For a one-dimensional quantum harmonic oscillator with frequency $\nu$, the total energy in the ground state (n=0) is given by the formula: $E_0 = \frac{1}{2}h\nu$ where $h$ is the Planck constant.
A key result for the harmonic oscillator potential ($V(x) = \frac{1}{2}kx^2$) is derived from the Virial Theorem. It states that the average kinetic energy ($\langle K \rangle$) is equal to the average potential energy ($\langle V \rangle$) over any energy eigenstate.
The total energy $E_0$ is the sum of the average kinetic and potential energies: $E_0 = \langle K \rangle + \langle V \rangle$
Substituting $\langle K \rangle = \langle V \rangle$ into the energy equation, we get: $E_0 = 2 \langle V \rangle$
Therefore, the average potential energy in the ground state is: $\langle V \rangle_0 = \frac{E_0}{2} = \frac{1}{2} \left( \frac{1}{2}h\nu \right) = \frac{h\nu}{4}$
Because $\langle K \rangle = \langle V \rangle$, the average kinetic energy in the ground state is also: $\langle K \rangle_0 = \frac{h\nu}{4}$
The average kinetic energy and the average potential energy for a one-dimensional harmonic oscillator in its ground state are both $\frac{h\nu}{4}$.
This matches the values stated in Option 3.
The lowest energy of a quantum mechanical one-dimensional simple harmonic oscillator is $300$ cm$^{-1}$. The energy (in cm$^{-1}$) of the next higher level is _________________