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popper-logic-scientific-discovery

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appendix *xi 473<br />

left. This will (according to Bohm) overthrow the balance of forces<br />

which keep the particle at rest; and the particle will start moving—<br />

presumably from left to right. But although we triggered only the left<br />

particle, the right particle will have to start simultaneously, and in the<br />

opposite direction. It is asking much of a physicist to acquiesce in the<br />

possibility of all these processes—all assumed ad hoc, in order to avoid<br />

the consequences of the argument of Pauli and Einstein.<br />

Einstein might have answered Bohm as follows, I think.<br />

In the case considered, our physical system was a big macroscopic<br />

ball. No reason has been given why in such a case the usual classical<br />

view of measurement should be inapplicable. And this is a view that<br />

conforms, after all, as well with experience as one can desire.<br />

But leaving measurement aside, is it seriously asserted that an oscillating<br />

ball (or two oscillating balls in a symmetric arrangement here<br />

described) simply cannot exist while unobserved? Or, what amounts to<br />

the same, is it seriously asserted that the assumption that it does move,<br />

or oscillate, while unobserved, must lead to the conclusion that it does<br />

not? And what happens if, once our observation has set the ball in<br />

motion, it is then no longer asymmetrically interfered with so that the<br />

system again becomes stationary? Does the particle then stop as suddenly<br />

as it started? And is its energy transformed into field energy? Or<br />

is the process irreversible?<br />

Even assuming that all these questions may be answered somehow,<br />

they illustrate, I think, the significance of Pauli’s and of Einstein’s criticism,<br />

and of the critical use of imaginary experiments, especially the<br />

experiment of Einstein, Podolsky, and Rosen. And I think that they also<br />

illustrate the danger of an apologetic use of imaginary experiments.<br />

(9) So far I have discussed the problem of pairs of particles, introduced<br />

into the discussion by Einstein, Podolsky, and Rosen. I now turn to<br />

some of the older imaginary experiments with single particles, such as<br />

Heisenberg’s famous imaginary microscope through which one could<br />

‘observe’ electrons, and ‘measure’ either their positions or their<br />

momenta. Few imaginary experiments have exerted a greater influence<br />

on thought about physics than this one.<br />

With the help of his imaginary experiment, Heisenberg tried to<br />

establish various points of which I may mention three: (a) the interpretation<br />

of the Heisenberg indeterminacy formulae as stating the existence

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