Well, from the phys.org article I don't even see what's a breakthrough here, because that what I learned in my quantum-theory-1 lecture, when we started with the usual heuristics of the formulation of non-relativistic QT as "wave mechanics" a la Schrödinger. The uncertainty relation between position and momentum is very natural since the wave function in momentum representation is the Fourier transform of the wave function in position representation and of course vice versa since the inverse of the Fourier transformation is a Fourier transformation (with a simple sign change in the exponential) too. Now it's easy to prove that the width of a wave packet in position representation is (at least qualitatively) proportional to the inverse width in momentum representation and vice versa. So "wave-particle duality" and the position-momentum uncertainty are very naturally connected in the wave-mechanics representation of quantum theory.
Now, fortunately our professor had thought much more carefully about the foundations of QT, and very soon he told us that there is no wave-particle duality but just quantum kinematics and dynamics + the Born rule, i.e., the probabilistic meaning of the quantum theory. Also the connection to information theory (with the von-Neumann-Shannon-Jaynes entropy as a measure for missing information, given a probability distribution, which turns out to be the same as thermodynamic entropy). So there is no surprise for me here, but of course, I've to read the original paper first to get a more qualified opinion.
Another question is, how "complicated" quantum theory is. This is a very subjective question of course. As a student, I had the feeling that quantum mechanics 1 (non-relativistic quantum theory) is "less complicated" than classical electromagnetism, as far as the formalism and the math is involved. It's much simpler a task to solve the Schrödinger equation or manipulate Hilbert-space vectors in terms of "bras and kets" and "operators" than to solve a complicated charge-current-field problem with boundary conditions and what not in classical electromagnetism.
On the other hand, quantum theory is "more complicated" than any classical physics, because the latter usually describes directly observables in a deterministic way. There may be auxiliary quantities for convenience and elegance of calculation (like the scalar and vector potentials in electromagnetism, which are not observable but used to derive the observable electromagnetic field finally), but in principle everything in the formalism is pretty easily mapped to what's measured in the lab.
That's not so easy in QT, as we all know from all our lively discussions on interpretation in this forum and the sometimes seemingly pretty bizarre implications of entanglement (possibility of postselection as in the quantum-eraser experiment, the strong correlations of totally indetermined quantities as the polarizations of polarization entangled photons in this and the quantum-teleportation experiment, or (for me the most fascinating example) the possibility to separate properties of the same particle at separate locations as in the Chesire-cat experiment with neutrons). Usually, after reading the papers of such experiments, I can pretty easily follow the formal analysis of these experiments with pretty simple calculations in quantum theory, but the phenomena as such are not so easy to comprehend intuitively. The reason is of course, that in our everyday experience we deal with macroscopic objects in interaction with the environment, so that coherence and entanglement are "washed out" or "course grained" by our quite unprecise persception of the objects around us.