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FOUNDATIONS OF QUANTUM MECHANICS

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86 CHAPTER IV. THE COPENHAGEN INTERPRETATION<br />

The meaning Bohr attaches to the uncertainty relations can be summarized this way: the sharper<br />

we can, in a phenomenon, define the position of the object, the fuzzier the momentum must be defined,<br />

and vice versa. The quantities δq and δp in the relation δqδp ∼ h therefore represent the fuzziness in<br />

the definition. Bohr emphasizes an epistemological role of these quantities stronger than an ontological<br />

role.<br />

IV. 2. 2<br />

REMARKS AND PROBLEMS<br />

Bohr’s supposition that classical language is a definite means of expression for physical observations<br />

which cannot be improved upon, is radical and at first sight even fairly unacceptable. Language<br />

develops and history teaches us that from time to time new concepts are necessary. Aristotle had,<br />

for example, no momentum concept, Newton knew nothing of energy, Coulomb had no theory of<br />

fields, etc. Doesn’t it speak for itself that quantum mechanics also asks for new concepts? Bohr,<br />

however, (ibid., p. 16), says<br />

[. . . ] it would be a misconception to believe that the difficulties of the atomic theory may<br />

be evaded by eventually replacing the concepts of classical physics by new conceptual<br />

forms.<br />

Bohr emphasizes that with this point of view he does not reject the introduction of new entities,<br />

e.g. quarks, superstrings or black holes. The aspects of classical language which are the reason<br />

that it cannot be improved upon are, according to him, descriptions in terms of space and time and<br />

descriptions in terms of cause and effect. These are the only categories with which we can describe<br />

observational results.<br />

Another problem with the idea that the classical concepts cannot be improved upon is Bohr’s<br />

immediate conclusion that the quantum of action cannot occur in the description of a phenomenon,<br />

because a statement such as ‘h = 6.6 · 10 −34 Js’ is also an unambiguous summary of experimental<br />

evidence, although not of one phenomenon. The idea that h cannot appear in the language of observations<br />

is a weak, and in fact untenable point in his argumentation. The prohibition of the use of h<br />

in the language of observations also brought Bohr to the conclusion that the spin of an electron, 1 2 ,<br />

would be fundamentally unobservable. This conclusion has been proven to be incorrect.<br />

In some articles Bohr gives a more abstract explanation of the quantum postulate and emphasizes<br />

the ‘symbolic’ role of h. It does not so much represent the inevitable interaction, or measurement<br />

disturbance, between object and measuring apparatus, as the fundamental impossibility to make a<br />

sharp distinction between object and observation apparatus. It is, in any case, clear that Bohr does not<br />

regard the formalism of quantum mechanics, with its wave functions and operators, as an extension<br />

or improvement of classical language. He emphasizes that this formalism is purely symbolic and<br />

cannot be taken as a description, as the quantum state of a system is given without reference to the<br />

experimental setup.<br />

It should be noted that Bohr, at emphasizing the applicability of concepts, has more in mind than<br />

the ‘logical’ question of ’definiteness’. For Bohr a term like ‘position of a particle’ is applicable if we<br />

can in fact control and secure this position, using firmly bolted apparatuses. Bohr’s use of the term<br />

‘determination’ refers both to a measurement as to a state preparation.

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