Show that a complex PE yields a time dependant probability of finding a particle

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SUMMARY

The discussion centers on demonstrating that a complex potential energy, defined as V=α+iβ, leads to a time-dependent probability P of locating a particle, indicating its instability and inability to maintain normalization over time. The Schrödinger Equation (SE) is utilized, specifically the form ih/2m=-h^2/2m(∫∂ψ/∂x )+(α+iβ)ψ, to analyze the implications of this complex potential. The conversation highlights the necessity of proving that the Hamiltonian is not self-adjoint, which prevents the application of Stone's theorem for unitary evolution and conservation of probability.

PREREQUISITES
  • Understanding of Schrödinger's Equation (SE)
  • Knowledge of complex potential energy in quantum mechanics
  • Familiarity with Hamiltonian mechanics
  • Concept of unitary evolution in quantum states
NEXT STEPS
  • Study the implications of complex potentials in quantum mechanics
  • Learn about the self-adjointness of operators in quantum systems
  • Research Stone's theorem and its application in quantum mechanics
  • Explore normalization conditions for quantum states over time
USEFUL FOR

Students of quantum mechanics, physicists analyzing unstable systems, and educators seeking to clarify the implications of complex potentials in Schrödinger's Equation.

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Homework Statement


Starting from Schrödinger's Equation show that a complex potential energy V=α+iβ yields a time dependent probability P of finding the particle in (-inf,inf), i.e. the particle is unstable and normalization cannot be insured over time. Compute P(+)


Homework Equations


SE: ih/2m=-h^2/2m(∫∂ψ/∂x )+Vψ

The Attempt at a Solution


I tried inserting my value of potential energy into the SE as follows
ih/2m=-h^2/2m(∫∂ψ/∂x )+(α+iβ)ψ
and then i got stuck, am i supposed to integrate next or stick an an A and try to normalize and then prove that because it is not normalizeable it is unstable. Also what is P(+)

Thanks for any advice you can offer me.
 
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I don't know what they mean by P(+). Look it up in the book / ask your instructor/adviser.

Well, ensuring the conservation of probability (density) over time relies heavily on the fact that this follows from a unitary evolution of states. What you can do is to show that the Hamiltonian will no longer be self-adjoint, since that wouldn't allow us to use Stone's theorem to obtain a unitary evolution.
 

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