Quantum Physics For Dummies

Quantum Physics and the Hamiltonian

One of the central problems of quantum mechanics is to calculate the energy levels of a system. The energy operator, called the Hamiltonian, abbreviated H, gives you the total energy. Finding the energy levels of a system breaks down to finding the eigenvalues of the problem

The same equation in matrix terms looks like this:

Quantum Physics and the Heisenberg Uncertainty Principle

In quantum physics, you encounter the Heisenberg uncertainty principle, which says that the better you know the position of a particle, the less you know the momentum, and vice versa. In the x direction, for example, that looks like this:

where Dx is the measurement uncertainty in the particle’s x position, Dp_x is its measurement uncertainty in its momentum in the x direction, and

This relation holds for all three dimensions:

Quantum Physics and the Schrödinger Equation

In quantum physics, the Schrödinger equation describes the energies and probable locations of electrons. Much of quantum physics is largely about solving this differential equation for a variety of potentials, V(r):

The Schrödinger equation work in three dimensions as well:

Spin Operators and Commutation in Quantum Physics

Don’t think quantum physics is devoid of anything but dry science. The fact is that it’s full of relationships, they’re just commutation relationships — which are pretty dry science after all. In any case, among the angular momentum operators L_x, L_y, and L_z, are these commutation relations:

All the orbital angular momentum operators, such as L_x, L_y, and L_z, have analogous spin operators: S_x, S_y, and S_z. And the commutation relations work the same way for spin:

Quantum Physics and the Compton Effect

In quantum physics, you may deal with the Compton effect of X-ray and gamma ray qualities in matter. To calculate these effects, use the following formula, which assumes that the light is represented by a photon with energy E = hu and that its momentum is p = E/c: