Keeping the spin constant during an experiment?

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Discussion Overview

The discussion revolves around the challenges of maintaining a constant spin state of electrons during quantum computing experiments. Participants explore concepts related to spin measurement, decoherence, and the implications of quantum mechanics on spin states over time.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question how electrons can be kept in a definite spin state given the probability of changing spin states over time, suggesting that decoherence may be a relevant factor.
  • Others argue that the spin state should remain unchanged if the initial configuration is an eigenstate of the Hamiltonian, although this raises questions about the nature of measurement and state evolution.
  • One participant expresses uncertainty about the relationship between eigenstates, eigenvalues, and expectation values, seeking clarification on how these concepts connect to the stability of spin states.
  • Another participant emphasizes that while a definite spin is established upon measurement, it does not necessarily change immediately afterward, depending on external influences.
  • Technical details are discussed regarding the time evolution of quantum states, with a focus on how states described by a Hamiltonian evolve over time without changing their spin configuration.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement. While some agree on the stability of eigenstates under certain conditions, others challenge the implications of measurement and the effects of decoherence, indicating that the discussion remains unresolved on several points.

Contextual Notes

Participants note the complexity of the concepts involved, including the dependence on definitions of measurement and the influence of environmental factors on spin states. There are also references to specific time scales related to decoherence, highlighting the nuanced nature of the discussion.

Who May Find This Useful

This discussion may be of interest to those studying quantum mechanics, quantum computing, or anyone seeking to understand the implications of spin states and measurement in quantum systems.

nomadreid
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In texts about quantum computing, one prepares electrons or other particles in definite spins (up or down), then pass them through various gates, etc. But since the probability that an electron changes spin state within a very short time, then how can this be realistically done? Is there a way to keep the electron in a fixed state long enough? Or does one simply create a lot of particles and assume that statistically a certain percentage will be in the desired state? Am I just stating the problem called decoherence?
 
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nomadreid said:
But since the probability that an electron changes spin state within a very short time
Why should it?
Also, what is a very short time for you?

This has some relation to decoherence, but "keeps the spin orientation" is more demanding than "does not lead to decoherence"
 
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If the initial spin configuration of your system is an eigenstate of the Hamiltonian then it should remain the same.
 
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Thank you, mfb and Einj, for your replies.
First, to mfb
mfb said:
Why should it?
As I understand it, the electron has a definite spin value only upon being measured. So, after measurement, it would seem that it would have a high probability of being in some other state than upon being measured. Apart from that, the system evolves with time, doesn't it?
mfb said:
Also, what is a very short time for you?
From one point of view, right after being measured; it would of course also depend on its environment: for example, however, in terms of flipping from an indefinite state to a definite one, in the environment of a human brain, Max Tegmark comes up with a value of about 10-13 seconds.
mfb said:
This has some relation to decoherence, but "keeps the spin orientation" is more demanding than "does not lead to decoherence"
Yes, I see that now. Thank you for pointing that out.

To Einj
Einj said:
If the initial spin configuration of your system is an eigenstate of the Hamiltonian then it should remain the same.
Alas, I do not completely understand. If the eigenstate of the Hamiltonian has two eigenvalues, then supposedly each one has a non-zero expectation value, so why should it continue to be one rather than the other? I have no doubt that your answer is correct, but I am missing the connection between the premise and the conclusion. I would be grateful if you could spell it out for me.
 
nomadreid said:
As I understand it, the electron has a definite spin value only upon being measured.
No. It has to have one when it is measured, but it does not lose it afterwards (or at least not necessarily). This definite spin refers to a single axis only, and that is a key point if you want to make other measurements with it afterwards.
nomadreid said:
Apart from that, the system evolves with time, doesn't it?
So does the solar system system and we are still revolving around sun in the same direction we always did, because all influences on it are tiny.
 
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nomadreid said:
Alas, I do not completely understand. If the eigenstate of the Hamiltonian has two eigenvalues, then supposedly each one has a non-zero expectation value, so why should it continue to be one rather than the other? I have no doubt that your answer is correct, but I am missing the connection between the premise and the conclusion. I would be grateful if you could spell it out for me.

You are not considering how a state evolves with time in Quantum Mechanics. Suppose that your system is described by an Hamiltonian H and that at the initial time t=0 it is in a state ##|\psi(t=0)\rangle=|\psi_0\rangle##. Then your state for any time is given by:

$$
|\psi(t)\rangle=e^{iHt/\hbar}|\psi_0\rangle.
$$

Now, suppose that at t=0 your system is in a definite eigenstate of the Hamiltonian, say for example spin-up such that ##H|up\rangle=E_{up}|up\rangle##, where ##E_{up}## is the energy of the spin-up state. Then at any given time you'll have:
$$
|\psi(t)\rangle=e^{iHt/\hbar}|up\rangle=e^{iE_{up}t/\hbar}|up\rangle,
$$
so, you state only picks up a phase, i.e. it will remain in the spin-up configuration forever.

I hope this answers your question.
 
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Thank you again, Einj and mfb. Yes, this answers my question very satisfactorily. :)
Texts tend to skip such elementary questions, and it is super for non-experts such as myself to be able to get answers to them.
I have to try to understand the physical meaning of phase better...
 

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