Quantum Griffiths Example

In summary, to find the expectation value of potential energy in the nth state of the harmonic oscillator, you can use the equations a_{\pm}=1/Sqrt[2hmw](\mpip+mwx) and define constants A and B as a_{\pm}=Ap\mp Bx. By solving these equations simultaneously and simplifying with the defined constants, you can easily calculate the expectation value.
  • #1
kuahji
394
2
Find the expectation value of the potential energy in the nth state of the harmonic oscillator.

This is his example 2.5 in the book, he uses a[itex]\pm[/itex]=1/Sqrt[2hmw]([itex]\mp[/itex]ip+mwx) to get x=Sqrt[h/2mw](a[itex]_{+}[/itex]+a[itex]_{-}[/itex])

My question how does he do this? I can't seem to make the algebraic manipulations to get it into that form to follow out his example.
 
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  • #2
You have two equations, one for [itex]a_+[/itex] and one for [itex]a_-[/itex].

All you have to do is solve them simultaneously for x and p. i.e. Solve one for x, solve the other for p, plug the first into the second, etc. etc.

It may help to simplify things by defining some constants A and B such that:

[tex]a_{\pm}=Ap\mp Bx[/tex]
 
  • #3
That was easy enough, thank you for the tip!
 
  • #4
No problem! :smile:
 
  • #5


The expectation value of the potential energy in the nth state of the harmonic oscillator can be calculated using the Schrödinger equation and the Hamiltonian operator. However, in this specific example, Griffiths uses the creation and annihilation operators, a+ and a-, to simplify the calculations.

To understand how he arrives at the expression x=Sqrt[h/2mw](a_{+}+a_{-}), we need to look at the definitions of these operators. The creation operator, a+, is defined as a linear combination of the position and momentum operators:

a_{+}=\sqrt{\frac{m\omega}{2\hbar}}(x+\frac{i}{m\omega}p)

Similarly, the annihilation operator, a-, is defined as:

a_{-}=\sqrt{\frac{m\omega}{2\hbar}}(x-\frac{i}{m\omega}p)

Substituting these definitions into the expression for x, we get:

x=\frac{1}{2}\sqrt{\frac{2\hbar}{m\omega}}(a_{+}+a_{-})

Simplifying further, we get:

x=\sqrt{\frac{\hbar}{2m\omega}}(a_{+}+a_{-})

Therefore, the expectation value of the potential energy in the nth state can be calculated as:

<V>=\frac{1}{2}m\omega^{2}<x^{2}>=\frac{\hbar\omega}{4}(<a_{+}^{2}>+<a_{-}^{2}>+2<a_{+}a_{-}>)

Using the commutation relation for these operators, we can simplify this expression to:

<V>=\frac{\hbar\omega}{4}(2n+1)

This is the final expression for the expectation value of potential energy in the nth state of the harmonic oscillator, which can be obtained using the creation and annihilation operators.
 

Related to Quantum Griffiths Example

1. What is a Quantum Griffiths Example?

A Quantum Griffiths Example is a theoretical model used to study the behavior of quantum disordered systems. It involves the interaction between quantum particles and a disordered environment, leading to the emergence of new properties and phenomena.

2. How is a Quantum Griffiths Example different from a classical Griffiths Example?

A Quantum Griffiths Example takes into account the effects of quantum mechanics, whereas a classical Griffiths Example only considers classical mechanics. This leads to different behaviors and properties in the two systems.

3. What are some real-world applications of Quantum Griffiths Examples?

Quantum Griffiths Examples have been used to study the properties of superconductors, quantum magnets, and other materials with quantum disorder. They also have potential applications in quantum computing and information processing.

4. How does disorder affect the behavior of a Quantum Griffiths Example?

The disorder in a Quantum Griffiths Example can lead to the emergence of new phases and critical points, as well as modify the properties of existing phases. It can also affect the dynamics and transport of quantum particles in the system.

5. What are the current challenges in studying Quantum Griffiths Examples?

One of the main challenges is developing accurate theoretical models that can capture the complex interplay between quantum particles and disorder. Another challenge is finding experimental systems that exhibit the necessary conditions for a Quantum Griffiths Example to occur.

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