Quantum Mechanics: Normalization Requirements (E>Vmin)

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SUMMARY

The discussion centers on the normalization requirements of the wavefunction Ψ(x,t) in quantum mechanics when the energy E is less than the minimum potential Vmin. The user explores the implications of the 1-D Schrödinger Equation, specifically the equation ψ''(x) = 2m(V(x) - E)(ψ(x))/h^2, and attempts to derive a general solution. The consensus is that if E < Vmin, the wavefunction cannot be normalized, as indicated in DJ Griffiths' "Introduction to Quantum Mechanics." The conversation highlights the necessity for the wavefunction's continuity and the physical implications of having E less than Vmin.

PREREQUISITES
  • Understanding of the 1-D Schrödinger Equation
  • Familiarity with the concepts of wavefunctions and probability densities
  • Knowledge of the principles of quantum mechanics, particularly energy and potential energy relationships
  • Basic calculus, specifically differential equations and their solutions
NEXT STEPS
  • Study the implications of boundary conditions on wavefunctions in quantum mechanics
  • Learn about the concept of potential wells and their effect on wavefunction normalization
  • Investigate the role of the continuity of wavefunction derivatives in quantum mechanics
  • Explore the physical significance of energy levels in quantum systems, particularly in relation to potential energy
USEFUL FOR

Students of quantum mechanics, physicists, and educators seeking to deepen their understanding of wavefunction normalization and the implications of energy levels in quantum systems.

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I have just begun using the 1-D Schrödinger Equation in my quantum mechanics course. We are assuming the potential, V, is solely a function of x (V(x)). I have been examining the solution to the differential equation through separation of variables. Ψ(x,t) = ψ(x)φ(t)

(Assuming Ψ(x,t) is seperable) I understand the proof to show that the solutions of Ψ(x,t) produce probabilitiy densities that are invariant to time. And that |Ψ(x,t)|^2 = |ψ(x)|^2. I also understand why E must be real.

When the assumption of seperability is made we have:

-(h^2)ψ''(x)/2m +V(x)ψ(x) = Eψ(x) (h is hbar)

Which is equivalent to:

ψ''(x) = 2m(V(x) - E)(ψ(x))/h^2 (1)

My textbook (DJ Griffiths Introduction to Quantum Mechanics) claims that if E < Vmin => that Ψ(x,t) cannot be normalized. Because |Ψ(x,t)|^2 = |ψ(x)|^2 I can divert my attention to (1) and ignore φ(t).

Solving the differential equation for:

ψ''(x) = c^2(ψ(x), c is real

Gets me the general solution (I think!):

ψ(x) = Aexp(cx+b) + Bexp(-cx+d) A,B,b,d are constants

If we take a piecewise solution like ψ(x) = exp(-|x|) the integral of |ψ(x)|^2 over the whole real line is finite (and equal to 1, I believe). |ψ(x)|^2 is continuous as well.

The textbook also hints that it has to do with the the fact that the second derivative is always the same sign as the function itself. I can't formulate a proof as to why this should necessarily imply the function cannot be normalized. In fact, to the best of my knowledge I've provided a perfectly valid counterexample...

I've thought about it for an hour or so and I can't figure out why this answer is unacceptable. Can someone please tell me what I have done incorrectly?

I'm also curious about if there is something unphysical about having E<Vmin. Thanks for the help!
 
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Your "general solution" is not, in general, a solution to the correct equation, with a position-dependent V(x) [your c is not a function of x].

Also, as long as |V(x)| is finite, the wavefunction's derivative has to be continuous, too.

So, two reasons for your counter example to be incorrect.

Oh, and of course there is something unphysical about E being less than the minimum potential energy when E=T+V!
 

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