What Is the Significance of 'n' in the Solutions of the Quantum SHO?

In summary, the even solutions of an SHO can be expressed as h^+(y) = \sum_{s = 0}^{\infty}a_s y^{2s}, where the coefficients a_s are given by the recursion a_{s+1} = a_s \left( \frac{4s + 1 - \epsilon}{2(s+1)(2s+1)} \right). These solutions are square integrable if a_n = 0, meaning the polynomial is finite. However, there is some confusion regarding the solution for n = 0, as the book states h_0(y) = 1 instead of 0 when a_0 = 0. It is suggested
  • #1
ehrenfest
2,020
1
The even solutions of an SHO are:

[tex]h^+(y) = \sum_{s = 0}^{\infty}a_s y^{2s} [/tex]

where a is given by the recursion

[tex] a_{s+1} = a_s \left( \frac{4s + 1 - \epsilon}{2(s+1)(2s+1)} \right)[/tex]

The solutions are square integrable iff

a_n = 0 so that the polynomial is finite.

What I do not understand is why my book (Robinett) says

h_0(y) = 1 and not 0 when a_0 = 0 for n = 0?
 
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  • #2
Who's "n" and what does it have to do with what you wrote ?
 
  • #3
dextercioby said:
Who's "n" and what does it have to do with what you wrote ?

So, there should be one solution for every n because

a_n = 0 --> epsilon = (4n +1).

So, I guess n is the degree (maybe +/- 1 of the polynomial). It is also the energy level.
 

Related to What Is the Significance of 'n' in the Solutions of the Quantum SHO?

What is a solution of the quantum SHO?

A solution of the quantum SHO (simple harmonic oscillator) refers to the mathematical representation of the allowed energy states of a particle in a harmonic potential. These solutions are obtained through the Schrodinger equation and can be expressed as a sum of wavefunctions, each corresponding to a different energy level.

How does the quantum SHO differ from the classical SHO?

The quantum SHO takes into account the principles of quantum mechanics, such as wave-particle duality and uncertainty principle, while the classical SHO is based on classical mechanics. In the quantum SHO, the energy states are quantized, meaning they can only take on discrete values, while in the classical SHO, energy can take on any value.

What is the significance of the ground state in the quantum SHO?

The ground state of the quantum SHO is the lowest energy state that a particle can occupy. It has a well-defined energy and wavefunction, and all other energy states are measured relative to the ground state. The ground state also has the highest probability of being occupied by a particle at any given time.

What is a wavefunction in the context of the quantum SHO?

A wavefunction in the quantum SHO is a mathematical function that describes the probability amplitude of finding a particle in a particular energy state. It is a complex-valued function that depends on the position of the particle and changes over time according to the Schrodinger equation.

How do the energy levels of the quantum SHO relate to the classical SHO?

The energy levels of the quantum SHO are quantized, meaning they can only take on discrete values, while the energy levels of the classical SHO can take on any value. However, in the limit of large quantum numbers, the energy levels of the quantum SHO approach the energy levels of the classical SHO, making them consistent with each other.

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