Principles of Quantum Mechanics · Problem 7.3.1

The Harmonic Oscillator — R. Shankar

Physics — Quantum Mechanics · harmonic-oscillator-power-series

Problem

∗^* Consider the question why we tried a power-series solution for Eq. (7.3.11) but not Eq. (7.3.8). By feeding in a series into the latter, verify that a three-term recursion relation between Cn+2C_{n+2}, CnC_n, and Cn−2C_{n-2} obtains, from which the solution does not follow so readily. The problem is that ψ′′\psi'' has two powers of yy less than 2εψ2\varepsilon\psi, while the −2yu′-2yu' piece has two more powers of yy. In Eq. (7.3.11) on the other hand, of the three pieces u′′u'', −2yu′-2yu', and (2ε−1)u(2\varepsilon-1)u, the last two have the same powers of yy.
Intuitive explanation

The key insight is recognizing why power-series solutions work better for some differential equations than others: you need the dominant terms to have matching powers of yy so they can be collected and balanced together. In Eq. (7.3.8), the ψ′′\psi'' and −2yu′-2yu' terms differ by two powers of yy, creating a three-term recursion that couples non-adjacent coefficients—much harder to solve. By contrast, Eq. (7.3.11) has −2yu′-2yu' and (2ε−1)u(2\varepsilon-1)u at the same order, yielding a two-term recursion that closes neatly. This structural difference determines whether the series ansatz leads to a solvable recurrence.

Intuitive explanation

The key insight is recognizing why power-series solutions work better for some differential equations than others: you need the dominant terms to have matching powers of yy so they can be collected and balanced together. In Eq. (7.3.8), the ψ′′\psi'' and −2yu′-2yu' terms differ by two powers of yy, creating a three-term recursion that couples non-adjacent coefficients—much harder to solve. By contrast, Eq. (7.3.11) has −2yu′-2yu' and (2ε−1)u(2\varepsilon-1)u at the same order, yielding a two-term recursion that closes neatly. This structural difference determines whether the series ansatz leads to a solvable recurrence.

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