Ladder Operator for Harmonic Oscillator: a|0> = |0>

In summary: However, it can also be thought of as a|0> = 0|0> = 0 (number). In summary, for the harmonic oscillator, the correct statement is that a|0> = null vector, and for the number operator, \hat{N}|0> = 0 (number).
  • #1
KFC
488
4
For harmonic oscillator, let |0> be the ground state, so which statement is correct?

a|0> =|0>

or

a|0> = 0 (number)

where a is the destroy operator
 
Physics news on Phys.org
  • #2
It is the number zero. If a were the identity operator, you would get |0> back.
 
  • #3
clem said:
It is the number zero. If a were the identity operator, you would get |0> back.

you sure about that? i know that the books say zero but those operators aren't hermitian anyway hence unphysical so what does it matter what it does to |0> ?
 
  • #4
Neither. [tex] a|0\rangle = [/tex] the zero ket.

EDIT: The zero ket and [tex] |0\rangle [/tex] are different things.
 
Last edited:
  • #5
dx said:
Neither. [tex] a|0\rangle = [/tex] the zero ket.

zero ket? Do you mean [tex] a|0\rangle = |0\rangle[/tex] ?
 
  • #6
No. The zero ket is the zero vector in the state space. [tex] |0\rangle [/tex] is not the zero vector, it's just the vector with eigenvalue [itex] \hbar \omega ( 0 + \frac{1}{2}) [/itex].
 
  • #7
dx said:
No. The zero ket is the zero vector in the state space. [tex] |0\rangle [/tex] is not the zero vector, it's just the vector with eigenvalue [itex] \hbar \omega ( 0 + \frac{1}{2}) [/itex].

Oh, got it :)
 
  • #8
Or better yet, a|0> = null vector.
 
  • #9
Yes. The thing to remember is that all physical states must be normalizable. So

<0|0> = 1
 
  • #10
and what about [tex]\hat{N}|0\rangle[/tex], where [tex]\hat{N}=\hat{a}^\dagger\hat{a}[/tex] is the number operator? Should it be

[tex]\hat{N}|0\rangle = 0|0\rangle = 0 [/tex] (number) ?
 
  • #11
KFC said:
and what about [tex]\hat{N}|0\rangle[/tex], where [tex]\hat{N}=\hat{a}^\dagger\hat{a}[/tex] is the number operator? Should it be

[tex]\hat{N}|0\rangle = 0|0\rangle = 0 [/tex] (number) ?

Technically speaking, it is the null vector.
 

FAQ: Ladder Operator for Harmonic Oscillator: a|0> = |0>

1. What is a ladder operator for a harmonic oscillator?

A ladder operator for a harmonic oscillator is a mathematical tool used in quantum mechanics to describe the energy levels and transitions of a quantum system. It allows for the creation and annihilation of energy quanta, or "quanta of action", which are responsible for the discrete energy levels observed in quantum systems.

2. How does a ladder operator work?

A ladder operator works by acting on a quantum state to either increase or decrease its energy level by a fixed amount. In the case of a harmonic oscillator, the ladder operator "a" increases the energy by one quantum, while its conjugate "a†" decreases the energy by one quantum.

3. What is the significance of the ladder operator for a harmonic oscillator?

The ladder operator for a harmonic oscillator is significant because it allows for a simple and elegant description of the energy levels and transitions in a quantum system. It also provides a way to calculate the probabilities of different energy states and transitions between them.

4. How is the ladder operator related to the Heisenberg uncertainty principle?

The ladder operator for a harmonic oscillator is related to the Heisenberg uncertainty principle through the commutation relation between the position and momentum operators. This relation shows that it is impossible to simultaneously know the exact position and momentum of a quantum particle, and the ladder operator is a mathematical representation of this uncertainty.

5. Can the ladder operator be applied to other quantum systems?

Yes, the ladder operator can be applied to other quantum systems besides the harmonic oscillator. It can be used to describe the energy levels and transitions in any system that exhibits discrete energy levels, such as atoms or molecules. However, the specific form of the ladder operator may differ depending on the system being studied.

Back
Top