In this paper I address the most common objections to the claim that Schrodinger was right in 1926: the wavefunction provides the correct, and complete, description of atomic phenomena. I suggest that the line of droplets in the Wilson cloud chamber, the click of the photon detector", and that dot on the screen" can all be explained within a context of wavefunction models and Schrodinger’s-type equations, albeit nonlinear. No auxiliary hypotheses about point particles or probabilities are required. The random locations of the triggered particle detectors" can be explained by chaos" (meaning sensitive dependence on initial conditions). Even Born’s ad hoc invocation of probabilities may be justifiable in certain circumstances. As an illustration, I present simulations from a (toy) wavefunction ``particle-detectors" model.

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