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popper-logic-scientific-discovery

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some observations on quantum theory 235<br />

hypothesis. For the statement (which corresponds to Heisenberg’s view)<br />

that exact single predictions are impossible, turns out to be equivalent<br />

to the hypothesis that predictive measurements and physical selections are inseparably<br />

linked. With this new theoretical system—the conjunction of the<br />

quantum theory with this auxiliary ‘hypothesis of linkage’—my conception<br />

must indeed clash. 1<br />

With this, point (3) of my programme has been carried out. But<br />

point (4) has still to be established; that is, we have still to show that<br />

the system which combines the statistically interpreted quantum theory<br />

(including, we assume, the conservation laws for momentum and<br />

energy) with the ‘hypothesis of linkage’, is self-contradictory. There is,<br />

I suppose, a deep-seated presumption that predictive measurement and<br />

physical selection are always linked. The prevalence of this presumption<br />

may explain why the simple arguments which would establish the<br />

opposite have never been worked out.<br />

I wish to stress that the mainly physical considerations now to be<br />

presented do not form part of the assumptions or premises of my<br />

<strong>logic</strong>al analysis of the uncertainty relations although they might be<br />

described as its fruit. In fact, the analysis so far carried out is quite<br />

independent of what follows; especially of the imaginary physical experiment<br />

described below,* 2 which is intended to establish the possibility<br />

of arbitrarily precise predictions of the path of single particles.<br />

By way of introduction to this imaginary experiment I will first<br />

discuss a few simpler experiments. These are intended to show that we<br />

can without difficulty make arbitrarily precise path predictions, and<br />

also test them. At this stage I only consider predictions which do not<br />

refer to definite single particles, but refer to (all) particles within a<br />

definite small space-time region (∆x.∆y.∆z.∆t). In each case there is<br />

only a certain probability that particles are present in that region.<br />

We again imagine a beam (an electron or light beam) of particles<br />

1 The auxiliary hypothesis here discussed can of course appear in a different form. My<br />

reason for choosing this particular form for critical analysis and discussion is that the<br />

objection which asserts the linkage of measurement and physical selection was actually<br />

(in conversations as well as in letters) raised against the view here advanced.<br />

* 2 Those of my critics who rightly rejected the idea of this imaginary experiment appear<br />

to have believed that they had thereby also refuted the preceding analysis, in spite of the<br />

warning here given.

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