Wave function of Stationary State

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Discussion Overview

The discussion revolves around the wave function of a particle in a stationary state, particularly focusing on the implications of having a definite energy and momentum. Participants explore concepts related to probability density, uncertainty principles, and the nature of stationary states in quantum mechanics, including the behavior of free particles and electrons in atomic orbits.

Discussion Character

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

Main Points Raised

  • Some participants assert that a wave function of a particle with definite energy is time-independent, leading to a constant probability density.
  • Others argue that a free particle with definite momentum does not exist due to normalization issues and the implications of the uncertainty principle.
  • A participant questions the assumption of a starting position for a particle with definite momentum, suggesting that such a particle cannot be localized.
  • Concerns are raised about the implications of stationary states for electrons in atoms, with some suggesting that the uncertainty in position cannot be infinite as electrons are localized around the nucleus.
  • Some participants discuss the nature of excited states, indicating that they do not remain stationary indefinitely and can relax to lower energy states.
  • A later reply points out that while a free particle can have a definite velocity, this results in a complete loss of positional information.
  • Questions are raised about the normalization of wavefunctions over infinite spaces and the implications for energy measurements.
  • Participants note that the electron's behavior in stationary states differs from that of free particles, as the former can exhibit both position and momentum uncertainty without being infinite.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of stationary states, the implications of definite momentum, and the behavior of particles in free space versus those in atomic orbits. The discussion remains unresolved with no consensus on several key points.

Contextual Notes

Limitations include the dependence on definitions of stationary states, the implications of the uncertainty principle, and the normalization of wavefunctions in infinite spaces. The discussion also highlights the complexities of excited states and their relaxation processes.

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I learned (University Physics, 9th Edition, Extended Version) that the wave function of a particle having a definite energy is independent of time. This means the probability Density of the particle don't change with time, i.e. If a particle is 90% likely to be found some where now, There is always 90% chance of finding the particle at the same place.

What I am confused on is in this Scenario---
Suppose a particle is moving in freely in free space with certain constant velocity therefore having constant Energy.
Then How is it possible that the particle is always most likely to be found at its starting position.?
My institution Tells me that the probability density should constantly change with time as the particle moves.
 
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A particle in free space that has a definite energy, and for a free particle that also means a precisely defined momentum, that is [tex]\Delta p = 0[/tex]. So the uncertainty principle tells us that uncertainty in position must be infinite; the particle cannot be specifically located, so it has the same probability of being located anywhere.
 
You said it yourself: Definite velocity (momentum) and a starting position...

What starting position?

If you have a certain velocity you don't have a starting position because you could be anywhere.

You cannot assume a starting position as well as a definite energy. If your particle is in a "starting position", then we would have to argue that the electron must somehow be localized, but then you wouldn't have a pure momentum state.
 
kanato said:
A particle in free space that has a definite energy, and for a free particle that also means a precisely defined momentum, that is [tex]\Delta p = 0[/tex]. So the uncertainty principle tells us that uncertainty in position must be infinite; the particle cannot be specifically located, so it has the same probability of being located anywhere.

I quite got where I was slipping. But one question still remains.
For an electron revolving round the nucleus in stationary state, It can't be true that the uncertainty in position is infinite. We at least Know that the electron is somewhere around the nucleus, It obviously can't be in the another corner of the solar system.
 
thecritic said:
I quite got where I was slipping. But one question still remains.
For an electron revolving round the nucleus in stationary state, It can't be true that the uncertainty in position is infinite. We at least Know that the electron is somewhere around the nucleus, It obviously can't be in the another corner of the solar system.

By making similar arguments, it can't be true that the electron is revolving with a "pure" momentum state. Because the levels are always "broadened", they are not "real" discrete states (delta functions).

Remember all these are really toy examples, and do not faithfully represent reality.
 
sokrates said:
By making similar arguments, it can't be true that the electron is revolving with a "pure" momentum state. Because the levels are always "broadened", they are not "real" discrete states (delta functions).
Remember all these are really toy examples, and do not faithfully represent reality.
The electrons are in stationary State, Thats for sure, Right?
Then The wave function is time independent, Right?
And don't this means that there is the equal probability of finding the electron anywhere?
 
thecritic said:
I learned (University Physics, 9th Edition, Extended Version) that the wave function of a particle having a definite energy is independent of time. This means the probability Density of the particle don't change with time, i.e. If a particle is 90% likely to be found some where now, There is always 90% chance of finding the particle at the same place.
Are you sure about what you imply?
To me it seems that "the wave function of a particle having a definite energy is independent of time" means that sum of potential energy and kinetic energy is independent of time while separately potential energy and kinetic energy can vary with time.
 
