A QM problem on finding eigenvalues

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This discussion centers on solving a quantum mechanics problem involving the Hamilton operator defined as H = P²/(2M) - |v⟩V⟨v|, where V is a positive constant and |v⟩ has the position wave function ⟨x|v⟩ = √κ e^{-κ|x|}. Participants explore the process of finding negative eigenvalues of H, applying Hamiltonian mechanics in both position and momentum bases, and addressing the complexities of the potential operator. The conclusion is that the potential does not admit physical states for a continuous energy spectrum in the negative real numbers.

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  • #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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