What are the energy eigenvalues of a harmonic oscillator?

In summary: Instead, we use the so-called "Planck's constant h/2π##. So ##E_n## will always be written in terms of the "energy level number" ##n## and the "quantum number" ##\hbar##. This formula describes the energy of an oscillator that is in a state of definite energy. This energy is described by the eigenvalues of the Hamiltonian, which are the energies of the individual energy levels of the oscillator.
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TL;DR Summary
I have this formula ##E_n=hf\left(n+\frac 12 \right)##. I don't understand what energy it describes.
Is it a total energy of a vibrating molecule? So is it a sum of potential and kinetic energy? Or it is only a total energy of a vibrational motion of the molecule? Or is it only a potencial energy, when it is related to a dissociation curve? I am confused.
 
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Lotto said:
TL;DR Summary: I have this formula ##E_n=hf\left(n+\frac 12 \right)##. I don't understand what energy it describes.

Is it a total energy of a vibrating molecule? So is it a sum of potential and kinetic energy? Or it is only a total energy of a vibrational motion of the molecule? Or is it only a potencial energy, when it is related to a dissociation curve? I am confused.
It looks the energy levels of an ideal harmonic oscillator, and will be the sum of the potential and kinetic energy of the oscillator. How this relates to a vibrating molecule depends on how accurately the molecule can be modeled as an ideal harmonic oscillator.

In general, we know what energies are involved by looking at the Hamiltonian that we started with. In the case of the ideal harmonic oscillator, that Hamiltonian contains a kinetic energy term and a potential energy term.
 
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Indeed, these are the energy eigenvalues of a harmonic oscillator. It describes the conserved total energy of the oscillator, when it is prepared in a state of determined energy. The possible values of this total energy are the eigenvalues of the Hamilton operator,
$$\hat{H}=\frac{1}{2m} \hat{p}^2 + \frac{m \omega^2}{2} \hat{x}^2.$$
The energy eigenvalues are
$$E_n=h f \left (n+\frac{1}{2} \right) = \hbar \omega \left (n+\frac{1}{2} \right), \quad n \in \{0,1,2,3,\ldots \}=\mathbb{N}_0,$$
where ##\hbar=h/(2 \pi)## is the "modified quantum of action/Planck's constant)". Nowadays almost nobody uses the original ##h## anymore.
 
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FAQ: What are the energy eigenvalues of a harmonic oscillator?

What are the energy eigenvalues of a harmonic oscillator?

The energy eigenvalues of a quantum harmonic oscillator are given by the formula \( E_n = \left(n + \frac{1}{2}\right)\hbar\omega \), where \( n \) is a non-negative integer (0, 1, 2, ...), \( \hbar \) is the reduced Planck's constant, and \( \omega \) is the angular frequency of the oscillator.

How is the quantization of energy levels in a harmonic oscillator explained?

The quantization of energy levels in a harmonic oscillator arises from the boundary conditions imposed by the Schrödinger equation. The solutions to the Schrödinger equation for a harmonic oscillator are wavefunctions that must be normalizable, leading to discrete energy levels.

What is the significance of the zero-point energy in a harmonic oscillator?

The zero-point energy is the lowest possible energy that a quantum mechanical physical system may have, and it is \( \frac{1}{2}\hbar\omega \) for a harmonic oscillator. This means that even in its ground state (n=0), the harmonic oscillator has a non-zero energy due to quantum fluctuations.

How do the energy eigenvalues of a harmonic oscillator differ from those of a classical oscillator?

In a classical harmonic oscillator, the energy can take any continuous value depending on the amplitude of oscillation. In contrast, a quantum harmonic oscillator has discrete energy levels, meaning the energy can only take specific quantized values given by \( E_n = \left(n + \frac{1}{2}\right)\hbar\omega \).

What role do Hermite polynomials play in the solutions of the harmonic oscillator?

Hermite polynomials are part of the mathematical form of the wavefunctions (eigenfunctions) of the quantum harmonic oscillator. The solutions to the Schrödinger equation for the harmonic oscillator are products of a Gaussian function and Hermite polynomials, which ensure that the wavefunctions are normalizable and satisfy the boundary conditions.

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