that particle numbers are no longer conserved, i.e., given enough energy in collisions (which is what's particularly meant by high-energy/relativistic particle physics) you can always destroy particles and produce new ones, and this is most conveniently described by quantum field theory ("2nd quantiation"). In fact it was Jordan who has seen this early on already in 1926, when he insisted that also the electromagnetic field should be "quantized", i.e., made to "non-commuting matrices" in the matrix-mechanics representation of quantum theory developed by him together with Born, building on Heisenberg's heuristic Helgoland paper and then being finally formulated by Born, Jordan, and Heisenberg in the famous "Dreimännerarbeit" (Three-Men Paper, literally translated). At this time this idea was not appreciated by many other quantum physicists, perhaps mainly because of the unfamiliar matrix formalism and the difficulty to express continuous phenomena like scattering within this formalism. That's why many physicists preferred Schrödinger's wave mechanics, for which the scattering phenomena were a quite familiar thing, known from the scattering of light via classical Maxwell electromagnetics. That's why usually Dirac's work of 1928 on quantization of the radiation field is taken as the birth of quantum field theory rather than Jordan's pioneer work within matrix mechanics.