I would definitely recommend working your way through Dirac's 'The Principles of Quantum Mechanics'.
I had taken two or three courses on quantum theory a while ago and have read many books on the subject over the years, but I always had the impression that there was a kind of arbitrariness or lack of justification to some of the 'postulates' and a kind of 'magic' related to the applications of those postulates. Yes they give answers that agree with experiments, but what are the founding principles? Where do they come from?
Some examples:
- Why is the wave function complex?
- Where does $[\hat{q},\hat{p}]=i\hbar \hat{I}$ come from?
- What is the difference between the Schrodinger, momentum and Heisenberg representations. What is a representation for that matter and why use them?
- Can you derive Born's rule?
- Where does Dirac's delta function come from?
etc. etc. Hundreds of questions like this...
So I worked through Dirac's book line by line.
And the book really is a work of genius. With very few assumptions (starting with the Principle of Superposition), Dirac builds up an entire architecture for quantum mechanics in a way that is understandable and generalizable.
Yes, it's a slower read than Griffiths, Shankar, Levi, Binney et al. or Cohen-Tannoudji et. al (which are all superb). And of course there are no modern experiments described. But it will provide you with an extremely strong theoretical foundation with which you can try to understand quantum theory without getting completely bogged down in the mathematics. (Mathematicians might enjoy the less readable but perhaps more pedagogical 'Mathematical Foundations of Quantum Mechanics' by von Neumann).
There is no bibliography. None. Because everything is derived from a few assumptions. It is completely self-sufficient as a text.
And of course in his Nobel lecture ("The Development of the Space-Time View of Quantum Electrodynamics", Nobel Lecture, December 11, 1965), Richard Feynman credited Dirac's book. He said it inspired him to strive to develop new descriptions of the world which lead to his version of Quantum Field Theory.
[The answers to the above are all in the book! Very very briefly: 1) This follows from the Principle of Superposition; 2) From the assumptions that two observables $u$ and $v$ in quantum theory have a commutator related the classical Poisson bracket and that observables need to have real values (so need to be represented by self-adjoint operators); 3) A representation is just a way of describing abstract quantities like vectors, operators etc. in a simple way via a set of numbers (like coordinates relative to basis vectors in geometry). The Schrodinger representation is a description that focuses on position co-ordinates where states are time dependent, whereas in the Heisenberg representation states are stationary; 4) Yes. Dirac tells probabilities can be viewed as expectations of an indicator function(!); 5) It arises naturally when we describe orthogonal states in the case where observables can be continuous.]
So I would strongly recommend that anyone interested in Quantum Theory reads it. Even if it takes a while.