Introduction to Quantum Mechanics · Problem 3.37

Formalism — David J. Griffiths

Physics — Quantum Mechanics · virial_theorem

Problem

Virial theorem. Use Equation 3.73 to show that ddt⟨xp⟩=2⟨T⟩−⟨x∂V∂x⟩,(3.112)\frac{d}{dt}\langle xp \rangle = 2\langle T \rangle - \left\langle x \frac{\partial V}{\partial x} \right\rangle, \tag{3.112} where TT is the kinetic energy (H=T+VH = T + V). In a stationary state the left side is zero (why?) so 2⟨T⟩=⟨xdVdx⟩.(3.113)2\langle T \rangle = \left\langle x \frac{dV}{dx} \right\rangle. \tag{3.113} This is called the virial theorem. Use it to prove that ⟨T⟩=⟨V⟩\langle T \rangle = \langle V \rangle for stationary states of the harmonic oscillator, and check that this is consistent with the results you got in Problems 2.11 and 2.12.

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