Expectation value of kinetic energy operator

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SUMMARY

The expectation value of the kinetic energy operator in the ground state wave function ##\psi_0## is calculated using the formula $$<\psi_0|\frac{\hat{p^2}}{2m}|\psi_0>$$, resulting in a value of $$\frac{\hbar w}{4}$$. This calculation involves the operators ##\hat{a}## and ##\hat{a^{\dagger}}##, demonstrating that both kinetic and potential energy are equally distributed between the ground state and excited states, aligning with classical mechanics principles. The analysis confirms that the kinetic energy in quantum mechanics mirrors classical expectations, specifically that energy is divided equally between kinetic and potential forms.

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The expectation value of the kinetic energy operator in the ground state ##\psi_0## is given by
$$<\psi_0|\frac{\hat{p^2}}{2m}|\psi_0>$$
$$=<\psi_0|\frac{1}{2m}\Big(-i\sqrt{\frac{\hbar mw}{2}}(\hat{a}-\hat{a^{\dagger}})\Big)^2|\psi_0>$$
$$=\frac{-\hbar w}{4}<\psi_0|\hat{a}^2+-\hat{a}\hat{a^{\dagger}}-\hat{a^{\dagger}}\hat{a}+\hat{a^{\dagger}}^2|\psi_0>$$
$$=\frac{-\hbar w}{4}<\psi_0|\Big(\hat{a}^2|\psi_0>-\hat{a}\hat{a^{\dagger}}|\psi_0>-\hat{a^{\dagger}}\hat{a}|\psi_0>+\hat{a^{\dagger}}^2|\psi_0>\Big)$$
$$=\frac{-\hbar w}{4}<\psi_0|\Big(|-\psi_0>+\sqrt{2}|\psi_2>\Big)$$
$$=\frac{-\hbar w}{4}<-\psi_0|\psi_0>+<\psi_0|\psi_2>$$

$$=\frac{\hbar w}{4}$$
 
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So we know for ground state energy as well as excited states energy kinetic energy and potential energy are half and half. That coincide with classical mechanics.
 
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