I think the most basic objection to an argument that involved a free particle of definite momentum is that a free particle with definite momentum simply DOES NOT EXIST. The stationary states (definite momentum) of a free particle are not normalizable and hence, are unphysical.
 
nnnm4 said:
I think the most basic objection to an argument that involved a free particle of definite momentum is that a free particle with definite momentum simply DOES NOT EXIST. The stationary states (definite momentum) of a free particle are not normalizable and hence, are unphysical.
A side question.
Does it mean that free particle (photon) with definite velocity does not exist?
 
  • #10
I think what the original poster is asking in another way is,

If you have a particle in an infinite space with no potential, and perform an energy measurement of that particle, do you not collapse the wavefunction into a single energy eigenstate which is time-independent?

Is the solution that the energy of the particle gives you no information about the position or momentum?

Also, I am not certain if the problem is well-defined- how can you normalise a wavefunction which is defined over an infinite space, and by symmetry, transnationally invariant? (but non-zero!)
 
  • #11
thecritic said:
The electrons are in stationary State, Thats for sure, Right?

No, that's not right.

An electron in an excited state will relax, right? If the excited level was really a stationary state, then there would be no relaxation to the ground state. An excited electron would stay in that energy forever.

One-particle Schrödinger equation does not capture this, there's always a slight broadening in the levels.

These are toy examples. Don't take them seriously. Or study many-body perturbation theory.
 
  • #12
zonde said:
A side question.
Does it mean that free particle (photon) with definite velocity does not exist?

Not at all... It just means that because you know the velocity exactly

you have lost all the information regarding the position. Exact frequencies are both theoretically and experimentally possible (,say, for a free electron in vacuum) - it is the coupling to the environment that corrupts pure states. This "environment effect" is usually much more stronger. It "broadens" the energy levels and introduces effects like relaxation etc..
 
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  • #13
thecritic said:
I quite got where I was slipping. But one question still remains.
For an electron revolving round the nucleus in stationary state, It can't be true that the uncertainty in position is infinite. We at least Know that the electron is somewhere around the nucleus, It obviously can't be in the another corner of the solar system.

The case of the the electron orbitting a nucleus is different from the free particle case. The reason is that in this case a definite energy state does not correspond to a definite momentum state (in the case of a free particle it does). So it is in fact possible for the particle to sit in a stationary state (an energy eigenstate). And in this state there is both an uncertainty in the position and the momentum (but it doesn't stretch out to infinity).

sokrates said:
No, that's not right.

An electron in an excited state will relax, right? If the excited level was really a stationary state, then there would be no relaxation to the ground state. An excited electron would stay in that energy forever.

One-particle Schrödinger equation does not capture this, there's always a slight broadening in the levels.

These are toy examples. Don't take them seriously. Or study many-body perturbation theory.
The relaxation process is a different process. For that to take place you need some way to divert the energy away from the nucleus/electron system. For that to take place you need some sort of interaction process. In fact, what happens is that the electron interacts with the QED vacuum -- in some sense a virtual photon can kick the electron to a lower energy state. As a result the electron emits a photon.

But strictly speaking, in the absence of interactions quantum mechanics does not predict any relaxation and the energy eigenstates become truly stationary. But you are right that this is just a toy model.
 
  • #14
thecritic said:
The electrons are in stationary State, Thats for sure, Right?
Then The wave function is time independent, Right?
And don't this means that there is the equal probability of finding the electron anywhere?

NO,the equal proabability of finding the electron anywhere means the electron is in a momentum eigenstate.However an electron revolving round the nucleus is effected by a potential,so its momentum doesn't commute with the Hamiltonnian.That means although the electron is just in stationary state,it's not in a momentum eigenstate.
 
  • #15
xepma said:
The relaxation process is a different process. For that to take place you need some way to divert the energy away from the nucleus/electron system. For that to take place you need some sort of interaction process. In fact, what happens is that the electron interacts with the QED vacuum -- in some sense a virtual photon can kick the electron to a lower energy state. As a result the electron emits a photon.

But strictly speaking, in the absence of interactions quantum mechanics does not predict any relaxation and the energy eigenstates become truly stationary. But you are right that this is just a toy model.

What do you mean the relaxation process is different? After interacting with the vacuum, electron still -relaxes- right? I'd still call it "relaxation" even if the excited atom falls back on a lower sate in vacuum.

Relaxation is pretty loose terminology so I couldn't figure whether you are saying anything different.
 
  • #16
Seems Like I have to do further Drilling into the subject. I quite don't know what's meant by momentum eigenstate
 
  • #17
I think you would be able answer this for me.
Suppose I go into a large vacant space (to get rid of all environment influences). Then I project single electron with an electron gun.
--Do this electron now have a definite velocity/momentum or not?
--What is the wave function of this electron like?
(Since the electron always moves in zero potential region, I guess that its Kinetic Energy (whatever that may be) remains constant. Since the only energy involved is the kinetic Energy, I find it sensible to say that the Total Energy of the electron also remains constant. Then there should be no objection in saying the the electron is in Stationary State, is there? Correct me where I am wrong.)
 

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