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470<br />

new appendices<br />

based upon his famous formula E = mc 2 , Bohr had recourse to arguments<br />

from Einstein’s gravitational theory (that is to say, from general<br />

relativity). 10 But E = mc 2 can be derived from special relativity, and even<br />

from non-relativistic arguments. In any case, in assuming E = mc 2 , we<br />

certainly do not assume the validity of Einstein’s theory of gravitation.<br />

If, therefore, as Bohr suggests, we must assume certain characteristic<br />

formulae of Einstein’s gravitational theory in order to rescue the consistency<br />

of quantum theory (in the presence of E = mc 2 ), then this<br />

amounts, I hold, to the strange assertion that quantum theory contradicts<br />

Newton’s gravitational theory, and further to the still stranger<br />

assertion that the validity of Einstein’s gravitational theory (or at least<br />

the characteristic formulae used, which are part of the theory of the<br />

gravitational field) can be derived from quantum theory. I do not think<br />

that even those who are prepared to accept this result will be happy<br />

about it.<br />

Thus we have again an imaginary experiment which makes<br />

extravagant assumptions, with an apologetic purpose.<br />

(7) David Bohm’s reply to the experiment of Einstein, Podolsky,<br />

and Rosen seems to me also highly unsatisfactory. 11 He believes that he<br />

has to show that Einstein’s particle A which has run far away from B<br />

and from the measuring apparatus does nevertheless become smeared<br />

in its position (or momentum) when the momentum (or position) of<br />

B is measured, and he tries, to this end, to show that A, in spite of<br />

having run away, is still interfered with in an unpredictable way. In this<br />

way he tries to show that his own theory agrees with Heisenberg’s<br />

interpretation of the indeterminacy relations. But he does not succeed.<br />

This becomes manifest if we consider that the ideas of Einstein,<br />

Podolsky, and Rosen allow us, by a slight extension of their experiment,<br />

to determine simultaneously positions and momenta of both A<br />

and B—although the result of this determination will have predictive<br />

10 Bohr, in Albert Einstein: Philosopher-Scientist, ed. by P. A. Schilpp; the case is discussed on<br />

pp. 225–228. Dr. J. Agassi has drawn my attention to the invalidity of the argument.<br />

*We must remember that the ‘equivalence’ m i = m g is part of Newton’s theory.<br />

11 See D. Bohm, Phys. Rev. 85, 1952, pp. 166 ff., 180 ff; see especially pp. 186 f. (I understand<br />

that Bohm does not any longer uphold some of the views expressed in the papers<br />

here criticized. But it seems to me that at least part of my argument may still be applicable<br />

to his later theories.)

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