15.4 The Quantum Harmonic Oscillator 679
EXAMPLE15.7
Find the classical amplitude of vibration of a hydrogen molecule with an energy equal to that
of thev0 quantum state. Express it as a percentage of the bond length, 0. 74 × 10 −^10 m.
The force constantkis equal to 576 N m−^1 and the reduced mass is equal to 8. 363 × 10 −^28 kg
(half the mass of a hydrogen nucleus).
Solution
From Table A.22 of Appendix A, the frequency of vibration is
ν(4401.2cm−^1 )(2. 9979 × 1010 cm s−^1 ) 1. 319 × 1014 s−^1
For thev0 state,
E 1
1
2
hv
1
2
(6. 6261 × 10 −^34 J s)(1. 319 × 1014 s−^1 ) 4. 371 × 10 −^20 J
The amplitude of oscillation corresponds to
Vmax
1
2
kx^2 tE
wherextis the value ofxat the turning point.
xt
√
2 E
k
(
2(4. 371 × 10 −^20 J)
576 N m−^1
) 1 / 2
1. 23 × 10 −^11 m
This value is 16.6% of the bond length.
PROBLEMS
Section 15.4: The Quantum Harmonic Oscillator
15.19a.Construct an accurate graph of thev2 wave
function of a harmonic oscillator as a function of
√
ax.
b.Express the value of the wave function at the turning
point in terms of the parametera.
c.Ifmis equal tomp/2, the reduced mass of the H 2
molecule, and ifk 574 .75 N m−^1 , the value for the
H 2 molecule, find the value ofψ 22 at the turning point.
Express your value forψ^22 in m−^1 and in
Å
− 1
(1 Å 10 −^10 m).
15.20a.Construct an accurate graph of thev3 wave
function of a harmonic oscillator as a function of
√
ax.
b.Find the value of the wave function at the turning
point.
15.21Using the recursion relation, Eq. (15.4-6), obtain the
unnormalized energy eigenfunctionsψ 4 andψ 5 for the
harmonic oscillator.
15.22 a.Sketch a graph of the product ofψ 0 andψ 1 , the first
two energy eigenfunctions of a harmonic oscillator
and argue from the graph that the two functions are
orthogonal, which means for these real functions
that
∫∞
−∞
ψ 1 (x)ψ 2 (x)dx 0
b.Work out the integral and show thatψ 0 andψ 1 are
orthogonal.
15.23 a.Construct an accurate graph ofψ^22 , the square of the
third energy eigenfunction of the harmonic
oscillator.
b.Find the locations of the relative maxima and minima
inψ^22 in terms of the parametera.
c.Express the locations of the relative maxima as
fractions of the classical turning point for the energy
corresponding to this energy eigenfunction.