A QM problem on finding eigenvalues

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Homework Help Overview

The discussion revolves around a quantum mechanics problem involving the determination of negative eigenvalues of a one-dimensional Hamiltonian operator. The Hamiltonian is expressed in terms of a kinetic term and a potential term defined by a normalized projector. Participants are exploring the implications of the Hamiltonian's structure and the nature of the potential involved.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to apply the Hamiltonian to specific states and are discussing the implications of expressing the Hamiltonian in different bases. Questions about the meaning of the potential operator and its application to wave functions are raised. Some participants express confusion about the notation and the steps involved in the calculations.

Discussion Status

The discussion is ongoing, with various approaches being explored. Some participants have provided insights into the structure of the Hamiltonian and the potential operator, while others are questioning the clarity of the problem setup. There is a mix of attempts to derive equations and expressions related to the eigenvalues, but no consensus has been reached on a specific method or solution.

Contextual Notes

Participants note the complexity introduced by the mixing of bra-ket notation with wave function notation, which may be contributing to the confusion. The original poster is also reminded to post in the appropriate section for homework help.

  • #31
HackaB Think about a slighly different version, say a spin dependent problem, with

H0(m,n) = S*S + V (|m><n| where S is spin (S*S has eigenvalues s(s=1), and the |m> states are Sz eigenstates. The problem specifies the potential to be proportional to a "projector", a single state projection operator. The only choice of m & n that conforms to the properties of a single-state projection operator is m=n. Generalize this reasoning, and get the delta function.
Regards,
Reilly Atkinson
 
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  • #32
By the way, Seratend's solution is the correct one for the non-diagonal version -- the projection operator is replaced by a transition operator. -- which is the equation and solution that Cooper used in his original Cooper Pair paper.
Regards,
Reilly Atkinson
 
  • #33
So you do not agree that <x|v>V<v|y> = kV exp(-k|x|)exp(-k|y|) ?

reilly said:
The only choice of m & n that conforms to the properties of a single-state projection operator is m=n. Generalize this reasoning, and get the delta function.
I'm sorry, but I don't follow this reasoning. |v> is not a "single state" in the x-representation. So I do not see how a delta function would arise. Could you show the mathematical steps to get it?

By the way, Seratend's solution is the correct one for the non-diagonal version -- the projection operator is replaced by a transition operator.

What is a transition operator? Is it similar to a projection operator?
 
  • #34
HackaB -- I blew it with the Bessels -- too good to be true, I suppose. So with egg on my face, I retract the delta function, and remain,
Reilly Atkinson
 
  • #35
If the assistance this thread has given the OP, has not convinced him that quantum mechanics is impossibly difficult, I wonder what it would take.

Carl
 

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