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Harmonic Oscillator Family

The harmonic oscillator is an exact model of a quadratic potential and a useful approximation near a stable minimum. It connects differential equations to ladder-operator algebra and provides simple examples of number states, coherent packets, squeezing, and collective normal modes.

For H=P2/(2m)+mω2X2/2H=P^2/(2m)+m\omega^2X^2/2 with ω>0\omega>0,

En=ℏω(n+1/2),n=0,1,2,…,ℓ=ℏmω.E_n=\hbar\omega(n+1/2),\qquad n=0,1,2,\ldots, \qquad \ell=\sqrt{\frac{\hbar}{m\omega}}.

The differential-equation method imposes normalizability on a Gaussian times a Hermite polynomial. The ladder method writes H=ℏω(a†a+1/2)H=\hbar\omega(a^\dagger a+1/2) and builds excited states from a∣0⟩=0a\lvert0\rangle=0. Both solve the same problem and expose different useful features.

The ground-state position width is ℓ/2\ell/\sqrt2, not ℓ\ell. Its nonzero energy and momentum spread do not imply a hidden classical orbit. A number-state density is stationary; a coherent-state center oscillates while its Gaussian width stays fixed under the ideal harmonic Hamiltonian.

Displacement moves the center of a Gaussian state. Squeezing changes its covariance, narrowing one quadrature while widening a conjugate one. An ideal displaced squeezed vacuum remains a pure superposition of number states, not an incoherent mixture. For a rotated squeezing ellipse, the position–momentum covariance must be included in the strengthened uncertainty relation.

Page Central question
Quantum Harmonic Oscillator What are the model, natural scales, spectrum, and eigenstates?
Differential-Equation Solution How does normalizability produce Hermite functions and quantized energy?
Ladder-Operator Solution: First Encounter How do commutators and a lowest state generate the spectrum?
Hermite Functions Which normalized functions, recurrences, and transform identities represent number states?
Zero-Point Energy Why can the oscillator not occupy the classical minimum with zero energy?
Number States What does oscillator excitation number count, and how do ladders act?
Coherent States Which Gaussian packet preserves shape while its center follows classical motion?
Squeezed States: First Encounter How can one quadrature be narrowed without violating uncertainty?
Displaced Oscillator What changes when a static linear force moves the equilibrium?
Coupled Oscillators: First Encounter How do interacting quadratic coordinates become independent collective modes?
Oscillator as a Universal Local Model Why and when is a stable system locally harmonic?

Learn one complete solution method first, then compare it with the other. Continue from number states to coherent and squeezed states, or from a displaced oscillator to coupled oscillators and normal modes.

The local oscillator approximation requires positive curvature and states concentrated in the nearly quadratic region. Flat minima, unstable directions, high excitations, and separated wells need additional terms or methods. For many-mode occupation language, continue to many-body quantum mechanics; a single trapped particle’s ladder operator changes its excitation level, not its particle number.

Hold the potential curvature K=mω2K=m\omega^2 fixed and multiply mm by four. How do the frequency, level spacing, and ground-state position width change?

Solution

ω=K/m\omega=\sqrt{K/m} and ℏω\hbar\omega are halved. The length ℓ=(ℏ2/(mK))1/4\ell=(\hbar^2/(mK))^{1/4} and width ℓ/2\ell/\sqrt2 are divided by 2\sqrt2. This differs from changing mass at fixed frequency, where the width is halved because the curvature changes too.

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