Propagator Equation at t=0 Explained

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Homework Help Overview

The discussion revolves around the propagator equation at time t=0, specifically the expression involving the Dirac delta function and its interpretation in the context of quantum mechanics. Participants are exploring the meaning of the variables involved, particularly the distinction between x and x'.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants are questioning the nature of the variables x and x', with some confusion about their continuity and representation. There is a discussion about whether the Kronecker delta might be more appropriate than the Dirac delta in this context.

Discussion Status

The conversation is ongoing, with participants providing insights into the nature of the variables and the implications of the propagator. Some clarification has been offered regarding the continuous nature of x and x', but there is still uncertainty and exploration of the topic.

Contextual Notes

Participants are navigating the definitions and assumptions related to the propagator and its mathematical representation, indicating a need for further clarification on the underlying concepts.

ehrenfest
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I understand the progator in general but could someone explain this equation for the propagator at t = 0 for me:

\delta(x' - x) = K(x',x;0,0) = \sum_m \psi_n(x')\psi_n(x)

?

I am confused about the dfiference between x' and x. It seems like the Kronecker would make more sense than Dirac here?
 
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x is continuous.
 
Gokul43201 said:
x is continuous.
And x' is discrete? What do they represent?
 
No, x and x' are both positions. They (and t, t') are continuously varying parameters; hence the Dirac delta.

The propagator K(x,x';t-t') is the amplitude for a particle initially at (x',t') to be observed at (x,t). With t=t', this is the probability amplitude that a particle at x' is also at x, which is given by the Dirac delta distribution.
 
Last edited:

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