Why Must the Expectation Value of Momentum Squared Be Strictly Positive?

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SUMMARY

The expectation value of momentum squared, denoted as \(\langle p^2 \rangle\), must be strictly positive for all normalized wavefunctions in quantum mechanics. This is established through the operator \(p = -i\hbar \frac{d}{dx}\), which is Hermitian, ensuring that \(\langle \psi | p^2 | \psi \rangle \geq 0\). The strict inequality arises because if \(\langle \psi | p^2 | \psi \rangle = 0\), the wavefunction \(\psi\) would not be normalizable, leading to a contradiction in the context of quantum mechanics.

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  • Understanding of quantum mechanics principles, particularly wavefunctions and operators.
  • Familiarity with Hermitian operators and their properties.
  • Knowledge of normalization conditions for wavefunctions.
  • Basic calculus, specifically differentiation and inner product spaces.
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  • Study the properties of Hermitian operators in quantum mechanics.
  • Learn about normalization conditions and their implications for wavefunctions.
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Homework Statement


Why is [itex]\langle p^2\rangle >0[/itex] where [itex]p=-i\hbar{d\over dx}[/itex], (noting the ***strict*** inequality) for all normalized wavefunctions? I would have argued that because we can't have [itex]\psi=[/itex]constant, but then I thought that we can normalize such a wavefunction by using periodic boundary conditions... So I don't how to argue that the inequality should be strict... Is it that otherwise it would be trivial?


Homework Equations


[itex]p=-i\hbar{d\over dx}[/itex]


The Attempt at a Solution


clearly, [itex]\langle \psi|p^2|\psi\rangle = \langle p\psi|p\psi\rangle \geq 0[/itex] since p is Hermitian. But why the strict inequality??
 
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When would that inner product with zero? and what would happen then? ;)
 
Well, if there exists [itex]\psi \in D(p)[/itex], so that [itex]\langle \psi,p^2 \psi\rangle[/itex] = 0, then [itex]||p\psi||[/itex] has 0 norm. Which vector has 0 norm ? Is it normalizable ?
 

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