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[^11]: A hundred years later, after the discovery of quantum mechanics, the following sentence was written: “In the light of modern quantum mechanics this would be an obvious statement, but it is nonetheless, one which requires some explanation” [@bell].
[^12]: We are very grateful to a reviewer of ref. [@Cocciaro] for this remark.
[^13]: The case of a measurement of the quantum state of the system is quite different. In fact, the measurement has two effects: it disturbs the system, consequently it “erases” the [*cognitive*]{} information about the state, and it modifies the state in such a way that it is no more a quantum state but an observable in the new Hilbert space defined by the measurement.
[^14]: In this sense, the process of measurement is a kind of “measurement of the measurement”.
[^15]: Although in the general case the appearance of probabilities $p_n$ is not a trivial issue (see, e.g. [@Redhead; @vonNeumann]), in the case of spin operators, which are hermitian operators, can be normalized and the $p_n$ are just their eigenvalues. Then, the probability is just the square of the eigenvalue, which can be written as $p_n=|u_n|^2$.
[^16]: Einstein was also interested in the role of the observer in the measurement problem: “If the apparatus is in a definite state, the result of a measurement can be observed only by the person who performs the measurement. It is therefore possible to speak of the [*observer’s*]{} state and [*the state of the apparatus at the moment of the measurement*]{}. Clearly, the observer’s state is a mixture of two states, the state of the apparatus and an observer’s state” [@einstein].
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