Solving the Mystery of Energy Eigenfunctions

In summary: However, in this particular case, \psi is an eigenfunction of energy because \psi_1 and \psi_2 have the same eigenvalue.
  • #1
pivoxa15
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It seems the Schrodinger equation is written so that psi is an energy eigenfunction. So all psi are energy eigenfunctions? But how can it turn into other eigenfunctions like momentum? Or is it already a momentum eigenfunction as welll as the energy eigenfunction and so also position and so on...
 
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  • #2
The time-dependent version of the Schroedinger equation makes no reference to energy eigenvalues. However, since the Hamiltonian is a Hermitian operator, any wavefunction can be expanded as a sum of its eigenvectors. If you crank out the resulting differential equation, the weighting coefficient of each eigenvector obeys a simple exponential relationship, which means that once the eigenvectors are found, it is a fairly simple matter to find the time-dependent behavior of the wavefunction. Thus, solving the Schroedinger equation is really just a problem of finding the Hamiltonian's eigenvalues.
 
  • #3
The great postulate of Schrodinger is that -i(hbar)d(psi)/dt = H(psi) where H is the hamiltonian.

So -i(hbar)d(psi)/dt = E(psi) = H(psi)

Which as you say nothing more than finding the Hamiltonian's eigenvalues.

So the schrodinger equation is not that mysterious after all? psi as we know it is related to the eigenfunction of the hamiltonian. But has the intepretation as |psi|^2 is the probability density.

I've just realized that there are no momentum nor position eigenfunctions so there could have been some error in my OP.
 
  • #4
pivoxa15 said:
The great postulate of Schrodinger is that -i(hbar)d(psi)/dt = H(psi) where H is the hamiltonian.

So -i(hbar)d(psi)/dt = E(psi) = H(psi)

Which as you say nothing more than finding the Hamiltonian's eigenvalues.

So the schrodinger equation is not that mysterious after all? psi as we know it is related to the eigenfunction of the hamiltonian. But has the intepretation as |psi|^2 is the probability density.

I've just realized that there are no momentum nor position eigenfunctions so there could have been some error in my OP.


There is no real error in your op. Position eigenfunctions are dirac delta functions, and momentum eigenfunctions are plane waves (in the position basis at least.)
 
  • #5
pivoxa15 said:
It seems the Schrodinger equation is written so that psi is an energy eigenfunction. So all psi are energy eigenfunctions?

Let me amplify an answer you've already been given here. You can take any two solutions to the Schroedinger equation and combine them into another solution. For example:

[tex]\psi(x,t) = \psi_1(x,t) + \psi_2(x,t)[/tex]

is also a solution if [tex]\psi_1, \psi_2[/tex] are. Now think about what happens if [tex]\psi_1[/tex] and [tex]\psi_2[/tex] are eigenfunctions of energy with different eigenvalues. In general, [tex]\psi[/tex] is not an eigenfunction of energy.
 

FAQ: Solving the Mystery of Energy Eigenfunctions

What is the concept of energy eigenfunctions?

The concept of energy eigenfunctions is a fundamental principle in quantum mechanics. It refers to the wave functions that describe the energy states of a quantum system. These functions are solutions to the Schrödinger equation and represent the probability of finding a particle in a particular energy state.

Why is solving the mystery of energy eigenfunctions important?

Solving the mystery of energy eigenfunctions is crucial for understanding the behavior of quantum systems and predicting their energy levels. It allows us to determine the allowed energy states of a system and calculate the probability of a particle being in a particular energy state.

What methods are used to solve the mystery of energy eigenfunctions?

There are various mathematical methods used to solve the energy eigenfunctions of a quantum system. These include the separation of variables, perturbation theory, and variational methods. Each method has its advantages and is used depending on the complexity of the system.

How do energy eigenfunctions relate to the uncertainty principle?

The uncertainty principle states that it is impossible to simultaneously know the exact position and momentum of a particle. Energy eigenfunctions play a crucial role in this principle as they represent the probability of finding a particle in a particular energy state, which is related to its momentum. Therefore, the more precisely we know the energy of a particle, the less we know about its position.

What are the applications of understanding energy eigenfunctions?

Understanding energy eigenfunctions has various practical applications in fields such as quantum mechanics, solid-state physics, and chemistry. It is crucial for predicting the behavior of atomic and molecular systems, designing electronic devices, and solving problems in quantum computing. Additionally, it allows us to understand the properties of materials and their behavior under different conditions.

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