Schrodinger Equation and wavefunctions

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SUMMARY

The discussion centers on the nature of wavefunctions in quantum mechanics, specifically regarding their relationship with the Schrödinger Equation and the Hamiltonian operator. It is established that not all wavefunctions must be eigenfunctions of the Hamiltonian to describe a system; wavefunctions can still be valid even when influenced by external forces. The key takeaway is that any differentiable and normalizable wavefunction can be considered, expanding the understanding of quantum systems beyond traditional eigenfunction constraints.

PREREQUISITES
  • Understanding of the Schrödinger Equation
  • Familiarity with Hamiltonian operators in quantum mechanics
  • Knowledge of wavefunction properties, including differentiability and normalizability
  • Basic concepts of quantum systems under external forces
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  • Research the implications of non-eigenfunction wavefunctions in quantum mechanics
  • Study the role of external forces on wavefunctions and their time evolution
  • Explore the concept of normalizable wavefunctions in quantum theory
  • Learn about the mathematical framework of Hamiltonian mechanics
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Students and professionals in physics, particularly those specializing in quantum mechanics, as well as researchers exploring the properties and applications of wavefunctions in various physical systems.

Chemist20
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not all functions are wavefunctions. For functions to be wavefunctions they have to obey a series of "rules". Now, my question is:

there are many functions, which obey these rules which aren't eigenfunctions of the hamiltonian, thereby meaning that they don't obey the Schrödinger Equation. Can systems described by these kind of wavefunctions exist or is it, as I think it is, not physically possible??
 
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Hello Chemist20,

I do not think the psi-function has to be an eigenfunction of the Hamiltonian to describe the system in general. Many calculations deal only with such functions, but there are situations in which the psi-function cannot be of such nature; this is when the atom is under action of external forces. The wave function governed by Schroedinger's equation of motion then varies with time and is not an eigenfunction of the Hamiltonian. I think generally any differentiable and normalizable wave function is conceivable.
 

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