Study Notes On Simple Harmonic Oscillator
One-Dimensional Simple Harmonic Oscillator:
A diatomic vibration molecule can be represented with the help of a simple model which is known as a simple harmonic oscillator (S.H.O). The force that acts on the molecule is given by:
f=kx
Here, x is the displacement from the equilibrium position and k is the force constant.
The expression of potential energy V(x) is given by:
Here, m1 and m2 are the atomic masses of the two atoms.
By using the expression of potential energy given in Equation (1), for one-dimensional S.H.O., the Schrodinger equation can be represented as:
Equation (11) is identical in form to a well-known second-order differential equation, called the Hermite equation, that is:
The Hermite equation has solutions which depend upon the value of n.
The Hermite Polynomial having degree n can be defined as:
The energy of S.H.O.: On comparing equations (11) and (12), the energy of the S.H.O. can be obtained.
It has been found out that:
α/β = 2n + 1 …(15)
Substituting for α and β Equation (7),
Or …(17)
From Equation (2),
(k /m)1/2 = 2π …(18)
Combining Equations (17) and (18),
This energy is called the zero-point energy of the oscillator. Classical mechanics predicts that the zero-point energy of the oscillator is zero while quantum mechanics predicts that the zero-point energy is non-zero.
The occurrence of the zero-point energy is consistent with the Heisenberg uncertainty principle.
Graph of the wave function and probability:
Degeneracy for a 2-D harmonic oscillator:
The energy, E = Ex + Ey
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