3. Introduction
• The quantum harmonic oscillator is the
quantum-mechanical analog of the classical harmonic
oscillator.
• Quantum harmonic oscillator provides a useful model for
a variety of vibrational phenomena that are encountered
for instance in classical mechanics, electrodynamics,
statistical mechanics, solid state, atomic, nuclear, and
particle physics.
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4. Classical Harmonic Oscillator
Figure 1: Classical Harmonic Oscillator Oscillator
source: https://www.shutterstock.com
This system exhibits sinusoidal behavior. From Hook’s law,
the mathematical expression for the restoring force is,
F = −kx (1)
3
5. Totle Energy of the system
Figure 2: Classical hormonic oscillator
source: https://images.app.goo.gl/pN7ibGogwmQbKCwM7
The kinetic energy,
T =
1
2
mv2
0 cos2
r
k
m
t
!
(2)
4
6. Total Energy of the system
The potential energy of the system is,
V =
1
2
mv2
0 sin2
r
k
m
t
!
(3)
then the total energy of the system is,
E =
1
2
mv2
0 (4)
The total energy of the classical harmonic oscillator is a
constant value, which depends on v0 that can be any number.
But it is not the case for quantum harmonic oscillator.
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8. Quantum Harmonic Oscillator
The Hamiltonian of a particle is,
Ĥ =
1
2m
p̂2
+ (mwx)2
(5)
To find the energy eigenvalues and eigenstates of this
Hamiltonian we can use two methods,
• Analytic method
• Ladder or Algebraic method
Then slove the time independent Schrodinger equation,
−
ℏ2
2m
d2
ψ
dx2
+
1
2
mω2
x2
ψ = Eψ (6)
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9. Quantum Harmonic Oscillator
By analytic method get the wave function,
Ψn(x) =
1
p√
π2nn!x0
e−x2/2x2
0 Hn
x
x0
(7)
where Hn are nth
order polynomials called Hermite polynomials.
Hn(y) = (−1)n
ey2 dn
dyn
e−y2
(8)
The energy levels of the quantum harmonic oscillator are,
E =
n +
1
2
ℏω (9)
where (n = 0, 1, 2, 3....)
The above equation represents lowest allowed energy range.
8
10. Energy states of different particle or molecules
Figure 4: Energy states of different particle or molecules
9
11. Probability distribution
Figure 5: Probability distributionsource : http://hyperphysics
The solution of the Schrodinger equation for the quantum
harmonic oscillator gives the probability distributions for the
quantum states of the oscillator.
10
16. Molecular vibration
The energy levels are quantized at equally spaced values.the
angular frequency is given by,
ω =
s
k
µ
where µ =
m1m2
m1 + m2
is the reduced mass and m1 and m2 are
the masses of the two atoms and k is bond force constant.
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17. Molecular vibration
• This form of the frequency is the same as that for the
classical simple harmonic oscillator.
• The transition energy is nearly equal to ℏω
• The most surprising difference for the quantum case is
called ”zero-point vibration” of the n=0 ground state.
This implies that molecules are not completely at rest,
even at absolute zero temperature.
16
18. Conclusion
• The quantum harmonic oscillator is one of the foundation
problems of quantum mechanics.
• Is the foundation for the understanding of complex modes
of vibration in larger molecules, the motion of atoms in a
solid lattice etc.
17
19. Reference
Books
• Griffiths, David J. (2004). Introduction to Quantum
Mechanics (2nd ed.). Prentice Hall. ISBN
978-0-13-805326-0.
• Zettili, N. (2003). Quantum mechanics: concepts and
applications.
Online sources
• https://blog.cupcakephysics.com/thermodynamics
• ”Quantum Harmonic Oscillator”. Hyperphysics.
Retrieved 24 September 2009
• https://blog.cupcakephysics.com/thermodynamics
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