How can we know initial state of a particle

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Discussion Overview

The discussion centers around the challenge of determining the initial state of a particle in quantum mechanics, particularly in the context of preparing a system for experimentation and the implications of measurements on the initial wave function, ψ(x,0). The scope includes theoretical considerations, measurement techniques, and the limitations of initial state preparation in quantum experiments.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants describe the standard procedure for solving the Schrödinger equation, which involves obtaining stationary state solutions and combining them based on the initial state, ψ(x,0).
  • Others suggest that the initial state can be prepared through measurements, asserting that the postulates of quantum mechanics ensure knowledge of the state post-measurement.
  • One participant questions whether the state can be fully known after measurement, highlighting the limitations of measurement accuracy and the ambiguity of the wave function within a detected range.
  • Another participant acknowledges that while exact knowledge of the state post-measurement is not achievable, theoretical calculations often assume the system is in an exact eigenstate for practical purposes.
  • Some participants reference advanced texts, such as Ballentine's QM book, as providing deeper insights into these issues, while cautioning against getting sidetracked by such complexities at an introductory level.

Areas of Agreement / Disagreement

Participants express differing views on the completeness of knowledge regarding the initial state after measurement, with some asserting that it can be known to a good approximation, while others emphasize the inherent uncertainties and ambiguities involved. The discussion remains unresolved regarding the implications of these uncertainties on practical calculations.

Contextual Notes

Limitations include the dependence on measurement accuracy and the unresolved nature of how to specify the wave function within the detected range after measurement. The discussion also reflects varying levels of comfort with the complexities of quantum mechanics as presented in different texts.

bob900
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In textbooks (such as Griffiths, for example), the general method for a solution to the Shrodinger's equation for a single particle, for some V(x), is given as : 1. Get the stationary state solutions 2. Combine them into a linear combination and figure out the coefficients from the known initial state at time 0, ψ(x,0).

But it never states how exactly do we know this initial ψ(x,0) in the first place? If we are conducting an experiment with the particle, how do we prepare it to be in exactly the right initial state?
 
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If you can get ahold of Ballentine's QM book, Ch. 8 explains this well.
 
capandbells said:
If you can get ahold of Ballentine's QM book, Ch. 8 explains this well.

Yes. As well it develops QM in a much more logical way. The only issue is it is a graduate level book. It would be quite reasonable to just accept at the level of Griffiths there are a few issues that get resolved in more advanced treatments and wait until you study them.

I was concerned about such things when I first studied QM from books like Griffiths many moons ago. I took long detours sorting them out and while I learned a lot and managed to resolve the issues, I now think it was probably better simply to wait until I was ready for the more advanced texts.

Thanks
Bil
 
Last edited:
Preparations are measurements. A typical QM experiment goes like this:

1) you have an unknown initial state
2) you prepare it by a measurement (the postulates of QM guarantee you that you know the state afterwards)
3) you let your system evolve in time
4) you do your measurement of interest
 
kith said:
Preparations are measurements. A typical QM experiment goes like this:

1) you have an unknown initial state
2) you prepare it by a measurement (the postulates of QM guarantee you that you know the state afterwards)
3) you let your system evolve in time
4) you do your measurement of interest

But do you really know the state fully after step 2? Let's say you have a detector that measures the position of a particle (in one dimension). Any detector has some finite accuracy, so the result of the measurement only tells you that the particle was found in some (very small) range [x1,x2]. In other words, you know that

ψ(x,0) = 0 | x outside of [x1,x2]

but ψ(x,0) is still completely unspecified inside [x1,x2]. There are infinitely many ways to specify it inside there. Which one do you use for your calculations thereafter?
 
bob900 said:
But do you really know the state fully after step 2?

No practical measurement will allow you to know the state after the measurement exactly - but to good approximation for most if not all theoretical calculations assuming it is in an exact eigenstate is good enough. It's the principle that counts - namely conceptually it is possible.

There are other ways of determining the initial state as well such as what is called filtering - see the Chapter 8 mentioned previously. But my advice is not to worry about it for now - getting sidetracked on this sort of stuff can be time consuming and counterproductive to the aims of a book at the level of Griffiths.

Thanks
Bill
 

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