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FOUNDATIONS OF QUANTUM MECHANICS

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164 CHAPTER VIII. THE MEASUREMENT PROBLEM<br />

between processes which serve as measurements and processes that do not. Every physical process<br />

or every mutual influence of physical systems can, under suitable circumstances, be considered as<br />

a measurement. Since it is the physical theory that indicates which physical processes in nature are<br />

possible, the theory itself also provides the criterion for the kinds of measurements which are possible.<br />

According to Von Neumann’s postulates, in quantum mechanics this is exactly the other way<br />

around. First we must, according to the aforementioned postulates, have a criterion to know when a<br />

process is a measurement, before we can indicate what the theory has to say concerning the process,<br />

before we can apply the postulates. That the term measurement in this way gets a more fundamental<br />

status than the physical theory, is also expressed by the words of Pauli as quoted in chapter I, p. 9,<br />

that a measurement creating values is “outside the laws of nature”.<br />

Intuition tells us that measurements are just an ‘ordinary kind’ of physical interactions, and this<br />

intuition cannot easily be wept out, from which we will give an illustration. Consider a photon which<br />

has gone through a slit and is on its way to a photographic plate. If we presume the interaction with<br />

this photographic plate to be a measurement, the wave function of the photon must, according to the<br />

projection postulate, collapse on arrival at the plate. But we also know that the photographic plate has<br />

a microscopic structure. It contains silver atoms in an emulsion which can be excited by the photon<br />

and start a chemical process in such a way that we can see something when the plate is developed.<br />

Would it not be plausible that quantum mechanics could describe such a process using a Schrödinger<br />

equation?<br />

In every way this event looks like a physical interaction which falls completely within the well -<br />

known laws of nature, instead of without. And if this is denied, how shall we decide at all when<br />

a microscopic interaction between a photon and an atom can and when it cannot be labeled as a<br />

measurement? Asking an experimental physicist how her measurement setup works, one will be<br />

given an answer in which physical interactions, generally of electromagnetic nature, are of uppermost<br />

importance. It seems absurd to deny that events take place in the laboratory that are “outside the laws<br />

of nature”.<br />

The clash between the conception that measurements do not differ from other physical interactions<br />

on the one hand, and the fact that measurements in quantum mechanics acquired a special status<br />

because they are not classified to be physical interactions on the other hand, is called the quantum<br />

mechanical measurement problem in the broad sense.<br />

VIII. 2<br />

MEASUREMENT ACCORDING TO CLASSICAL PHYSICS<br />

Although usually no special attention is given to measurements in classical physics, it is no problem<br />

to give a general, schematic description of how a measurement is treated classically.<br />

A measurement brings about a correlation between a quantity A of a physical system S which<br />

is, within the context of a measurement, frequently called an object system, and a quantity R, where<br />

the R comes from reading, which is characteristic for the measuring apparatus M, the apparatus<br />

being a physical system also. In classical physics we assume that A has a certain value a ∈ R,<br />

where a is an element from a set of possible values, for instance a 1 , . . . , a n ⊂ R, and that after the<br />

measurement process R has a value r j = m(a j ), where m is a bijection of the possible values of A<br />

before the measurement, to the possible values of R after the measurement.

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