What happens to an electron's quantum state after measurement?

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Discussion Overview

The discussion centers on the implications of measurement on an electron's quantum state, particularly focusing on quantum state transitions, the evolution of states, and the concept of transition probabilities in quantum mechanics. Participants explore theoretical scenarios involving superposition, eigenstates, and the effects of measurement on these states.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about the meaning of quantum state transition and describes a scenario involving an electron in a superposition of energy eigenstates, questioning the effects of measurement on this state.
  • Another participant clarifies that a position eigenstate of a free particle is not an eigenstate of its Hamiltonian, leading to state evolution over time.
  • A participant suggests the existence of transition probabilities between position eigenstates and questions whether these probabilities are time-dependent.
  • There is a discussion about the definition of transition probability between states, with one participant providing a mathematical expression related to the probability per unit time for state transitions.
  • Another participant emphasizes that probabilities in quantum mechanics are contextually tied to measurement, asserting that without measurement, the system evolves deterministically according to the Schrödinger equation.
  • A question is raised about whether a non-zero transition probability implies that the system's state is a superposition of the states involved.
  • A participant confirms that the initial and final states considered are superpositions of eigenstates of the Hamiltonian, particularly in the context of perturbations applied for finite durations.
  • One participant references Fermi's Golden Rule and discusses its interpretive aspects, noting a disagreement with a specific interpretation by Ballentine, while cautioning against derailing the thread.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of transition probabilities and the nature of quantum state evolution post-measurement. There is no consensus on the interpretations of these concepts, and the discussion remains unresolved regarding the implications of measurement on quantum states.

Contextual Notes

Some participants highlight the dependence on definitions and the context of measurement in quantum mechanics. The discussion includes unresolved aspects regarding the nature of state transitions and the implications of perturbations.

amedeo_fisi
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Hello everyone.
Can someone explains me the meaning of quantum state transition?
For example consider an electron which is in the superposition of two energy eigenstates of a given hamiltonian, now, if no one perturbs the state with a measure, nothing happens and the superposition remains the same for all the time. Suppose you had been able to measure one of the states, this means that the electron decays in that state and it remains there if no perturbation is applied on the system and you have all the probability on that state, am I right? If so, I think this is described by the fact that the two states are orthogonal.
Consider the case where the wave function is a dirac delta in 0 with the hamiltonian of the free particle, what happens theorically after you made the measure of the position? The state remains the same or it evolves spontaneously?
 
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A position eigenstate of a free particle is not an eigenstate of the Hamiltonian of a free particle. Therefore, the state will evolve. You can see this with Gaussian wave packets that spread out with time.
 
So I conlude that there is a transition probability between the position eigenstates, does it have any sense?
Does the probability transition have anything to do with time?
 
I've never heard "transition" used in that way, as it usually refers to discrete states.
 
What is meant by transition probability between two sates? Physically speaking.
 
The transition probability between states ##|i\rangle## and ##|f\rangle## is the probability per unit of time that a system initially in state ##|i\rangle## will be found in state ##|f\rangle##. It is proportional to ##\left| \langle f | \hat{W} i \rangle \right|^2##, where ##\hat{W}## is the perturbation responsible for the transition.
 
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Just to add to DrClaude's remarks - when a probability is used in quantum mechanics, it is ultimately always in the context of measurement. If no measurement is made, the system evolves deterministically according to the Shroedinger equation.
 
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Does the fact that there is a non zero transition probability between two states imply that the state of the system is a superposition of them?
 
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amedeo_fisi said:
Does the fact that there is a non zero transition probability between two states imply that the state of the system is a superposition of them?
Yes. The original (initial and final) states that are considered are those of the unperturbed Hamiltonian. But the initial and final states are superpositions of eigenstates of the Hamiltonian including the perturbation. Often, the perturbation applies for a finite amount of time, hence it makes sense to talk about the problem in terms of unperturbed states.
 
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Just to add a bit more detail to Dr Claude's excellent reply, this is what's called Fermi's Golden Rule:
http://moleng.physics.upatras.gr/personnel/Koukaras/download/FermiGR.pdf

Of interest is the interpretive aspect of it and the quote from Ballentine.

Don't agree with Ballentine adopts a view that's different to the orthodox one (presumably Copenhagen) but that would be a whole new thread and I don't want to derail this one.

Thanks
Bill
 
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