FOUNDATIONS OF QUANTUM MECHANICS
FOUNDATIONS OF QUANTUM MECHANICS
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.