1-D simple harmonic oscillator

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Homework Help Overview

The discussion revolves around the differences between the Heisenberg picture and the Schrödinger picture in the context of a one-dimensional simple harmonic oscillator (SHO). Participants are exploring the implications of these two frameworks in quantum mechanics.

Discussion Character

  • Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants are attempting to clarify the roles of time evolution in both pictures, specifically how dynamic variables and state vectors are treated differently. Questions are raised about the implications of these differences for understanding the simple harmonic oscillator.

Discussion Status

The discussion is ongoing, with participants sharing their interpretations and seeking further clarification on the relationship between the two pictures and their application to the SHO. Some guidance has been offered regarding the equivalence of the two approaches, but no consensus has been reached.

Contextual Notes

There is an indication of confusion regarding the relationship between the two pictures and the specific application to the simple harmonic oscillator, suggesting that further exploration of these concepts is needed.

indigojoker
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I was just wondering what the difference was in the 1-D simple harmonic oscillator in the Heisenberg picture versus the Schrödinger picture?
 
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What is generally the difference b/w the Heisenberg and the Schrödinger pictures ?
 
dextercioby, please correct me if I'm wrong but this is my understanding of the two pictures (involving time):

In the Schrödinger picture, the time evolution operator operates on the state vector and the dynamic variabs x and p do not change. So:

x->x
p->p
|a> -> U|a>

However, in the Heisenberg picture, the dynamic variables x and p changes, while the state vector stays the same:

let *=dagger

x(t)->U*xU
p(t)->U*pU
|a> -> |a>

i guess I'm confused as to how this related to the SHO?
 
The difference is if we tag the time dependence onto the states or onto the operators.
In one picture (Schrödinger) the operators are not time-dependent, and the states generally are. In the Heisenberg picture it's the other way around.
Of course, they're completely equivalent (when you calculate the physically relevant quantities like expectation values etc. you get the same answer in both), it's just that sometimes one is more efficient than the other.
 

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