2
$\begingroup$

Dirac writes in page number 4 of his "Principles of Quantum Mechanics":

It is usually assumed that, by being careful, we may cut down the disturbance accompanying our observation to any desired extent. The concepts of big and small are then purely relative and refer to the gentleness of our means of observation as well as to the object being described. In order to give an absolute meaning to size, such as is required for any theory of the ultimate structure of matter, we have to assume that there is a limit to the fineness of our powers of observation and the smallness of the accompanying disturbance-a limit which is inherent in the nature of things and can never be surpassed by improved technique or increased skill on the part of the observer. If the object under observation is such that the unavoidable limiting disturbance is negligible, then the object is big in the absolute sense and we may apply classical mechanics to it. If, on the other hand, the limiting disturbance is not negligible, then the object is small in the absolute sense and we require a new theory for dealing with it.

A consequence of the preceding discussion is that we must revise our ideas of causality. Causality applies only to a system which is left undisturbed. If a system is small, we cannot observe it without producing a serious disturbance and hence we cannot expect to find any causal connexion between the results of our observations. Causality will still be assumed to apply to undisturbed systems and the equations which will be set up to describe an undisturbed system will be differential equations expressing a causal connexion between conditions at one time and conditions at a later time. These equations will be in close correspondence with the equations of classical mechanics, but they will be connected only indirectly with the results of observations. There is an unavoidable indeterminacy in the calculation of observational results, the theory enabling us to calculate in general only the probability of our obtaining a particular result when we make an observation.

I want to make sure that I correctly understand this:

What we have are two observations and those observations do not seem to be causally related (meaning in an identically prepared system we are not guaranteed to have the same observations and therefore we cannot set up a deterministic mathematical equation for the system).

In such a context we assume that the system evolves determinsistically after an observation and it is only due to the indeterminacy introduced by the next observation that our result of the observation can no longer be predicted with accuracy.

Questions:

1) How does this line of reasoning explain that consecutive measurements give the same result? And that the measured value will only be one of the eigenvalue of the operation? It seems to me that the indeterminacy is not in any way similar to the disturbance inherent in measuring "fragile" or "sensitive" properties of classical systems as those disturbances are totally random.

2) Is it possible to set up a mathematical framework for quantum mechanics that does not make this assumption. (For example, the new framework may postulate that a system non-deterministically takes many paths of evolution but it is only on subsequent observation that it settles on one particular value.)

3) Does this line of thought by Dirac ascribe to any of the interpretations of quantum mechanics (Copenhagen, Many-World, Bohmian, etc.)? Does it go against any of the interpretations?

$\endgroup$
2
  • $\begingroup$ It still seems that the cited passage cannot furnish the answers to your questions. It's strictly introductory, and to properly frame the questions you would have to quote from specific material from other places in Dirac's work. In other words, the cited material is not intended to answer any of the questions it raises. $\endgroup$
    – daniel
    Jun 17, 2017 at 11:07
  • $\begingroup$ Hmmm. Well, I was wondering if someone else could work it out and let me know because now that my introductory course to quantum mechanics is over and other things have started I am not that prepared to read the complete book. $\endgroup$ Jun 17, 2017 at 11:49

1 Answer 1

3
$\begingroup$

The passage leading up to this quote (p.3) explains it in a non-technical but convincing way. He says (am paraphrasing), there is a limit to the fineness of our powers of observation. When we are dealing with large objects we can observe them with relatively minimal disruption. As objects or systems become smaller, our inevitable disruption in the process of measurement becomes relatively large.

There is a point beyond which we cannot assume that what we are observing is not the result of our own disruption. We are not then free to say, "X caused Y," since we cannot rule out that Y was the result of our intrusion into a microscopic system.

This passage is in the introductory part of his text, so it is just meant to give a non-technical flavor of issues that are covered in a technically more satisfying way later on.

I should add that I don't think it is possible to answer the questions this passage raises, or judge the validity of his assertions, until one has finished Dirac's book and then examined the preliminary remarks in light of the technical explanation.

$\endgroup$
1
  • $\begingroup$ Plus one. I was good-to-go with your answer but then I realized: how does this argument explain that consecutive measurements give the same result? And that the measured value will only be one of the eigenvalue of the operation? So, I edited the question and expanded it a bit. $\endgroup$ Jun 17, 2017 at 8:50

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service, privacy policy and cookie policy

Not the answer you're looking for? Browse other questions tagged or ask your own question.