Explaining Time Dependent Potentials

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Discussion Overview

The discussion revolves around the concept of time-dependent potentials in quantum mechanics, particularly in the context of the Schrödinger equation and its solutions. Participants explore examples of time-dependent potentials and their implications for particle behavior, as well as the differences between classical and quantum mechanical perspectives.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant expresses difficulty in imagining a scenario where a potential changes over time without affecting the particle's position.
  • Another participant suggests that time-dependent potentials can be represented by external factors, such as an applied electric field that varies with time.
  • A different example is provided where two charges rotating around a center create a time-dependent potential while leaving a particle at rest.
  • There is a discussion about the distinction between classical and quantum mechanics regarding potential energy, with a mention of the Ehrenfest theorem and how expectation values can vary over time even if the potential operator does not depend on time.
  • Participants note that in stationary states, the expectation value of potential energy remains time-independent, which contrasts with classical mechanics.

Areas of Agreement / Disagreement

Participants generally agree on the existence and implications of time-dependent potentials, but there are varying interpretations and examples provided. The discussion remains unresolved regarding the nuances of how these potentials interact with particle behavior in quantum mechanics.

Contextual Notes

Participants acknowledge that classical mechanics and quantum mechanics handle potentials differently, leading to potential confusion regarding time dependence and expectation values.

pmiranda
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Hello,

I am trying to self learn a little bit of quantum mechanics in order to describe the magnetic resonance phenomenon. I am following Griffiths book and i am understanding most of it.

Now, there is a particular thing that is bogging me.

The Schrödinger equation can be easily solved by separation of variables if the potential does not depend on time, which i understand as:
[itex]\frac{\partial V(x,t)}{\partial t}=0[/itex]

in other words it can simply be
[itex]V(x,t)\rightarrow V(x)[/itex]

Now i can think of a many motions where the potential is constant at any given position in time. For instance the Harmonic oscillator or an electron orbiting.

Now i can't imagine in my naive approach, a possible scenario where the potential changes with time without changing the position of a particle.

Is there any easy explanation for that?

Ty in advance
 
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pmiranda said:
Now i can't imagine in my naive approach, a possible scenario where the potential changes with time without changing the position of a particle.

Ty in advance

Not sure I understand that question.

If you want a simple example of a potential that varies with time, you can think of any kind of applied electric field. For example one that depends linearly on time or more realistically one that oscillates with a given frequency (a model for monochromatic light). Potentials that are time-dependent are usually so-called "external" potentials because they do not have their origin in the particles themselves (such as coulomb attraction between two charged particles). Maybe that's why you're having a hard time imagining such a potential.
 
I didn´t though of it as an "external" thing. That way it makes sense now!
Thanks a lot
 
An example of a potential that varies over time but leaves the particle in its position would be the potential in the center of the axes, while two charges in opposite sides of the diameter of a circle around the center of the axes, are rotating in circular trajectory.
 
pmiranda said:
I didn´t though of it as an "external" thing. That way it makes sense now!
Thanks a lot

Yes, a potential like that can be a function that depends explicitly on time. That doesn't mean that potential energy will not vary (the expecation value) with time if the operator V isn't a function of t. I guess the confusion comes from the fact in classical physics, in the case of a harmonic oscillator for example, V would depend implicitly on time, since it would be a function of x(t). In QM the operator V(x) is not a function of time (for the harmonic oscillator), but the expectation value <V> could depend on time since V does not commute with H. Check out the Ehrenfest theorem:

http://en.wikipedia.org/wiki/Ehrenfest_theorem

However, if you are in a stationary state <V> will indeed be time independent, which to me was always kinda weird (when compared to classical mechanics). But I guess that comes from the fact there are such things as stationary states in QM and no trajectories.
 
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