there are problems with the fundamental assumptions you are making in your question when you mention the QFT approach. You say: "because of the conservation laws,on average the number of particles remains constant" but this statement is actually incorrect. Consider the decay of the neutron by electroweak process: $$n \rightarrow p \, + e^-\, +\, \overline{\nu}_e$$ the "number of particles" before and after is clearly not conserved. As a matter of fact, the conservation of particles was historically one of the flaws of the early version of Quantum Mechanics: in Schrodinger equation, the probability associated to the wave function is conserved , i.e. the famous "probability current conservation" identity, which means that a particle basically can't transform into another, because that would mean its probability would go from non-zero (before) to zero (after). In the above equation, the probability to have a neutron before and after the weak interaction process is clearly not identical. QFT of course solves all this issues through the formalism of creation/destruction operators. It was not, as you certainly know, the only problem of Schrodinger equations, but just one out of many.