We derive simple expressions for the energy corrections to the Born-Oppenheimer approximation valid for a harmonic oscillator. We apply these corrections to the electronic and rotational ground state of H2+ and show that the diabatic energy corrections are linearly dependent on the vibrational quantum numbers as seen in recent variational calculations [D. A. Kohl and E. J. Shipsey, J. Chem. Phys. 84, 2707 (1986)].PACS number(s): 31.30.i, 03.65.GeIn this paper, we derive rather simple formulas for the wave-functions and energy corrections to the Born-Oppenheimer approximation for a harmonic oscillator.We derive a coupled pair of equations for these corrections. These equations are valid to first order in the particle-to-oscillator mass ratio m/M and are the timeindependent analog to the time-dependent equations for a forced oscillator. Such time-dependent treatments have recently been described for a particle in a box with oscillating walls (the quantum Fermi accelerator) [1,2] and a particle in a harmonic potential with an oscillating spring constant [3]. For slow oscillations compared to the particle motion, this paper describes the corresponding timeindependent treatment for the coupling between the particle and oscillator, which is ignored in the Born-Oppenheimer approximation.Our wave functions may be derived from a recent work by Babb and Dalgarno [4] if one applies their diabatic coupling operators to a harmonic-oscillator basis. However, we give here an independent derivation for both wave functions and energies in a harmonic-oscillator basis that simplifies the results in Ref. [4] and that shows an important connection between time-dependent and -independent perturbation theory.Our theory is particularly useful for describing the electronic-vibrational coupling in molecules and solids. To show its usefulness, we apply it to vibrational states of the H2+ electronic and rotational ground state. Recently, Kohl and Shipsey [5] have shown from a variational treatment that the diabatic energy corrections to the H2 electronic ground states are linearly dependent on the vibrational quantum number n (at least up to n =2). This behavior is shown to be a direct result of our treatment and is seen in other variational studies as well [6 -8]. Let us first consider the standard treatment of Hz+ in the Born-Oppenheimer approximation.For simplicity, we shall assume that the center of mass is between the two nuclei and shall ignore the mass corrections that give the proper dissociation energy [9]. Our interest here is in the vibrationally dependent diabatic corrections that are more difficult to obtain. Because the electron moves much faster than the nucleus, we may consider the nuclei to be fixed with internuclear distance R = IRI in order to determine the electron wave function. If r is the position of the electron relative to the center of mass, we may write the total wave function as a product of the electron wave function hatt(r, R ) and nuclear wave function p(R), or (T, + V, )f; =W;(R)Q;,where T, is the kineti...