Expected Values in a Harmonic Oscillator

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SUMMARY

The discussion focuses on proving that in the nth state of a harmonic oscillator, the expected values satisfy the equations \(\langle x^2 \rangle = (\Delta x)^2\) and \(\langle p^2 \rangle = (\Delta p)^2\). It is established that \(\langle x \rangle = 0\) due to the even parity of the probability density function. The relationship \((\Delta x)^2 = \langle x^2 \rangle - \langle x \rangle^2\) simplifies to \((\Delta x)^2 = \langle x^2 \rangle\) when substituting \(\langle x \rangle = 0\). The discussion also suggests using raising and lowering operators to further analyze the expected values.

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  • Understanding of quantum mechanics principles, particularly harmonic oscillators
  • Familiarity with the concepts of expected values and uncertainty in quantum systems
  • Knowledge of raising and lowering operators in quantum mechanics
  • Basic proficiency in mathematical notation used in quantum physics
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Domnu
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Problem
Show that in the [tex]n[/tex]th state of the harmonic oscillator


[tex]\langle x^2 \rangle = (\Delta x)^2[/tex]
[tex]\langle p^2 \rangle = (\Delta p)^2[/tex]​

Solution
This seems too simple... I'm not sure if it's correct...

It is obvious that [tex]\langle x \rangle = 0[/tex]... this is true because the parity of the square of the eigenfunction is [tex]1[/tex] (in other words, the probabiliity density is an even function). Now, we know that [tex](\Delta x)^2 = \langle x^2 \rangle - \langle x \rangle ^2[/tex], but [tex]\langle x \rangle = 0[/tex], so by substitution, the desired result follows. A similar argument can be made for the momentum. [tex]\blacksquare[/tex]
 
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You can always explicitly show that <x> = 0 in the nth state if you feel you need to show more work.

To get started try representing x in terms of the raising and lowering operators in the following line, letting the operators act on any kets to their right, and simplifying:

<n|x|n> = ... |n> is the eigenket for the nth eigenstate.You should end up with delta functions that have to be zero.
 

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