QM · Ch 3 · Square-well uncertainty product σ_x σ_p

Physics · Quantum Mechanics · Griffiths Ch 3

Problem

For a particle in the 1D infinite square well of width aa in the ground state ψ1(x)=2/asin⁡(πx/a)\psi_1(x) = \sqrt{2/a}\sin(\pi x/a), compute σx\sigma_x and σp\sigma_p, then form σxσp\sigma_x\sigma_p and compare with ℏ/2\hbar/2.
Intuitive explanation

The uncertainty principle isn't just a limit—it's a measurable consequence of how wave functions are shaped. Here, you'll calculate how "spread out" the particle's position and momentum are around their average values, then see that the ground state's compact, smooth shape naturally produces an uncertainty product right at the quantum limit. The key is recognizing that σx\sigma_x and σp\sigma_p both follow from integrals of the probability density ∣ψ∣2|\psi|^2, and the ground state's single hump minimizes their product.

Intuitive explanation

The uncertainty principle isn't just a limit—it's a measurable consequence of how wave functions are shaped. Here, you'll calculate how "spread out" the particle's position and momentum are around their average values, then see that the ground state's compact, smooth shape naturally produces an uncertainty product right at the quantum limit. The key is recognizing that σx\sigma_x and σp\sigma_p both follow from integrals of the probability density ∣ψ∣2|\psi|^2, and the ground state's single hump minimizes their product.

Related theory

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