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popper-logic-scientific-discovery

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484<br />

new appendices<br />

statistical description of an aggregate of systems, rather than a description<br />

of one single system. But first of all, he ought to say so clearly; and<br />

secondly, I do not believe that we shall have to be satisfied for ever with<br />

so loose and flimsy a description of nature.<br />

It should be noticed that some of the precise predictions which I can<br />

obtain for the system B (according to the freely chosen way of measuring<br />

A) may well be related to each other in the same way as are<br />

measurements of momentum and of position. One can therefore<br />

hardly avoid the conclusion that the system B has indeed a definite<br />

momentum and a definite position co-ordinate. For if, upon freely<br />

choosing to do so [that is, without interfering with it], I am able to<br />

predict something, then this something must exist in reality.<br />

A [method of] description which, like the one now in use, is<br />

statistical in principle, can only be a passing phase, in my opinion.<br />

I wish to say again* that I do not believe that you are right in your<br />

thesis that it is impossible to derive statistical conclusions from a<br />

deterministic theory. Only think of classical statistical mechanics (gas<br />

theory, or the theory of Brownian movement). Example: a material<br />

point moves with constant velocity in a closed circle; I can calculate the<br />

probability of finding it at a given time within a given part of the<br />

periphery. What is essential is merely this: that I do not know the initial<br />

state, or that I do not know it precisely!<br />

* This is an allusion to a previous letter. K. R. P.<br />

With kind regards,<br />

Yours,<br />

A. Einstein.

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